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2025-03-28
10:39
Conversion of East Hall T8 line (DIRAC Experiments) from transport to MAD program / Zani, L
CERN-PS-CA-Note-2000-003.- Geneva : CERN, 2000 - 6 p. Fulltext: PDF;

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2024-03-27
08:55
Experience DIRAC : Calcul des blindages / Danloy, L
CERN-PS-PA-Note-95-18.- Geneva : CERN, 1995 - 10 p. Fulltext: PDF;

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2024-01-08
15:58
DIRAC (I191) preliminary optics in East Hall / Durieu, Luc
CERN-PS-PA-Note-94-13.- Geneva : CERN, 1994 - 8 p. Fulltext: PDF;

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2023-10-05
15:00
Measurement of beam halo in FT61S for the DIRAC experiment / Durieu, L ; Giovannozzi, Μ ; Hémery, J Y
CERN-PS-PA-Note-96-09.- Geneva : CERN, 1996 - 12 p. Fulltext: PDF;

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2023-09-14
17:15
Test of a dispersion sweep correction system by using a centroid in the DIRAC beam line / Bosser, J ; Molinari, G ; Nonglaton, J M ; Prieto, V ; Steerenberg, R
CERN-PS-OP-Note-2001-011; CERN-PS-BD-Note-2001-013.- Geneva : CERN, 2001 - 18 p. Fulltext: PDF;

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2022-09-20
17:27
Test of a dispersion sweep correction system using a Centroid in the DIRAC beam line / Bosser, J ; Molinari, G ; Nonglaton, J-M ; Prieto, V ; Steerenberg, R
CERN-PS-2002-041-OP.- Geneva : CERN, 2002 - 4 p. Fulltext: PDF;

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2022-09-20
16:54
EHNL 5N : Design of T8 Line (DIRAC Experiments) for EHNL / Ferrando, O ; Hémery, J Y
CERN-PS-CA-Note-97-16.- Geneva : CERN, 1997 - 25 p. Note Fulltext: PS-CA-Note-97-16 - PDF; PS-CA-Note-97-16-plan - PDF;

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2017-06-02
06:23
Vacuum systems for the ILC helical undulator / Malyshev, O B (Daresbury ; Cockcroft Inst. Accel. Sci. Tech.) ; Scott, D J (Daresbury ; Cockcroft Inst. Accel. Sci. Tech.) ; Clarke, J A (Daresbury ; Cockcroft Inst. Accel. Sci. Tech.) ; Bailey, I R (Liverpool U. ; Cockcroft Inst. Accel. Sci. Tech.) ; Dainton, J B (Liverpool U. ; Cockcroft Inst. Accel. Sci. Tech.) ; Malysheva, L I (Liverpool U. ; Cockcroft Inst. Accel. Sci. Tech.) ; Barber, D P (DESY) ; Cooke, P (Liverpool U.) ; Baynham, E (Rutherford) ; Bradshaw, T (Rutherford) et al.
The International Linear Collider (ILC) positron source uses a helical undulator to generate polarized photons of ∼10MeV∼10MeV at the first harmonic. Unlike many undulators used in synchrotron radiation sources, the ILC helical undulator vacuum chamber will be bombarded by photons, generated by the undulator, with energies mostly below that of the first harmonic. [...]
EUROTEV-REPORT-2006-086.- 2007 - 28 p. - Published in : J. Vac. Sci. Technol. A A 25 (2007) 791 Fulltext: PDF; External link: DESY

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2014-07-10
09:27
Development of radiation hardened pixel sensors for charged particle detection / Koziel, Michal
CMOS Pixel Sensors are being developed since a few years to equip vertex detectors for future high-energy physics experiments with the crucial advantages of a low material budget and low production costs [...]
EuCARD-BOO-2014-008 ; CERN-ACC-2014-0090 - 2014 - 239. (EuCARD monograph ; 26)


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2014-07-10
09:21
Designing the Four Rod Crab Cavity for the High-Luminosity LHC upgrade. / Hall, Ben
This thesis presents the design for a novel compact crab cavity for the HL-LHC upgrade at CERN, Geneva [...]
EuCARD-BOO-2014-007 ; CERN-ACC-2014-0089 - 2014 - 214. (EuCARD monograph ; 25)


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