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<dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:invenio="http://invenio-software.org/elements/1.0" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd"><dc:identifier>doi:10.1088/1475-7516/2021/10/034</dc:identifier><dc:language>eng</dc:language><dc:creator>Knirck S.</dc:creator><dc:creator>Schütte-Engel J.</dc:creator><dc:creator>Beurthey S.</dc:creator><dc:creator>Breitmoser D.</dc:creator><dc:creator>Caldwell A.</dc:creator><dc:creator>Diaconu C.</dc:creator><dc:creator>Diehl J.</dc:creator><dc:creator>Egge J.</dc:creator><dc:creator>Esposito M.</dc:creator><dc:creator>Gardikiotis A.</dc:creator><dc:creator>Garutti E.</dc:creator><dc:creator>Heyminck S.</dc:creator><dc:creator>Hubaut F.</dc:creator><dc:creator>Jochum J.</dc:creator><dc:creator>Karst P.</dc:creator><dc:creator>Kramer M.</dc:creator><dc:creator>Krieger C.</dc:creator><dc:creator>Labat D.</dc:creator><dc:creator>Lee C.</dc:creator><dc:creator>Li X.</dc:creator><dc:creator>Lindner A.</dc:creator><dc:creator>Majorovits B.</dc:creator><dc:creator>Martens S.</dc:creator><dc:creator>Matysek M.</dc:creator><dc:creator>Öz E.</dc:creator><dc:creator>Planat L.</dc:creator><dc:creator>Pralavorio P.</dc:creator><dc:creator>Raffelt G.</dc:creator><dc:creator>Ranadive A.</dc:creator><dc:creator>Redondo J.</dc:creator><dc:creator>Reimann O.</dc:creator><dc:creator>Ringwald A.</dc:creator><dc:creator>Roch N.</dc:creator><dc:creator>Schaffran J.</dc:creator><dc:creator>Schmidt A.</dc:creator><dc:creator>Shtembari L.</dc:creator><dc:creator>Steffen F.</dc:creator><dc:creator>Strandhagen C.</dc:creator><dc:creator>Strom D.</dc:creator><dc:creator>Usherov I.</dc:creator><dc:creator>Wieching G.</dc:creator><dc:title>Simulating MADMAX in 3D: Requirements for dielectric axion haloscopes</dc:title><dc:identifier>ART-2021-125791</dc:identifier><dc:description>We present 3D calculations for dielectric haloscopes such as the currently envisioned MADMAX experiment. For ideal systems with perfectly flat, parallel and isotropic dielectric disks of finite diameter, we find that a geometrical form factor reduces the emitted power by up to 30 % compared to earlier 1D calculations. We derive the emitted beam shape, which is important for antenna design. We show that realistic dark matter axion velocities of 10-3 c and inhomogeneities of the external magnetic field at the scale of 10 % have negligible impact on the sensitivity of MADMAX. We investigate design requirements for which the emitted power changes by less than 20 % for a benchmark boost factor with a bandwidth of 50 MHz at 22 GHz, corresponding to an axion mass of 90 µ eV. We find that the maximum allowed disk tilt is 100 µ m divided by the disk diameter, the required disk planarity is 20 µ m (min-to-max) or better, and the maximum allowed surface roughness is 100 µ m (min-to-max). We show how using tiled dielectric disks glued together from multiple smaller patches can affect the beam shape and antenna coupling. © 2021 The Author(s).</dc:description><dc:date>2021</dc:date><dc:source>http://zaguan.unizar.es/record/111992</dc:source><dc:doi>10.1088/1475-7516/2021/10/034</dc:doi><dc:identifier>http://zaguan.unizar.es/record/111992</dc:identifier><dc:identifier>oai:zaguan.unizar.es:111992</dc:identifier><dc:identifier.citation>Journal of Cosmology and Astroparticle Physics 2021, 10 (2021), 034 [25 pp]</dc:identifier.citation><dc:rights>by</dc:rights><dc:rights>http://creativecommons.org/licenses/by/3.0/es/</dc:rights><dc:rights>info:eu-repo/semantics/openAccess</dc:rights></dc:dc>

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