来自iii型跷跷板框架的不对称长寿命暗物质和纤生现象

IF 5.3 2区 物理与天体物理 Q1 Physics and Astronomy
Satyabrata Mahapatra, Partha Kumar Paul, Narendra Sahu, Prashant Shukla
{"title":"来自iii型跷跷板框架的不对称长寿命暗物质和纤生现象","authors":"Satyabrata Mahapatra, Partha Kumar Paul, Narendra Sahu, Prashant Shukla","doi":"10.1103/physrevd.111.015043","DOIUrl":null,"url":null,"abstract":"We propose a simple model in the type-III seesaw framework to explain the neutrino mass, asymmetric dark matter (DM), and baryon asymmetry of the Universe. We extend the Standard Model with a vectorlike singlet lepton (χ</a:mi></a:math>) and a hypercharge zero scalar triplet (<c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mi mathvariant=\"normal\">Δ</c:mi></c:math>) in addition to three hypercharge zero triplet fermions (<f:math xmlns:f=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><f:msub><f:mi mathvariant=\"normal\">Σ</f:mi><f:mi>i</f:mi></f:msub><f:mo>,</f:mo><f:mi>i</f:mi><f:mo>=</f:mo><f:mn>1</f:mn></f:math>, 2, 3). A <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:msub><i:mi>Z</i:mi><i:mn>2</i:mn></i:msub></i:math> symmetry is imposed under which <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:mi>χ</k:mi></k:math> and <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:mi mathvariant=\"normal\">Δ</m:mi></m:math> are odd, while all other particles are even. As a result, the lightest <p:math xmlns:p=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><p:msub><p:mi>Z</p:mi><p:mn>2</p:mn></p:msub></p:math> odd particle <r:math xmlns:r=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><r:mi>χ</r:mi></r:math> behaves as a candidate of DM. In the early Universe, the <t:math xmlns:t=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><t:mi>C</t:mi><t:mi>P</t:mi></t:math>-violating out-of-equilibrium decay of heavy triplet fermions to the Standard Model lepton (<v:math xmlns:v=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><v:mi>L</v:mi></v:math>) and Higgs (<x:math xmlns:x=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><x:mi>H</x:mi></x:math>) generate a net lepton asymmetry, while that of triplet fermions to <z:math xmlns:z=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><z:mi>χ</z:mi></z:math> and <bb:math xmlns:bb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><bb:mi mathvariant=\"normal\">Δ</bb:mi></bb:math> generate a net asymmetric DM. The lepton asymmetry is converted to the required baryon asymmetry of the Universe via the electroweak sphalerons, while the asymmetry in <eb:math xmlns:eb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><eb:mi>χ</eb:mi></eb:math> remains as a DM relic that we observe today. We introduce a singlet scalar <gb:math xmlns:gb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gb:mi mathvariant=\"normal\">Φ</gb:mi></gb:math>, with mass <jb:math xmlns:jb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jb:msub><jb:mi>M</jb:mi><jb:mi mathvariant=\"normal\">Φ</jb:mi></jb:msub><jb:mo>&lt;</jb:mo><jb:msub><jb:mi>M</jb:mi><jb:mi>χ</jb:mi></jb:msub></jb:math>, which not only assists to deplete the symmetric component of <mb:math xmlns:mb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mb:mi>χ</mb:mi></mb:math> through the annihilation process <ob:math xmlns:ob=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ob:mover accent=\"true\"><ob:mi>χ</ob:mi><ob:mo stretchy=\"false\">¯</ob:mo></ob:mover><ob:mi>χ</ob:mi><ob:mo stretchy=\"false\">→</ob:mo><ob:mi mathvariant=\"normal\">Φ</ob:mi><ob:mi mathvariant=\"normal\">Φ</ob:mi></ob:math>, but also paves a path to detect DM <vb:math xmlns:vb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><vb:mi>χ</vb:mi></vb:math> at direct search experiments through <xb:math xmlns:xb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><xb:mi mathvariant=\"normal\">Φ</xb:mi><xb:mo>−</xb:mo><xb:mi>H</xb:mi></xb:math> mixing. The electroweak symmetry breaking induces a nonzero vacuum expectation value to Δ</ac:mi></ac:math>, which leads to an unstable asymmetric DM ranging from a few MeV to hundreds of GeV. We then explore the displaced vertex signatures of the charged components of the scalar triplet <dc:math xmlns:dc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><dc:mi mathvariant=\"normal\">Δ</dc:mi></dc:math> at colliders. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"128 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-01-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Asymmetric long-lived dark matter and leptogenesis from the type-III seesaw framework\",\"authors\":\"Satyabrata Mahapatra, Partha Kumar Paul, Narendra Sahu, Prashant Shukla\",\"doi\":\"10.1103/physrevd.111.015043\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We propose a simple model in the type-III seesaw framework to explain the neutrino mass, asymmetric dark matter (DM), and baryon asymmetry of the Universe. We extend the Standard Model with a vectorlike singlet lepton (χ</a:mi></a:math>) and a hypercharge zero scalar triplet (<c:math xmlns:c=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><c:mi mathvariant=\\\"normal\\\">Δ</c:mi></c:math>) in addition to three hypercharge zero triplet fermions (<f:math xmlns:f=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><f:msub><f:mi mathvariant=\\\"normal\\\">Σ</f:mi><f:mi>i</f:mi></f:msub><f:mo>,</f:mo><f:mi>i</f:mi><f:mo>=</f:mo><f:mn>1</f:mn></f:math>, 2, 3). A <i:math xmlns:i=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><i:msub><i:mi>Z</i:mi><i:mn>2</i:mn></i:msub></i:math> symmetry is imposed under which <k:math xmlns:k=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><k:mi>χ</k:mi></k:math> and <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><m:mi mathvariant=\\\"normal\\\">Δ</m:mi></m:math> are odd, while all other particles are even. As a result, the lightest <p:math xmlns:p=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><p:msub><p:mi>Z</p:mi><p:mn>2</p:mn></p:msub></p:math> odd particle <r:math xmlns:r=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><r:mi>χ</r:mi></r:math> behaves as a candidate of DM. In the early Universe, the <t:math xmlns:t=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><t:mi>C</t:mi><t:mi>P</t:mi></t:math>-violating out-of-equilibrium decay of heavy triplet fermions to the Standard Model lepton (<v:math xmlns:v=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><v:mi>L</v:mi></v:math>) and Higgs (<x:math xmlns:x=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><x:mi>H</x:mi></x:math>) generate a net lepton asymmetry, while that of triplet fermions to <z:math xmlns:z=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><z:mi>χ</z:mi></z:math> and <bb:math xmlns:bb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><bb:mi mathvariant=\\\"normal\\\">Δ</bb:mi></bb:math> generate a net asymmetric DM. The lepton asymmetry is converted to the required baryon asymmetry of the Universe via the electroweak sphalerons, while the asymmetry in <eb:math xmlns:eb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><eb:mi>χ</eb:mi></eb:math> remains as a DM relic that we observe today. We introduce a singlet scalar <gb:math xmlns:gb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><gb:mi mathvariant=\\\"normal\\\">Φ</gb:mi></gb:math>, with mass <jb:math xmlns:jb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><jb:msub><jb:mi>M</jb:mi><jb:mi mathvariant=\\\"normal\\\">Φ</jb:mi></jb:msub><jb:mo>&lt;</jb:mo><jb:msub><jb:mi>M</jb:mi><jb:mi>χ</jb:mi></jb:msub></jb:math>, which not only assists to deplete the symmetric component of <mb:math xmlns:mb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mb:mi>χ</mb:mi></mb:math> through the annihilation process <ob:math xmlns:ob=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ob:mover accent=\\\"true\\\"><ob:mi>χ</ob:mi><ob:mo stretchy=\\\"false\\\">¯</ob:mo></ob:mover><ob:mi>χ</ob:mi><ob:mo stretchy=\\\"false\\\">→</ob:mo><ob:mi mathvariant=\\\"normal\\\">Φ</ob:mi><ob:mi mathvariant=\\\"normal\\\">Φ</ob:mi></ob:math>, but also paves a path to detect DM <vb:math xmlns:vb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><vb:mi>χ</vb:mi></vb:math> at direct search experiments through <xb:math xmlns:xb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><xb:mi mathvariant=\\\"normal\\\">Φ</xb:mi><xb:mo>−</xb:mo><xb:mi>H</xb:mi></xb:math> mixing. The electroweak symmetry breaking induces a nonzero vacuum expectation value to Δ</ac:mi></ac:math>, which leads to an unstable asymmetric DM ranging from a few MeV to hundreds of GeV. We then explore the displaced vertex signatures of the charged components of the scalar triplet <dc:math xmlns:dc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><dc:mi mathvariant=\\\"normal\\\">Δ</dc:mi></dc:math> at colliders. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>\",\"PeriodicalId\":20167,\"journal\":{\"name\":\"Physical Review D\",\"volume\":\"128 1\",\"pages\":\"\"},\"PeriodicalIF\":5.3000,\"publicationDate\":\"2025-01-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical Review D\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/physrevd.111.015043\",\"RegionNum\":2,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"Physics and Astronomy\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review D","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevd.111.015043","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"Physics and Astronomy","Score":null,"Total":0}
引用次数: 0

摘要

我们在iii型跷跷板框架中提出了一个简单的模型来解释中微子质量、不对称暗物质(DM)和宇宙重子的不对称。我们用一个类矢量的单重轻子(χ)和一个超荷零标量三重态(Δ)以及三个超荷零三重态费米子(Σi,i= 1,2,3)扩展了标准模型。施加了一个Z2对称,其中χ和Δ是奇数,而所有其他粒子都是偶数。结果,最轻的Z2奇粒子χ表现为DM的候选者。在早期宇宙中,重三重态费米子对标准模型轻子(L)和希格斯(H)的违反cp的失平衡衰变产生净轻子不对称,而三重态费米子对χ和Δ的失平衡衰变产生净不对称DM。轻子不对称通过电弱弹跳子转化为宇宙所需的重子不对称。而χ的不对称性仍然是我们今天观察到的DM遗迹。我们引入了一个质量为MΦ<;Mχ的单重标量Φ,它不仅有助于通过湮灭过程χ¯χ→ΦΦ耗尽χ的对称分量,而且为通过Φ−H混合直接搜索实验检测DM χ铺平了道路。电弱对称性破缺导致真空期望值为Δ,导致不稳定的非对称DM在几MeV到数百GeV之间。然后,我们在对撞机上探索标量三重态Δ带电分量的位移顶点特征。2025年由美国物理学会出版
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Asymmetric long-lived dark matter and leptogenesis from the type-III seesaw framework
We propose a simple model in the type-III seesaw framework to explain the neutrino mass, asymmetric dark matter (DM), and baryon asymmetry of the Universe. We extend the Standard Model with a vectorlike singlet lepton (χ) and a hypercharge zero scalar triplet (Δ) in addition to three hypercharge zero triplet fermions (Σi,i=1, 2, 3). A Z2 symmetry is imposed under which χ and Δ are odd, while all other particles are even. As a result, the lightest Z2 odd particle χ behaves as a candidate of DM. In the early Universe, the CP-violating out-of-equilibrium decay of heavy triplet fermions to the Standard Model lepton (L) and Higgs (H) generate a net lepton asymmetry, while that of triplet fermions to χ and Δ generate a net asymmetric DM. The lepton asymmetry is converted to the required baryon asymmetry of the Universe via the electroweak sphalerons, while the asymmetry in χ remains as a DM relic that we observe today. We introduce a singlet scalar Φ, with mass MΦ<Mχ, which not only assists to deplete the symmetric component of χ through the annihilation process χ¯χΦΦ, but also paves a path to detect DM χ at direct search experiments through ΦH mixing. The electroweak symmetry breaking induces a nonzero vacuum expectation value to Δ, which leads to an unstable asymmetric DM ranging from a few MeV to hundreds of GeV. We then explore the displaced vertex signatures of the charged components of the scalar triplet Δ at colliders. Published by the American Physical Society 2025
求助全文
通过发布文献求助,成功后即可免费获取论文全文。 去求助
来源期刊
Physical Review D
Physical Review D 物理-天文与天体物理
CiteScore
9.20
自引率
36.00%
发文量
0
审稿时长
2 months
期刊介绍: Physical Review D (PRD) is a leading journal in elementary particle physics, field theory, gravitation, and cosmology and is one of the top-cited journals in high-energy physics. PRD covers experimental and theoretical results in all aspects of particle physics, field theory, gravitation and cosmology, including: Particle physics experiments, Electroweak interactions, Strong interactions, Lattice field theories, lattice QCD, Beyond the standard model physics, Phenomenological aspects of field theory, general methods, Gravity, cosmology, cosmic rays, Astrophysics and astroparticle physics, General relativity, Formal aspects of field theory, field theory in curved space, String theory, quantum gravity, gauge/gravity duality.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术官方微信