{"paper":{"title":"Expression of Interest for Evolution of the Mu2e Experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.ins-det","authors_text":"A. Artikov, A. Daniel, A. Edmonds, A. Ferrari, A. Gaponenko, A. Hocker, A. Luca, A. Mazzacane, A. Pla-Dalmau, A. Popov, A. Saputi, B. Echenard, B. Kiburg, B. Pollack, C. Bloise, C. Gatto, C. Group, C. Hu, D. Ambrose, D. Bowring, D. Brown, D. Chokheli, D. Cronin-Hennessy, D. Denisov, D. Glenzinski, D. Hedin, D. Hitlin, D. Lin, D. Neuffer, D. Pasciuto, D. Pushka, D. Stratakis, E.C. Dukes, E. Diociaiuti, E. Hungerford, E. Pedreschi, E. Prebys, F. Abusalma, F. Cervelli, F. Happacher, F. Porter, F. Spinella, G.C. Blazey, G. Drake, G. Horton-Smith, G. Lukicov, G. Pezzullo, G. Rakness, H. Glass, I. Logashenko, I. Sarra, J. Bono, J.-F. Caron, J. Kozminski, J. Miller, J. Mott, J. Popp, J. Quirk, J. Whitmore, K. Byrum, K. Ciampa, K. Heller, K. Lynch, K. S. Khaw, L. Goodenough, L. Harkness-Brennan, L. Morescalchi, L. Xia, L. Zhang, M.A. Cummings, M. Campbell, M. Frank, M. Jenkins, M. Jones, M. Kargiantoulakis, M. Lancaster, M. Martini, M. Ricci, M. R\\\"ohrken, M. Schmitt, M. Velasco, N. Tran, P. Fabbricatore, P. Murat, P.Q. Hung, P. Winter, R. Bernstein, R. Bonventre, R. Ciolini, R. Coleman, R. Culbertson, R. Djilkibaev, R. Donghia, R. Ehrlich, R. Hooper, R. Kutschke, R. Ray, R. Talaga, R. Tschirhart, R. Wagner, R.-Y. Zhu, R. Zwaska, S. Boi, S. Demers, S. Denisov, S. Di Falco, S. Donati, S. E. Mueller, S. Giovannella, S. Miscetti, S. Werkema, T. Bolton, T. Strauss, V. Evdokimov, V. Giusti, V. Lombardo, V. Nagaslaev, V. Pronskikh, V. Rusu, V. Tereshchenko, V. Zutshi, Y. Davydov, Y. Kolomensky, Y. Oksuzian, Y. Wang, Z. Giorgio, Z. Usubov","submitted_at":"2018-02-07T19:14:55Z","abstract_excerpt":"We propose an evolution of the Mu2e experiment, called Mu2e-II, that would leverage advances in detector technology and utilize the increased proton intensity provided by the Fermilab PIP-II upgrade to improve the sensitivity for neutrinoless muon-to-electron conversion by one order of magnitude beyond the Mu2e experiment, providing the deepest probe of charged lepton flavor violation in the foreseeable future. Mu2e-II will use as much of the Mu2e infrastructure as possible, providing, where required, improvements to the Mu2e apparatus to accommodate the increased beam intensity and cope with "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.02599","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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"}