The Scotogenic model extends the standard model with three singlet fermion N i and one inert doublet scalar η to address the common origin of tiny neutrino mass and dark matter. For fermion dark matter N 1, a hierarchical Yukawa structure $$ \mid {y}_{1e}\mid \ll \mid {y}_{1\mu}\mid \sim \mid {y}_{1\tau}\mid \sim \mathcal{O}(1) $$ is usually favored to satisfy constraints from lepton flavor violation and relic density. Such large μ-related Yukawa coupling would greatly enhance the pair production of charged scalar η ± at the muon collider. In this paper, we investigate the dilepton and mono-photon signature of the Scotogenic model at a 14 TeV muon collider. For the dimuon signature , we find that most viable samples can be probed with 200 fb −1 data. The ditau signature is usually less promising, but it is important to probe the small |y 1μ | region. The mono-photon signature could also probe the compressed mass region M 1 ≲ $$ {M}_{\eta^{\pm }} $$ . Masses of charged scalar η ± and dark matter N 1 can be further extracted by a binned likelihood fit of the dilepton energy.
{ "_oai": { "updated": "2023-03-26T00:32:20Z", "id": "oai:repo.scoap3.org:74533", "sets": [ "JHEP" ] }, "authors": [ { "affiliations": [ { "country": "China", "value": "School of Physics and Technology, University of Jinan, Jinan, Shandong, 250022, China", "organization": "University of Jinan" }, { "country": "China", "value": "Guangxi Key Laboratory of Nuclear Physics and Nuclear Technology, Guangxi Normal University, Guilin, Guangxi, 541004, China", "organization": "Guangxi Normal University" } ], "surname": "Liu", "email": "2298715807@qq.com", "full_name": "Liu, Jiao", "given_names": "Jiao" }, { "affiliations": [ { "country": "China", "value": "School of Physics and Technology, University of Jinan, Jinan, Shandong, 250022, China", "organization": "University of Jinan" } ], "surname": "Han", "email": "sps_hanzl@ujn.edu.cn", "full_name": "Han, Zhi-Long", "given_names": "Zhi-Long" }, { "affiliations": [ { "country": "China", "value": "School of Physics and Technology, University of Jinan, Jinan, Shandong, 250022, China", "organization": "University of Jinan" }, { "country": "China", "value": "Guangxi Key Laboratory of Nuclear Physics and Nuclear Technology, Guangxi Normal University, Guilin, Guangxi, 541004, China", "organization": "Guangxi Normal University" } ], "surname": "Jin", "email": "ss_jiny@ujn.edu.cn", "full_name": "Jin, Yi", "given_names": "Yi" }, { "affiliations": [ { "country": "China", "value": "School of Physics and Technology, University of Jinan, Jinan, Shandong, 250022, China", "organization": "University of Jinan" } ], "surname": "Li", "email": "sps_lihl@ujn.edu.cn", "full_name": "Li, Honglei", "given_names": "Honglei" } ], "titles": [ { "source": "Springer", "title": "Unraveling the Scotogenic model at muon collider" } ], "dois": [ { "value": "10.1007/JHEP12(2022)057" } ], "publication_info": [ { "page_end": "34", "journal_title": "Journal of High Energy Physics", "material": "article", "journal_volume": "2022", "artid": "JHEP12(2022)057", "year": 2022, "page_start": "1", "journal_issue": "12" } ], "$schema": "http://repo.scoap3.org/schemas/hep.json", "acquisition_source": { "date": "2023-03-26T00:31:20.281148", "source": "Springer", "method": "Springer", "submission_number": "57ba2b5ecb6d11eda920065bd8dc6b20" }, "page_nr": [ 34 ], "license": [ { "url": "https://creativecommons.org/licenses//by/4.0", "license": "CC-BY-4.0" } ], "copyright": [ { "holder": "The Author(s)", "year": "2022" } ], "control_number": "74533", "record_creation_date": "2022-12-16T09:30:16.826038", "_files": [ { "checksum": "md5:2f76c42d34d7368337dfb04a4f1f27c1", "filetype": "xml", "bucket": "3a9d99e9-5e66-45c1-a9cd-fb2ffb2a844e", "version_id": "0d6bb10e-d17a-417e-98a1-7357a512b266", "key": "10.1007/JHEP12(2022)057.xml", "size": 16652 }, { "checksum": "md5:a6af5d62026856187c1577bf611a6428", "filetype": "pdf/a", "bucket": "3a9d99e9-5e66-45c1-a9cd-fb2ffb2a844e", "version_id": "360cf400-26b9-4c34-91ab-c60e184fa759", "key": "10.1007/JHEP12(2022)057_a.pdf", "size": 16568002 } ], "collections": [ { "primary": "Journal of High Energy Physics" } ], "arxiv_eprints": [ { "categories": [ "hep-ph", "hep-ex" ], "value": "2207.07382" } ], "abstracts": [ { "source": "Springer", "value": "The Scotogenic model extends the standard model with three singlet fermion N i and one inert doublet scalar \u03b7 to address the common origin of tiny neutrino mass and dark matter. For fermion dark matter N 1, a hierarchical Yukawa structure <math> <mo>\u2223</mo> <msub> <mi>y</mi> <mrow> <mn>1</mn> <mi>e</mi> </mrow> </msub> <mo>\u2223</mo> <mo>\u226a</mo> <mo>\u2223</mo> <msub> <mi>y</mi> <mrow> <mn>1</mn> <mi>\u03bc</mi> </mrow> </msub> <mo>\u2223</mo> <mo>\u223c</mo> <mo>\u2223</mo> <msub> <mi>y</mi> <mrow> <mn>1</mn> <mi>\u03c4</mi> </mrow> </msub> <mo>\u2223</mo> <mo>\u223c</mo> <mi>O</mi> <mfenced> <mn>1</mn> </mfenced> </math> $$ \\mid {y}_{1e}\\mid \\ll \\mid {y}_{1\\mu}\\mid \\sim \\mid {y}_{1\\tau}\\mid \\sim \\mathcal{O}(1) $$ is usually favored to satisfy constraints from lepton flavor violation and relic density. Such large \u03bc-related Yukawa coupling would greatly enhance the pair production of charged scalar \u03b7 \u00b1 at the muon collider. In this paper, we investigate the dilepton and mono-photon signature of the Scotogenic model at a 14 TeV muon collider. For the dimuon signature , we find that most viable samples can be probed with 200 fb \u22121 data. The ditau signature is usually less promising, but it is important to probe the small |y 1\u03bc | region. The mono-photon signature could also probe the compressed mass region M 1 \u2272 <math> <msub> <mi>M</mi> <msup> <mi>\u03b7</mi> <mo>\u00b1</mo> </msup> </msub> </math> $$ {M}_{\\eta^{\\pm }} $$ . Masses of charged scalar \u03b7 \u00b1 and dark matter N 1 can be further extracted by a binned likelihood fit of the dilepton energy." } ], "imprints": [ { "date": "2022-12-12", "publisher": "Springer" } ] }