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    <subfield code="a">Cirone, A.</subfield>
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    <subfield code="m">alessio.cirone@ge.infn.it</subfield>
    <subfield code="u">Genoa U.</subfield>
    <subfield code="u">INFN, Genoa</subfield>
    <subfield code="v">INFN, Sezione di Genova, I-16146 Genova, Italy</subfield>
    <subfield code="v">Dipartimento di Fisica, Università degli Studi di Genova, I-16146 Genova, Italy</subfield>
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    <subfield code="9">arXiv</subfield>
    <subfield code="a">Investigation of magnetic noise in Advanced Virgo</subfield>
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    <subfield code="c">2019-10-18</subfield>
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    <subfield code="c">2019-08-29</subfield>
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    <subfield code="a">The advanced Virgo (AdV) sensitivity might be influenced by the effects of environmental noise, in particular magnetic noise (MN). In order to show the impact on the gravitational-wave strain signal h(t) and on the AdV sensitivity, we must understand the coupling between the environmental magnetic activity and the strain. The relationship between the environmental noise—measured by a physical environment monitor (PEM)—and h(t) is investigated using injection studies, where an intentional stimulus is introduced and the responses of both PEM sensors and the instrument are analyzed. We also present the most outstanding measurements and results obtained from both the characterization and the mitigation studies of the environmental MN. Results show that MN does not affect AdV sensitivity up to 100 Mpc in BNS range.</subfield>
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    <subfield code="a">The Advanced Virgo (AdV) sensitivity might be influenced by the effects of environmental noise, in particular magnetic noise (MN). In order to show the impact on the gravitational-wave strain signal h(t) and on the AdV sensitivity, we must understand the coupling between the environmental magnetic activity and the strain. The relationship between the environmental noise - measured by a physical environment monitor (PEM) - and h(t) is investigated using injection studies, where an intentional stimulus is introduced and the responses of both PEM sensors and the instrument are analyzed. We also present the most outstanding measurements and results obtained from both the characterization and the mitigation studies of the environmental MN. Results show that MN does not affect AdV sensitivity up to $\approx 100$ Mpc in BNS range.</subfield>
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    <subfield code="f">© 2019 IOP Publishing Ltd</subfield>
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    <subfield code="2">SzGeCERN</subfield>
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    <subfield code="a">Fiori, I.</subfield>
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    <subfield code="v">European Gravitational Observatory (EGO), I-56021 Cascina, Pisa, Italy</subfield>
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    <subfield code="a">Paoletti, F.</subfield>
    <subfield code="j">ORCID:0000-0001-8898-1963</subfield>
    <subfield code="u">INFN, Pisa</subfield>
    <subfield code="v">INFN, Sezione di Pisa, I-56127 Pisa, Italy</subfield>
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    <subfield code="a">Perez, M.M.</subfield>
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    <subfield code="a">Rodríguez, A.R.</subfield>
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    <subfield code="a">Swinkels, B.L.</subfield>
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    <subfield code="u">NIKHEF, Amsterdam</subfield>
    <subfield code="v">Nikhef, Science Park 105, 1098 XG Amsterdam, The Netherlands</subfield>
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    <subfield code="a">Vazquez, A.M.</subfield>
    <subfield code="u">Mexico U.</subfield>
    <subfield code="v">IFAE, Barcelona Institute of Science and Technology, Barcelona, and ICREA, Spain</subfield>
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    <subfield code="a">Gemme, G.</subfield>
    <subfield code="j">ORCID:0000-0002-1127-7406</subfield>
    <subfield code="u">Enrico Fermi Ctr., Rome</subfield>
    <subfield code="u">Genoa U.</subfield>
    <subfield code="u">INFN, Genoa</subfield>
    <subfield code="v">INFN, Sezione di Genova, I-16146 Genova, Italy</subfield>
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    <subfield code="a">Chincarini, A.</subfield>
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    <subfield code="u">INFN, Genoa</subfield>
    <subfield code="v">INFN, Sezione di Genova, I-16146 Genova, Italy</subfield>
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    <subfield code="c">225004</subfield>
    <subfield code="n">22</subfield>
    <subfield code="p">Class. Quantum Gravity</subfield>
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    <subfield code="y">00010 Magnetic noise projection with coherence. a) Maximum coherence at each frequency between the strain channel and the 3 magnetic probes in the "Central Building" (blue line); the dashed red line indicates the statistical significance level of the coherence, calculated according to the 95$\%$ confidence level of the coherence distribution between randomly resampled data (orange line). b) Related magnetic noise projection (blue for statistically reliable bins, grey for coherence below significance level), compared to the most recent one obtained by the far-field injections (red diamonds) and the Advanced Virgo sensitivity (orange line).</subfield>
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    <subfield code="y">00014 "Finite Element Analysis" of two possible magnetic field shielding solutions: a) the Helmholtz coils and a spherical shell (different shapes and sizes). b) Longitudinal studies (along z) of the normalized reduction of the magnetic field. c) Orthogonal studies (along y) within a height range of [-1,7] m, along the "Tower" axis. d) Frequency evolution of the normalized field at the Test Mass location.</subfield>
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    <subfield code="y">00015 "Finite Element Analysis" of two possible magnetic field shielding solutions: a) the Helmholtz coils and a spherical shell (different shapes and sizes). b) Longitudinal studies (along z) of the normalized reduction of the magnetic field. c) Orthogonal studies (along y) within a height range of [-1,7] m, along the "Tower" axis. d) Frequency evolution of the normalized field at the Test Mass location.</subfield>
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    <subfield code="y">00016 "Finite Element Analysis" of two possible magnetic field shielding solutions: a) the Helmholtz coils and a spherical shell (different shapes and sizes). b) Longitudinal studies (along z) of the normalized reduction of the magnetic field. c) Orthogonal studies (along y) within a height range of [-1,7] m, along the "Tower" axis. d) Frequency evolution of the normalized field at the Test Mass location.</subfield>
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    <subfield code="y">00004 Frequency evolution of the West-End Tower (WET) shielding power: a) The 3 "injection coil - external magnetic probe" configurations for their positioning inside the experimental area: coil at 7.3 m, probe near the WET (config. 1); coil at 10.3 m, probe near the WET (config. 2); coil at 6.8 m, specular probe (config. 3). b) The measurement results, along with the fits to a first order lower pass filter model of Butterworth type.</subfield>
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    <subfield code="y">00011 Magnetic noise projection with coherence. a) Maximum coherence at each frequency between the strain channel and the 3 magnetic probes in the "Central Building" (blue line); the dashed red line indicates the statistical significance level of the coherence, calculated according to the 95$\%$ confidence level of the coherence distribution between randomly resampled data (orange line). b) Related magnetic noise projection (blue for statistically reliable bins, grey for coherence below significance level), compared to the most recent one obtained by the far-field injections (red diamonds) and the Advanced Virgo sensitivity (orange line).</subfield>
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    <subfield code="y">00006 From left to right the "West-End, North-End and Central Buildings" floor plans. The thunderbolt and the blue cylinder correspond respectively to the coil and the probe locations inside the three facilities; the red spots identifies the four TMs and the red lines follow the main laser path.</subfield>
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