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    <subfield code="a">An interaction potential energy between and adsorbate (Xe and Ar) and the 10-fold Al-Ni-Co quasicrystal is computed by summing over all adsorbate-substrate interatomic interactions. The quasicrystal atoms' coordinates are obtained from LEED experiments and the Lennard-Jones parameters of Xe-Al, Xe-Ni and Xe-Co are found using semiempirical combining rules. The resulting potential energy function of position is highly corrugated. Monolayer adsorption of Xe and Ar on the quasicrystal surface is investigated in two cases: 1) in the limit of low coverage (Henry's law regime), and 2) at somewhat larger coverage, when interactions between adatoms are considered through the second virial coefficient, C_{AAS}. A comparison with adsorption on a flat surface indicates that the corrugation enhances the effect on Xe-Xe (Ar-Ar) interactions. The theoretical results for the low coverage adsorption regime are compared to experimental (LEED isobar) data.</subfield>
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    <subfield code="a">Recent studies of DNA sequence of letters A, C, G and T exhibit the inverse power law form frequency spectrum. Inverse power-law form of the power spectra of fractal space-time fluctuations is generic to the dynamical systems in nature and is identified as self-organized criticality. In this study it is shown that the power spectra of the frequency distributions of bases C+G in the Human chromosome X DNA exhibit self-organized criticality. DNA is a quasicrystal possessing maximum packing efficiency in a hierarchy of spirals or loops. Self-organized criticality implies that non-coding introns may not be redundant, but serve to organize the effective functioning of the coding exons in the DNA molecule as a complete unit.</subfield>
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    <subfield code="a">Model sets play a fundamental role in structure analysis of quasicrystals. The diffraction diagram of a quasicrystal admits as symmetry group a finite group G, and there is a G-cluster C (union of orbits of G) such that the quasicrystal can be regarded as a quasiperiodic packing of interpenetrating copies of C. We present an algorithm which leads from any G-cluster C directly to a multi-component model set Q such that the arithmetic neighbours of any point x belonging to Q are distributed on the sites of the translated copy x+C of C. Our mathematical algorithm may be useful in quasicrystal physics.</subfield>
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    <subfield code="a">First-principles prediction of a decagonal quasicrystal containing boron</subfield>
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    <subfield code="a">We interpret experimentally known B-Mg-Ru crystals as quasicrystal approximants. These approximant structures imply a deterministic decoration of tiles by atoms that can be extended quasiperiodically. Experimentally observed structural disorder corresponds to phason (tile flip) fluctuations. First-principles total energy calculations reveal that many distinct tilings lie close to stability at low temperatures. Transfer matrix calculations based on these energies suggest a phase transition from a crystalline state at low temperatures to a high temperature state characterized by tile fluctuations. We predict B$_{38}$Mg$_{17}$Ru$_{45}$ forms a decagonal quasicrystal that is metastable at low temperatures and may be thermodynamically stable at high temperatures.</subfield>
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    <subfield code="a">The nearly dispersionless, so-called ``optical'' vibrational modes observed by inelastic neutron scattering from icosahedral Al-Pd-Mn and Zn-Mg-Y quasicrystals are interpreted as modes of a continuum elastic sphere that has the same diameter as the corresponding icosahedral nanoclusters. When the sphere is considered as free, most of the experimentally found modes can be accounted for, in both systems. Taking into account the mechanical connection between the clusters and the remainder of the quasicrystal allows a complete assignment of all optical modes in the case of Al-Pd-Mn.</subfield>
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    <subfield code="a">In this thesis, studies which concern two different subjects related to phase transitions in fluids and crystalline solids are presented. Condensed matter formation, structure, and phase transitions are modeled using molecular dynamics simulations of simple discontinuous potentials with attractive and repulsive interactions. Novel phase diagrams are proposed for quasicrystals, crystals, and liquids. In the first part of the thesis, the formation of a quasicrystal in a two dimensional monodisperse system is investigated using molecular dynamics simulations of hard sphere particles interacting via a two-dimensional square-well potential. It is found that for certain values of the square-well parameters more than one stable crystalline phase can form. By quenching the liquid phase at a very low temperature, an amorphous phase is obtained. When this the amorphous phase is heated, a quasicrystalline structure with five-fold symmetry forms. From estimations of the Helmholtz potentials of the stable crystalline phases and of the quasicrystal, it is concluded that within a specific temperature range, the observed quasicrystal phase can be the stable phase. The second part of the thesis concerns a study of the liquid-liquid phase transition for a single-component system in three dimensions, interacting via an isotropic potential with a repulsive soft-core shoulder at short distance and an attractive well at an intermediate distance. The potential is similar to potentials used to describe such liquid systems as colloids, protein solutions, or liquid metals. It is shown that the phase diagram for such a potential can have two lines of first- order fluid-fluid phase transitions: one separating a gas and a low-density liquid (LDL), and another between the LDL and a high-density liquid (HDL). Both phase transition lines end in a critical point, a gas-LDL critical point and, depending on the potential parameters, either a gas-HDL critical point or a LDL-HDL critical point. A systematic study through varying potential parameters is carried out to determine the influence of attractive and repulsive interactions on the formation and stability of the liquid-liquid phase transitions and the two fluid critical points. No hints of the density anomaly are found, suggesting that the absence of the density anomaly, such as the one found in water, is independent of the choice of the parameters and that the liquid-liquid phase transition and density anomaly are not directly related.</subfield>
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    <subfield code="a">We present new results on the separation of the atomic-partial vibrational density of states for the ternary quasicrystal i-Al sub 6 sub 2 Cu sub 2 sub 5 sub . sub 5 Fe sub 1 sub 2 sub . sub 5. The decomposition into three atomic-partial functions, Al-, Cu- and Fe-g(E), has been performed self-consistently with the calculation of the multi-phonon contributions. The results show the surprising result that both Cu- and Fe-g(E) are strongly peaked. The low-energy regions of Al- and Cu-g(E) show strong deviations from Debye behaviour due to the presence of non-propagating low-energy vibrational states. (orig.)</subfield>
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    <subfield code="a">In the review the basis theoretical principles of EXAFS spectroscopy are given, as one of principal directions of an absorption spectroscopy permitting with a high accuracy to gain parameters of the short-range order in multicomponent amorphous and quasi-crystal mediums. The methods of the analysis of EXAFS spectra with allowance of effects of multiply scattering are featured. The exposition of the experimental set-ups, which realize the method of EXAFS spectroscopy on beams of SR, requirement of the monochromatization of radiation beams are given. For investigation of phase transition and external effects the energy-dispersive EXAFS spectrometer is creating at the National center of SR Kurchatov Institute which can measure the EXAFS spectrum with a time resolution 3-5 ms. The experimental results on investigation (by the EXAFS spectroscopy method) of oxides of tungsten and molybdenum are given, which have unique property: the variable valence of an ion of metal is depending on external action. The most interesting of structural problems in the field of physics fullerides, successfully solved with the help of EXAFS spectroscopy, is the spatial location of metal atoms depending on temperature</subfield>
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    <subfield code="a">We consider the spin 1/2 Heisenberg antiferromagnet on a two dimensional quasiperiodic tiling. The T=0 state is long range ordered, with an inhomogeneous distribution of the staggered moment. An approximate real space renormalization scheme first developed for the square lattice is generalized and used to obtain information on the ground state energy as well as the distribution of local correlations in the quasicrystal.</subfield>
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    <subfield code="a">A local and medium range atomic structure model for the face centred icosahedral (fci) Mg25Y11Zn64 alloy has been established in a sphere of r = 27 A. The model was refined by least squares techniques using the atomic pair distribution (PDF) function obtained from synchrotron powder diffraction. Three hierarchies of the atomic arrangement can be found: (i) five types of local coordination polyhedra for the single atoms, four of which are of Frank-Kasper type. In turn, they (ii) form a three-shell (Bergman) cluster containing 104 atoms, which is condensed sharing its outer shell with its neighbouring clusters and (iii) a cluster connecting scheme corresponding to a three-dimensional tiling leaving space for few glue atoms. Inside adjacent clusters, Y8-cubes are tilted with respect to each other and thus allow for overall icosahedral symmetry. It is shown that the title compound is essentially isomorphic to its holmium analogue. Therefore fci-Mg-Y-Zn can be seen as the representative structure type for the other rare earth analogues fci-Mg-Zn-RE (RE = Dy, Er, Ho, Tb) reported in the literature.</subfield>
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    <subfield code="a">We present a general method for the design of 2-dimensional nonlinear photonic quasicrystals that can be utilized for the simultaneous phase-matching of arbitrary optical frequency-conversion processes. The proposed scheme--based on the generalized dual-grid method that is used for constructing tiling models of quasicrystals--gives complete design flexibility, removing any constraints imposed by previous approaches. As an example we demonstrate the design of a color fan--a nonlinear photonic quasicrystal whose input is a single wave at frequency $\omega$ and whose output consists of the second, third, and fourth harmonics of $\omega$, each in a different spatial direction.</subfield>
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    <subfield code="a">We identify several new quasicrystal approximants in alloy systems in which quasicrystals have not been previously reported. Some occur in alloys with large size contrast between the constituent elements, either containing small Boron atoms, or large Ca/Eu atoms, leading to quasicrystal structures quite different from currently known systems where the size contrast is smaller. Another group of the approximants are layered Frank--Kasper structures, demonstrating competition between decagonal and dodecagonal ordering within this family of structures.</subfield>
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    <subfield code="a">We report results of the first computer simulation studies of a physically adsorbed gas on a quasicrystalline surface, Xe on decagonal Al-Ni-Co. The grand canonical Monte Carlo method is employed, using a semi-empirical gas-surface interaction, based on conventional combining rules, and the usual Lennard-Jones Xe-Xe interaction. The resulting adsorption isotherms and calculated structures are consistent with the results of LEED experimental data. The evolution of the bulk film begins in the second layer, while the low coverage behavior is epitaxial. This transition from 5-fold to 6-fold ordering is temperature dependent, occurring earlier (at lower coverage) for the higher temperatures.</subfield>
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    <subfield code="a">We analyze the physics of Bose-Einstein condensates confined in quasi-periodic optical lattices (optical quasicrystals), which offer an intermediate situation between ordered and disordered systems. First, we analyze the time-of-flight interference pattern that reveals quasi-periodic long-range order. Second, we demonstrate localization effects associated with quasi-disorder as well as Bloch-like oscillations associated with the extended nature of the wavefunction of a Bose-Einstein condensate in an optical quasicrystal. In addition, we discuss in detail the crossover between diffusive and localized regimes when the quasi-periodic potential is switched on, as well as the effects of interactions.</subfield>
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    <subfield code="a">A simulation study demonstrates that localization can arise as the result of the breakdown of stable quasi-crystal-like atomic configurations. Samples produced at elevated quench rates and via more energetic processes contain a lower fraction of such configurations and exhibit significantly less pronounced localization and shorter spacing between bands. In the samples produced by the lowest quench rates localization is accompanied by the amorphization of material with initially quasi-crystal-like medium range order. This result is of particular significance in light of recent experimental evidence of local quasi-crystal order in the most stable of the bulk metallic glasses.</subfield>
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    <subfield code="a">To understand an aperiodic tiling (or a quasicrystal modeled on an aperiodic tiling), we construct a space of similar tilings, on which the group of translations acts naturally. This space is then an (abstract) dynamical system. Dynamical properties of the space (such as mixing, or the spectrum of the translation operator) are closely related to bulk properties of the individual tilings (such as the diffraction pattern). The topology of the space of tilings, particularly the Cech cohomology, gives information on how the original tiling can be deformed. Tiling spaces can be constructed as inverse limits of branched manifolds.</subfield>
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    <subfield code="a">The complex arrangements of atoms near a grain boundary are difficult to describe theoretically. We propose a phenomenological (Ginzburg-Landau-like) description of crystalline phases based on symmetries and some fairly general energy and stability arguments. This method allows a very detailed description of defects at the lattice scale with virtually no tunning parameters, unlike usual phase-field methods. The model equations are directly inspired from those used in a very different physical context, namely, the formation of periodic patterns in systems out-of-equilibrium ({\it e.g.} Rayleigh-B\'enard convection, Turing patterns).We apply the formalism to symmetric tilt boundaries in two-dimensional crystalline patterns. Our results are in quantitative agreement with those predicted by a recent crystallographic theory of grain boundaries based on a geometrical quasicrystal-like construction. These results suggest that frustration and competition effects near a defect in crystalline arrangements have some universal features, of interest in solids or other periodic phases.</subfield>
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    <subfield code="a">We investigate the transport properties of a classical wave propagating through a quasi-periodic Fibonacci array of waveguide segments in the form of loops. The formulation is general, and applicable for electromagnetic or acoustic waves through such structures. We examine the conditions for resonant transmission in a Fibonacci waveguide structure. The local positional correlation between the loops are found to be responsible for the resonance. We also show that, depending on the number of segments attached to a particular loop, the intensity at the nodes displays a perfectly periodic or a self-similar pattern. The former pattern corresponds to a perfectly extended mode of propagation, which is to be contrasted to the electron or phonon characteristics of a pure one dimensional Fibonacci quasi-crystal.</subfield>
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    <subfield code="a">Many of the mathematical models used in quasicrystal physics are based on tilings of the plane or space obtained by using strip projection method in a superspace of dimension four, five or six. We present some mathematical results which allow one to use this very elegant method in spaces of dimension much higher and to generate directly quasiperiodic packings of multi-shell clusters. We show that in the case of a two-dimensional (resp. three-dimensional) cluster we have to compute only determinants of order three (resp. four), independently of the dimension of the superspace we use. The computer program based on our mathematical results is very efficient. For example, we can easily generate quasiperiodic packings of three-shell icosahedral clusters (icosahedron + dodecahedron + icosidodecahedron) by using strip projection method in a 31-dimensional space (hundreds of points are obtained in a few minutes on a personal computer).</subfield>
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    <subfield code="a">Quasicrystals constitute a distinct class of solids as they differ both from crystals, because they are not periodic, and from glasses, because they have long-range orientation order. The main challenge of quasicrystal physics is certainly to elucidate how the quasiperiodic order can extend up to the centimetre size of the single grains routinely grown nowadays. In particular, the dynamics of quasicrystal growth remains an unsolved problem in condensed matter. Here, owing to the incisiveness of synchrotron live imaging, we show evidences that the solidification front of icosahedral AlPdMn quasicrystal is facetted all along the growth which proceeds by the tangential motion of ledges at the solid-melt interface, with a measurable effect of interface kinetics. Increasing the applied solidification rate, the kinetic undercooling becomes large enough for the nucleation and free growth of new facetted grains in the melt. The evolution of these grains is explained in details, which reveals the crucial role of aluminium rejection, both in the poisoning of grain growth and driving fluid flow.</subfield>
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    <subfield code="a">Solid state vacuum sintering was studied in tap densified Al powder and in hot quasi-isostatically forged samples composed of commercial inert gas atomized or high purity Al powder, generated by a gas atomization reaction synthesis (GARS) technique. The GARS process results in spherical Al powder with a far thinner surface oxide. The overall results indicated the enhanced ability of GARS- processed Al and Al alloy powders for solid state sintering, which may lead to simplification of current Al powder consolidation processing methods. Elemental Al-based composites reinforced with spherical Al-Cu-Fe alloy powders were produced by quasi-isostatic forging and vacuum hot pressing (VHP) consolidation methods. It was proved that spherical Al-Cu-Fe alloy powders can serve as an effective reinforcement particulate for elemental Al-based composites, because of their high hardness and a preferred type of matrix/reinforcement interfacial bonding, with reduced strain concentration around the particles. Ultimate tensile strength and yield strength of the composites were increased over the corresponding Al matrix values, far beyond typical observations. This remarkable strengthening was achieved without precipitation hardening and without severe strain hardening during consolidation because of the matrix choice (elemental Al) and the &amp;ldquo;low shear&amp;rdquo; consolidation methods utilized. This reinforcement effectiveness is further evidenced by elastic modulus measurements of the composites that are very close to the upper bound predictions of the rule of mixtures. The load partitioning measurements by neutron diffraction showed that composite samples made from GARS powders present significantly higher load transfer efficiency than the composites made from commercially atomized powders. Further analysis of the load sharing measurements and the calculated values of the mismatch of coefficient of thermal expansion (CTE) and the geometrically necessary dislocation (GND) effects suggest that these strengthening mechanisms can be combined to predict accurately the strength of the composites. By neutron diffraction measurements, it also was found that the composites consolidated from Al and Al&lt;sub>63&lt;/sub>Cu&lt;sub>25&lt;/sub>Fe&lt;sub>12&lt;/sub> quasicrystal alloy reinforcement powders have compressive residual stress in the Al matrix, contrary to the tensile residual stress in typical Al/SiC composites. The composites made by the quasi-isostatic forging process exhibited higher tensile strengths and much higher compressive residual stresses than the composites made by the VHP process.</subfield>
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    <subfield code="a">In this paper, we consider the Frenkel-Kontorova model of a one dimensional chain of atoms submitted to a potential. This potential splits into an interaction potential and a potential induced by an underlying substrate which is a quasicrystal. Under standard hypotheses, we show that every minimal configuration has a rotation number, that the rotation number varies continuously with the minimal configuration, and that every non negative real number is the rotation number of a minimal configuration. This generalizes well known results obtained by S. Aubry and P.Y. le Daeron in the case of a crystalline substrate.</subfield>
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    <subfield code="a">An extinction rule for a class of 1D quasicrystals</subfield>
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    <subfield code="a">We study decorated one-dimensional quasicrystal obtained by a non-standard projection of a part of two-dimensional lattice. We focus on the impact of varying relative positions of decorated sites. First, we give general expression for the structure factor. Subsequently we analyze an example of extinction rule.</subfield>
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    <subfield code="a">We apply systematic methods previously used by Mihalkovic et al. to predict the structure of the `basic' Co-rich modification of the decagonal Al70 Co20 Ni10 layered quasicrystal, based on known lattice constants and previously calculated pair potentials. The modelling is based on Penrose tile decoration and uses Monte Carlo annealing to discover the dominant motifs, which are converted into rules for another level of description. The result is a network of edge-sharing large decagons on a binary tiling of edge 10.5 A. A detailed analysis is given of the instability of a four-layer structure towards $c$-doubling and puckering of the atoms out of the layers, which is applied to explain the (pentagonal) orientational order.</subfield>
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    <subfield code="a">Discussion on clusters, phasons, and quasicrystal stabilisation</subfield>
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    <subfield code="a">This paper summarises a two-hour discussion at the Ninth International Conference on Quasicrystals, including nearly 20 written comments sent afterwards, concerning (i) the meaning [if any] of clusters in quasicrystals; (ii) phason elasticity, and (iii) thermodynamic stabilisation of quasicrystals.</subfield>
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    <subfield code="a">We use energy minimization principles to predict the structure of a decagonal quasicrystal - d(AlCoNi) - in the Cobalt-rich phase. Monte Carlo methods are then used to explore configurations while relaxation and molecular dynamics are used to obtain a more realistic structure once a low energy configuration has been found. We find five-fold symmetric decagons 12.8 A in diameter as the characteristic formation of this composition, along with smaller pseudo-five-fold symmetric clusters filling the spaces between the decagons. We use our method to make comparisons with a recent experimental approximant structure model from Sugiyama et al (2002).</subfield>
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    <subfield code="a">Modelling Disorder In Quasicrystals. Decagonal Aluminium- Cobalt-nickel</subfield>
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    <subfield code="a">The theme of this doctoral thesis is the modelling of structural disorder phenomena from decagonal Al-Co-Ni quasicrystals by an analysis of full diffuse X-ray scattering data as a function of temperature. The motivation for this study is to reveal the complex ordering principles of decagonal Al-Co-Ni quasicrystals and, consequently, to understand the driving force for the formation and stability of these materials. For the first time, the 3D difference Patterson (autocorrelation) function of a disordered quasicrystal (&lt;italic>Edagawa-phase&lt;/italic>) has been analysed. A new technique, the punch-and-fill method has been developed to separate diffuse scattering and Bragg reflections. Its potential and limits are discussed in detail. The calculated difference Patterson maps are interpreted in terms of inter-cluster correlations as a function of temperature. Both, at high and low temperatures, clusters decorate the vertices of the same quasiperiodic covering. At high temperatures, medium-range inter-cluster correlations are present, whereas at low temperatures, the ordering between the clusters becomes less concise. Qualitatively, the Patterson maps may be interpreted by inter-cluster correlations, which take place mainly inside pentagonal superclusters below 1120 K, and inside larger decagonal superclusters at 1120 K. The pentagonal supercluster consists of five &lt;italic>Gummelt&lt;/italic> clusters at the corners of a star-centered pentagon with &amp;ap;20 &amp;Aring; edge length; the decagonal supercluster is composed of one central &lt;italic>Gummelt&lt;/italic> cluster edge-joiningly surrounded by a ring of ten further overlapping &lt;italic>Gummelt&lt;/italic> clusters. The hydrodynamic theory of phasonic and phononic disorder has been applied successfully to describe the short- range, disordered structure of the &lt;italic> Edagawa- phase&lt;/italic>. Moreover, model calculations demonstrate that the main features of diffuse scattering can equally well be described by phasonic disorder and fivefold orientational disorder of clusters. The calculations allow to distinguish the different cluster types published so far and the best agreement with experimental data could be achieved with the mirror-symmetric Abe- cluster. Modelling of phasonic diffuse scattering associated with the S1 and S2 superstructure reflections indicates disorder of superclusters. The former show basically inter-cluster correlations inside quasiperiodic layers, while the latter exhibit intra- and inter-cluster correlations, both between adjacent and inside quasiperiodic layers. The feasibility, potential and limits of the Patterson method in combination with the &lt;italic>punch-and-fill &lt;/italic> method employed is shown on the example of a phasonic disordered rhombic Penrose tiling. A variation of the elastic constants within the framework of the hydrodynamic theory does not change qualitatively the way phasonic disorder is realized in the &lt;italic>local&lt;/italic> quasicrystalline structure. For the same model system it is also shown that phasonic fluctuations of the atomic surfaces give average clusters in the cut-space, which correspond to fivefold orientationally disordered clusters, &lt;italic>i.e&lt;/italic>. phasons induce fivefold orientational disorder of clusters. A Patterson analysis of the diffuse interlayers from the Edagawa-phase showed that the main unit for correlated displacements along the periodic direction is a disordered structure motif (cluster) with a diameter of &amp;ap;15 &amp;Aring;, the fine structure of which does hardly change as a function of temperature. At 1120 K, the displacements of the clusters are uncorrelated along quasiperiodic directions, while at lower temperatures &amp;ap;42 &amp;Aring;-sized superclusters of a well-defined shape are formed. The spatial distribution but not the internal structure of the superclusters differs significantly at 1070 K and 300 K.</subfield>
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    <subfield code="a">The Study Of Band Gap Engineering For Phononic Crystals And Gap Structures In Phononic Quasicrystals</subfield>
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    <subfield code="a">sine loco</subfield>
    <subfield code="b">Hong Kong Univ Sci And Tech peoples Republic Of China</subfield>
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    <subfield code="a">PhD</subfield>
    <subfield code="b">Hong Kong Univ Sci And Tech peoples Republic Of China</subfield>
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    <subfield code="a">Phononic crystals and quasicrystals are solid-solid, fluid-solid or fluid-fluid composites with periodic or quasiperiodic long-range order, respectively. They are of interest not only because of the profound effects of their periodic or quasiperiodic structure on wave propagation (e.g. the existence of elastic or acoustic band gaps), but also because of potential applications like sound filters, transducer design and acoustic mirrors, etc. In this thesis, I will present some research progress in the study of both phononic crystals and quasicrystals. For phononic crystals, we have proposed a simple, systematic and efficient method to engineer elastic (acoustic) band gaps. A gap can be enhanced or created by altering the microstructure according to the field-energy distributions of the Bloch states at the band edges as well as their derivatives. Due to the structure of the acoustic wave equation, the engineering of acoustic band gaps is much more efficient than that of photonic band gaps. For elastic waves, a large absolute band gap can be enhanced or created by inserting air inclusions in a two- component elastic phononic crystal or quasicrystal with small density contrast and filling fraction. The positions of the insertion are chosen to suppress the shear potential energy of the acoustic branches and lower their frequencies. The validity of the proposed methods is supported by multiple-scattering calculations in various two-dimensional systems, such as steel cylinders in air, water cylinders in mercury and aluminum cylinders in epoxy. Our methods make the acoustic band gap 'designable' and the realization of a light and effective sonic insulator possible. The sonic band-gap structures of a 12-fold symmetric quasicrystal consisting of rigid cylinders in air are investigated by using the multiple scattering method. Large full gaps are found owing to its high symmetry. However, the gap structure evolves with the sample size. By using the SMCG method, we have observed a self-similar like behavior of states emerging inside original gaps and gaps emerging inside original bands when the sample size is increased. The long-range order has been proved important for the formation of gaps at low frequencies. We have also studied the properties of wave functions in large samples (up to 33919 cylinders). Various types of wave functions have been seen, including extended state, self-similar state with a power-law decay and confined state.</subfield>
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    <subfield code="a">This thesis investigates photonic quasicrystals and ellipsoid packings, two problems in which geometry plays an important role in condensed matter physics and where the use of stereolithographically fabricated macroscopic models helps to solve fundamental problems. &lt;italic>Part I&lt;/italic>. Photonic quasicrystals may have bandgap properties that make them well-suited for scientific and technological applications in which photonic crystals are normally considered. They are constructed from two or more types of dielectric material arranged in a quasiperiodic pattern whose rotational symmetry is forbidden for periodic crystals. Because quasicrystals have higher point group symmetry (are closer to spherical) than ordinary crystals, their gap center frequencies are closer and the gaps widths are more uniform, optimal conditions for forming a complete, more spherical bandgap. Our calculations on 2-D Penrose quasicrystals show very isotropic bandgaps. Analogous computations 3-D quasicrystals are challenging and have not been performed to date. Here we circumvent the 3-D computational problem by doing an experiment. Using stereolithography we constructed an icosahedral photonic quasicrystal with centimeter-scale cells and performed microwave transmission measurements. We show that the quasicrystal exhibits sizeable stopgaps and determine their effective Brillouin zones. As a check, we perform calculations and experiments on a similar photonic crystal with diamond symmetry. Our studies confirm that quasicrystals are excellent candidates for photonic bandgap materials. &lt;italic>Part II&lt;/italic>. The measurements of the overall density &amp;phis;&lt;sub> avr&lt;/sub>, &amp;phis;(&lt;italic>r&lt;/italic>), and the core density agree with simulations. Recent simulations indicate that ellipsoids can randomly pack more densely than spheres and, remarkably, ellipsoids with aspect ratio 1.25:1:0.8 can approach the densest crystal packing (FCC) of spheres, with packing fraction 74%. We demonstrate that such dense packings are experimentally realizable. We introduce a novel way of determining packing density for a finite number of particles that minimizes wall effects. We have fabricated ellipsoids using stereolithography and show that in a spherical container of radius R, the radial packing fraction, &amp;phis;(r), can be obtained from V(h), the volume of added fluid to fill the sphere to height h. Additionally, we perform an MRI scan of our packing and obtain &amp;phis;(r) from it. The measurements of the overall density &amp;phis;&lt;sub>avr&lt;/sub>, &amp;phis;(r), and the core density &amp;phis;&lt;sub> 0&lt;/sub> = 0.74 &amp;plusmn; 0.005agree with simulations.</subfield>
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    <subfield code="a">Modified strip projection method</subfield>
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    <subfield code="a">The diffraction image of a quasicrystal admits a finite group $G$ as a symmetry group, and the quasicrystal can be regarded as a quasiperiodic packing of copies of a $G$-cluster $\mathcal{C}$, joined by glue atoms. The physical space $E$ containing $\mathcal{C}$ can be embedded into a higher-dimensional space $\mathbb{R}^k$ such that, up to an inflation factor, $\mathcal{C}$ is the orthogonal projection of the set $\{(\pm 1,0,...,0)$, $(0,\pm 1,0,...,0)$, ... $(0,...,0,\pm 1)\}$. The projections of the points of $\mathbb{Z}^k$ lying in the strip $S=E+[-1/2,1/2]^k+t$ obtained by shifting a hypercube $[-1/2,1/2]^k+t$ along $E$ is a quasiperiodic packing of partially occupied copies of $\mathcal{C}$, but unfortunately, the occupation of clusters is very low. In our modified strip projection method we firstly determine for each point $x\in \mathbb{Z}^k\cap S$ the number $n(x)$ of all the arithmetic neighbours of $x$ lying in the strip $S$, and project the points of $\mathbb{Z}^k\cap S$ on $E$ in the decreasing order of the occupation number $n(x)$. In the case when $n(x)$ represents more than $p%$ of all the points of the cluster $C$ we project all the arithmetic neighbours of $x$ (lying inside or outside $S$). We choose $p$ such that to avoid the superposition of the fully occupied clusters. The projection of a point $x$ with $n(x)$ less than $p%$ of all the points of the cluster $C$ is added to the pattern only if it is not too close to the already obtained points.</subfield>
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    <subfield code="a">Light-induced Forces On Small Particles</subfield>
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    <subfield code="a">sine loco</subfield>
    <subfield code="b">Hong Kong Univ Sci And Tech peoples Republic Of China</subfield>
    <subfield code="c">2005</subfield>
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    <subfield code="a">PhD</subfield>
    <subfield code="b">Hong Kong Univ Sci And Tech peoples Republic Of China</subfield>
    <subfield code="c">2005</subfield>
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    <subfield code="a">Light-trapping is generally associated with the phenomenon that small particles are driven toward the intensity maxima of a carefully sculpted laser beam. There is another type of inter-particle optical force arising from the coherent multiple-scattering of light between the particles, previously observed in various experiments. This thesis is mainly devoted to the theoretical study of such optical binding force for a cluster of dielectric particles. In contrast to the intensity-driven light-trapping, the optical binding force is present even when a plane wave (with homogeneous intensity) is incident upon a collection of microparticles. Firstly, the theory of optical force for neutral dielectric Rayleigh particles is presented. We then show through rigorous calculations that the optical binding force (with the incident intensity &amp;sim;10&lt;super>6&lt;/super> W/cm&lt;super>2&lt;/super>) can dominate other interactions and bind dielectric microspheres in stable structures that behave like 'molecules.' Such photonic clusters can exhibit a multiplicity of static and drifting equilibrium configurations, with some having remarkable geometries such as a quasicrystal-like arrangement. The photonic clusters exhibit exotic dynamics, and the equilibrium configurations can correspond with either stable or a type of quasi-stable states in which the cluster maintains an average shape, with individual particles executing periodic motion in the presence of frictional dissipation. Photonic clusters consist of Rayleigh particles are also investigated. A stable one-dimensional lattice is found and analyzed, localized vibration modes are observed. Finally, we consider an interesting type of resonant inter-particle optical force. We shall see that tuning of the incident light's frequency to the morphology- dependent resonances of a cluster of transparent microspheres induces a strong, resonant optical force between the spheres. The resonant force can be enhanced by orders of magnitude so that it dominates other interactions (at a modest incident intensity of &amp;sim;10&lt;super>4&lt;/super> W/cm&lt;super>2&lt;/super>). We also proposed various ways to utilize the resonant force in the binding of a microsphere cluster.</subfield>
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    <subfield code="a">Prejean, J J</subfield>
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    <subfield code="a">Experimental study of the competition between Kondo and RKKY interactions for Mn spins in a model alloy system</subfield>
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    <subfield code="c">2006</subfield>
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    <subfield code="a">18 p</subfield>
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    <subfield code="a">The quasicrystal Al-Pd-Mn is a model system for an experimental study of the competition between Ruderman-Kittel-Kasuya-Yoshida (RKKY) and Kondo interactions. First, specific of such alloys, only a few Mn atoms carry an effective spin and their concentration x is tunable over several orders of magnitude, even though the Mn amount is almost constant. Second, the characteristic energy scales for the interactions lie in the Kelvin range. Hence we could study the magnetization on both side of these energy scales, covering a range of temperatures [0.1-100 K] and magnetic fields (mu_B H/k_B= 0 to 5 K) for 22 samples and x varying over 2 decades. Using very general Kondo physics arguments, and thus carrying out the data analysis with no preconceived model, we found a very robust and simple result: The magnetization is a sum of a pure Kondo (T_K=3.35K) and a pure RKKY contributions, whatever the moment concentration is and this surprisingly up to the concentration where the RKKY couplings dominate fully and thus cannot be considered as a perturbation.</subfield>
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    <subfield code="a">Hippert, F</subfield>
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    <subfield code="c">214205</subfield>
    <subfield code="p">Phys. Rev. B</subfield>
    <subfield code="v">73</subfield>
    <subfield code="y">2006</subfield>
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    <subfield code="a">Introducing and studying the pattern frequency algebra, we prove the analogue of L\"uck's approximation theorems on $L^2$-spectral invariants in the case of aperiodic order. These results imply a uniform convergence theorem for the integrated density of states as well as the positivity of the logarithmic determinant of certain discrete Schrodinger operators.</subfield>
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    <subfield code="a">A circle pattern is a configuration of circles in the plane whose combinatorics is given by a planar graph G such that to each vertex of G corresponds a circle. If two vertices are connected by an edge in G, the corresponding circles intersect with an intersection angle in $(0,\pi)$. Two sequences of circle patterns are employed to approximate a given conformal map $g$ and its first derivative. For the domain of $g$ we use embedded circle patterns where all circles have the same radius decreasing to 0 and which have uniformly bounded intersection angles. The image circle patterns have the same combinatorics and intersection angles and are determined from boundary conditions (radii or angles) according to the values of $g'$ ($|g'|$ or $\arg g'$). For quasicrystallic circle patterns the convergence result is strengthened to $C^\infty$-convergence on compact subsets.</subfield>
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    <subfield code="a">The inverse problem of diffraction theory in essence amounts to the reconstruction of the atomic positions of a solid from its diffraction image. From a mathematical perspective, this is a notoriously difficult problem, even in the idealised situation of perfect diffraction from an infinite structure. Here, the problem is analysed via the autocorrelation measure of the underlying point set, where two point sets are called homometric when they share the same autocorrelation. For the class of mathematical quasicrystals within a given cut and project scheme, the homometry problem becomes equivalent to Matheron's covariogram problem, in the sense of determining the window from its covariogram. Although certain uniqueness results are known for convex windows, interesting examples of distinct homometric model sets already emerge in the plane. The uncertainty level increases in the presence of diffuse scattering. Already in one dimension, a mixed spectrum can be compatible with structures of different entropy. We expand on this example by constructing a family of mixed systems with fixed diffraction image but varying entropy. We also outline how this generalises to higher dimension.</subfield>
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    <subfield code="a">The paper develops a method for discrete computational Fourier analysis of functions defined on quasicrystals and other almost periodic sets. A key point is to build the analysis around the emerging theory of quasicrystals and diffraction in the setting on local hulls and dynamical systems. Numerically computed approximations arising in this way are built out of the Fourier module of the quasicrystal in question, and approximate their target functions uniformly on the entire infinite space. The methods are entirely group theoretical, being based on finite groups and their duals, and they are practical and computable. Examples of functions based on the standard Fibonacci quasicrystal serve to illustrate the method (which is applicable to all quasicrystals modeled on the cut and project formalism).</subfield>
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    <subfield code="a">Luminescence Properties of a Fibonacci Photonic Quasicrystal</subfield>
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    <subfield code="a">We report the realization of an active one-dimensional Fibonacci photonic quasi-crystal via spin coating. Manipulation of the luminescence properties of an organic dye embedded in the quasi-crystal is presented and compared to theoretical simulations. The luminescence occurs via the pseudo-bandedge mode and follows the dispersion properties of the Fibonacci crystal. Time resolved luminescence measurement of the active structure shows faster spontaneous emission rate, indicating the effect of the large photon densities available at the bandedge due to the presence of critically localized states. The experimental results are in excellent agreement with the theoretical calculations.</subfield>
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    <subfield code="a">In this Letter, we present a study of the confinement properties of point-defect resonators in finite-size photonic-bandgap structures composed of aperiodic arrangements of dielectric rods, with special emphasis on their use for the design of cavities for particle accelerators. Specifically, for representative geometries, we study the properties of the fundamental mode (as a function of the filling fraction, structure size, and losses) via 2-D and 3-D full-wave numerical simulations, as well as microwave measurements at room temperature. Results indicate that, for reduced-size structures, aperiodic geometries exhibit superior confinement properties by comparison with periodic ones.</subfield>
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    <subfield code="a">Cathodoluminescence VUV spectra of free pure nitrogen clusters produced by condensation of gas mixtures in supersonic jets expanding into vacuum were studied. The clusters were of icosahedral structure, as evidenced by our electron diffraction measurements, i.e., quasicrystals, and contained about 1000 atoms. The cluster temperature was about 40 K. The luminescence spectra measured in the range of 45,000-75,000 cm^-1 clearly showed three vibronic w -> X series of transitions from the excited 'w' to the ground 'X' state, which are intrinsic to nitrogen molecules. All the transitions revealed a strong dependence of the matrix shift of their peak positions on vibration quantum number, while for bulk samples of N2 the matrix shift is known to remain unchanged. Our analysis showed that in clusters the vibrational anharmonicity parameter changes drastically for both the upper and lower states, while the change in the vibrational frequencies is much less prominent. The results obtained provide information about an abnormally strong influence of cluster environment on the nonlinear contribution to the vibrations of nitrogen molecules.</subfield>
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    <subfield code="a">On the spectrum of the Thue-Morse quasicrystal and the rarefaction phenomenon</subfield>
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    <subfield code="a">The spectrum of a weighted Dirac comb on the Thue-Morse quasicrystal is investigated, and characterized up to a measure zero set, by means of the Bombieri-Taylor conjecture, for Bragg peaks, and of another conjecture that we call Aubry-Godr\`eche-Luck conjecture, for the singular continuous component. The decomposition of the Fourier transform of the weighted Dirac comb is obtained in terms of tempered distributions. We show that the asymptotic arithmetics of the $p$-rarefied sums of the Thue-Morse sequence (Dumont; Goldstein, Kelly and Speer; Grabner; Drmota and Skalba,...), namely the fractality of sum-of-digits functions, play a fundamental role in the description of the singular continous part of the spectrum, combined with some classical results on Riesz products of Peyri\`ere and M. Queff\'elec. The dominant scaling of the sequences of approximant measures on a part of the singular component is controlled by certain inequalities in which are involved the class number and the regulator of real quadratic fields.</subfield>
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    <subfield code="a">Classical crystals are solid materials containing arbitrarily long periodic repetitions of a single motif. In this paper, we study the maximal possible repetition of the same motif occurring in beta-integers -- one dimensional models of quasicrystals. We are interested in beta-integers realizing only a finite number of distinct distances between neighboring elements. In such a case, the problem may be reformulated in terms of combinatorics on words as a study of the index of infinite words coding beta-integers. We will solve a particular case for beta being a quadratic non-simple Parry number.</subfield>
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    <subfield code="a">Using the eigen-decomposition method, we investigated the plasmonic modes in a two-dimensional quasicrystalline array of metal nanoparticles. Various properties of the plasmonic modes, such as their symmetry, radiation loss and spatial localization are studied. Some collective plasmonic modes are found to be leaky with out-of-plane radiation loss, but some modes can have very high fidelity. To facilitate the analysis on the complex behavior of the collective plasmonic modes, we considered a trajectory map in a three dimension parameter space defined by the frequency of the mode, the participation ratio of the mode that gives the spatial distribution, and the eigenvalue that is related to the inverse lifetime of the mode. With the help of the trajectory map method, we found that there are modes that are localized in some special ways and the plasmonic mode with highest spatial localization and highly fidelity is found to be a type of anti-phase ring modes. In general, the spatial decay behaviors of localized modes are highly dependent on mode patterns. There is no special relationship between the fidelity of the modes and their spatial localization.</subfield>
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    <subfield code="a">Perfect colourings of the rings of cyclotomic integers with class number one are studied. It is shown that all colourings induced by ideals (q) are chirally perfect, and vice versa. A necessary and sufficient condition for a colouring to be perfect is obtained, depending on the factorisation of q. This result yields the colour symmetry group H in general. Furthermore, the colour preserving group K is determined in all but finitely many cases. An application to colourings of quasicrystals is given.</subfield>
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    <subfield code="a">We investigate the use of quasicrystals in image sampling. Quasicrystals produce space-filling, non-periodic point sets that are uniformly discrete and relatively dense, thereby ensuring the sample sites are evenly spread out throughout the sampled image. Their self-similar structure can be attractive for creating sampling patterns endowed with a decorative symmetry. We present a brief general overview of the algebraic theory of cut-and-project quasicrystals based on the geometry of the golden ratio. To assess the practical utility of quasicrystal sampling, we evaluate the visual effects of a variety of non-adaptive image sampling strategies on photorealistic image reconstruction and non-photorealistic image rendering used in multiresolution image representations. For computer visualization of point sets used in image sampling, we introduce a mosaic rendering technique.</subfield>
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    <subfield code="a">We numerically analyze, using Finite Difference Time Domain simulations, the bandgap properties of photonic quasicrystals with a low index contrast. We compared 8-, 10- and 12-fold symmetry aperiodically ordered lattices with different spatial tiling. Our results show that tiling design, more than symmetry, determines the transmission properties of these structures.</subfield>
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    <subfield code="a">We study measures on the real line and present various versions of what it means for such a measure to take only finitely many values. We then study perturbations of the Laplacian by such measures. Using Kotani-Remling theory, we show that the resulting operators have empty absolutely continuous spectrum if the measures are not periodic. When combined with Gordon type arguments this allows us to prove purely singular continuous spectrum for some continuum models of quasicrystals.</subfield>
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    <subfield code="a">In this paper, we present a comparative study of the tuning efficiency and sensitivity of guided resonances (GRs) in photonic crystal (PC) holed slabs based on periodic and aperiodically-ordered unit cells, aimed at assessing the applicability of these important technology platforms to ultra-compact optical sensors and active devices. In particular, with specific reference to square-lattice periodic PCs and aperiodically-ordered Ammann-Beenker photonic quasi-crystals, we study the effects of the hole radius, slab thickness, and refractive index on the GR sensitivity and tunability with respect to variation in the hole refractive index. Finally, we carry out a theoretical and numerical analysis in order to correlate the GR shift with the field distribution of the unperturbed (air holes) structures. Our results indicate that the spatial arrangement of the holes may strongly influence the tuning and sensitivity efficiency, and provide new degrees of freedom and tools for the design and optimization of novel photonic devices for both sensing and telecommunication applications.</subfield>
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    <subfield code="a">We introduce a novel optimization method to design the first examples of photonic quasicrystals with substantial, complete photonic band gaps (PBGs): that is, a range of frequencies over which electromagnetic wave propagation is forbidden for all directions and polarizations. The method can be applied to photonic quasicrystals with arbitrary rotational symmetry; here, we illustrate the results for 5- and 8-fold symmetric quasicrystals. The optimized band gaps are highly isotropic, which may offer advantages over photonic crystals for certain applications.</subfield>
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    <subfield code="o">M. Florescu, S. Torquato, and P. J. Steinhardt, Phys. Rev. B 80, 155112 (2009)</subfield>
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    <subfield code="v">80</subfield>
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    <subfield code="a">Matei and Meyer proved that `simple quasicrystals' are universal sets of sampling and interpolation for signals with a band-limited spectrum. We ask if the corresponding exponential system is a universal Riesz basis for appropriate multiband sets on the circle. We prove that the answer depends on a diophantine property of the quasicrystal. For the proof we extend to BMO a theorem of Kesten on the discrepancy of irrational rotations of the circle.</subfield>
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    <subfield code="a">Wood anomalies in resonant photonic quasicrystals</subfield>
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    <subfield code="a">A theory of light diffraction from planar quasicrystalline lattice with resonant scatterers is presented. Rich structure, absent in the periodic case, is found in specular reflection spectra, and interpreted as a specific kind of Wood anomalies, characteristic for quasicrystals. The theory is applied to semiconductor quantum dots arranged in Penrose tiling.</subfield>
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    <subfield code="a">This paper introduces a simple Markov process inspired by the problem of quasicrystal growth. It acts over two-letter words by randomly performing \emph{flips}, a local transformation which exchanges two consecutive different letters. More precisely, only the flips which do not increase the number of pairs of consecutive identical letters are allowed. Fixed-points of such a process thus perfectly alternate different letters. We show that the expected number of flips to converge towards a fixed-point is bounded by $O(n^3)$ in the worst-case and by $O(n^{5/2}\ln{n})$ in the average-case, where $n$ denotes the length of the initial word.</subfield>
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    <subfield code="a">On Bravais Colorings Associated with Periodic and Non-Periodic Crystals</subfield>
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    <subfield code="a">In this work, a theory of color symmetry is presented that extends the ideas of traditional theories of color symmetry for periodic crystals to apply to non-periodic crystals. The color symmetries are associated to each of the crystalline sites and may correspond to different chemical species, various orientations of magnetic moments and colorings of a non-periodic tiling. In particular, we study the color symmetries of periodic and non-periodic structures via Bravais colorings of planar modules that emerge as the ring of integers in cyclotomic fields with class number one. Using an approach involving matrices, we arrive at necessary and sufficient conditions for determining the color symmetry groups and color fixing groups of the Bravais colorings associated with the modules M_n = Z[exp(2{\pi}i/n)], and list the findings for M_{15} = Z[exp(2{\pi}i/15)] and M_{16} = Z[exp({\pi}i/8)]. In the second part of the paper, we discuss magnetic point groups of crystal and quasicrystal structures and give some examples of structures whose magnetic point group symmetries are described by Bravais colorings of planar modules.</subfield>
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    <subfield code="a">All-optical diode action in asymmetric nonlinear photonic multilayers with perfect transmission resonances</subfield>
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    <subfield code="a">Light propagation in asymmetric Kerr-nonlinear multilayers with perfect transmission resonances is theoretically investigated. It is found that hybrid Fabry-P\'erot/photonic-crystal structures of the type (BA)^k(AB)^k(AABB)^m exhibit both pronounced unidirectionality (due to strong spatial asymmetry of the resonant mode) and high transmission (due to the existence of a perfect transmission resonance). This results in nonlinear optical diode action with low reflection losses without need for a pumping beam or input pulse modulation. By slightly perturbing the perfect transmission resonance condition, the operating regime of the optical diode can be tuned, with a trade-off between minimizing the reflection losses and maximizing the frequency bandwidth where unidirectional transmission exists. Optical diode action is demonstrated in direct numerical simulation, showing >92% transmittance in one direction and about 22% in the other. The effect of perfect transmission resonance restoration induced by nonlinearity was observed analytically and numerically. The proposed geometry is shown to have advantages over previously reported designs based on photonic quasicrystals.</subfield>
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    <subfield code="a">Colourings of lattices and coincidence site lattices</subfield>
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    <subfield code="a">The relationship between the coincidence indices of a lattice $\Gamma_1$ and a sublattice $\Gamma_2$ of $\Gamma_1$ is examined via the colouring of $\Gamma_1$ that is obtained by assigning a unique colour to each coset of $\Gamma_2$. In addition, the idea of colour symmetry, originally defined for symmetries of lattices, is extended to coincidence isometries of lattices. An example involving the Ammann-Beenker tiling is provided to illustrate the results in the quasicrystal setting.</subfield>
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    <subfield code="a">A discrete set $A$ in the Euclidian space is almost periodic if the measure with the unite masses at points of the set is almost periodic in the weak sense. We investigate properties of such sets in the case when $A-A$ is discrete. In particular, if $A$ is a Bohr almost periodic set, we prove that $A$ is a union of a finite number of translates of a certain full--rank lattice. If $A$ is a Besicovitch almost periodic set, then there exists a full-rank lattice such that in most cases a nonempty intersection of its translate with $A$ is large.</subfield>
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    <subfield code="a">In-plane plasmonic modes in a quasicrystalline array of metal nanoparticles</subfield>
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    <subfield code="a">We investigated the plasmonic modes in a two-dimensional quasicrystalline array of metal nanoparticles. The polarization of the modes is in the array plane. A simplified eigen-decomposition method is presented with the help of rotational symmetry. Two kinds of anti-phase ring modes with radial and tangential polarizations are of highest spatial localizations among all of plasmonic modes. For the leaky characteristic of the anti-phase ring modes, the highest fidelity mode is found to be tangential polarized mode in the quasicrystal array, whereas normal-to-plane polarized mode in the solo ring. The leaky characteristics and spatial localizations of other plasmonic modes are also studied, for example, collective vortex mode that may be potentially useful to form negative responses in plasmonic device, and collective radial mode that may be used to generate light sources with radial polarizations.</subfield>
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    <subfield code="a">All hard, convex shapes are conjectured by Ulam to pack more densely than spheres, which have a maximum packing fraction of {\phi} = {\pi}/\sqrt18 ~ 0.7405. For many shapes, simple lattice packings easily surpass this packing fraction. For regular tetrahedra, this conjecture was shown to be true only very recently; an ordered arrangement was obtained via geometric construction with {\phi} = 0.7786, which was subsequently compressed numerically to {\phi} = 0.7820. Here we show that tetrahedra pack much better than this, and in a completely unexpected way. Following a conceptually different approach, using thermodynamic computer simulations that allow the system to evolve naturally towards high-density states, we observe that a fluid of hard tetrahedra undergoes a first-order phase transition to a dodecagonal quasicrystal, which can be compressed to a packing fraction of {\phi} = 0.8324. By compressing a crystalline approximant of the quasicrystal, the highest packing fraction we obtain is {\phi} = 0.8503. If quasicrystal formation is suppressed, the system remains disordered, jams, and compresses to {\phi} = 0.7858. Jamming and crystallization are both preceded by an entropy-driven transition from a simple fluid of independent tetrahedra to a complex fluid characterized by tetrahedra arranged in densely packed local motifs that form a percolating network at the transition. The quasicrystal that we report represents the first exa mple of a quasicrystal formed from hard or non-spherical particles. Our results demonstrate that particle shape and entropy can produce highly complex, ordered structures.</subfield>
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    <subfield code="a">We develop a general notion of orthogonal wavelets `centered' on an irregular knot sequence. We present two families of orthogonal wavelets that are continuous and piecewise polynomial. As an application, we construct continuous, piecewise quadratic, orthogonal wavelet bases on the quasi-crystal lattice consisting of the $\tau$-integers where $\tau$ is the golden-mean. The resulting spaces then generate a multiresolution analysis of $L^2(\mathbf{R})$ with scaling factor $\tau$.</subfield>
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    <subfield code="a">We report on the formation and development of the photonic band gap in two-dimensional 8-, 10- and 12-fold symmetry quasicrystalline lattices of low index contrast. Finite size structures made of dielectric cylindrical rods were studied and measured in the microwave region, and their properties compared with a conventional hexagonal crystal. Band gap characteristics were investigated by changing the direction of propagation of the incident beam inside the crystal. Various angles of incidence from 0 \degree to 30\degree were used in order to investigate the isotropic nature of the band gap. The arbitrarily high rotational symmetry of aperiodically ordered structures could be practically exploited to manufacture isotropic band gap materials, which are perfectly suitable for hosting waveguides or cavities.</subfield>
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    <subfield code="a">We consider Frenkel-Kontorova models corresponding to 1 dimensional quasicrystals. We present a KAM theory for quasi-periodic equilibria. The theorem presented has an \emph{a-posteriori} format. We show that, given an approximate solution of the equilibrium equation, which satisfies some appropriate non-degeneracy conditions, then, there is a true solution nearby. This solution is locally unique. Such a-posteriori theorems can be used to validate numerical computations and also lead immediately to several consequences a) Existence to all orders of perturbative expansion and their convergence b) Bootstrap for regularity c) An efficient method to compute the breakdown of analyticity. Since the system does not admit an easy dynamical formulation, the method of proof is based on developing several identities. These identities also lead to very efficient algorithms.</subfield>
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    <subfield code="a">Kinematic Diffraction from a Mathematical Viewpoint</subfield>
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    <subfield code="a">Mathematical diffraction theory is concerned with the analysis of the diffraction image of a given structure and the corresponding inverse problem of structure determination. In recent years, the understanding of systems with continuous and mixed spectra has improved considerably. Simultaneously, their relevance has grown in practice as well. In this context, the phenomenon of homometry shows various unexpected new facets. This is particularly so for systems with stochastic components. After the introduction to the mathematical tools, we briefly discuss pure point spectra, based on the Poisson summation formula for lattice Dirac combs. This provides an elegant approach to the diffraction formulas of infinite crystals and quasicrystals. We continue by considering classic deterministic examples with singular or absolutely continuous diffraction spectra. In particular, we recall an isospectral family of structures with continuously varying entropy. We close with a summary of more recent results on the diffraction of dynamical systems of algebraic or stochastic origin.</subfield>
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    <subfield code="a">Photonic stop bands in quasi-random nanoporous anodic alumina structures</subfield>
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    <subfield code="c">05 May 2011</subfield>
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    <subfield code="a">The existence of photonic stop bands in the self-assembled arrangement of pores in porous anodic alumina structures is investigated by means of rigorous 2D finite- difference time-domain calculations. Self-assembled porous anodic alumina shows a random distribution of domains, each of them with a very definite triangular pattern, constituting a quasi-random structure. The observed stop bands are similar to those of photonic quasicrystals or random structures. As the pores of nanoporous anodic alumina can be infiltrated with noble metals, nonlinear or active media, it makes this material very attractive and cost-effective for applications including inhibition of spontaneous emission, random lasing, LEDs and biosensors.</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
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    <subfield code="c">Hidden</subfield>
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<record>
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    <subfield code="a">arXiv:1105.3337</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Rochal, S B</subfield>
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    <subfield code="a">Lorman, V L</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1105.3337.pdf</subfield>
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    <subfield code="s">n</subfield>
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    <subfield code="a">Chiral quasicrystalline order in an exceptional family of viruses</subfield>
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    <subfield code="c">18 May 2011</subfield>
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    <subfield code="a">Understanding of virus capsid organization and self-assembly mechanisms helps to get an insight into the protein interactions which render virus infectious, but also to advance new methods in nanotechnology which use capsid self-assembly to produce virus-like nanoparticles. As in abiotic nanostructures, the obstacles along this way are related not only to the nanoscopic size of capsids but also to their unconventional topology and symmetry. In the present work on the example of exceptional families of viruses we : i) show the existence of a completely new type of organization, resulting in a chiral pentagonal quasicrystalline order of protein positions in a capsid with spherical topology and dodecahedral geometry; ii) generalize the classical theory of quasicrystals (QC) to explain this organization and demonstrate that a particular non-linear phason strain induces chirality in QC; and iii) establish the relation between chiral order and inhomogeneous buckling strain of the capsid shell.</subfield>
  </datafield>
  <datafield tag="500" ind1=" " ind2=" ">
    <subfield code="a">Comments: 8 pages, 2 figures</subfield>
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    <subfield code="a">LANL EDS</subfield>
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  <datafield tag="650" ind1="1" ind2="7">
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    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="a">q-bio.SC</subfield>
    <subfield code="2">arXiv</subfield>
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    <subfield code="a">physics.bio-ph</subfield>
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    <subfield code="a">11</subfield>
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    <subfield code="a">PREPRINT</subfield>
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="c">Hidden</subfield>
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<record>
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    <subfield code="a">arXiv:1106.4765</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Haji-Akbari, Amir</subfield>
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    <subfield code="a">Engel, Michael</subfield>
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    <subfield code="a">Glotzer, Sharon C</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1106.4765.pdf</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201125</subfield>
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    <subfield code="a">Phase Diagram of Hard Tetrahedra</subfield>
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    <subfield code="c">24 Jun 2011</subfield>
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    <subfield code="a">Advancements in the synthesis of faceted nanoparticles and colloids have spurred interest in the phase behavior of polyhedral shapes. Regular tetrahedra have attracted particular attention because they prefer local symmetries that are incompatible with periodicity. Two dense phases of regular tetrahedra have been reported recently. The densest known tetrahedron packing is achieved in a crystal of triangular bipyramids (dimers) with packing density 4000/4671=85.63%. In simulation a dodecagonal quasicrystal is observed; its approximant, with periodic tiling (3.4.3^2.4), can be compressed to a packing fraction of 85.03%. Here, we show that the quasicrystal approximant is more stable than the dimer crystal for packing densities below 84% using Monte Carlo computer simulations and free energy calculations. To carry out the free energy calculations, we use a variation of the Frenkel-Ladd method for anisotropic shapes and thermodynamic integration. The enhanced stability of the approximant can be attributed to a network substructure, which maximizes the free volume (and hence the 'wiggle room') available to the particles and facilitates correlated motion of particles, which further contributes to entropy and leads to diffusion for packing densities below 65%. The existence of a solid-solid transition between structurally distinct phases not related by symmetry breaking -- the approximant and the dimer crystal-- is unusual for hard particle systems.</subfield>
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    <subfield code="a">Comments: 11 pages, 10 figures</subfield>
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    <subfield code="2">arXiv</subfield>
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    <subfield code="2">arXiv</subfield>
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    <subfield code="2">arXiv</subfield>
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    <subfield code="b">Chemical Physics and Chemistry</subfield>
    <subfield code="2">arXiv</subfield>
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    <subfield code="a">physics.chem-ph</subfield>
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    <subfield code="c">2011</subfield>
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    <subfield code="a">11</subfield>
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    <subfield code="a">PREPRINT</subfield>
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="c">Hidden</subfield>
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    <subfield code="9">arXiv</subfield>
    <subfield code="a">oai:arXiv.org:1107.5083</subfield>
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    <subfield code="a">arXiv:1107.5083</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Aliste-Prieto, José</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">Almost periodic structures and the semiconjugacy problem</subfield>
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  <datafield tag="260" ind1=" " ind2=" ">
    <subfield code="c">2011</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">27 Jul 2011</subfield>
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    <subfield code="a">The description of almost periodic or quasiperiodic structures has a long tradition in mathematical physics, in particular since the discovery of quasicrystals in the early 80's. Frequently, the modelling of such structures leads to different types of dynamical systems which include, depending on the concept of quasiperiodicity being considered, skew products over quasiperiodic or almost-periodic base flows, mathematical quasicrystals or maps of the real line with almost-periodic displacement. An important problem in this context is to know whether the considered system is semiconjugate to a rigid translation. We solve this question in a general setting that includes all the above-mentioned examples and also allows to treat scalar differential equations that are almost-periodic both in space and time. To that end, we study a certain class of flows that preserve a one-dimensional foliation and show that a semiconjugacy to a minimal translation flow exists if and only if a boundedness condition, concerning the distance of orbits of the flow to those of the translation, holds.</subfield>
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    <subfield code="a">10.1364/OE.19.023631</subfield>
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    <subfield code="a">oai:arXiv.org:1109.3726</subfield>
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    <subfield code="d">2016-02-18</subfield>
    <subfield code="h">2016-02-18T06:29:01Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1109.3726</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Liew, Seng Fatt</subfield>
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    <subfield code="a">Noh, Heeso</subfield>
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    <subfield code="a">Trevino, Jacob</subfield>
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    <subfield code="a">Negro, Luca Dal</subfield>
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    <subfield code="a">Cao, Hui</subfield>
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  <datafield tag="773" ind1=" " ind2=" ">
    <subfield code="p">Optics Express vol.</subfield>
    <subfield code="v">19</subfield>
    <subfield code="y">2011</subfield>
    <subfield code="c">23631-23642</subfield>
    <subfield code="o">Optics Express vol. 19, pp. 23631-23642 (2011)</subfield>
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    <subfield code="a">Comments: 12pages, 12 figures</subfield>
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    <subfield code="a">Comments: 12pages, 12 figures</subfield>
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    <subfield code="a">We present a numerical study on photonic bandgap and bandedge modes in the golden-angle spiral array of air cylinders in dielectric media. Despite the lack of long-range translational and rotational order, there is a large PBG for the TE polarized light. Due to spatial inhomogeneity in the air hole spacing, the bandedge modes are spatially localized by Bragg scattering from the parastichies in the spiral structure. They have discrete angular momenta that originate from different families of the parastichies whose numbers correspond to the Fibonacci numbers. The unique structural characteristics of the golden-angle spiral lead to distinctive features of the bandedge modes that are absent in both photonic crystals and quasicrystals.</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
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    <subfield code="a">The discovery of topological insulators has sparked considerable interest in the study of topological phases of matter. The hallmark of these novel phases is the emergence of topologically protected boundary phenomena, e.g. quantum pumping, surface states related to exotic models from particle physics, and quasi-particles with non-Abelian statistics. Yet, realizations of these phases of matter are scarce. Moreover, one-dimensional systems without any additional symmetries are considered to lack such topological phenomena. Here we show, both theoretically and experimentally, that quasicrystals reveal new types of topological phases. We demonstrate that one-dimensional quasicrystals exhibit topological properties that were, thus far, thought to be limited to two-dimensional systems. Using photonic quasicrystals, we observe localized boundary states, which manifest these topological properties. These topological boundary states are used to realize an adiabatic optical pumping effect in which photons are uni-directionally pumped across the sample. Generalization to various types of quasicrystals and higher dimensions are also discussed, suggesting the existence of topological effects on surfaces of three-dimensional quasicrystals. This work opens a path to realizing new types of topological phases, and provides new insights to the physics of quasicrystals and topological insulators.</subfield>
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    <subfield code="a">Motivated by recent results in mathematical virology, we present novel asymmetric Z[tau]-integer-valued affine extensions of the non-crystallographic Coxeter groups H_2, H_3 and H_4 derived in a Kac-Moody-type formalism. In particular, we show that the affine reflection planes which extend the Coxeter group H_3 generate (twist) translations along 2-, 3- and 5-fold axes of icosahedral symmetry and classify these translations in terms of Fibonacci recursion relations, thus providing a framework to explain results of Keef et al and Wardman at the group level. Finally, we extend this classification to the case of the non-crystallographic Coxeter groups H_2 and H_4. These results should have applications in physics (quasicrystals), biology (viruses) and chemistry (fullerenes).</subfield>
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    <subfield code="h">2013-10-22T02:02:49Z</subfield>
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    <subfield code="a">Dechant, Pierre-Philippe</subfield>
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    <subfield code="a">Boehm, Celine</subfield>
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  <datafield tag="773" ind1=" " ind2=" ">
    <subfield code="p">J. Math. Phys.</subfield>
    <subfield code="v">54</subfield>
    <subfield code="y">2013</subfield>
    <subfield code="c">093508</subfield>
    <subfield code="o">J. Math. Phys. 54, 093508 (2013)</subfield>
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    <subfield code="a">Affine extensions of non-crystallographic Coxeter groups induced by projection</subfield>
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    <subfield code="c">2013</subfield>
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    <subfield code="a">In this paper, we show that affine extensions of non-crystallographic Coxeter groups can be derived via Coxeter-Dynkin diagram foldings and projections of the root systems E_8, D_6 and A_4. Using the known extensions for these root systems, we induce affine extensions of the non-crystallographic groups H_4, H_3 and H_2, and show that they correspond to Kac-Moody-type extensions considered in Dechant et al. This class of extensions was motivated by physical applications in icosahedral systems in biology (viruses), physics (quasicrystals) and chemistry (fullerenes); the connection with the affine extension of E_8 derived here suggests potential for high energy physics applications. The invertibility of the projection suggests a generalisation of Cartan matrices by relaxing some of the usual requirements.</subfield>
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    <subfield code="a">Comments: 23 pages, 9 figures</subfield>
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    <subfield code="a">oai:arXiv.org:1110.6142</subfield>
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    <subfield code="a">arXiv:1110.6142</subfield>
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    <subfield code="a">Korepin, Vladimir</subfield>
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    <subfield code="a">Gaehler, Franz</subfield>
    <subfield code="u">Mathematics, University of Bielefeld</subfield>
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    <subfield code="a">Rhyner, Jakob</subfield>
    <subfield code="u">United Nations University, Institute for Environment and Human Security</subfield>
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    <subfield code="p">Acta Crystallographica Section A</subfield>
    <subfield code="y">1988</subfield>
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    <subfield code="o">Acta Crystallographica Section A (1988) A44, pages 667-672</subfield>
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    <subfield code="a">Quasiperiodic Tilings: A Generalized Grid--Projection Method</subfield>
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    <subfield code="c">28 Oct 2011</subfield>
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    <subfield code="a">9 p</subfield>
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    <subfield code="a">In 1988 we discovered generalized grid--projection method. Since then the method proved to be useful for description of symmetries of quasicrystals also for analysis of interacting spins.</subfield>
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    <subfield code="a">arXiv:1110.6894</subfield>
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    <subfield code="a">On the spectrum of 1D quantum Ising quasicrystal</subfield>
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    <subfield code="c">01 Nov 2011</subfield>
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    <subfield code="a">We consider one dimensional quantum Ising spin-1/2 chains with two-valued nearest neighbor couplings arranged in a quasi-periodic sequence, with uniform, transverse magnetic field. By employing the Jordan-Wigner transformation of the spin operators to spinless fermions, the energy spectrum can be computed exactly on a finite lattice. By employing the transfer matrix technique and investigating the dynamics of the corresponding trace map, we show that in the thermodynamic limit the energy spectrum is a Cantor set of zero Lebesgue measure. Moreover, we show that local Hausdorff dimension is continuous and nonconstant over the spectrum. This forms a rigorous counterpart of numerous numerical studies.</subfield>
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    <subfield code="a">Comments: 29 pages</subfield>
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    <subfield code="a">This paper introduces a Markov process inspired by the problem of quasicrystal growth. It acts over dimer tilings of the triangular grid by randomly performing local transformations, called {\em flips}, which do not increase the number of identical adjacent tiles (this number can be thought as the tiling energy). Fixed-points of such a process play the role of quasicrystals. We are here interested in the worst-case expected number of flips to converge towards a fixed-point. Numerical experiments suggest a bound quadratic in the number n of tiles of the tiling. We prove a O(n^2.5) upper bound and discuss the gap between this bound and the previous one. We also briefly discuss the average-case.</subfield>
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    <subfield code="a">Comments: 8 pages, 11 figures. Accepted for a Special issue on Photonics of Physica Scripta</subfield>
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    <subfield code="a">Comments: 8 pages, 11 figures. Accepted for a Special issue on Photonics of Physica Scripta</subfield>
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    <subfield code="a">We construct families of ordinary and gap solitons (GSs), including solitary vortices, in the two-dimensional (2D) system based on the nonlinear-Schr\"Aodinger/Gross-Pitaevskii equation with the 2D or quasi-1D (Q1D) periodic linear potential, combined with the periodic modulation of the cubic nonlinearity (also in the 2D or Q1D form), which is, generally, incommensurate with the linear potential, thus forming a \nonlinear quasicrystal". Stable vortices are built as complexes of four peaks with the separation between them equal to the double period of the linear potential. The system may be realized in photonic crystals or Bose-Einstein condensates (BECs). The variational approximation (VA) is applied to ordinary solitons (residing in the semi-infinite gap), and numerical methods are used to construct solitons of all the types. Stability regions are identified for soliton families in all the versions of the model.</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
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    <subfield code="2">arXiv</subfield>
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  <controlfield tag="005">20170907220421.0</controlfield>
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    <subfield code="a">oai:arXiv.org:1202.2240</subfield>
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    <subfield code="a">arXiv:1202.2240</subfield>
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    <subfield code="a">Integral cohomology of rational projection method patterns</subfield>
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    <subfield code="c">13 Feb 2012</subfield>
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    <subfield code="a">We study the cohomology and hence K-theory of the aperiodic tilings formed by the so called `cut and project' method, i.e., patterns in d dimensional Euclidean space which arise as sections of higher dimensional, periodic structures. They form one of the key families of patterns used in quasicrystal physics, where their topological invariants carry quantum mechanical information. Our work develops both a theoretical framework and a practical toolkit for the discussion and calculation of their integral cohomology, and extends previous work that only successfully addressed rational cohomological invariants. Our framework unifies the several previous methods used to study the cohomology of these patterns. We obtain explicit calculational results for the main examples of icosahedral patterns in R^3 -- the Danzer tiling, the Ammann-Kramer tiling and the Canonical and Dual Canonical D_6 tilings -- as well as results for many of the better known 2 dimensional examples.</subfield>
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    <subfield code="a">Comments: Extends, corrects and replaces 2005 preprint math-ph/0505048 'Torsion in Tiling Homology and Cohomology'</subfield>
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    <subfield code="a">LANL EDS</subfield>
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    <subfield code="a">Properties of 1D classical and quantum Ising quasicrystals: rigorous results</subfield>
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    <subfield code="a">In this paper we consider one-dimensional classical and quantum spin-1=2 quasiperiodic Ising chains, with two-valued nearest neighbor interaction modulated by a Fibonacci substitution sequence on two letters. In the quantum case, we investigate the energy spectrum of the Ising Hamiltonian, in presence of constant transverse magnetic field, by employing the techniques that were developed in our previous work. In the classical case, we investigate and prove analyticity of the free energy function when the magnetic field, together with interaction strength couplings, is modulated by the same Fibonacci substitution (thus proving absence of phase transitions of any order at finite temperature). We also investigate the distribution of Lee-Yang zeros of the partition function in the complex magnetic field regime, and prove its Cantor set structure (together with some additional qualitative properties), thus providing a rigorous justification for the observations in some previous works. In both, quantum and classical models, we concentrate on the ferromagnetic class.</subfield>
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    <subfield code="a">Comments: 29 pages, 84 references</subfield>
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    <subfield code="a">oai:arXiv.org:1203.3646</subfield>
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    <subfield code="a">arXiv:1203.3646</subfield>
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    <subfield code="a">Schroedinger difference equation with deterministic ergodic potentials</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">19 Mar 2012</subfield>
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    <subfield code="a">We review the recent developments in the theory of the one-dimensional tight-binding Schr\"odinger equation for a class of deterministic ergodic potentials. In the typical examples the potentials are generated by substitutional sequences, like the Fibonacci or the Thue-Morse sequence. We concentrate on rigorous results which will be explained rather than proved. The necessary mathematical background is provided in the text.</subfield>
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    <subfield code="a">Comments: 51 pages</subfield>
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    <subfield code="a">Title has not been found in the knowledge base. Please add "" </subfield>
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    <subfield code="9">LANL EDS</subfield>
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  <datafield tag="695" ind1=" " ind2=" ">
    <subfield code="a">cond-mat.stat-mech</subfield>
    <subfield code="9">LANL EDS</subfield>
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  <datafield tag="773" ind1=" " ind2=" ">
    <subfield code="p">.</subfield>
    <subfield code="y">1995</subfield>
    <subfield code="o">Beyond Quasicrystals, eds. F. Axel &amp; D. Gratias, Springer-Verlag/Les Editions de Physique 1995, pp. 481-549</subfield>
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    <subfield code="c">2012</subfield>
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  <controlfield tag="005">20170910091159.0</controlfield>
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    <subfield code="a">oai:arXiv.org:1204.4904</subfield>
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    <subfield code="a">arXiv:1204.4904</subfield>
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    <subfield code="a">Spectral Envelopes - A Preliminary Report</subfield>
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    <subfield code="c">2012</subfield>
  </datafield>
  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">24 Apr 2012</subfield>
  </datafield>
  <datafield tag="500" ind1=" " ind2=" ">
    <subfield code="a">Comments: To appear in Proceedings the Annual Meeting in Mathematics, Bangkok, Thailand, April 12, 2012. Sponsored by the Center for Promotion of Mathematical Research of Thailand</subfield>
  </datafield>
  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">The spectral envelope S(F) of a subset of integers is the set of probability measures on the circle group that are weak star limits of squared moduli of trigonometric polynomials with frequencies in F. Fourier transforms of these measures are positive and supported in F - F but the converse generally fails. The characteristic function chiF of F is a binary sequence whose orbit closure gives a symbolic dynamical system O(F). Analytic properties of S(F) are related to dynamical properties of chiF. The Riemann-Lebesque lemma implies that if chiF is minimal, then S(F) is convex and hence S(F) is the closure of the convex hull of its extreme points Se(F). In this paper we (i) review the relationship between these concepts and the special case of the still open 1959 Kadison-Singer problem called Feichtinger's conjecture for exponential functions, (ii) partially characterize of elements in Se(F), for minimal chiF, in terms of ergodic properties of (O(F),lambda) where lambda is a shift invariant probability measure whose existence in ensured by the 1937 Krylov-Bogoyubov theorem, (iii) refine previous numerical studies of the Morse-Thue minimal binary sequence by exploiting a new MATLAB algorithm for computing smallest eigenvalues of 4,000,000 x 4,000,000 matrices, (iv) describe recent results characterizing S(F) for certain Bohr sets F related to quasicrystals, (v) extend these concepts to general discrete groups including those with Kazhdan's T-property, such as SL(n,Z), n > 2, which can be characterized by several equivalent properties such as: any sequence of positive definite functions converging to 1 uniformly on compact subsets converges uniformly. This exotic property may be useful to construct a counterexample to the generalization of Feichtinger's conjecture and hence to provide a no answer to the question of Kadison and Singer whcih they themselves tended to suspect.</subfield>
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    <subfield code="w">201217</subfield>
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    <subfield code="a">11</subfield>
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    <subfield code="b">Comments: To appear in Proceedings the Annual Meeting in Mathematics, Bangkok, Thailand, April 12, 2012. Sponsored by the Center for Promotion of Mathematical Research of Thailand</subfield>
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    <subfield code="a">PREPRINT</subfield>
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    <subfield code="2">DOI</subfield>
    <subfield code="a">10.1088/0031-9120/47/5/568</subfield>
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    <subfield code="a">oai:arXiv.org:1205.3858</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2015-06-05</subfield>
    <subfield code="h">2015-06-06T05:23:26Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1205.3858</subfield>
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  <datafield tag="100" ind1=" " ind2=" ">
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    <subfield code="a">Tomasik, Boris</subfield>
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  <datafield tag="856" ind1="4" ind2=" ">
    <subfield code="u">http://arxiv.org/pdf/1205.3858.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201220</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">Mpemba Effect, Shechtman's Quasicrystals and Students' Exploring Activities</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">18 May 2012</subfield>
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  <datafield tag="300" ind1=" " ind2=" ">
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    <subfield code="a"></subfield>
    <subfield code="9">arXiv</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">In the 1960s, Tanzanian student Erasto Mpemba and his teacher published an article with the title "Cool" in the journal Physics Education (Mpemba, E. B. - Osborne, D. G.: Cool?. In: Physics Education, vol.4, 1969, pp. 172-175.). In this article they claimed that hot water freezes faster than cold water. The article raised not only a wave of discussions, and other articles about this topic, but also a whole series of new experiments, which should verify this apparent thermodynamic absurdity and find an adequate explanation. Here we give a review with references to explanations and we bring some proposals for experimental student work in this area. We introduce Mpemba Effect not only as a paradoxical physics phenomenon, but we shall present a strong educational message that the Mpemba story brings to the teachers and their students. This message also creates a bridge between this phenomenon and the discovery for which the 2011 Nobel Prize in Chemistry was awarded. It leads to critical adoption of traditional knowledge and encourages resilience in investigative exploration of new things.</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
    <subfield code="b">arXiv</subfield>
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  <datafield tag="650" ind1="1" ind2="7">
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    <subfield code="2">arXiv</subfield>
  </datafield>
  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="a">Other Fields of Physics</subfield>
    <subfield code="2">arXiv</subfield>
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    <subfield code="a">PREPRINT</subfield>
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="c">Hidden</subfield>
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  <controlfield tag="001">1471142</controlfield>
  <controlfield tag="003">SzGeCERN</controlfield>
  <controlfield tag="005">20170907220920.0</controlfield>
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    <subfield code="2">DOI</subfield>
    <subfield code="a">10.1007/s00006-013-0422-4</subfield>
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  <datafield tag="035" ind1=" " ind2=" ">
    <subfield code="a">oai:arXiv.org:1207.5005</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2016-07-13</subfield>
    <subfield code="h">2016-07-14T05:19:24Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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  <datafield tag="035" ind1=" " ind2=" ">
    <subfield code="9">Inspire</subfield>
    <subfield code="a">1244672</subfield>
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    <subfield code="a">arXiv:1207.5005</subfield>
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    <subfield code="a">DCPT-12-98</subfield>
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  <datafield tag="100" ind1=" " ind2=" ">
    <subfield code="a">Dechant, Pierre-Philippe</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">A Clifford algebraic framework for Coxeter group theoretic computations</subfield>
  </datafield>
  <datafield tag="260" ind1=" " ind2=" ">
    <subfield code="c">2012</subfield>
  </datafield>
  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">01 Aug 2012</subfield>
  </datafield>
  <datafield tag="300" ind1=" " ind2=" ">
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  <datafield tag="500" ind1=" " ind2=" ">
    <subfield code="a">Comments: Best Paper Award at AGACSE 2012, La Rochelle, France; 14 pages, 3 figures</subfield>
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  <datafield tag="500" ind1=" " ind2=" ">
    <subfield code="a">Comments: Best Paper Award at AGACSE 2012, La Rochelle, France; 18 pages, 4 figures, 2 tables; accepted in Advances in Applied Clifford Algebras</subfield>
    <subfield code="9">arXiv</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">Real physical systems with reflective and rotational symmetries such as viruses, fullerenes and quasicrystals have recently been modeled successfully in terms of three-dimensional (affine) Coxeter groups. Motivated by this progress, we explore here the benefits of performing the relevant computations in a Geometric Algebra framework, which is particularly suited to describing reflections. Starting from the Coxeter generators of the reflections, we describe how the relevant chiral (rotational), full (Coxeter) and binary polyhedral groups can be easily generated and treated in a unified way in a versor formalism. In particular, this yields a simple construction of the binary polyhedral groups as discrete spinor groups. These in turn are known to generate Lie and Coxeter groups in dimension four, notably the exceptional groups D_4, F_4 and H_4. A Clifford algebra approach thus reveals an unexpected connection between Coxeter groups of ranks 3 and 4. We finally discuss how to extend these considerations and computations to the Conformal Geometric Algebra setup.</subfield>
  </datafield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
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    <subfield code="a">LANL EDS</subfield>
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  <datafield tag="650" ind1="1" ind2="7">
    <subfield code="a">Mathematical Physics and Mathematics</subfield>
    <subfield code="2">arXiv</subfield>
  </datafield>
  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="a">cond-mat.mtrl-sci</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="b">Mathematical Physics and Mathematics</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
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    <subfield code="2">arXiv</subfield>
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    <subfield code="a">PREPRINT</subfield>
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    <subfield code="a">math-ph</subfield>
    <subfield code="9">LANL EDS</subfield>
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  <datafield tag="695" ind1=" " ind2=" ">
    <subfield code="a">cond-mat.mtrl-sci</subfield>
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    <subfield code="9">LANL EDS</subfield>
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  <datafield tag="695" ind1=" " ind2=" ">
    <subfield code="a">physics.bio-ph</subfield>
    <subfield code="9">LANL EDS</subfield>
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  <datafield tag="773" ind1=" " ind2=" ">
    <subfield code="p">Volume</subfield>
    <subfield code="y">2014</subfield>
    <subfield code="o">Advances in Applied Clifford Algebras, March 2014, Volume 24, Issue 1, pp 89-108</subfield>
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  <datafield tag="856" ind1="4" ind2=" ">
    <subfield code="u">http://arxiv.org/pdf/1207.5005.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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  <datafield tag="916" ind1=" " ind2=" ">
    <subfield code="s">n</subfield>
    <subfield code="w">201231</subfield>
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  <datafield tag="960" ind1=" " ind2=" ">
    <subfield code="a">11</subfield>
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    <subfield code="a">PREPRINT</subfield>
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    <subfield code="c">Hidden</subfield>
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  <controlfield tag="001">1495017</controlfield>
  <controlfield tag="003">SzGeCERN</controlfield>
  <controlfield tag="005">20160413100434.0</controlfield>
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    <subfield code="a">oai:arXiv.org:1211.4476</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2012-11-20</subfield>
    <subfield code="h">2012-11-20T12:24:37Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="9">Inspire</subfield>
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    <subfield code="a">arXiv:1211.4476</subfield>
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    <subfield code="a">Verbin, Mor</subfield>
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    <subfield code="a">Kraus, Yaacov E</subfield>
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    <subfield code="a">Zilberberg, Oded</subfield>
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    <subfield code="a">Lahini, Yoav</subfield>
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    <subfield code="a">Silberberg, Yaron</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1211.4476.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201247</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">Observation of Topological Phase Transitions in Photonic Quasicrystals</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">20 Nov 2012</subfield>
  </datafield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">Topological insulators and topological superconductors are distinguished by their bulk phase transitions and gapless states at a sharp boundary with the vacuum. Quasicrystals have recently been found to be topologically nontrivial. In quasicrystals, the bulk phase transitions occur in the same manner as standard topological materials, but their boundary phenomena are more subtle. In this work we directly observe bulk phase transitions, using photonic quasicrystals, by constructing a smooth boundary between topologically-distinct one-dimensional quasicrystals. Moreover, we use the same method to experimentally verify the topological equivalence between the Harper and Fibonacci quasicrystals.</subfield>
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    <subfield code="a">Comments: 7 pages, 6 figures, 2 appendices. Comments are welcome</subfield>
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    <subfield code="2">arXiv</subfield>
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    <subfield code="a">General Theoretical Physics</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
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    <subfield code="2">arXiv</subfield>
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    <subfield code="c">2012</subfield>
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  <datafield tag="960" ind1=" " ind2=" ">
    <subfield code="a">11</subfield>
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    <subfield code="a">PREPRINT</subfield>
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    <subfield code="c">Hidden</subfield>
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  <controlfield tag="001">1503454</controlfield>
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  <controlfield tag="005">20171105115753.0</controlfield>
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    <subfield code="a">oai:arXiv.org:1212.3326</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2012-12-17</subfield>
    <subfield code="h">2013-01-07T15:29:24Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1212.3326</subfield>
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    <subfield code="a">Jiang, Kai</subfield>
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    <subfield code="a">Zhang, Pingwen</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1212.3326.pdf</subfield>
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    <subfield code="a">Numerical Methods for Quasicrystals</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">17 Dec 2012</subfield>
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    <subfield code="a">A new projection method, implemented in higher-dimensional reciprocal space, is developed to compute quasicrystals. The approach enables us to represent quasicrystals as periodic structures in higher-dimensional space. A proposed projective matrix can project a higher-dimensional periodic structure into a quasicrystal in physical space. Compared with the traditional crystalline approximant method, the projection method overcomes the restrictions of the Simultaneous Diophantine Approximation, and can use periodic boundary conditions conveniently. Meanwhile, the proposed method can efficiently reduce the computational complexity through implementing in a unit cell and using pseudospectral method. By applying the projection method to the Lifshitz-Petrich model, we can compute quasicrystals rather than crystalline approximants, maintaining the rotational symmetry accurately. More significantly, the algorithm can calculate the free energy density to high precision.</subfield>
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    <subfield code="c">255503</subfield>
    <subfield code="o">Phys. Rev. Lett. 110, 255503 (2013)</subfield>
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    <subfield code="a">Computing phase diagrams for a quasicrystal-forming patchy-particle system</subfield>
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    <subfield code="c">12 Feb 2013</subfield>
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    <subfield code="a">We introduce an approach to computing the free energy of quasicrystals, which we use to calculate equilibrium phase diagrams for systems of two-dimensional patchy particles with five regularly arranged patches that have previously been shown to form dodecagonal quasicrystals. We find that the quasicrystal is a thermodynamically stable phase for a wide range of conditions and remains a robust feature of the system as the potential's parameters are varied. We also demonstrate that the quasicrystal is entropically stabilised over its crystalline approximants.</subfield>
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    <subfield code="a">Perk, Jacques H H</subfield>
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    <subfield code="p">Indagationes Mathematicae</subfield>
    <subfield code="v">24</subfield>
    <subfield code="y">2013</subfield>
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    <subfield code="o">Indagationes Mathematicae 24 (2013) 996-1017</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">Quasicrystals -- The impact of N.G. de Bruijn</subfield>
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    <subfield code="c">27 Jun 2013</subfield>
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    <subfield code="a">33 p</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">In this paper we put the work of Professor N.G. de Bruijn on quasicrystals in historical context. After briefly discussing what went before, we shall review de Bruijn's work together with recent related theoretical and experimental developments. We conclude with a discussion of Yang-Baxter integrable models on Penrose tilings, for which essential use of de Bruijn's work has been made.</subfield>
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    <subfield code="a">Comments: pdfLaTeX, 33 pages, 15 figures, submitted to Indagationes Mathematicae</subfield>
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    <subfield code="a">11</subfield>
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    <subfield code="a">PREPRINT</subfield>
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    <subfield code="c">Hidden</subfield>
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    <subfield code="h">2013-07-04T02:07:46Z</subfield>
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    <subfield code="a">Bond orientational ordering in liquids: Towards a unified description of water-like anomalies, liquid-liquid transition, glass transition, and crystallization</subfield>
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    <subfield code="c">02 Jul 2013</subfield>
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    <subfield code="a">85 p</subfield>
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    <subfield code="a">There are at least three fundamental states of matter, depending upon temperature and pressure: gas, liquid, and solid (crystal). These states are separated by first-order phase transitions between them. In both gas and liquid phases the complete translational and rotational symmetry exist, whereas in a solid phase both symmetries are broken. In intermediate phases between liquid and solid, which include liquid crystal and plastic crystal phases, only one of the two symmetries is preserved. Among the fundamental states of matter, the liquid state is most poorly understood. We argue that it is crucial for a better understanding of liquid to recognize that a liquid generally has a tendency to have local structural order and its presence is intrinsic and universal to any liquid. Such structural ordering is a consequence of many body correlations, more specifically, bond angle correlations, which we believe are crucial for the description of the liquid state. We show that this physical picture may naturally explain difficult unsolved problems associated with the liquid state, such as anomalies of water-type liquids (water, Si, Ge, ...), liquid-liquid transition, liquid-glass transition, crystallization and quasicrystal formation, in a unified manner. In other words, we need a new order parameter representing low local free-energy configuration, which is bond orientational order parameter in many cases, in addition to density order parameter for the physical description of these phenomena. Here we review our two-order-parameter model of liquid and consider how transient local structural ordering is linked to all of the above-mentioned phenomena. The relationship between these phenomena are also discussed.</subfield>
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    <subfield code="a">Comments: Colloquium paper, 85 pages, 62 figures</subfield>
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    <subfield code="p">Eur. Phys. J. E</subfield>
    <subfield code="v">35</subfield>
    <subfield code="y">2012</subfield>
    <subfield code="c">113</subfield>
    <subfield code="o">Eur. Phys. J. E 35, 113 (2012)</subfield>
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    <subfield code="d">2013-09-16</subfield>
    <subfield code="h">2013-09-16T02:03:36Z</subfield>
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    <subfield code="a">arXiv:1309.3286</subfield>
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    <subfield code="a">R, Ajith P</subfield>
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    <subfield code="a">Yallapragada, V J</subfield>
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    <subfield code="a">Patil, Raj</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">V., Nikesh V</subfield>
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    <subfield code="a">Mulay, Gajendra</subfield>
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    <subfield code="a">Gopal, Achanta Venu</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1309.3286.pdf</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201337</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">Plasmonic quasicrystals for designable ultra broadband transmission enhancement and second harmonic generation</subfield>
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    <subfield code="c">12 Sep 2013</subfield>
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    <subfield code="a">10 p</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">Quasi-crystals are intriguing as they exhibit rotational symmetry and long range ordering but lack translational symmetry. 2-dimensional metal-dielectric patterns are interesting to make use of surface plasmon polariton (SPP) mediated local field enhancement and for near dispersionless SPP modes. In plasmonic crystals, the orientation and periodicity of the pattern dictate the polarization response and the discrete plasmon resonances while the interfaces define the plasmon dispersion. However, unique properties of plasmonic quasicrystals lead to polarization independence, designable k-space and broadband transmission enhancement due to SPP mediation. These are useful in many applications like energy harvesting, nonlinear optics and quantum plasmonics. We demonstrate design and fabrication of large area quasicrystal air hole patterns of pi/5 symmetry in metal film in which broadband, launch angle and polarization independent transmission enhancement as well as broadband second harmonic generation are observed. Designable transmission response, other symmetries and tilings are possible.</subfield>
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    <subfield code="a">Comments: 10 pages, 4 figures</subfield>
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    <subfield code="a">LANL EDS</subfield>
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    <subfield code="a">10.1088/1464-4258/11/2/024007</subfield>
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    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1311.0386</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Zito, G</subfield>
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    <subfield code="a">Piccirillo, B</subfield>
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    <subfield code="a">Santamato, E</subfield>
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    <subfield code="a">Marino, A</subfield>
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    <subfield code="a">Tkachenko, V</subfield>
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    <subfield code="a">Abbate, G</subfield>
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    <subfield code="p">Pure Appl. Opt.</subfield>
    <subfield code="v">11</subfield>
    <subfield code="y">2009</subfield>
    <subfield code="c">024007</subfield>
    <subfield code="o">J. Opt. A: Pure Appl. Opt. 11 (2009) 024007 (8pp)</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1311.0386.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201344</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">FDTD analysis of photonic quasicrystals with different tiling geometries and fabrication by single beam computer-generated holography</subfield>
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    <subfield code="c">02 Nov 2013</subfield>
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    <subfield code="a">8 p</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">Multiple-beam holography has been widely used for the realization of photonic quasicrystals with high rotational symmetries not achievable by the conventional periodic crystals. Accurate control of the properties of the interfering beams is necessary to provide photonic band-gap structures. Here we show, by FDTD simulations of the transmission spectra of 8-fold quasiperiodic structures, how the geometric tiling of the structure affects the presence and properties of the photonic band-gap for low refractive index contrasts. Hence, we show an interesting approach to the fabrication of photonic quasicrystals based on the use of a programmable Spatial Light Modulator encoding Computer-Generated Holograms, that permits an accurate control of the writing pattern with almost no limitations in the pattern design. Using this single-beam technique we fabricated quasiperiodic structures with high rotational symmetries and different geometries of the tiling, demonstrating the great versatility of our technique.</subfield>
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    <subfield code="a">Comments: 8 pages, 6 figures</subfield>
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    <subfield code="a">LANL EDS</subfield>
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  <datafield tag="650" ind1="1" ind2="7">
    <subfield code="a">Other Fields of Physics</subfield>
    <subfield code="2">arXiv</subfield>
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    <subfield code="a">Article</subfield>
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    <subfield code="c">Hidden</subfield>
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    <subfield code="a">10.1088/2040-8978/13/1/015602</subfield>
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    <subfield code="a">oai:arXiv.org:1311.0392</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2013-11-05</subfield>
    <subfield code="h">2013-11-05T03:04:50Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1311.0392</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Matarazzo, V</subfield>
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    <subfield code="a">De Nicola, S</subfield>
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    <subfield code="a">Zito, G</subfield>
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    <subfield code="a">Mormile, P</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Rippa, M</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Abbate, G</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Zhou, J</subfield>
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    <subfield code="a">Petti, L</subfield>
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  <datafield tag="773" ind1=" " ind2=" ">
    <subfield code="p">J. Opt.</subfield>
    <subfield code="v">13</subfield>
    <subfield code="y">2011</subfield>
    <subfield code="c">015602</subfield>
    <subfield code="o">Journal of Optics 13 015602 2011</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1311.0392.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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  <datafield tag="916" ind1=" " ind2=" ">
    <subfield code="s">n</subfield>
    <subfield code="w">201344</subfield>
  </datafield>
  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">Spectral characterization of two-dimensional Thue-Morse quasicrystals realized with high resolution lithography</subfield>
  </datafield>
  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">02 Nov 2013</subfield>
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  <datafield tag="300" ind1=" " ind2=" ">
    <subfield code="a">8 p</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">One-dimensional Thue-Morse (ThMo) lattices are examples of self-similar structures that exhibit bandgap phenomena. ThMo multilayers may also possess fractal photonic bandgaps that give rise to large omnidirectional reflectance and light emission enhancement effects. Two-dimensional (2D) ThMo aperiodic quasicrystals possess interesting properties for photonic applications too. Here we demonstrate the experimental fabrication of large area 2D ThMo lattices into polymeric substrates at nanometer scale by electron beam lithography (EBL). Far field diffraction patterns of the experimental Thue-Morse structures have been measured and compared with the calculated theoretical Fourier spectra. Scanning electron microscopy and far field diffraction are used to characterize the experimental structures.</subfield>
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    <subfield code="a">Comments: 8 pages, 5 figures</subfield>
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    <subfield code="a">LANL EDS</subfield>
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  <datafield tag="650" ind1="1" ind2="7">
    <subfield code="a">Other Fields of Physics</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="695" ind1=" " ind2=" ">
    <subfield code="a">physics.optics</subfield>
    <subfield code="9">LANL EDS</subfield>
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    <subfield code="a">Article</subfield>
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    <subfield code="c">Hidden</subfield>
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    <subfield code="2">DOI</subfield>
    <subfield code="a">10.1364/OE.21.019972</subfield>
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    <subfield code="a">oai:arXiv.org:1311.2963</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2013-11-14</subfield>
    <subfield code="h">2013-11-14T03:04:05Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1311.2963</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Man, Weining</subfield>
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    <subfield code="a">Florescu, Marian</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Matsuyama, Kazue</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Yadak, Polin</subfield>
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    <subfield code="a">Nahal, Geev</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Hashemizad, Seyed</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Williamson, Eric</subfield>
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    <subfield code="a">Steinhardt, Paul</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Torquato, Salvatore</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Chaikin, Paul</subfield>
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  <datafield tag="773" ind1=" " ind2=" ">
    <subfield code="o">Optics Express 21 (17), 19972-19981 (2013)</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1311.2963.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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  <datafield tag="916" ind1=" " ind2=" ">
    <subfield code="s">n</subfield>
    <subfield code="w">201345</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">Photonic band gap in isotropic hyperuniform disordered solids with low dielectric contrast</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">12 Nov 2013</subfield>
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    <subfield code="a">mult. p</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">We report the first experimental demonstration of a TE-polarization photonic band gap (PBG) in a 2D isotropic hyperuniform disordered solid (HUDS) made of dielectric media with a index contrast of 1.6:1, very low for PBG formation. The solid is composed of a connected network of dielectric walls enclosing air-filled cells. Direct comparison with photonic crystals and quasicrystals permitted us to investigate band-gap properties as a function of increasing rotational isotropy. We present results from numerical simulations proving that the PBG observed experimentally for HUDS at low index contrast has zero density of states. The PBG is associated with the energy difference between complementary resonant modes above and below the gap, with the field predominantly concentrated in the air or in the dielectric. The intrinsic isotropy of HUDS may offer unprecedented flexibilities and freedom in applications (i. e. defect architecture design) not limited by crystalline symmetries.</subfield>
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    <subfield code="a">LANL EDS</subfield>
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  <datafield tag="650" ind1="1" ind2="7">
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    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="a">cond-mat.mtrl-sci</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="b">Other Fields of Physics</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="695" ind1=" " ind2=" ">
    <subfield code="a">cond-mat.mes-hall</subfield>
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    <subfield code="a">physics.optics</subfield>
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    <subfield code="c">2013</subfield>
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    <subfield code="a">13</subfield>
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    <subfield code="c">Hidden</subfield>
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    <subfield code="2">DOI</subfield>
    <subfield code="a">10.1103/PhysRevB.91.064201</subfield>
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    <subfield code="a">oai:arXiv.org:1403.7124</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
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    <subfield code="h">2015-03-05T06:19:50Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1403.7124</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Verbin, Mor</subfield>
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    <subfield code="a">Zilberberg, Oded</subfield>
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    <subfield code="a">Lahini, Yoav</subfield>
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    <subfield code="a">Kraus, Yaacov E</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Silberberg, Yaron</subfield>
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  <datafield tag="773" ind1=" " ind2=" ">
    <subfield code="p">Phys. Rev. B</subfield>
    <subfield code="v">91</subfield>
    <subfield code="y">2015</subfield>
    <subfield code="c">064201</subfield>
    <subfield code="o">Phys. Rev. B 91, 064201 (2015)</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1403.7124.pdf</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201412</subfield>
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    <subfield code="a">Topological Pumping over a Photonic Fibonacci Quasicrystal</subfield>
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    <subfield code="c">27 Mar 2014</subfield>
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    <subfield code="a">5 p</subfield>
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    <subfield code="a">Comments: 5 pages, 4 figures, comments are welcome</subfield>
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    <subfield code="a">Comments: 5 pages, 4 figures, comments are welcome</subfield>
    <subfield code="9">arXiv</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">Quasiperiodic lattices have recently been shown to be a non-trivial topological phase of matter. Charge pumping -- one of the hallmarks of topological states of matter -- was recently realized for photons in a one-dimensional (1D) off-diagonal Harper model implemented in a photonic waveguide array. The topologically nontrivial 1D Fibonacci quasicrystal (QC) is expected to facilitate a similar phenomenon, but its discrete nature and lack of pumping parameter hinder the experimental study of such topological effects. In this work we overcome these obstacles by utilizing a family of topologically equivalent QCs which ranges from the Fibonacci QC to the Harper model. Implemented in photonic waveguide arrays, we observe the topological properties of this family, and perform a topological pumping of photons across a Fibonacci QC.</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
    <subfield code="b">arXiv</subfield>
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    <subfield code="a">LANL EDS</subfield>
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    <subfield code="2">arXiv</subfield>
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    <subfield code="a">General Theoretical Physics</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="b">cond-mat.mtrl-sci</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
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    <subfield code="2">arXiv</subfield>
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    <subfield code="a">cond-mat.mtrl-sci</subfield>
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    <subfield code="a">physics.optics</subfield>
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  <datafield tag="695" ind1=" " ind2=" ">
    <subfield code="a">quant-ph</subfield>
    <subfield code="9">LANL EDS</subfield>
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  <datafield tag="260" ind1=" " ind2=" ">
    <subfield code="c">2014</subfield>
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    <subfield code="a">11</subfield>
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    <subfield code="a">0210359CERCER</subfield>
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    <subfield code="a">Bovier, A</subfield>
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    <subfield code="a">Schrödinger operators generated by substitutions</subfield>
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  <datafield tag="260" ind1=" " ind2=" ">
    <subfield code="c">1995</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">12 Oct 1995</subfield>
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    <subfield code="a">mult. p</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">Schr\"odinger operators with potentials generated by primitive substitutions are simple models for one dimensional quasi-crystals. We review recent results on their spectral properties. These include in particular an algorithmically verifiable sufficient condition for their spectrum to be singular continuous and supported on a Cantor set of zero Lebesgue measure. Applications to specific examples are discussed.</subfield>
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    <subfield code="a">LANL EDS</subfield>
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  <datafield tag="650" ind1="1" ind2="7">
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    <subfield code="a">We report on the fabrication of what we believe is the first example of a two dimensional nonlinear periodic crystal\cite{berger}, where the refractive index is constant but in which the 2nd order nonlinear susceptibility is spatially periodic. Such a crystal allows for efficient quasi-phase matched 2nd harmonic generation using multiple reciprocal lattice vectors of the crystal lattice. External 2nd harmonic conversion efficiencies > 60% were measured with picosecond pulses. The 2nd harmonic light can be simultaneously phase matched by multiple reciprocal lattice vectors, resulting in the generation of multiple coherent beams. The fabrication technique is extremely versatile and allows for the fabrication of a broad range of 2-D crystals including quasi-crystals.</subfield>
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    <subfield code="a">In the same fashion that Einstein's General Relativity required Riemannian Geometry for its foundations, the New Relativity Theory requires a Cantorian-Fractal Spacetime, which is an example of Von Neumann's Noncommutative Geometry. Starting from first principles, an ensemble distribution for all the infinite dimensions of quantum spacetime is derived that required Fermat's last theorem. An explicit computation of the average dimension yields a value very close to the exact number $4+\phi^3 $, obtained previously from the Cantorian-Fractal Spacetime Model. The quantity $\phi$ is the Golden Mean. The Cosmological " constant problem " is never an issue within the framework of the New Relativity, since the Universe automatically self-organizes and self-tunes itself according to the Renormalization Group flow with respect to a local scaling microscopic arrow of time. The world began as a result of a non-equilibrium process of self-organized critical phenomena due to vacuum fluctuations in Cantorian-Fractal Spacetime. It is proven why we live today in a metastable vacuum and are flowing to the RG fixed point of $ D = 4 +\phi^3$. A new phase transition will then drive the Universe to a quasi-crystal phase of lower average dimensions given by $\phi^3$. Finally, we write down the Unique Quantum Master Interacting Action functional for the world in {\bf C}-space, (outside spacetime), that governs the quantum dynamics for the creation of spacetime, gravity and all of the fundamental forces in Nature.</subfield>
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    <subfield code="a">The structures formation of the Universe appears as if it were a classically self-similar random process at all astrophysical scales. An agreement is demonstrated for the present hypotheses of segregation with a size of astrophysical structures by using a comparison between quantum quantities and astrophysical ones. We present the observed segregated Universe as the result of a fundamental self-similar law, which generalizes the Compton wavelength relation. It appears that the Universe has a memory of its quantum origin as suggested by R.Penrose with respect to quasi-crystal. A more accurate analysis shows that the present theory can be extended from the astrophysical to the nuclear scale by using generalized (stochastically) self-similar random process. This transition is connected to the relevant presence of the electromagnetic and nuclear interactions inside the matter. In this sense, the presented rule is correct from a subatomic scale to an astrophysical one. We discuss the near full agreement at organic cell scale and human scale too. Consequently the Universe, with its structures at all scales (atomic nucleus, organic cell, human, planet, solar system, galaxy, clusters of galaxy, super clusters of galaxy), could have a fundamental quantum reason. In conclusion, we analyze the spatial dimensions of the objects in the Universe as well as spacetime dimensions. The result is that it seems we live in an El Naschie's E infinity Cantorian spacetime; so we must seriously start considering fractal geometry as the geometry of nature, a type of arena where the laws of physics appear at each scale in a self--similar way as advocated long ago by the Swedish school of astrophysics.</subfield>
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    <subfield code="a">Intrinsic Localized Modes (ILM) (or Discrete Breathers, DB) are localized oscillatory modes known to occur in atomic or molecular chains characterized by coupling and/or on-site potential nonlinearity. Quasi-crystals of charged mesoscopic dust grains (dust lattices), which have been observed since hardly a decade ago, are an exciting paradigm of such a nonlinear chain. In gas-discharge experiments, these crystals are subject to forces due to an externally imposed electric and/or magnetic field(s), which balance(s) gravity at the levitated equilibrium position, as well as to electrostatic inter-grain interaction forces. Despite the profound role of nonlinearity, which may be due to inter-grain coupling, mode- coupling and to the sheath environment, the elucidation of the nonlinear mechanisms governing dust crystals is still in a preliminary stage. This study is devoted to an investigation, from very first principles, of the existence of discrete localized modes in dust layers. Relying on a set of evolution equation for transverse charged grain displacements, we examine the conditions for the existence and sustainance of discrete localized modes and discuss the dependence of their characteristics on intrinsic plasma parameters. In addition, the possibility of DB stabilisation via an external force is discussed.</subfield>
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    <subfield code="a">Quasi-crystals formed by charged mesoscopic dust grains (dust lattices), observed since hardly a decade ago, are an exciting paradigm of a nonlinear chain. In laboratory discharge experiments, these quasi-lattices are formed spontaneously in the sheath region near a negative electrode, usually at a levitated horizontal equilibrium configuration where gravity is balanced by an electric field. It is long known (and experimentally confirmed) that dust-lattices support linear oscillations, in the longitudinal (acoustic mode) as well as in the transverse, in plane (acoustic-) or off-plane (optic-like mode) directions. Either due to the (typically Yukawa type) electrostatic inter-grain interaction forces or to the (intrinsically nonlinear) sheath environment, nonlinearity is expected to play an important role in the dynamics of these lattices. Furthermore, the coupling between the different modes may induce coupled nonlinear modes. Despite this evidence, the elucidation of the nonlinear mechanisms governing dust crystals is in a rather preliminary stage. In this study, we derive a set of (coupled) discrete equations of motion for longitudinal and transverse (out-of-plane) motion in a one dimensional model chain of charged dust grains. In a continuum approximation, i.e. assuming a variation scale which is larger than the lattice constant, one obtains a set of coupled modified Boussinesq-like equations. Different nonlinear solutions of the coupled system are discussed, based on localized travelling wave ansatze and on coupled equations for the envelopes of co-propagating quasi-linear waves.</subfield>
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    <subfield code="a">The first explicit realization of the conjecture that phason dynamics leads to self-diffusion in quasicrystals is presented for the icosahedral Ammann tilings. On short time scales, the transport is found to be subdiffusive with the exponent \beta\approx0.57(1), while on long time scales it is consistent with normal diffusion that is up to an order of magnitude larger than in the typical room temperature vacancy-assisted self-diffusion. No simple finite-size scaling is found, suggesting anomalous corrections to normal diffusion, or existence of at least two independent length scales.</subfield>
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    <subfield code="a">We present a simple model for the observed temperature dependence of the thermal conductivity of AlPdMn (Chernikov et al, Phys.Rev.B vol.51, (1995),153). We account for the low temperature data, upto and including the plateau of the thermal conductivity, and discuss the similarities and the differences between the quasicrystal and amorphous solids.</subfield>
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    <subfield code="a">We introduce a new transfer matrix method for calculating the thermodynamic properties of random-tiling models of quasicrystals in any number of dimensions, and describe how it may be used to calculate the phason elastic properties of these models, which are related to experimental measurables such as phason Debye-Waller factors, and diffuse scattering wings near Bragg peaks. We apply our method to the canonical-cell model of the icosahedral phase, making use of results from a previously-presented calculation in which the possible structures for this model under specific periodic boundary conditions were cataloged using a computational technique. We give results for the configurational entropy density and the two fundamental elastic constants for a range of system sizes. The method is general enough allow a similar calculation to be performed for any other random tiling model.</subfield>
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    <subfield code="a">We have studied the influence of a particular kind of phason-defect on the Landauer resistance of a Fibonacci chain. Depending on parameters, we sometimes find the resistance to decrease upon introduction of defect or temperature, a behavior that also appears in real quasicrystalline materials. We demonstrate essential differences between a standard tight-binding model and a full continuous model. In the continuous case, we study the conductance in relation to the underlying chaotic map and its invariant. Close to conducting points, where the invariant vanishes, and in the majority of cases studied, the resistance is found to decrease upon introduction of a defect. Subtle interference effects between a sudden phason-change in the structure and the phase of the wavefunction are also found, and these give rise to resistive behaviors that produce exceedingly simple and regular patterns.</subfield>
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    <subfield code="a">Scattering of electrons due to fractons can result in a resistivity that {\it decreases} with temperature. Such a behavior also appears in real quasicrystals. If this is then attributed to fracton scattering, fracton-superconductivity would be theoretically possible. By fitting with the scattering result the experimental resistivity data for the AlPdMn quasicrystal, we estimate the corresponding T_c. This effective fracton interpretation, not unexpected for a self-similar system, is also found consistent with other experiments on thermal and acoustic properties of the AlPdMn quasicrystal.</subfield>
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    <subfield code="a">We present a molecular dynamics study on atomic self-diffusion in Frank-Kasper type dodecagonal quasicrystals. It is found that the quasicrystal-specific flip mechanism for atomic diffusion as predicted by Kalugin and Katz, indeed occurs in this system. However, in order to be effective, this mechanism needs to be catalyzed by other defects such as half-vacancies if the structure is truly three-dimensional. For this reason, flip diffusion is difficult to distinguish from standard vacancy diffusion. In a quasi-two-dimensional setup, however, the flips may occur without other defects. Activation energies and flip frequencies are also determined.</subfield>
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    <subfield code="a">A generalization of the Drude model is studied. On the one hand, the free motion of the particles is allowed to be sub- or superdiffusive; on the other hand, the distribution of the time delay between collisions is allowed to have a long tail and even a non-vanishing first moment. The collision averaged motion is either regular diffusive or Lévy-flight like. The anomalous diffusion coefficients show complex scaling laws. The conductivity can be calculated in the diffusive regime. The model is of interest for the phenomenological study of electronic transport in quasicrystals.</subfield>
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    <subfield code="a">A combination of classical density-functional theory and thermodynamic perturbation theory is applied to a survey of finite-temperature trends in the relative stabilities of one-component crystals and quasicrystals interacting via effective metallic pair potentials derived from pseudopotential theory. Comparing the free energies of several periodic crystals and rational approximant models of quasicrystals over a range of pseudopotential parameters, thermodynamically stable quasicrystals are predicted for parameters approaching the limits of mechanical stability of the crystal structures. Quasicrystalline stability is attributed to vibrational stiffness and energetically favorable medium- and long-range interactions. The results support and significantly extend conclusions of previous ground-state lattice-sum studies.</subfield>
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    <subfield code="a">To describe structural peculiarities in inhomogeneous media caused by the tendency to the close packing of atoms a formalism based on the using of the Riemann geometry methods (which were successfully applied lately to the description of structures of quasicrystals and glasses) is developed. Basing on this formalism we find in particular the criterion of stability of precipitates of the Frank-Kasper phases in metallic systems. The nature of the ''rhenium effect'' in W-Re alloys is discussed.</subfield>
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    <subfield code="a">Three-dimensional icosahedral random tilings with rhombohedral cells are studied in the semi-entropic model. We introduce a global energy measure defined by the variance of the quasilattice points in the orthogonal space. The internal energy, the specific heat, the configuration entropy and the sheet magnetization (as defined by Dotera and Steinhardt [Phys.Rev.Lett. 72 (1994) 1670]) have been calculated. The specific heat shows a Schottky anomaly which might indicate a phase transition from an ordered quasicrystal to a random tiling. But the divergence with the sample size as well as the divergence of the susceptibility are too small to pinpoint the phase transition conclusively. The self-diffusion coefficients closely follow an Arrhenius law, but show plateaus at intermediate temperature ranges which are explained by energy barriers between different tiling configurations due to the harmonic energy measure. There exists a correlation between the temperature behavior of the self-diffusion coefficient and the frequency of vertices which are able to flip (simpletons). Furthermore we demonstrate that the radial distribution function and the radial structure factor only depend slightly on the random tiling configuration. Hence, radially symmetric pair potentials lead to an energetical equidistribution of all configurations of a canonical random tiling ensemble and do not enforce matching rules.</subfield>
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    <subfield code="a">Formation of a Dodecagonal Quasicrystalline Phase in a Simple Monatomic Liquid</subfield>
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    <subfield code="a">In a recent paper M. Dzugutov, Phys. Rev. Lett. 70 2924 (1993), describes a molecular dynamics cooling simulation where he obtained a large monatomic dodecagonal quasicrystal from a melt. The structure was stabilized by a special potential [Phys. Rev. A46 R2984 (1992)] designed to prevent the nucleation of simple dense crystal structures. In this comment we will give evidence that the ground state structure for Dzugutov's potential is an ordinary bcc crystal.</subfield>
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    <subfield code="a">A Universal Formula for Percolation Thresholds; 2, Extension to Anisotropic and Aperiodic Lattices</subfield>
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    <subfield code="a">In a recent paper, we have reported a universal power law for both site and bond percolation thresholds in any Bravais lattice with q equivalent nearest neighbors in dimension d. We now extend it to three different classes of lattices which are, respectively, anisotropic lattices whith not equivalent nearest neighbors, non-Bravais lattices with two atom unit cells, and quasicrystals. The investigation is focussed on d=2 and d=3, due to the lack of experimental data at higher dimensions. The extension to these lattices requires the substitution of q by an effective (non integer) value $q_{eff}$ in the universal law. For each out of 17 lattices which constitute our sample, we argue the existence of one $q_{eff}$ which reproduces both the site and the percolation threshold, with a deviation with respect to numerical estimates which does not exceed $\mp 0.01$.</subfield>
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    <subfield code="a">A dislocation moving through a quasicrystal is leaving in its wake a fault denoted phason wall. For a two-dimensional model quasicrystal the disregistry energy of this phason wall is studied to determine possible Burgers vectors of the quasicrystalline structure. Contrary to periodic crystals, the disregistry energy is an average quantity with large fluctuations on the atomic scale. Therefore the dislocation core structure and mobility cannot be linked to this quantity e.g. by a Peierls-Nabarro model. Atomistic simulations show that dislocation motion is controlled by local obstacles inherent to the atomic structure of the quasicrystal.</subfield>
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    <subfield code="a">We present a review of some results concerning electronic transport properties of quasicrystals. After a short introduction to the basic concepts of quasiperiodicity, we consider the experimental transport properties of electrical conductivity with particular focus on the effect of temperature, magnetic field and defects. Then, we present some heuristic approaches that tend to give a coherent view of different, and to some extent complementary, transport mechanisms in quasicrystals. Numerical results are also presented and in particular the evaluation of the linear response Kubo-Greenwood formula of conductivity in quasiperiodic systems in presence of disorder.</subfield>
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    <subfield code="a">The notion of magnetic symmetry is reexamined in light of the recent observation of long range magnetic order in icosahedral quasicrystals [Charrier et al., Phys. Rev. Lett. 78, 4637 (1997)]. The relation between the symmetry of a magnetically-ordered (periodic or quasiperiodic) crystal, given in terms of a ``spin space group,'' and its neutron diffraction diagram is established. In doing so, an outline of a symmetry classification scheme for magnetically ordered quasiperiodic crystals is provided. Predictions are given for the expected diffraction patterns of magnetically ordered icosahedral crystals, provided their symmetry is well described by icosahedral spin space groups.</subfield>
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    <subfield code="a">The elastic theory of quasicrystals considers, in addition to the normal displacement field, three phason degrees of freedom. We present an approximative solution for the elastic Green's function of icosahedral quasicrystals, assuming that the coupling between the phonons and phasons is small.</subfield>
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    <subfield code="a">Freezing of charge-stabilized colloidal suspensions and relative stabilities of crystals and quasicrystals are studied using thermodynamic perturbation theory. Macroion interactions are modelled by effective pair potentials combining electrostatic repulsion with polymer-depletion or van der Waals attraction. Comparing free energies -- counterion terms included -- for elementary crystals and rational approximants to icosahedral quasicrystals, parameters are identified for which one-component quasicrystals are stabilized by a compromise between packing entropy and cohesive energy.</subfield>
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    <subfield code="a">Conway and Radin's ``quaquaversal'' tiling of R^3 is known to exhibit statistical rotational symmetry in the infinite volume limit. A finite patch, however, cannot be perfectly isotropic, and we compute the rates at which the anisotropy scales with size. In a sample of volume N, tiles appear in O(N^{1/6}) distinct orientations. However, the orientations are not uniformly populated. A small (O(N^{1/84})) set of these orientations account for the majority of the tiles. Furthermore, these orientations are not uniformly distributed on SO(3). Sample averages of functions on SO(3) seem to approach their ergodic limits as N^{-1/336}. Since even macroscopic patches of a quaquaversal tiling maintain noticable anisotropy, a hypothetical physical quasicrystal whose structure was similar to the quaquaversal tiling could be identified by anisotropic features of its electron diffraction pattern.</subfield>
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    <subfield code="a">Model sets (or cut and project sets) provide a familiar and commonly used method of constructing and studying nonperiodic point sets. Here we extend this method to situations where the internal spaces are no longer Euclidean, but instead spaces with p-adic topologies or even with mixed Euclidean/p-adic topologies. We show that a number of well known tilings precisely fit this form, including the chair tiling and the Robinson square tilings. Thus the scope of the cut and project formalism is considerably larger than is usually supposed. Applying the powerful consequences of model sets we derive the diffractive nature of these tilings.</subfield>
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    <subfield code="a">A guide to mathematical quasicrystals</subfield>
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    <subfield code="a">For the orthorhombic intermetallic semiconductor Al$_2$Ru, the bandstructure, valence charge density, zone center optical phonon frequencies, and Born effective charge and electronic dielectric tensors are calculated using variational density functional perturbation theory with {\em ab initio} pseudopotentials and a plane wave basis set. Good agreement is obtained with recent measurements on polycrystalline samples which showed anomalously strong far IR absorption by optical phonons, while analysis of the valence charge density shows that the static ionic charges of Al and Ru are negligible. Hybridization is proposed as the single origin both of the semiconducting gap and the anomalous Born effective charges. Analogous behavior is expected in related compounds such as NiSnZr, PbTe, skutterudites, and Al-transition-metal quasicrystals.</subfield>
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    <subfield code="a">When the charge density in a crystal or a quasicrystal is reconstructed from its Fourier modes, the global minimum value of the density is sensitively dependent on the relative phases of the modes. The set of phases that maximizes the value of the global minimum, corresponds, by positivity of the density, to the charge density having the minimum total charge that is consistent with the measured Fourier amplitudes. Phases which minimize the total charge (i.e. the average charge density) also have the property that the lowest minima of the charge density become exactly degenerate and proliferate within the unit cell. The large number of degenerate minima have the effect that density maxima are forced to occupy ever smaller regions of the unit cell. Thus by minimizing charge, the atomicity of the charge density is enhanced as well. Charge minimization applied to simulated crystalline and quasicrystalline diffraction data successfully reproduces the correct phases starting from random initial values.</subfield>
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    <subfield code="a">Understanding the growth of quasicrystals poses a challenging problem, not the least because the quasiperiodic order present in idealized mathematical models of quasicrystals prohibit simple local growth algorithms. This can only be circumvented by allowing for some degree of disorder, which of course is always present in real quasicrystalline samples. In this review, we give an overview of the present state of theoretical research, addressing the problems, the different approaches and the results obtained so far.</subfield>
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    <subfield code="a">Comparing different approaches to model the atomic structure of a ternary decagonal quasicrystal</subfield>
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    <subfield code="a">It is shown that the covering approach with a single decagonal prototile can be transformed into a hexagon, boat and star tiling. Particularly, the atomic decoration recently proposed by Cockayne and Widom (Phys. Rev. Lett. 81, 598 (1998)) as a structure model for the decagonal phase is investigated. There, conflicts with the prototile approach arise which are due to specific peculiarities of the decoration. The above model is compared with recent experimental images which give strong support to its main features, but contradict competing structure proposals. The implications for the stabilization mechanism are discussed.</subfield>
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    <subfield code="a">Surfaces in i-Al68Pd23Mn9 as observed with STM and LEED experiments show atomic terraces in a Fibonacci spacing. We analyze them in a bulk tiling model due to Elser which incorporates many experimental data. The model has dodecahedral Bergman clusters within an icosahedral tiling T^*(2F) and is projected from the 6D face-centered hypercubic lattice. We derive the occurrence and Fibonacci spacing of atomic planes perpendicular to any 5fold axis, compute the variation of planar atomic densities, and determine the (auto-) correlation functions. Upon interpreting the planes as terraces at the surface we find quantitative agreement with the STM experiments.</subfield>
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    <subfield code="a">Quasicrystals</subfield>
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    <subfield code="a">In this paper, a technique for describing quasiperiodic structures is suggested, which allows one by the assigned matching to restore the atom density distribution formula of a corresponding quasicrystal. The algorithm to restore the atom density distribution has been considered on the example of the Penrose matching. The analytical record of a Penrose quasicrystal is given.</subfield>
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    <subfield code="a">In the window approach to quasicrystals, the atomic position space E_parallel is embedded into a space E^n = E_parallel + E_perp. Windows are attached to points of a lattice Lambda in E^n . For standard 5fold and icosahedral tiling models, the windows are perpendicular projections of dual Voronoi and Delone cells from Lambda. Their cuts by the position space E_parallel mark tiles and atomic positions. In the alternative covering approach, the position space is covered by overlapping copies of a quasi-unit cell which carries a fixed atomic configuration. The covering and window approach to quasicrystals are shown to be dual projects: D- and V-clusters are defined as projections to position space E_parallel of Delone or Voronoi cells. They are linked, cover position space and have definite windows. For functions compatible with the tilings they form domains of definition. Decagonal V-clusters in the Penrose tiling, related to the decagon covering, and two types of pentagonal D-clusters in the 5fold triangle tiling with their windows are analyzed. For icosahedral tilings the V-clusters are Kepler triacontahedra, the D-clusters are two icosahedra and one dodecahedron.</subfield>
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    <subfield code="a">The shelling of crystals is concerned with counting the number of atoms on spherical shells of a given radius and a fixed centre. Its straight-forward generalization to quasicrystals, the so-called central shelling, leads to non-universal answers. As one way to cope with this situation, we consider shelling averages over all quasicrystal points. We express the averaged shelling numbers in terms of the autocorrelation coefficients and give explicit results for the usual suspects, both perfect and random.</subfield>
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    <subfield code="a">Generic quantum interference effects occuring in 1D-quasicrystals are shown and discussed in details. By defining specific geometrical defects, so-called phasons, one shows that conversely to metallic systems quantum conductance in quasiperiodic systems enclosed original behavior with respect to the alteration of its properties while downgrading long range order. This is in close conjunction with the still open problematic in real quasicrystalline materials.</subfield>
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    <subfield code="a">Contributions of quantum interference effects occuring in quasicrystals are emphasized. First conversely to metallic systems, quasiperiodic ones are shown to enclose original alterations of their conductive properties while downgrading long range order. Besides, origins of localization mechanisms are outlined within the context of the original metal-insulator transition (MIT) found in these materials.</subfield>
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    <subfield code="a">This paper considers the problem of characterizing the simplest discrete point sets that are aperiodic, using invariants based on topological dynamics. A Delone set whose patch-counting function N(T), for radius T, is finite for all T is called repetitive if there is a function M(T) such that every ball of radius M(T)+T contains a copy of each kind of patch of radius T that occurs in the set. This is equivalent to the minimality of an associated topological dynamical system with R^n-action. There is a lower bound for M(T) in terms of N(T), namely N(T) = O(M(T)^n), but no general upper bound. The complexity of a repetitive Delone set can be measured by the growth rate of its repetitivity function M(T). For example, M(T) is bounded if and only if the set is a crystal. A set is called is linearly repetitive if M(T) = O(T) and densely repetitive if M(T) = O(N(T))^{1/n}). We show that linearly repetitive sets and densely repetitive sets have strict uniform patch frequencies, i.e. the associated topological dynamical system is strictly ergodic. It follows that such sets are diffractive. In the reverse direction, we construct a repetitive Delone set in R^n which has M(T) = O(T(log T)^{2/n}(log log log T)^{4/n}), but does not have uniform patch frequencies. Aperiodic linearly repetitive sets have many claims to be the simplest class of aperiodic sets, and we propose considering them as a notion of "perfectly ordered quasicrystal".</subfield>
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    <subfield code="a">The theory of magnetic symmetry in quasicrystals is used to characterize the nature of magnetic peaks, expected in elastic neutron diffraction experiments. It is established that there is no symmetry-based argument which forbids the existence of quasiperiodic long-range magnetic order. Suggestions are offered as to where one should look for the simplest kinds of antiferromagnetic quasicrystals.</subfield>
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    <subfield code="a">A phenomenological diffusion law $L(t)\propto t^{\beta}$, where L(t) measures the spreading of a wave-packet in a time t, is assumed for perfect quasicrystals. We show that it affects their conductivity with striking differences compared to the case of periodic metals. In the absence of defects the dissipative part of conductivity is non zero even at low frequencies contrary to the case of crystals. Also if $\beta&lt;1/2$ the d.c. conductivity increases when disorder increases and the so-called Drude peak, characteristic of metals, is replaced by a dip . Experimental results are briefly discussed.</subfield>
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    <subfield code="a">Although the effects of interactions in solid state systems still remains a widely open subject, some limiting cases such as the three dimensional Fermi liquid or the one-dimensional Luttinger liquid are by now well understood when one is dealing with interacting electrons in {\it periodic} crystalline structures. This problem is much more fascinating when periodicity is lacking as it is the case in {\it quasicrystalline} structures. Here, we discuss the influence of the interactions in quasicrystals and show, on a controlled one-dimensional model, that they lead to anomalous transport properties, intermediate between those of an interacting electron gas in a periodic and in a disordered potential.</subfield>
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    <subfield code="a">We study the Lyapunov exponent for electron and phonon excitations, in pure and random Fibonacci quasicrystal chains, using an exact real space renormalization group method, which allows the calculation of the Lyapunov exponent as a function of the energy. It is shown that the Lyapunov exponent on a pure Fibonacci chain has a self-similar structure, characterized by a scaling index that is independent of the energy for the electron excitations, ''diagonal'' or ''off-diagonal'' quasiperiodic, but is a function of the energy for the phonon excitations. This scaling behavior implies the vanishing of the Lyapunov exponent for the states on the spectrum, and hence the absence of localization on the Fibonacci chain, for the various excitations considered. It is also shown that disordered Fibonacci chains, with random tiling that introduces phason flips at certain sites on the chain, exhibit the same Lyapunov exponent as the pure Fibonacci chain, and hence this type of disorder is irrelevant, either in the case of electron or phonon excitations.</subfield>
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    <subfield code="a">The magnetoconductivity of quasicrystals is often discussed in the frame of quantum corrections, namely weak (anti-) localiza-tion and electron-electron interaction. A premise for both effects is a strong elastic scattering of conduction electrons. Amorphous and icosahedral phases are discussed as Hume-Rothery alloys with an electronically induced structural peak at the diameter of the Fermi sphere. Therefore, both should exhibit quantum corrections. The preparation of quasicrystalline films via the amorphous route offers the possibility to compare the magnetoconductivity on samples of identical composition but different structure. We report on magnetoconduc-tivity measurements at temperatures between 0.2 K and 22 K and for magnetic fields up to 16 T. With the exception of the electronic diffusion constant, amorphous as well as icosahedral Al-Pd-Re films can be described by nearly the same set of parameters if the samples are well on the metallic side of the metal-insulator transition.</subfield>
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    <subfield code="a">In recent computer simulations of a simple monatomic system interacting viathe Dzugutov pair potential, freezing of the fluid into an equilibriumdodecagonal quasicrystal has been reported [M. Dzugutov, Phys. Rev. Lett. 70,2924 (1993)]. Here, using a combination of molecular dynamics simulation andthermodynamic perturbation theory, we conduct a detailed analysis of therelative stabilities of solid-phase structures of the Dzugutov-potentialsystem. At low pressures, the most stable structure is found to be a bcccrystal, which gives way at higher pressures to an fcc crystal. Although adodecagonal quasicrystal and a sigma-phase crystal compete with the bcc crystalfor stability, they remain always metastable.</subfield>
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    <subfield code="a">We show how quasicystals can be used to improve the statistical properties of PRNGs. We discuss the statistical properties of both the aperiodic pseudorandom number generators (APRNGs) and the aperiodic pseudorandom bit generators (APRBGs). We show that there exists a class of APRNGs which generate pseudorandom sequences that cannot be distinguished from a truly random sequence using the spectral test (when the generated sequence is sufficiently long). We give empirical results using the Diehard test suite and the Maurer test. Finally, we describe the implementation of numeric and symbolic methods for generating quasicrystal points and discuss their respective computational complexity.</subfield>
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    <subfield code="a">How, in principle, could one solve the atomic structure of a quasicrystal, modeled as a random tiling decorated by atoms, and what techniques are available to do it? One path is to solve the phase problem first, obtaining the density in a higher dimensional space which yields the_averaged_ scattering density in 3-dimensional space by the usual construction of an incommensurate cut. A novel direct method for this is summarized and applied to an i(AlPdMn) data set. This averaged density falls short of a true structure determination (which would reveal the typical_unaveraged_ atomic patterns.) We discuss the problematic validity of inferring an ideal structure by simply factoring out a ``perp-space'' Debye-Waller factor, and we test this using simulations of rhombohedral tilings. A second, ``unified'' path is to relate the measured and modeled intensities directly, by adjusting parameters in a simulation to optimize the fit. This approach is well suited for unifying structural information from diffraction and from minimizing total energies derived ultimately from ab-initio calculations. Finally, we discuss the special pitfalls of fitting random-tiling decagonal phases.</subfield>
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    <subfield code="a">One-dimensional quasilattices, namely, the geometrical objects to represent quasicrystals, are classified into mutual local-derivability (MLD) classes. Besides the familiar class, there exist an infinite number of new MLD-classes, and different MLD-classes are distinguished by the inflation rules of their representatives. It has been found that one-electron properties of a new MLD-class are characterized by the presence of marginal critical states, which are considered to be nearly localized states.</subfield>
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    <subfield code="a">It is argued that the definition of quasicrystals should not include the requirement that they possess an axis of symmetry that is forbidden in periodic crystals. The term "quasicrystal" should simply be regarded as an abbreviation for "quasiperiodic crystal," possibly with two provisos, as discussed below. The argument is supported by theoretical as well as experimental examples of quasicrystals without any forbidden symmetry.</subfield>
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    <subfield code="a">The Rauzy tilings were proposed recently in a generalisation of the Fibonacci chain by Vidal and Mosseri. These tilings have a particularly simple theoretical description, making them appealing candidates for analytical solutions for electronic properties. We show by a numerical study of statistical properties of the tight-binding spectra that these tilings fall in an intermediate category between the crystal and the quasicrystal, i.e. in a class of almost integrable models.</subfield>
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    <subfield code="a">We report the observation of an anomalous {27}Al-NMR response of a single grain Al_{72.4}Pd_{20.5}Mn_{7.1} icosahedral quasicrystal at low temperatures. In an external magnetic field of 6 T and upon decreasing temperature, we observe a sharp 100 % increase of the resonance linewidth at 2.5 K. No further changes of the linewidth are observed down to 0.05 K. The linewidth enhancement is accompanied by a small but distinct increase of the spin-lattice relaxation rate T_{1}^{-1} and by a maximum of the spin-spin relaxation time T_{2}(T). All these anomalies are absent in external fields of 2.5 T and below. Our observations indicate unusual variations in the stability of isolated magnetic moments in a quasiperiodic metallic environment.</subfield>
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    <subfield code="a">In this paper the problem of the theory of a quasicrystal structures - the determination of coordinates of each atom of quasicrystal in analytical form - is solved. Within the framework of the proposed model a periodic crystal can be presented as a particular case of a quasicrystal. The simple and explicit analytical formulas which describe the location of each atom in a quasicrystal are given. The exact solutions for Penrose and Ammann-Beenker quasicrystal structures are given. On the basis of the analytical formulas the routines are created. The routines are inserted directly into graphical files generating the quasiperiodic structures.</subfield>
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    <subfield code="a">11</subfield>
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    <subfield code="a">PREPRINT</subfield>
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="c">Hidden</subfield>
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    <subfield code="t">true</subfield>
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    <subfield code="a">arXiv:1411.6318</subfield>
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    <subfield code="a">Tománek, David</subfield>
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    <subfield code="a">We present a scheme to categorize the structure of different layered phosphorene allotropes by mapping their non-planar atomic structure onto a two-color 2D triangular tiling pattern. In the buckled structure of a phosphorene monolayer, we assign atoms in "top" positions to dark tiles and atoms in "bottom" positions to light tiles. Optimum $sp^3$ bonding is maintained throughout the structure when each triangular tile is surrounded by the same number $N$ of like-colored tiles, with $0{\le}N{\le}2$. Our ab initio density functional calculations indicate that both the relative stability and electronic properties depend primarily on the structural index $N$. The proposed mapping approach may also be applied to phosphorene structures with non-hexagonal rings and 2D quasicrystals with no translational symmetry, which we predict to be nearly as stable as the hexagonal network.</subfield>
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    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="a">cond-mat.mtrl-sci</subfield>
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    <subfield code="c">Hidden</subfield>
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    <subfield code="a">10.1038/ncomms9269</subfield>
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    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1501.02591</subfield>
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    <subfield code="p">Nature Communications</subfield>
    <subfield code="v">6</subfield>
    <subfield code="y">2015</subfield>
    <subfield code="c">8269</subfield>
    <subfield code="o">Nature Communications 6, 8269 (2015)</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1501.02591.pdf</subfield>
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    <subfield code="a">Bloch-like wave dynamics in disordered potentials based on supersymmetry</subfield>
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    <subfield code="c">12 Jan 2015</subfield>
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    <subfield code="a"></subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">Bloch's theorem for the description of waves in crystals was a major milestone, establishing the principle of bandgaps for electrical, optical, and vibrational waves. Although it was once believed that bandgaps could form only under conditions of periodicity and long-range correlations as the prerequisites for Bloch's theorem, this restriction was disproven by the groundbreaking discoveries of amorphous media and quasicrystals. While network and liquid models have been suggested for the interpretation of Bloch-like waves in disordered media, these approaches 'searching' for random networks with bandgaps have failed in the deterministic creation of bandgaps. Here, we reveal a deterministic pathway to bandgap engineering in disordered media, by applying the notion of supersymmetry to the fundamental wave equation. Inspired by the problem for isospectrality, we follow a methodology in stark contrast to previous methods: we 'transform' ordered potentials into disordered potentials while 'preserving' bandgaps. Our approach enables the formation of bandgaps having disorder comparable to Brownian motion, and allows the 'tuning' of long-range correlations while maintaining identical bandgaps thereby creating 'Bloch wave family'. These results not only extend the frontier of disordered conditions for Bloch-like waves, but also introduce an intriguing postulate: the supersymmetry between ordered and disordered potentials, both with coherence.</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
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    <subfield code="c">2015</subfield>
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  <datafield tag="960" ind1=" " ind2=" ">
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="c">Hidden</subfield>
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  <controlfield tag="001">2009338</controlfield>
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    <subfield code="a">oai:arXiv.org:1504.03938</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2015-04-16</subfield>
    <subfield code="h">2015-04-16T08:07:25Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1504.03938</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Zhang, Xiao</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1504.03938.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201515</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">Two dimensional photonic quasicrystal edge states protected by second Chern number</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">15 Apr 2015</subfield>
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    <subfield code="a">mult. p</subfield>
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    <subfield code="a">Topological physics in photonic systems have attracted great attentions in recent years. In this work, we theoretically study the one and two dimensional photonic quasicrystal resonator lattices characterized by the first and second Chern number, which show exotic boundary states within the photonic energy band gap. In particular, the second Chern number protected edge states has opened up new possibilities for realizing topological physics of dimensions higher than three in photonic systems, which is highly sought for. Such photonic systems can be easily experimentally realized in regular photonic crystal with dielectric rods in air, by varying the radius of the rods, so we propose experiments realizing our predictions.</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
    <subfield code="b">arXiv</subfield>
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    <subfield code="a">LANL EDS</subfield>
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  <datafield tag="650" ind1="1" ind2="7">
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    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="a">Other Fields of Physics</subfield>
    <subfield code="2">arXiv</subfield>
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    <subfield code="a">cond-mat.mes-hall</subfield>
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  <datafield tag="960" ind1=" " ind2=" ">
    <subfield code="a">11</subfield>
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    <subfield code="a">PREPRINT</subfield>
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="c">Hidden</subfield>
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<record>
  <controlfield tag="001">2011952</controlfield>
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  <controlfield tag="005">20160412200159.0</controlfield>
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    <subfield code="2">DOI</subfield>
    <subfield code="a">10.1016/j.optmat.2015.04.051</subfield>
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    <subfield code="a">oai:arXiv.org:1504.06214</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2015-05-11</subfield>
    <subfield code="h">2015-05-11T05:18:20Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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  <datafield tag="037" ind1=" " ind2=" ">
    <subfield code="a">arXiv:1504.06214</subfield>
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    <subfield code="a">eng</subfield>
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  <datafield tag="100" ind1=" " ind2=" ">
    <subfield code="a">Brand, E R</subfield>
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    <subfield code="a">Costa, C H</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Vasconcelos, M S</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Anselmo, D H A L</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Mello, V D</subfield>
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  <datafield tag="856" ind1="4" ind2=" ">
    <subfield code="u">http://arxiv.org/pdf/1504.06214.pdf</subfield>
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    <subfield code="s">n</subfield>
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    <subfield code="a">Octonacci Photonic Quasicrystals</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">23 Apr 2015</subfield>
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  <datafield tag="500" ind1=" " ind2=" ">
    <subfield code="a">Comments: Submitted to Optical Materials</subfield>
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  <datafield tag="500" ind1=" " ind2=" ">
    <subfield code="a">Comments: Submitted to Optical Materials</subfield>
    <subfield code="9">arXiv</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">We study theoretically the transmission spectra in one-dimensional photonic quasicrystals, made up of SiO$_2$($A$) and TiO$_2$($B$) materials, organized following the Octonacci sequence, where the $n$th-stage of the multilayer $S_{n}$ is given by the rule $S_{n}=S_{n-1}S_{n-2}S_{n-1}$, for $n\geq 3$ and with $S_{1}=A$ and $S_{2}=B$. The expression for transmittance was obtained by employing a theoretical calculation based in the transfer-matrix method. To normally incident waves, we observe that, for a same generation, the transmission spectra for TE and TM waves are equal, at least qualitatively, and they present a scaling property where a self-similar behavior is obtained, as an evidence that these spectra are fractals. The spectra show regions where the omnidirectional band gaps emerges for specific generations of Octonacci photonic structure, except to TM waves. For TE waves, we note that all of them have the almost same width, for different generations. We also report the localization of modes as a consequence of the quasiperiodicity of the heterostructure</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
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    <subfield code="a">LANL EDS</subfield>
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    <subfield code="2">arXiv</subfield>
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    <subfield code="2">arXiv</subfield>
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    <subfield code="c">2015</subfield>
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  <datafield tag="960" ind1=" " ind2=" ">
    <subfield code="a">11</subfield>
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    <subfield code="a">PREPRINT</subfield>
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="c">Hidden</subfield>
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  <controlfield tag="001">2015791</controlfield>
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    <subfield code="a">oai:arXiv.org:1505.02400</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2015-05-12</subfield>
    <subfield code="h">2015-05-13T05:20:02Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1505.02400</subfield>
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  <datafield tag="100" ind1=" " ind2=" ">
    <subfield code="a">Ghulinyan, Mher</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1505.02400.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201519</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">One-dimensional photonic quasicrystals</subfield>
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    <subfield code="c">10 May 2015</subfield>
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    <subfield code="a">16 p</subfield>
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    <subfield code="a">In this chapter, first we will address principal aspects of 1D quasiperiodicity with a particular focus on 1D Fibonacci chains. Further, the rest of the chapter will be dedicated to the electromagnetic counterpart of 1D Fibonacci structures as a relatively simplest case of the large class of photonic quasicrystals.</subfield>
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    <subfield code="a">Comments: 16 pages, 17 figures, from "Light Localisation and Lasing", Eds. M. Ghulinyan, L. Pavesi, Cambridge Univ. Press (2015) Ch. 5, p. 99</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
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    <subfield code="a">LANL EDS</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="a">cond-mat.mes-hall</subfield>
    <subfield code="2">arXiv</subfield>
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    <subfield code="a">11</subfield>
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    <subfield code="a">PREPRINT</subfield>
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="c">Hidden</subfield>
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    <subfield code="a">10.1021/acsnano.5b04181</subfield>
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    <subfield code="p">ACS Nano</subfield>
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    <subfield code="a">Digital Alchemy for Materials Design and Optimization</subfield>
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    <subfield code="a">Starting with the early alchemists, a holy grail of science has been to make desired materials by modifying the attributes of basic building blocks. Building blocks that show promise for assembling new complex materials can be synthesized at the nanoscale with attributes that would astonish the ancient alchemists in their versatility. However, this versatility means that making direct connection between building block attributes and bulk behavior is both necessary for rationally engineering materials, and difficult because building block attributes can be altered in many ways. Here we show how to exploit the malleability of the valence of colloidal nanoparticle "elements" to directly and quantitatively link building block attributes to bulk behavior through a statistical thermodynamic framework we term "digital alchemy". We use this framework to optimize building blocks for a given target structure, and to determine which building block attributes are most important to control for self assembly, through a set of novel thermodynamic response functions, moduli and susceptibilities. We thereby establish direct links between the attributes of colloidal building blocks and the bulk structures they form. Moreover, our results give concrete solutions to the more general conceptual challenge of optimizing emergent behaviors in nature, and can be applied to other types of matter. As examples, we apply digital alchemy to systems of truncated tetrahedra, rhombic dodecahedra, and isotropically interacting spheres that self assemble diamond, FCC, and icosahedral quasicrystal structures, respectively.</subfield>
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    <subfield code="t">true</subfield>
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    <subfield code="a">Hasman, Erez</subfield>
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    <subfield code="p">Phys. Rev. Lett.</subfield>
    <subfield code="v">115</subfield>
    <subfield code="y">2015</subfield>
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    <subfield code="o">Phys. Rev. Lett. 115, 205501 (2015)</subfield>
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    <subfield code="a">Optical Mode Control by Geometric Phase in Quasicrystal Metasurface</subfield>
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    <subfield code="c">24 Jul 2015</subfield>
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    <subfield code="a">30 p</subfield>
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    <subfield code="a">Comments: 30 pages, 10 figures including Supplemental Material</subfield>
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    <subfield code="a">We report on the observation of optical spin-controlled modes from a quasicrystalline metasurface as a result of an aperiodic geometric phase induced by anisotropic subwavelength structure. When geometric phase defects are introduced in the aperiodic structured surface, the modes exhibit polarization helicity dependence resulting in the optical spin-Hall effect. The radiative thermal dispersion bands from a quasicrystal structure were studied where the observed bands arise from the optical spin-orbit interaction induced by the aperiodic space-variant orientations of anisotropic antennas. The optical spin-flip behavior of the revealed modes that arise from the geometric phase pickup was experimentally observed within the visible spectrum by measuring the spin-projected diffraction patterns. The introduced ability to manipulate the light-matter interaction of quasicrystals in a spin-dependent manner provides the route for molding light via spin-optical aperiodic artificial planar surfaces.</subfield>
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    <subfield code="a">physics.optics</subfield>
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    <subfield code="a">PREPRINT</subfield>
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    <subfield code="c">Hidden</subfield>
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    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1509.04028</subfield>
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    <subfield code="a">Barak, A</subfield>
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    <subfield code="a">Fisher, A</subfield>
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    <subfield code="a">Akkermans, E</subfield>
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    <subfield code="a">Topological properties of Fibonacci quasicrystals : A scattering analysis of Chern numbers</subfield>
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    <subfield code="c">14 Sep 2015</subfield>
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    <subfield code="a">mult. p</subfield>
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    <subfield code="a">We report on a study of topological properties of Fibonacci quasicrystals. Chern numbers which label the dense set of spectral gaps, are shown to result from the underlying palindromic symmetry. Topological and spectral features are related to the two independent phases of the scattering matrix: the total phase shift describing the frequency spectrum and the chiral phase sensitive to topological features. Conveniently designed gap modes with spectral properties directly related to the Chern numbers allow to scan these phases. An effective topological Fabry-Perot cavity is presented.</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
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    <subfield code="a">LANL EDS</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
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    <subfield code="c">Hidden</subfield>
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    <subfield code="a">10.1103/PhysRevB.94.064107</subfield>
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    <subfield code="a">oai:arXiv.org:1604.06426</subfield>
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    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="9">Inspire</subfield>
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    <subfield code="a">Boyle, Latham</subfield>
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    <subfield code="a">Steinhardt, Paul J</subfield>
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    <subfield code="p">Phys. Rev. B</subfield>
    <subfield code="v">94</subfield>
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    <subfield code="c">064107</subfield>
    <subfield code="o">Phys. Rev. B 94, 064107 (2016)</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1604.06426.pdf</subfield>
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    <subfield code="s">n</subfield>
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    <subfield code="a">Reflection Quasilattices and the Maximal Quasilattice</subfield>
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    <subfield code="c">21 Apr 2016</subfield>
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    <subfield code="a">5 p</subfield>
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    <subfield code="a">Comments: 6 pages, no figures, important references added, matches Phys Rev B version</subfield>
    <subfield code="9">arXiv</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">We introduce the concept of a {\it reflection quasilattice}, the quasiperiodic generalization of a Bravais lattice with irreducible reflection symmetry. Among their applications, reflection quasilattices are the reciprocal (i.e. Bragg diffraction) lattices for quasicrystals and quasicrystal tilings, such as Penrose tilings, with irreducible reflection symmetry and discrete scale invariance. In a follow-up paper, we will show that reflection quasilattices can be used to generate tilings in real space with properties analogous to those in Penrose tilings, but with different symmetries and in various dimensions. Here we prove that reflection quasilattices only exist in dimensions two, three and four, and we prove that there is a unique reflection quasilattice in dimension four: the "maximal reflection quasilattice" in terms of dimensionality and symmetry. We further show that, unlike crystallographic Bravais lattices, all reflection quasilattices are invariant under rescaling by certain discrete scale factors. We tabulate the complete set of scale factors for all reflection quasilattices in dimension $d>2$, and for all those with quadratic irrational scale factors in $d=2$.</subfield>
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    <subfield code="b">Mathematical Physics and Mathematics</subfield>
    <subfield code="2">arXiv</subfield>
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    <subfield code="a">10.1038/nphoton.2015.107</subfield>
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    <subfield code="h">2016-04-28T05:22:56Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1604.08124</subfield>
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    <subfield code="a">Boriskina, Svetlana V</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1604.08124.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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  <datafield tag="916" ind1=" " ind2=" ">
    <subfield code="s">n</subfield>
    <subfield code="w">201617</subfield>
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    <subfield code="a">Quasicrystals: Making invisible materials</subfield>
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    <subfield code="a">5 p</subfield>
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    <subfield code="a">All-dielectric photonic quasicrystals may act as zero-refractive-index homogeneous materials despite their lack of translational symmetry and periodicity, stretching wavelengths to infinity and offering applications in light wavefront sculpting and optical cloaking.</subfield>
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    <subfield code="a">Comments: 5 pages, 2 figures</subfield>
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    <subfield code="a">LANL EDS</subfield>
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    <subfield code="2">arXiv</subfield>
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    <subfield code="o">Nature Photonics 9(7):422-424, June 2015</subfield>
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    <subfield code="c">2016</subfield>
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    <subfield code="c">Hidden</subfield>
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  <controlfield tag="005">20171102143152.0</controlfield>
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    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1605.06107</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Xavier, Jolly</subfield>
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    <subfield code="a">Probst, Juergen</subfield>
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    <subfield code="a">Becker, Christiane</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1605.06107.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201621</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">Deterministic aperiodic composite lattice-structured silicon thin films for photon management</subfield>
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    <subfield code="c">19 May 2016</subfield>
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    <subfield code="a">Exotic manipulation of the flow of photons in nanoengineered semiconductor materials with an aperiodic distribution of nanostructures plays a key role in efficiency-enhanced and industrially viable broadband photonic technologies. Through a generic deterministic nanotechnological route, in addition to periodic, transversely quasicrystallographic or disordered random photonic lattices, here we show scalable nanostructured semiconductor thin films on large area nanoimprinted substrates up to 4cm^2 with advanced functional features of aperiodic composite nanophotonic lattices having tailorable supercell tiles. The richer Fourier spectra of the presented artificially nanostructured materials with well-defined lattice point morphologies are designed functionally akin to two-dimensional incommensurate intergrowth aperiodic lattices-comprising periodic photonic crystals and in-plane quasicrystals as subgroups. The composite photonic lattice-structured crystalline silicon thin films with tapered nanoholes or nanocone-nanoholes are presented showing up to +30 % achievable short circuit current density in comparison to a periodic counterpart where as it is up to +190 % in comparison to a reference unstructured silicon thin film of 300 nanometers of thickness. In view of scalable bottom-up integrated device fabrication processes, the structural analysis is further extended to liquid phase crystallized double-side-textured deterministic aperiodic lattice-structured 10 micrometers thick large area crystalline silicon film.</subfield>
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    <subfield code="2">arXiv</subfield>
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    <subfield code="2">arXiv</subfield>
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    <subfield code="9">LANL EDS</subfield>
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    <subfield code="c">2016</subfield>
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    <subfield code="a">PREPRINT</subfield>
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    <subfield code="a">11</subfield>
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    <subfield code="a">PREPRINT</subfield>
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="c">Hidden</subfield>
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<record>
  <controlfield tag="001">2194898</controlfield>
  <controlfield tag="003">SzGeCERN</controlfield>
  <controlfield tag="005">20171103220956.0</controlfield>
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    <subfield code="a">oai:arXiv.org:1606.08302</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2016-06-28</subfield>
    <subfield code="h">2016-06-28T05:18:34Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1606.08302</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Gao, Zhen</subfield>
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    <subfield code="a">Gao, Fei</subfield>
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    <subfield code="a">Zhang, Youming</subfield>
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    <subfield code="a">Xu, Hongyi</subfield>
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    <subfield code="a">Zhang, Baile</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1606.08302.pdf</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201626</subfield>
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    <subfield code="a">Surface-wave photonic quasicrystal</subfield>
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    <subfield code="c">27 Jun 2016</subfield>
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    <subfield code="a">In developing strategies of manipulating surface electromagnetic waves, it has been recently recognized that a complete forbidden band gap can exist in a periodic surface-wave photonic crystal, which has subsequently produced various surface-wave photonic devices. However, it is not obvious whether such a concept can be extended to a non-periodic surface-wave system that lacks translational symmetry. Here we experimentally demonstrate that a surface-wave photonic quasicrystal that lacks periodicity can also exhibit a forbidden band gap for surface electromagnetic waves. The lower cutoff of this forbidden band gap is mainly determined by the maximum separation between nearest neighboring pillars. Point defects within this band gap show distinct properties compared to a periodic photonic crystal for the absence of translational symmetry. A line-defect waveguide, which is crafted out of this surface-wave photonic quasicrystal by shortening a random row of metallic rods, is also demonstrated to guide and bend surface waves around sharp corners along an irregular waveguiding path.</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
    <subfield code="b">arXiv</subfield>
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    <subfield code="a">LANL EDS</subfield>
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    <subfield code="a">PREPRINT</subfield>
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    <subfield code="c">Hidden</subfield>
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<record>
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  <controlfield tag="005">20171102143213.0</controlfield>
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    <subfield code="a">oai:arXiv.org:1607.00901</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2016-07-05</subfield>
    <subfield code="h">2016-07-05T05:18:50Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1607.00901</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Dareau, A</subfield>
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    <subfield code="a">Levy, E</subfield>
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    <subfield code="a">Aguilera, M Bosch</subfield>
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    <subfield code="a">Bouganne, R</subfield>
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    <subfield code="a">Akkermans, E</subfield>
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    <subfield code="a">Gerbier, F</subfield>
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    <subfield code="a">Beugnon, J</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1607.00901.pdf</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201627</subfield>
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    <subfield code="a">Direct measurement of Chern numbers in the diffraction pattern of a Fibonacci chain</subfield>
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    <subfield code="c">04 Jul 2016</subfield>
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    <subfield code="a">mult. p</subfield>
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    <subfield code="a">Topological properties are now understood to be a key feature of many different physical systems, from topological insulators to quasicrystals. Such properties are often encoded into integer-valued topological invariants, such as winding or Chern numbers, usually related to transport or spectral measurements. We report on an experiment where the Chern numbers of quasicrystalline structures are directly determined by an interferometric approach. We show that all the possible Chern numbers for finite-length Fibonacci chains can be observed directly in their diffraction pattern. Finally, we also demonstrate quantitatively the stability of these topological invariants with respect to structural disorder.</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
    <subfield code="b">arXiv</subfield>
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    <subfield code="a">LANL EDS</subfield>
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    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="a">General Theoretical Physics</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="b">cond-mat.mtrl-sci</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="b">Other Fields of Physics</subfield>
    <subfield code="2">arXiv</subfield>
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    <subfield code="a">cond-mat.mes-hall</subfield>
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    <subfield code="a">cond-mat.mtrl-sci</subfield>
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    <subfield code="a">physics.optics</subfield>
    <subfield code="9">LANL EDS</subfield>
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  <datafield tag="695" ind1=" " ind2=" ">
    <subfield code="a">quant-ph</subfield>
    <subfield code="9">LANL EDS</subfield>
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    <subfield code="c">2016</subfield>
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    <subfield code="a">PREPRINT</subfield>
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  <datafield tag="960" ind1=" " ind2=" ">
    <subfield code="a">11</subfield>
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="a">PREPRINT</subfield>
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="c">Hidden</subfield>
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<record>
  <controlfield tag="001">2199093</controlfield>
  <controlfield tag="003">SzGeCERN</controlfield>
  <controlfield tag="005">20171102143236.0</controlfield>
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    <subfield code="a">oai:arXiv.org:1607.03813</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2016-07-14</subfield>
    <subfield code="h">2016-07-14T05:21:28Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1607.03813</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Baboux, F</subfield>
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    <subfield code="a">Levy, E</subfield>
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    <subfield code="a">Lemaître, A</subfield>
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    <subfield code="a">Gomez, C</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Galopin, E</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Gratiet, L Le</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Sagnes, I</subfield>
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    <subfield code="a">Amo, A</subfield>
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  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a">Bloch, J</subfield>
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    <subfield code="a">Akkermans, E</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1607.03813.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201628</subfield>
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    <subfield code="a">Exploring topological edge states in photonic quasicrystals</subfield>
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    <subfield code="c">13 Jul 2016</subfield>
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    <subfield code="a">5 p</subfield>
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    <subfield code="a">We experimentally investigate the topological properties of quasiperiodic chains using cavity polaritons confined in a potential following the Fibonacci sequence. Edge states forming in the gaps of a fractal energy spectrum are imaged both in real and momentum space. These edge states periodically traverse the gaps when varying a structural degree of freedom $\phi$ of the Fibonacci sequence. The period and direction of the traverses are directly related to the Chern numbers assigned to each gap by the gap-labeling theorem. Additionally, we show that the Chern numbers determine the spatial symmetry properties of the edge states. These results highlight the potential of cavity polaritons to emulate nontrivial topological properties in a controlled environment.</subfield>
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    <subfield code="a">Comments: 5 pages, 4 figures</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
    <subfield code="b">arXiv</subfield>
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    <subfield code="a">LANL EDS</subfield>
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    <subfield code="a">cond-mat.mes-hall</subfield>
    <subfield code="2">arXiv</subfield>
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    <subfield code="a">cond-mat.quant-gas</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="b">Other Fields of Physics</subfield>
    <subfield code="2">arXiv</subfield>
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    <subfield code="a">cond-mat.mes-hall</subfield>
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    <subfield code="a">physics.optics</subfield>
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  <datafield tag="260" ind1=" " ind2=" ">
    <subfield code="c">2016</subfield>
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  <datafield tag="690" ind1="C" ind2=" ">
    <subfield code="a">PREPRINT</subfield>
  </datafield>
  <datafield tag="960" ind1=" " ind2=" ">
    <subfield code="a">11</subfield>
  </datafield>
  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="a">PREPRINT</subfield>
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    <subfield code="h">2016-11-12T06:19:08Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1607.06626</subfield>
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    <subfield code="a">Schreck, John S</subfield>
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    <subfield code="a">Romano, Flavio</subfield>
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    <subfield code="p">Condens. Matter</subfield>
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    <subfield code="y">2017</subfield>
    <subfield code="c">014006</subfield>
    <subfield code="o">J. Phys.: Condens. Matter 29, 014006 (2017)</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1607.06626.pdf</subfield>
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    <subfield code="s">n</subfield>
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    <subfield code="a">Self-assembly of two-dimensional binary quasicrystals: A possible route to a DNA quasicrystal</subfield>
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    <subfield code="c">22 Jul 2016</subfield>
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    <subfield code="a"></subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">We use Monte Carlo simulations and free-energy techniques to show that binary solutions of penta- and hexavalent two-dimensional patchy particles can form thermodynamically stable quasicrystals even at very narrow patch widths, provided their patch interactions are chosen in an appropriate way. Such patchy particles can be thought of as a coarse-grained representation of DNA multi-arm `star' motifs, which can be chosen to bond with one another very specifically by tuning the DNA sequences of the protruding arms. We explore several possible design strategies and conclude that DNA star tiles that are designed to interact with one another in a specific but not overly constrained way could potentially be used to construct soft quasicrystals in experiment. We verify that such star tiles can form stable dodecagonal motifs using oxDNA, a realistic coarse-grained model of DNA.</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="a">Chemical Physics and Chemistry</subfield>
    <subfield code="2">arXiv</subfield>
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    <subfield code="9">LANL EDS</subfield>
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="c">Hidden</subfield>
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  <controlfield tag="005">20171106114900.0</controlfield>
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    <subfield code="a">oai:arXiv.org:1609.06625</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
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    <subfield code="h">2016-09-22T05:29:56Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1609.06625</subfield>
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    <subfield code="a">Laptev, Denis</subfield>
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    <subfield code="a">Irwin, Klee</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1609.06625.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201638</subfield>
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    <subfield code="a">Catalytic mechanism of LENR in quasicrystals based on localized anharmonic vibrations and phasons</subfield>
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    <subfield code="c">09 Aug 2016</subfield>
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  <datafield tag="300" ind1=" " ind2=" ">
    <subfield code="a">16 p</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">Quasicrystals (QCs) are a novel form of matter, which are neither crystalline nor amorphous. Among many surprising properties of QCs is their high catalytic activity. We propose a mechanism explaining this peculiarity based on unusual dynamics of atoms at special sites in QCs, namely, localized anharmonic vibrations (LAVs) and phasons. In the former case, one deals with a large amplitude (~ fractions of an angstrom) time-periodic oscillations of a small group of atoms around their stable positions in the lattice, known also as discrete breathers, which can be excited in regular crystals as well as in QCs. On the other hand, phasons are a specific property of QCs, which are represented by very large amplitude (~angstrom) oscillations of atoms be-tween two quasi-stable positions determined by the geometry of a QC. Large amplitude atomic motion in LAVs and phasons results in time-periodic driving of adjacent potential wells occupied by hydrogen ions (protons or deuterons) in case of hydrogenated QCs. This driving may result in the increase of amplitude and energy of zero-point vibrations (ZPV). Based on that, we demonstrate a drastic increase of the D-D or D-H fusion rate with increasing number of modulation periods evaluated in the framework of Schwinger model, which takes into account suppression of the Coulomb barrier due to lattice vibrations. In this context, we present numerical solution of Schrodinger equation for a particle in a non-stationary double well potential, which is driven time-periodically imitating the action of a LAV or phason. We show that the rate of tunneling of the particle through the potential barrier separating the wells is enhanced drastically by the driving, and it increases strongly with increasing amplitude of the driving. These results support the concept of nuclear catalysis in QCs that can take place at special sites provided by their inherent topology.</subfield>
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    <subfield code="a">Comments: 16 pages, 11 figures, Int. Conf. on Cold Fusion (ICCF20). arXiv admin note: text overlap with arXiv:1510.06081</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
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    <subfield code="a">LANL EDS</subfield>
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    <subfield code="2">arXiv</subfield>
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    <subfield code="a">physics.gen-ph</subfield>
    <subfield code="9">LANL EDS</subfield>
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    <subfield code="c">2016</subfield>
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    <subfield code="a">11</subfield>
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    <subfield code="b">Comments: 16 pages, 11 figures, Int. Conf. on Cold Fusion (ICCF20). arXiv admin note: text overlap with arXiv:1510.06081</subfield>
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    <subfield code="a">PREPRINT</subfield>
  </datafield>
  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="c">Hidden</subfield>
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  <controlfield tag="005">20171103220722.0</controlfield>
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    <subfield code="2">DOI</subfield>
    <subfield code="a">10.1038/nphys3482</subfield>
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    <subfield code="a">oai:arXiv.org:1609.07608</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
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    <subfield code="h">2016-11-22T06:18:51Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1609.07608</subfield>
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    <subfield code="a">Kondakci, H E</subfield>
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    <subfield code="a">Abouraddy, A F</subfield>
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    <subfield code="a">Saleh, B E A</subfield>
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    <subfield code="p">Nature Phys.</subfield>
    <subfield code="v">11</subfield>
    <subfield code="y">2015</subfield>
    <subfield code="c">930</subfield>
    <subfield code="o">Nature Phys. 11, 930 (2015)</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1609.07608.pdf</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201639</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">A photonic thermalization gap in disordered lattices</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">24 Sep 2016</subfield>
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  <datafield tag="300" ind1=" " ind2=" ">
    <subfield code="a">12 p</subfield>
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    <subfield code="a">Comments: 12 pages in pre-print format, 4 figures, selected as cover article for Nature Physics 2015 November issue</subfield>
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    <subfield code="a">Comments: 12 pages in pre-print format, 4 figures, selected as cover article for Nature Physics 2015 November issue</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">The formation of gaps -- forbidden ranges in the values of a physical parameter -- is a ubiquitous feature of a variety of physical systems: from energy bandgaps of electrons in periodic lattices and their analogs in photonic, phononic, and plasmonic systems to pseudo energy gaps in aperiodic quasicrystals. Here, we report on a `thermalization' gap for light propagating in finite disordered structures characterized by disorder-immune chiral symmetry -- the appearance of the eigenvalues and eigenvectors in skew-symmetric pairs. In this class of systems, the span of sub- thermal photon statistics is inaccessible to input coherent light, which -- once the steady state is reached -- always emerges with super-thermal statistics no matter how small the disorder level. We formulate an independent constraint that must be satisfied by the input field for the chiral symmetry to be `activated' and the gap to be observed. This unique feature enables a new form of photon-statistics interferometry: the deterministic tuning of photon statistics -- from sub-thermal to super-thermal -- in a compact device, without changing the disorder level, via controlled excitation-symmetry-breaking realized by sculpting the amplitude or phase of the input coherent field.</subfield>
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    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
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    <subfield code="a">LANL EDS</subfield>
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    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="a">General Theoretical Physics</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="650" ind1="2" ind2="7">
    <subfield code="b">Other Fields of Physics</subfield>
    <subfield code="2">arXiv</subfield>
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  <datafield tag="695" ind1=" " ind2=" ">
    <subfield code="a">physics.optics</subfield>
    <subfield code="9">LANL EDS</subfield>
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    <subfield code="c">2016</subfield>
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    <subfield code="a">13</subfield>
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    <subfield code="a">Article</subfield>
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    <subfield code="a">oai:arXiv.org:1611.00867</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2016-11-04</subfield>
    <subfield code="h">2016-11-07T09:06:07Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1611.00867</subfield>
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    <subfield code="a">Aznavourian, Ronald</subfield>
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    <subfield code="a">Puvirajesinghe, Tania</subfield>
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    <subfield code="a">Brule, Stephane</subfield>
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    <subfield code="a">Enoch, Stefan</subfield>
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    <subfield code="a">Guenneau, Sebastien</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1611.00867.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201645</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">Bio-inspired seismic metamaterials: Time domain simulations in transformed crystals</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">02 Nov 2016</subfield>
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  <datafield tag="300" ind1=" " ind2=" ">
    <subfield code="a">25 p</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">We introduce the concept of transformation crystallography which consists of the application of geometric transforms to periodic structures. We consider motifs with three-fold, four-fold and six-fold symmetries according to the crystallographic restriction theorem. Furthermore, we define motifs with five-fold symmetry such as quasi-crystals generated by a cut-and-projection method. We analyze elastic wave propagation in the transformed crystals and (Penrose-type) quasi-crystals with the finite difference time domain freeware SimSonic. We consider geometric transforms underpinning the design of seismic cloaks with square, circular, elliptical and peanut shapes in the context of triangular, square and honeycomb crystals. Interestingly, the use of morphing techniques leads to the design of cloaks with interpolated geometries reminiscent of Victor Vasarely's artwork. Employing the case of transformed graphene-like (honeycomb) structures allows one to draw useful analogies between large-scale seismic metamaterials such as soils structured with columns of concrete or grout with soil and nanoscale biochemical metamaterials. We further point out similarities between cloaks for elastodynamic and hydrodynamic waves and cloaks for diffusion (heat or mass) diffusion processes, notably with respect to invisibility and protection. Experimental data extracted from field test analysis of soil structured with boreholes demonstrates the application of bio-inspired seismic metamaterials. We conclude that these novel materials hold strong applications in biophysics and geophysics.</subfield>
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    <subfield code="a">Comments: 25 pages, 14 figures</subfield>
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  <datafield tag="540" ind1=" " ind2=" ">
    <subfield code="u">http://arxiv.org/licenses/nonexclusive-distrib/1.0/</subfield>
    <subfield code="b">arXiv</subfield>
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    <subfield code="a">LANL EDS</subfield>
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    <subfield code="2">arXiv</subfield>
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  <datafield tag="695" ind1=" " ind2=" ">
    <subfield code="a">physics.bio-ph</subfield>
    <subfield code="9">LANL EDS</subfield>
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    <subfield code="a">11</subfield>
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    <subfield code="a">PREPRINT</subfield>
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    <subfield code="c">Hidden</subfield>
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    <subfield code="2">DOI</subfield>
    <subfield code="a">10.1016/j.optmat.2016.11.013</subfield>
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    <subfield code="a">oai:arXiv.org:1611.05303</subfield>
    <subfield code="u">http://export.arxiv.org/oai2</subfield>
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    <subfield code="h">2016-11-17T06:24:47Z</subfield>
    <subfield code="m">arXiv</subfield>
    <subfield code="t">true</subfield>
    <subfield code="9">arXiv</subfield>
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    <subfield code="a">arXiv:1611.05303</subfield>
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    <subfield code="a">eng</subfield>
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    <subfield code="a">Brandao, E R</subfield>
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    <subfield code="a">Vasconcelos, M S</subfield>
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    <subfield code="a">Anselmo, D H A L</subfield>
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    <subfield code="o">Optical Materials,2016</subfield>
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    <subfield code="u">http://arxiv.org/pdf/1611.05303.pdf</subfield>
    <subfield code="y">Preprint</subfield>
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    <subfield code="s">n</subfield>
    <subfield code="w">201646</subfield>
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    <subfield code="a">Octonacci Photonic Crystals with Negative Refraction Index Materials</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">16 Nov 2016</subfield>
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    <subfield code="a">23 p</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">We investigate the optical transmission spectra for $s$-polarized (TE) and $p$-polarized (TM) waves in one-dimensional photonic quasicrystals on a quasiperiodic multilayer structure made up by alternate layers of SiO$_{2}$ and \textit{metamaterials}, organized by following the Octonacci sequence. Maxwell's equations and the transfer-matrix technique are used to derive the transmission spectra for the propagation of normaly and obliquely incident optical fields. We assume Drude-Lorentz-type dispersive response for the dielectric permittivity and magnetic permeability of the metamaterials. For normally incident waves, we observe that the spectra does not have self-similar behavior or mirror symmetry and it also features the absence of optical band gap. Also for normally incident waves, we show regions of full transmittance when the incident angle $\theta_{C} = 0^{\circ}$ in a particular frequency range.</subfield>
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    <subfield code="a">The goal of this work is to elaborate on new geometric methods of constructing exact and parametric quasiperiodic solutions for anamorphic cosmology models in modified gravity theories, MGTs, and general relativity, GR. There exist previously studied generic off-diagonal and diagonalizable cosmological metrics encoding gravitational and matter fields with quasicrystal like structures, QC, and holonomy corrections from loop quantum gravity, LQG. We apply the anholonomic frame deformation method, AFDM, in order to decouple the (modified) gravitational and matter field equations in general form. This allows us to find integral varieties of cosmological solutions determined by generating functions, effective sources, integration functions and constants. The coefficients of metrics and connections for such cosmological configurations depend, in general, on all spacetime coordinates and can be chosen to generate observable (quasi)-periodic/ aperiodic/ fractal / stochastic / (super) cluster / filament / polymer like (continuous, stochastic, fractal and/or discrete structures) in MGTs and/or GR. In this work, we study new classes of solutions for anamorphic cosmology with LQG holonomy corrections. Such solutions are characterized by nonlinear symmetries of generating functions for generic off--diagonal cosmological metrics and generalized connections, with possible nonholonomic constraints to Levi-Civita configurations and diagonalizable metrics depending only on a time like coordinate. We argue that anamorphic quasiperiodic cosmological models integrate the concept of quantum discrete spacetime, with certain gravitational QC-like vacuum and nonvacuum structures. And, that of a contracting universe that homogenizes, isotropizes and flattens without introducing initial conditions or multiverse problems.</subfield>
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    <subfield code="a">The goal of this work on mathematical cosmology and geometric methods in modified gravity theories, MGTs, is to investigate Starobinsky-like inflation scenarios determined by gravitational and scalar field configurations mimicking quasicrystal, QC, like structures. Such spacetime aperiodic QCs are different from those discovered and studied in solid state physics but described by similar geometric methods. We prove that an inhomogeneous and locally anisotropic gravitational and matter field effective QC mixed continuous and discrete "aether" can be modeled by exact cosmological solutions in MGTs and Einstein gravity. The coefficients of corresponding generic off-diagonal metrics and generalized connections depend (in general) on all spacetime coordinates via generating and integration functions and certain smooth and discrete parameters. Imposing additional nonholonomic constraints, prescribing symmetries for generating functions and solving the boundary conditions for integration functions and constants, we can model various nontrivial torsion QC structures or extract cosmological Levi--Civita configurations with diagonal metrics reproducing de Sitter (inflationary) like and other types homogeneous inflation and acceleration phases. Finally, we speculate how various dark energy and dark matter effects can be modeled by off-diagonal interactions and deformations of a nontrivial QC like gravitational vacuum structure and analogous scalar matter fields.</subfield>
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