{"title":"半光子过程的SMEFT预测","authors":"Siddhartha Karmakar, Amol Dighe, Rick S. Gupta","doi":"10.1103/physrevd.111.055002","DOIUrl":null,"url":null,"abstract":"The S</a:mi>U</a:mi>(</a:mo>2</a:mn>)</a:mo>L</a:mi></a:msub>×</a:mo>U</a:mi>(</a:mo>1</a:mn>)</a:mo>Y</a:mi></a:msub></a:math> invariance of the Standard Model effective field theory (SMEFT) predicts multiple restrictions in the space of Wilson coefficients of <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:mi>U</g:mi><g:mo stretchy=\"false\">(</g:mo><g:mn>1</g:mn><g:msub><g:mo stretchy=\"false\">)</g:mo><g:mrow><g:mi>e</g:mi><g:mi>m</g:mi></g:mrow></g:msub></g:math> invariant effective Lagrangians such as the low-energy effective field theory (LEFT), used for low-energy flavor physics observables, or the Higgs effective field theory (HEFT) in unitary gauge, appropriate for weak-scale observables. In this work, we derive and list all such predictions for semileptonic operators up to dimension 6. These predictions can be expressed as linear relations among the HEFT/LEFT Wilson coefficients (WCs), that are completely independent of any assumptions about the alignment of the mass and flavor bases. We find seven sets of relations among the WCs of vector operators, nine sets with scalar and tensor operators, and two sets with the <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:mi>Z</k:mi><k:mo>,</k:mo><k:msup><k:mi>W</k:mi><k:mo>±</k:mo></k:msup></k:math> couplings. These correspond to 2223 linear relations among the complex WCs when the quark and lepton generation indices are included. They connect diverse experimental searches such as rare meson decays, high-<m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:msub><m:mi>p</m:mi><m:mi>T</m:mi></m:msub></m:math> dilepton searches, top decays, <o:math xmlns:o=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><o:mi>Z</o:mi></o:math>-pole observables, charged lepton flavor violating observables, and nonstandard neutrino interaction searches. We demonstrate how these relations can be used to derive strong indirect constraints on multiple WCs that are currently either weakly constrained from direct experiments or have no direct bound at all. They also imply, in general, that evidence for new physics in a particular search channel must be accompanied by correlated anomalies in other channels. For example, the observed excess in <q:math xmlns:q=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><q:mi>B</q:mi><q:mo stretchy=\"false\">→</q:mo><q:mi>K</q:mi><q:mi>ν</q:mi><q:mover accent=\"true\"><q:mi>ν</q:mi><q:mo stretchy=\"false\">¯</q:mo></q:mover></q:math> would imply possible anomalies in <v:math xmlns:v=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><v:mi>B</v:mi><v:mo stretchy=\"false\">→</v:mo><v:msup><v:mi>D</v:mi><v:mrow><v:mo stretchy=\"false\">(</v:mo><v:mo>*</v:mo><v:mo stretchy=\"false\">)</v:mo></v:mrow></v:msup><v:mo>ℓ</v:mo><v:msub><v:mi>ν</v:mi><v:mo>ℓ</v:mo></v:msub></v:math>, B</ab:mi>→</ab:mo>K</ab:mi>(</ab:mo>*</ab:mo>)</ab:mo></ab:mrow></ab:msup>ℓ</ab:mo>+</ab:mo></ab:msup>ℓ</ab:mo>−</ab:mo></ab:msup></ab:math>, <fb:math xmlns:fb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><fb:msub><fb:mi>B</fb:mi><fb:mi>q</fb:mi></fb:msub><fb:mo stretchy=\"false\">→</fb:mo><fb:mi>τ</fb:mi><fb:msub><fb:mi>ν</fb:mi><fb:mi>τ</fb:mi></fb:msub></fb:math>, <ib:math xmlns:ib=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ib:msub><ib:mi>B</ib:mi><ib:mi>s</ib:mi></ib:msub><ib:mo stretchy=\"false\">→</ib:mo><ib:msup><ib:mi>τ</ib:mi><ib:mo>+</ib:mo></ib:msup><ib:msup><ib:mi>τ</ib:mi><ib:mo>−</ib:mo></ib:msup></ib:math>, <lb:math xmlns:lb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><lb:msub><lb:mi>D</lb:mi><lb:mi>s</lb:mi></lb:msub><lb:mo stretchy=\"false\">→</lb:mo><lb:msup><lb:mi>τ</lb:mi><lb:mo>+</lb:mo></lb:msup><lb:msub><lb:mi>ν</lb:mi><lb:mi>τ</lb:mi></lb:msub></lb:math>, <ob:math xmlns:ob=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ob:mi>t</ob:mi><ob:mo stretchy=\"false\">→</ob:mo><ob:mi>c</ob:mi><ob:msup><ob:mo>ℓ</ob:mo><ob:mo>+</ob:mo></ob:msup><ob:msup><ob:mo>ℓ</ob:mo><ob:mo>−</ob:mo></ob:msup></ob:math>, <rb:math xmlns:rb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><rb:mi>t</rb:mi><rb:mo stretchy=\"false\">→</rb:mo><rb:mi>u</rb:mi><rb:msup><rb:mo>ℓ</rb:mo><rb:mo>+</rb:mo></rb:msup><rb:msup><rb:mo>ℓ</rb:mo><rb:mo>−</rb:mo></rb:msup></rb:math>, etc., correlated according to the relations obtained in this paper. <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":"72 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-03-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"SMEFT predictions for semileptonic processes\",\"authors\":\"Siddhartha Karmakar, Amol Dighe, Rick S. Gupta\",\"doi\":\"10.1103/physrevd.111.055002\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The S</a:mi>U</a:mi>(</a:mo>2</a:mn>)</a:mo>L</a:mi></a:msub>×</a:mo>U</a:mi>(</a:mo>1</a:mn>)</a:mo>Y</a:mi></a:msub></a:math> invariance of the Standard Model effective field theory (SMEFT) predicts multiple restrictions in the space of Wilson coefficients of <g:math xmlns:g=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><g:mi>U</g:mi><g:mo stretchy=\\\"false\\\">(</g:mo><g:mn>1</g:mn><g:msub><g:mo stretchy=\\\"false\\\">)</g:mo><g:mrow><g:mi>e</g:mi><g:mi>m</g:mi></g:mrow></g:msub></g:math> invariant effective Lagrangians such as the low-energy effective field theory (LEFT), used for low-energy flavor physics observables, or the Higgs effective field theory (HEFT) in unitary gauge, appropriate for weak-scale observables. In this work, we derive and list all such predictions for semileptonic operators up to dimension 6. These predictions can be expressed as linear relations among the HEFT/LEFT Wilson coefficients (WCs), that are completely independent of any assumptions about the alignment of the mass and flavor bases. We find seven sets of relations among the WCs of vector operators, nine sets with scalar and tensor operators, and two sets with the <k:math xmlns:k=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><k:mi>Z</k:mi><k:mo>,</k:mo><k:msup><k:mi>W</k:mi><k:mo>±</k:mo></k:msup></k:math> couplings. These correspond to 2223 linear relations among the complex WCs when the quark and lepton generation indices are included. They connect diverse experimental searches such as rare meson decays, high-<m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><m:msub><m:mi>p</m:mi><m:mi>T</m:mi></m:msub></m:math> dilepton searches, top decays, <o:math xmlns:o=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><o:mi>Z</o:mi></o:math>-pole observables, charged lepton flavor violating observables, and nonstandard neutrino interaction searches. We demonstrate how these relations can be used to derive strong indirect constraints on multiple WCs that are currently either weakly constrained from direct experiments or have no direct bound at all. They also imply, in general, that evidence for new physics in a particular search channel must be accompanied by correlated anomalies in other channels. For example, the observed excess in <q:math xmlns:q=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><q:mi>B</q:mi><q:mo stretchy=\\\"false\\\">→</q:mo><q:mi>K</q:mi><q:mi>ν</q:mi><q:mover accent=\\\"true\\\"><q:mi>ν</q:mi><q:mo stretchy=\\\"false\\\">¯</q:mo></q:mover></q:math> would imply possible anomalies in <v:math xmlns:v=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><v:mi>B</v:mi><v:mo stretchy=\\\"false\\\">→</v:mo><v:msup><v:mi>D</v:mi><v:mrow><v:mo stretchy=\\\"false\\\">(</v:mo><v:mo>*</v:mo><v:mo stretchy=\\\"false\\\">)</v:mo></v:mrow></v:msup><v:mo>ℓ</v:mo><v:msub><v:mi>ν</v:mi><v:mo>ℓ</v:mo></v:msub></v:math>, B</ab:mi>→</ab:mo>K</ab:mi>(</ab:mo>*</ab:mo>)</ab:mo></ab:mrow></ab:msup>ℓ</ab:mo>+</ab:mo></ab:msup>ℓ</ab:mo>−</ab:mo></ab:msup></ab:math>, <fb:math xmlns:fb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><fb:msub><fb:mi>B</fb:mi><fb:mi>q</fb:mi></fb:msub><fb:mo stretchy=\\\"false\\\">→</fb:mo><fb:mi>τ</fb:mi><fb:msub><fb:mi>ν</fb:mi><fb:mi>τ</fb:mi></fb:msub></fb:math>, <ib:math xmlns:ib=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ib:msub><ib:mi>B</ib:mi><ib:mi>s</ib:mi></ib:msub><ib:mo stretchy=\\\"false\\\">→</ib:mo><ib:msup><ib:mi>τ</ib:mi><ib:mo>+</ib:mo></ib:msup><ib:msup><ib:mi>τ</ib:mi><ib:mo>−</ib:mo></ib:msup></ib:math>, <lb:math xmlns:lb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><lb:msub><lb:mi>D</lb:mi><lb:mi>s</lb:mi></lb:msub><lb:mo stretchy=\\\"false\\\">→</lb:mo><lb:msup><lb:mi>τ</lb:mi><lb:mo>+</lb:mo></lb:msup><lb:msub><lb:mi>ν</lb:mi><lb:mi>τ</lb:mi></lb:msub></lb:math>, <ob:math xmlns:ob=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ob:mi>t</ob:mi><ob:mo stretchy=\\\"false\\\">→</ob:mo><ob:mi>c</ob:mi><ob:msup><ob:mo>ℓ</ob:mo><ob:mo>+</ob:mo></ob:msup><ob:msup><ob:mo>ℓ</ob:mo><ob:mo>−</ob:mo></ob:msup></ob:math>, <rb:math xmlns:rb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><rb:mi>t</rb:mi><rb:mo stretchy=\\\"false\\\">→</rb:mo><rb:mi>u</rb:mi><rb:msup><rb:mo>ℓ</rb:mo><rb:mo>+</rb:mo></rb:msup><rb:msup><rb:mo>ℓ</rb:mo><rb:mo>−</rb:mo></rb:msup></rb:math>, etc., correlated according to the relations obtained in this paper. <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\":\"72 1\",\"pages\":\"\"},\"PeriodicalIF\":5.3000,\"publicationDate\":\"2025-03-05\",\"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.111.055002\",\"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.111.055002","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
标准模型有效场论(SMEFT)的SU(2)L×U(1)Y不变性预测了U(1)em不变有效拉格朗日的Wilson系数在空间中的多重限制,例如用于低能量flavor物理观测的低能有效场论(左),或适用于弱尺度观测的酉规希格斯有效场论(HEFT)。在这项工作中,我们推导并列出了6维以下的半子算子的所有这些预测。这些预测可以表示为HEFT/LEFT Wilson系数(WCs)之间的线性关系,它完全独立于关于质量和风味基排列的任何假设。我们找到了7组向量算子WCs之间的关系,9组标量和张量算子WCs之间的关系,以及2组Z,W±耦合的关系。当包括夸克和轻子产生指标时,这些对应于复杂WCs之间的2223个线性关系。他们将不同的实验搜索,如罕见介子衰变、高pt双轻子搜索、顶部衰变、z极观测、带电轻子味违反观测和非标准中微子相互作用搜索联系起来。我们演示了如何使用这些关系来推导对多个WCs的强间接约束,这些WCs目前要么受到直接实验的弱约束,要么根本没有直接约束。一般来说,它们还意味着,在一个特定的搜索通道中,新物理学的证据必须伴随着其他通道中相关的异常。例如,在B→Kνν¯中观测到的过剩可能意味着在B→D(*) r νν, B→K(*) r + r−,Bq→τντ, B→τ+ r−,Ds→τ+ντ, t→c r + r−,t→u r + r−等中存在异常,根据本文得到的关系进行相关。2025年由美国物理学会出版
The SU(2)L×U(1)Y invariance of the Standard Model effective field theory (SMEFT) predicts multiple restrictions in the space of Wilson coefficients of U(1)em invariant effective Lagrangians such as the low-energy effective field theory (LEFT), used for low-energy flavor physics observables, or the Higgs effective field theory (HEFT) in unitary gauge, appropriate for weak-scale observables. In this work, we derive and list all such predictions for semileptonic operators up to dimension 6. These predictions can be expressed as linear relations among the HEFT/LEFT Wilson coefficients (WCs), that are completely independent of any assumptions about the alignment of the mass and flavor bases. We find seven sets of relations among the WCs of vector operators, nine sets with scalar and tensor operators, and two sets with the Z,W± couplings. These correspond to 2223 linear relations among the complex WCs when the quark and lepton generation indices are included. They connect diverse experimental searches such as rare meson decays, high-pT dilepton searches, top decays, Z-pole observables, charged lepton flavor violating observables, and nonstandard neutrino interaction searches. We demonstrate how these relations can be used to derive strong indirect constraints on multiple WCs that are currently either weakly constrained from direct experiments or have no direct bound at all. They also imply, in general, that evidence for new physics in a particular search channel must be accompanied by correlated anomalies in other channels. For example, the observed excess in B→Kνν¯ would imply possible anomalies in B→D(*)ℓνℓ, B→K(*)ℓ+ℓ−, Bq→τντ, Bs→τ+τ−, Ds→τ+ντ, t→cℓ+ℓ−, t→uℓ+ℓ−, etc., correlated according to the relations obtained in this paper. Published by the American Physical Society2025
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.