Z工厂的三个Z签名

IF 5.3 2区 物理与天体物理 Q1 Physics and Astronomy
Takaaki Nomura, Kei Yagyu
{"title":"Z工厂的三个Z签名","authors":"Takaaki Nomura, Kei Yagyu","doi":"10.1103/physrevd.111.095012","DOIUrl":null,"url":null,"abstract":"We discuss triple Z</a:mi>′</a:mo></a:msup></a:math> boson signatures via the decay chain of <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mi>Z</c:mi><c:mo stretchy=\"false\">→</c:mo><c:msup><c:mi>Z</c:mi><c:mo>′</c:mo></c:msup><c:mi>ϕ</c:mi><c:mo stretchy=\"false\">→</c:mo><c:msup><c:mi>Z</c:mi><c:mo>′</c:mo></c:msup><c:msup><c:mi>Z</c:mi><c:mo>′</c:mo></c:msup><c:msup><c:mi>Z</c:mi><c:mo>′</c:mo></c:msup></c:math>, with a new light scalar <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:mi>ϕ</g:mi></g:math>, at future <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:mi>Z</i:mi></i:math> factories such as the Circular Electron-Positron Collider and Future Circular Collider. These new bosons <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:mi>ϕ</k:mi></k:math> and <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:msup><m:mi>Z</m:mi><m:mo>′</m:mo></m:msup></m:math> naturally appear in models with a new <o:math xmlns:o=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><o:mi>U</o:mi><o:mo stretchy=\"false\">(</o:mo><o:mn>1</o:mn><o:mo stretchy=\"false\">)</o:mo></o:math> gauge symmetry which is spontaneously broken and introduced in various new physics scenarios. The branching ratio of <s:math xmlns:s=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><s:mi>Z</s:mi><s:mo stretchy=\"false\">→</s:mo><s:msup><s:mi>Z</s:mi><s:mo>′</s:mo></s:msup><s:mi>ϕ</s:mi><s:mo stretchy=\"false\">→</s:mo><s:msup><s:mi>Z</s:mi><s:mo>′</s:mo></s:msup><s:msup><s:mi>Z</s:mi><s:mo>′</s:mo></s:msup><s:msup><s:mi>Z</s:mi><s:mo>′</s:mo></s:msup></s:math> can be larger than <w:math xmlns:w=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><w:msup><w:mn>10</w:mn><w:mrow><w:mo>−</w:mo><w:mn>12</w:mn></w:mrow></w:msup></w:math>, which gives <y:math xmlns:y=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><y:mi>O</y:mi><y:mo stretchy=\"false\">(</y:mo><y:mn>1</y:mn><y:mo stretchy=\"false\">)</y:mo></y:math> events at Tera-<cb:math xmlns:cb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cb:mi>Z</cb:mi></cb:math> experiments, when a product of <eb:math xmlns:eb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><eb:msub><eb:mi>g</eb:mi><eb:mi>X</eb:mi></eb:msub></eb:math> (new gauge coupling) and <gb:math xmlns:gb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gb:mi>ζ</gb:mi></gb:math> (<ib:math xmlns:ib=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ib:mi>Z</ib:mi><ib:mo>−</ib:mo><ib:msup><ib:mi>Z</ib:mi><ib:mo>′</ib:mo></ib:msup></ib:math> mixing) is larger than around <kb:math xmlns:kb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><kb:msup><kb:mn>10</kb:mn><kb:mrow><kb:mo>−</kb:mo><kb:mn>6</kb:mn></kb:mrow></kb:msup></kb:math>. We find that the search for <mb:math xmlns:mb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mb:mi>Z</mb:mi><mb:mo stretchy=\"false\">→</mb:mo><mb:msup><mb:mi>Z</mb:mi><mb:mo>′</mb:mo></mb:msup><mb:msup><mb:mi>Z</mb:mi><mb:mo>′</mb:mo></mb:msup><mb:msup><mb:mi>Z</mb:mi><mb:mo>′</mb:mo></mb:msup></mb:math> can significantly improve the current bound on a kinetic mixing parameter <pb:math xmlns:pb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><pb:mi>ε</pb:mi></pb:math> in the dark photon case, where <rb:math xmlns:rb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><rb:mi>e</rb:mi><rb:mi>ε</rb:mi><rb:mo>≳</rb:mo><rb:mi mathvariant=\"script\">O</rb:mi><rb:mo stretchy=\"false\">(</rb:mo><rb:msup><rb:mn>10</rb:mn><rb:mrow><rb:mo>−</rb:mo><rb:mn>5</rb:mn></rb:mrow></rb:msup><rb:mo stretchy=\"false\">)</rb:mo></rb:math> with <wb:math xmlns:wb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><wb:msub><wb:mi>g</wb:mi><wb:mi>X</wb:mi></wb:msub><wb:mo>=</wb:mo><wb:mi mathvariant=\"script\">O</wb:mi><wb:mo stretchy=\"false\">(</wb:mo><wb:mn>1</wb:mn><wb:mo stretchy=\"false\">)</wb:mo></wb:math> can be explored at Tera-<bc:math xmlns:bc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><bc:mi>Z</bc:mi></bc:math> experiments. We also show that a sufficiently large number of events with multilepton plus hadronic jets can be obtained in benchmark points, which cannot be realized by the usual decay of <dc:math xmlns:dc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><dc:mi>Z</dc:mi></dc:math> in the standard model. <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":"117 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-05-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Triple Z′ signatures at Z factories\",\"authors\":\"Takaaki Nomura, Kei Yagyu\",\"doi\":\"10.1103/physrevd.111.095012\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We discuss triple Z</a:mi>′</a:mo></a:msup></a:math> boson signatures via the decay chain of <c:math xmlns:c=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><c:mi>Z</c:mi><c:mo stretchy=\\\"false\\\">→</c:mo><c:msup><c:mi>Z</c:mi><c:mo>′</c:mo></c:msup><c:mi>ϕ</c:mi><c:mo stretchy=\\\"false\\\">→</c:mo><c:msup><c:mi>Z</c:mi><c:mo>′</c:mo></c:msup><c:msup><c:mi>Z</c:mi><c:mo>′</c:mo></c:msup><c:msup><c:mi>Z</c:mi><c:mo>′</c:mo></c:msup></c:math>, with a new light scalar <g:math xmlns:g=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><g:mi>ϕ</g:mi></g:math>, at future <i:math xmlns:i=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><i:mi>Z</i:mi></i:math> factories such as the Circular Electron-Positron Collider and Future Circular Collider. These new bosons <k:math xmlns:k=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><k:mi>ϕ</k:mi></k:math> and <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><m:msup><m:mi>Z</m:mi><m:mo>′</m:mo></m:msup></m:math> naturally appear in models with a new <o:math xmlns:o=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><o:mi>U</o:mi><o:mo stretchy=\\\"false\\\">(</o:mo><o:mn>1</o:mn><o:mo stretchy=\\\"false\\\">)</o:mo></o:math> gauge symmetry which is spontaneously broken and introduced in various new physics scenarios. The branching ratio of <s:math xmlns:s=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><s:mi>Z</s:mi><s:mo stretchy=\\\"false\\\">→</s:mo><s:msup><s:mi>Z</s:mi><s:mo>′</s:mo></s:msup><s:mi>ϕ</s:mi><s:mo stretchy=\\\"false\\\">→</s:mo><s:msup><s:mi>Z</s:mi><s:mo>′</s:mo></s:msup><s:msup><s:mi>Z</s:mi><s:mo>′</s:mo></s:msup><s:msup><s:mi>Z</s:mi><s:mo>′</s:mo></s:msup></s:math> can be larger than <w:math xmlns:w=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><w:msup><w:mn>10</w:mn><w:mrow><w:mo>−</w:mo><w:mn>12</w:mn></w:mrow></w:msup></w:math>, which gives <y:math xmlns:y=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><y:mi>O</y:mi><y:mo stretchy=\\\"false\\\">(</y:mo><y:mn>1</y:mn><y:mo stretchy=\\\"false\\\">)</y:mo></y:math> events at Tera-<cb:math xmlns:cb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><cb:mi>Z</cb:mi></cb:math> experiments, when a product of <eb:math xmlns:eb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><eb:msub><eb:mi>g</eb:mi><eb:mi>X</eb:mi></eb:msub></eb:math> (new gauge coupling) and <gb:math xmlns:gb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><gb:mi>ζ</gb:mi></gb:math> (<ib:math xmlns:ib=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ib:mi>Z</ib:mi><ib:mo>−</ib:mo><ib:msup><ib:mi>Z</ib:mi><ib:mo>′</ib:mo></ib:msup></ib:math> mixing) is larger than around <kb:math xmlns:kb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><kb:msup><kb:mn>10</kb:mn><kb:mrow><kb:mo>−</kb:mo><kb:mn>6</kb:mn></kb:mrow></kb:msup></kb:math>. We find that the search for <mb:math xmlns:mb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mb:mi>Z</mb:mi><mb:mo stretchy=\\\"false\\\">→</mb:mo><mb:msup><mb:mi>Z</mb:mi><mb:mo>′</mb:mo></mb:msup><mb:msup><mb:mi>Z</mb:mi><mb:mo>′</mb:mo></mb:msup><mb:msup><mb:mi>Z</mb:mi><mb:mo>′</mb:mo></mb:msup></mb:math> can significantly improve the current bound on a kinetic mixing parameter <pb:math xmlns:pb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><pb:mi>ε</pb:mi></pb:math> in the dark photon case, where <rb:math xmlns:rb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><rb:mi>e</rb:mi><rb:mi>ε</rb:mi><rb:mo>≳</rb:mo><rb:mi mathvariant=\\\"script\\\">O</rb:mi><rb:mo stretchy=\\\"false\\\">(</rb:mo><rb:msup><rb:mn>10</rb:mn><rb:mrow><rb:mo>−</rb:mo><rb:mn>5</rb:mn></rb:mrow></rb:msup><rb:mo stretchy=\\\"false\\\">)</rb:mo></rb:math> with <wb:math xmlns:wb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><wb:msub><wb:mi>g</wb:mi><wb:mi>X</wb:mi></wb:msub><wb:mo>=</wb:mo><wb:mi mathvariant=\\\"script\\\">O</wb:mi><wb:mo stretchy=\\\"false\\\">(</wb:mo><wb:mn>1</wb:mn><wb:mo stretchy=\\\"false\\\">)</wb:mo></wb:math> can be explored at Tera-<bc:math xmlns:bc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><bc:mi>Z</bc:mi></bc:math> experiments. We also show that a sufficiently large number of events with multilepton plus hadronic jets can be obtained in benchmark points, which cannot be realized by the usual decay of <dc:math xmlns:dc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><dc:mi>Z</dc:mi></dc:math> in the standard model. <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\":\"117 1\",\"pages\":\"\"},\"PeriodicalIF\":5.3000,\"publicationDate\":\"2025-05-12\",\"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.111.095012\",\"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.111.095012","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

我们通过Z→Z′φ→Z′Z′φ的衰变链,用一个新的轻标量φ,在未来的Z工厂如环形正电子对撞机和未来圆形对撞机中讨论了三重Z′玻色子特征。这些新的玻色子φ和Z '自然地出现在具有新的U(1)规范对称的模型中,这种对称性在各种新的物理场景中被自发地打破并引入。当gX(新规耦合)和ζ (Z−Z′混合)的乘积大于10−6时,Z→Z′φ→Z′Z′的分支比可以大于10−12,从而在terra -Z实验中产生O(1)个事件。我们发现寻找Z→Z ' Z ‘ Z ’可以显著改善暗光子情况下动力学混合参数ε的电流界,其中ε ε≥0(10−5)且gX= 0(1)可以在terra -Z实验中探索。我们还表明,在基准点上可以获得足够多的带有多轻子和强子射流的事件,这是标准模型中通常的Z衰变所无法实现的。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。
Triple Z′ signatures at Z factories
We discuss triple Z′ boson signatures via the decay chain of ZZϕZZZ, with a new light scalar ϕ, at future Z factories such as the Circular Electron-Positron Collider and Future Circular Collider. These new bosons ϕ and Z naturally appear in models with a new U(1) gauge symmetry which is spontaneously broken and introduced in various new physics scenarios. The branching ratio of ZZϕZZZ can be larger than 1012, which gives O(1) events at Tera-Z experiments, when a product of gX (new gauge coupling) and ζ (ZZ mixing) is larger than around 106. We find that the search for ZZZZ can significantly improve the current bound on a kinetic mixing parameter ε in the dark photon case, where eεO(105) with gX=O(1) can be explored at Tera-Z experiments. We also show that a sufficiently large number of events with multilepton plus hadronic jets can be obtained in benchmark points, which cannot be realized by the usual decay of Z in the standard model. Published by the American Physical Society 2025
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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.
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