{"paper":{"title":"Simulating MADMAX in 3D: Requirements for Dielectric Axion Haloscopes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","physics.ins-det"],"primary_cat":"hep-ex","authors_text":"A. Caldwell, A. Gardikiotis, A. Lindner, A. Ranadive, A. Ringwald, A. Schmidt, B. Majorovits, C. Diaconu, C. Krieger, C. Lee, C. Strandhagen, D. Breitmoser, D. Labat, D. Strom, E. Garutti, E. \\\"Oz, F. Hubaut, F. Steffen, G. Raffelt, G. Wieching (MADMAX collaboration), I. Usherov, J. Diehl, J. Egge, J. Jochum, J. Redondo, J. Schaffran, J. Sch\\\"utte-Engel, L. Planat, L. Shtembari, M. Esposito, M. Kramer, M. Matysek, N. Roch, O. Reimann, P. Karst, P. Pralavorio, S. Beurthey, S. Heyminck, S. Knirck, S. Martens, X. Li","submitted_at":"2021-04-13T23:50:47Z","abstract_excerpt":"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 inve"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2104.06553","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2104.06553/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}