Search for U1Lμ−Lτ charged dark matter with neutrino telescope
A bstract We study a simple Dirac fermion dark matter model in U 1 L μ − L τ theory. The new light gauge boson X plays important roles in both dark matter physics and the explanation for the muon g − 2 anomaly. The observed dark matter relic density is realized by a large U 1 L μ − L τ charge withou...
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container_title | The journal of high energy physics |
container_volume | 2021 |
creator | Asai, Kento Okawa, Shohei Tsumura, Koji |
description | A
bstract
We study a simple Dirac fermion dark matter model in
U
1
L
μ
−
L
τ
theory. The new light gauge boson
X
plays important roles in both dark matter physics and the explanation for the muon
g
−
2 anomaly. The observed dark matter relic density is realized by a large
U
1
L
μ
−
L
τ
charge without introducing a resonance effect of the
X
boson. As a by-product of the model, characteristic neutrino signatures from sub-GeV dark matter
ψ
are predicted depending on the mass spectrum. We formulate the analysis of
ψ
ψ
¯
→
ν
ν
¯
, and of
ψ
ψ
¯
→
XX
followed by
X
→
ν
ν
¯
in a model independent way. The energy spectrum of neutrinos in the former process is monochromatic while in the latter process is bowl-shape. We also evaluate sensitivity at Super-Kamiokande and future Hyper-Kamiokande detectors. The analysis is finally applied to the
U
1
L
μ
−
L
τ
dark matter model. |
doi_str_mv | 10.1007/JHEP03(2021)047 |
format | Article |
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bstract
We study a simple Dirac fermion dark matter model in
U
1
L
μ
−
L
τ
theory. The new light gauge boson
X
plays important roles in both dark matter physics and the explanation for the muon
g
−
2 anomaly. The observed dark matter relic density is realized by a large
U
1
L
μ
−
L
τ
charge without introducing a resonance effect of the
X
boson. As a by-product of the model, characteristic neutrino signatures from sub-GeV dark matter
ψ
are predicted depending on the mass spectrum. We formulate the analysis of
ψ
ψ
¯
→
ν
ν
¯
, and of
ψ
ψ
¯
→
XX
followed by
X
→
ν
ν
¯
in a model independent way. The energy spectrum of neutrinos in the former process is monochromatic while in the latter process is bowl-shape. We also evaluate sensitivity at Super-Kamiokande and future Hyper-Kamiokande detectors. The analysis is finally applied to the
U
1
L
μ
−
L
τ
dark matter model.</description><identifier>EISSN: 1029-8479</identifier><identifier>DOI: 10.1007/JHEP03(2021)047</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Classical and Quantum Gravitation ; Dark matter ; Elementary Particles ; Energy spectra ; Fermions ; High energy physics ; Neutrinos ; Physics ; Physics and Astronomy ; Quantum Field Theories ; Quantum Field Theory ; Quantum Physics ; Regular Article - Theoretical Physics ; Relativity Theory ; String Theory</subject><ispartof>The journal of high energy physics, 2021-03, Vol.2021 (3)</ispartof><rights>The Author(s) 2021</rights><rights>The Author(s) 2021. This work is published under CC-BY 4.0 (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0002-6454-4539</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/JHEP03(2021)047$$EPDF$$P50$$Gspringer$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://doi.org/10.1007/JHEP03(2021)047$$EHTML$$P50$$Gspringer$$Hfree_for_read</linktohtml><link.rule.ids>314,780,784,864,27922,27923,41118,42187,51574</link.rule.ids></links><search><creatorcontrib>Asai, Kento</creatorcontrib><creatorcontrib>Okawa, Shohei</creatorcontrib><creatorcontrib>Tsumura, Koji</creatorcontrib><title>Search for U1Lμ−Lτ charged dark matter with neutrino telescope</title><title>The journal of high energy physics</title><addtitle>J. High Energ. Phys</addtitle><description>A
bstract
We study a simple Dirac fermion dark matter model in
U
1
L
μ
−
L
τ
theory. The new light gauge boson
X
plays important roles in both dark matter physics and the explanation for the muon
g
−
2 anomaly. The observed dark matter relic density is realized by a large
U
1
L
μ
−
L
τ
charge without introducing a resonance effect of the
X
boson. As a by-product of the model, characteristic neutrino signatures from sub-GeV dark matter
ψ
are predicted depending on the mass spectrum. We formulate the analysis of
ψ
ψ
¯
→
ν
ν
¯
, and of
ψ
ψ
¯
→
XX
followed by
X
→
ν
ν
¯
in a model independent way. The energy spectrum of neutrinos in the former process is monochromatic while in the latter process is bowl-shape. We also evaluate sensitivity at Super-Kamiokande and future Hyper-Kamiokande detectors. The analysis is finally applied to the
U
1
L
μ
−
L
τ
dark matter model.</description><subject>Classical and Quantum Gravitation</subject><subject>Dark matter</subject><subject>Elementary Particles</subject><subject>Energy spectra</subject><subject>Fermions</subject><subject>High energy physics</subject><subject>Neutrinos</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Field Theories</subject><subject>Quantum Field Theory</subject><subject>Quantum Physics</subject><subject>Regular Article - Theoretical Physics</subject><subject>Relativity Theory</subject><subject>String Theory</subject><issn>1029-8479</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>C6C</sourceid><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNpFkM9Kw0AQhxdBsFbPXhe86CE6s9lks0ct1SoBBes55M9s01qTuNngC3jw7PP4DPoOPolbKniZgeFjfj8-xo4QzhBAnd_OpvcQnggQeApS7bARgtBBIpXeY_t9vwLACDWM2OUD5basuWktf8T06_Pn_SP9fuNlndsFVbzK7RN_zp0jy1-XruYNDc4um5Y7WlNfth0dsF2Tr3s6_NtjNr-aziezIL27vplcpEEXaxUUGJHBQkkjNCTCiDgiUQpN_gymiLBKdFzqokwwQYNSRypBVEKCiUIMKRyz4-3bzrYvA_UuW7WDbXxiJqSOReyn8hRsqb7zLRdk_ymEbCMn28rJNnIyLyf8Bc0CWc8</recordid><startdate>20210303</startdate><enddate>20210303</enddate><creator>Asai, Kento</creator><creator>Okawa, Shohei</creator><creator>Tsumura, Koji</creator><general>Springer Berlin Heidelberg</general><general>Springer Nature B.V</general><scope>C6C</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><orcidid>https://orcid.org/0000-0002-6454-4539</orcidid></search><sort><creationdate>20210303</creationdate><title>Search for U1Lμ−Lτ charged dark matter with neutrino telescope</title><author>Asai, Kento ; Okawa, Shohei ; Tsumura, Koji</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p697-b15ef1b74f29082f265e2c29e5ef0fb51d896c9bc8181f149578117240f5313e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Classical and Quantum Gravitation</topic><topic>Dark matter</topic><topic>Elementary Particles</topic><topic>Energy spectra</topic><topic>Fermions</topic><topic>High energy physics</topic><topic>Neutrinos</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quantum Field Theories</topic><topic>Quantum Field Theory</topic><topic>Quantum Physics</topic><topic>Regular Article - Theoretical Physics</topic><topic>Relativity Theory</topic><topic>String Theory</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Asai, Kento</creatorcontrib><creatorcontrib>Okawa, Shohei</creatorcontrib><creatorcontrib>Tsumura, Koji</creatorcontrib><collection>Springer Nature OA Free Journals</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection (ProQuest)</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><jtitle>The journal of high energy physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Asai, Kento</au><au>Okawa, Shohei</au><au>Tsumura, Koji</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Search for U1Lμ−Lτ charged dark matter with neutrino telescope</atitle><jtitle>The journal of high energy physics</jtitle><stitle>J. High Energ. Phys</stitle><date>2021-03-03</date><risdate>2021</risdate><volume>2021</volume><issue>3</issue><eissn>1029-8479</eissn><abstract>A
bstract
We study a simple Dirac fermion dark matter model in
U
1
L
μ
−
L
τ
theory. The new light gauge boson
X
plays important roles in both dark matter physics and the explanation for the muon
g
−
2 anomaly. The observed dark matter relic density is realized by a large
U
1
L
μ
−
L
τ
charge without introducing a resonance effect of the
X
boson. As a by-product of the model, characteristic neutrino signatures from sub-GeV dark matter
ψ
are predicted depending on the mass spectrum. We formulate the analysis of
ψ
ψ
¯
→
ν
ν
¯
, and of
ψ
ψ
¯
→
XX
followed by
X
→
ν
ν
¯
in a model independent way. The energy spectrum of neutrinos in the former process is monochromatic while in the latter process is bowl-shape. We also evaluate sensitivity at Super-Kamiokande and future Hyper-Kamiokande detectors. The analysis is finally applied to the
U
1
L
μ
−
L
τ
dark matter model.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1007/JHEP03(2021)047</doi><orcidid>https://orcid.org/0000-0002-6454-4539</orcidid><oa>free_for_read</oa></addata></record> |
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issn | 1029-8479 |
language | eng |
recordid | cdi_proquest_journals_2496262497 |
source | DOAJ Directory of Open Access Journals; Springer Nature OA Free Journals; EZB-FREE-00999 freely available EZB journals; Alma/SFX Local Collection |
subjects | Classical and Quantum Gravitation Dark matter Elementary Particles Energy spectra Fermions High energy physics Neutrinos Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quantum Physics Regular Article - Theoretical Physics Relativity Theory String Theory |
title | Search for U1Lμ−Lτ charged dark matter with neutrino telescope |
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