{"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
We discuss triple Z′ boson signatures via the decay chain of Z→Z′ϕ→Z′Z′Z′, 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 Z→Z′ϕ→Z′Z′Z′ can be larger than 10−12, which gives O(1) events at Tera-Z experiments, when a product of gX (new gauge coupling) and ζ (Z−Z′ mixing) is larger than around 10−6. We find that the search for Z→Z′Z′Z′ can significantly improve the current bound on a kinetic mixing parameter ε in the dark photon case, where eε≳O(10−5) 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 Society2025
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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.
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