{"title":"动力学混合和传送门物质的UV模型。7。3c3L1A1B模型中的一个亮暗光子","authors":"Thomas G. Rizzo","doi":"10.1103/physrevd.111.075018","DOIUrl":null,"url":null,"abstract":"The kinetic mixing (KM) portal, by which the Standard Model (SM) photon mixes with a light dark photon arising from a new U</a:mi>(</a:mo>1</a:mn>)</a:mo>D</a:mi></a:msub></a:math> gauge group, allows for the possibility of viable scenarios of sub-GeV thermal dark matter with appropriately suppressed couplings to the SM. This KM can only occur if particles having both SM and dark quantum numbers, here termed portal matter, also exist. The presence of such types of states and the strong suggestion of a need to embed <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><e:mi>U</e:mi><e:mo stretchy=\"false\">(</e:mo><e:mn>1</e:mn><e:msub><e:mo stretchy=\"false\">)</e:mo><e:mi>D</e:mi></e:msub></e:math> into a non-Abelian gauge structure not too far above the TeV scale based on the renormalization-group equation running of the <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:mi>U</i:mi><i:mo stretchy=\"false\">(</i:mo><i:mn>1</i:mn><i:msub><i:mo stretchy=\"false\">)</i:mo><i:mi>D</i:mi></i:msub></i:math> gauge coupling is potentially indicative of an enlarged group linking together the visible and dark sectors. The gauge group <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:mi>G</m:mi><m:mo>=</m:mo><m:mi>S</m:mi><m:mi>U</m:mi><m:mo stretchy=\"false\">(</m:mo><m:mn>3</m:mn><m:msub><m:mo stretchy=\"false\">)</m:mo><m:mi>c</m:mi></m:msub><m:mo>×</m:mo><m:mi>S</m:mi><m:mi>U</m:mi><m:mo stretchy=\"false\">(</m:mo><m:mn>3</m:mn><m:msub><m:mo stretchy=\"false\">)</m:mo><m:mi>L</m:mi></m:msub><m:mo>×</m:mo><m:mi>U</m:mi><m:mo stretchy=\"false\">(</m:mo><m:mn>1</m:mn><m:msub><m:mo stretchy=\"false\">)</m:mo><m:mi>A</m:mi></m:msub><m:mo>×</m:mo><m:mi>U</m:mi><m:mo stretchy=\"false\">(</m:mo><m:mn>1</m:mn><m:msub><m:mo stretchy=\"false\">)</m:mo><m:mi>B</m:mi></m:msub><m:mo>=</m:mo><m:msub><m:mn>3</m:mn><m:mi>c</m:mi></m:msub><m:msub><m:mn>3</m:mn><m:mi>L</m:mi></m:msub><m:msub><m:mn>1</m:mn><m:mi>A</m:mi></m:msub><m:msub><m:mn>1</m:mn><m:mi>B</m:mi></m:msub></m:math> is perhaps the simplest setup wherein the SM and dark interactions are partially unified in a non-Abelian fashion that is not a simple product group of the form <w:math xmlns:w=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><w:mi>G</w:mi><w:mo>=</w:mo><w:msub><w:mi>G</w:mi><w:mi>SM</w:mi></w:msub><w:mo>×</w:mo><w:msub><w:mi>G</w:mi><w:mi>D</w:mi></w:msub></w:math> encountered frequently in earlier work. The present paper describes the implications and phenomenology of this type of setup. <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":"40 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-04-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Toward UV models of kinetic mixing and portal matter. VII. A light dark photon in the 3c3L1A1B model\",\"authors\":\"Thomas G. Rizzo\",\"doi\":\"10.1103/physrevd.111.075018\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The kinetic mixing (KM) portal, by which the Standard Model (SM) photon mixes with a light dark photon arising from a new U</a:mi>(</a:mo>1</a:mn>)</a:mo>D</a:mi></a:msub></a:math> gauge group, allows for the possibility of viable scenarios of sub-GeV thermal dark matter with appropriately suppressed couplings to the SM. This KM can only occur if particles having both SM and dark quantum numbers, here termed portal matter, also exist. The presence of such types of states and the strong suggestion of a need to embed <e:math xmlns:e=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><e:mi>U</e:mi><e:mo stretchy=\\\"false\\\">(</e:mo><e:mn>1</e:mn><e:msub><e:mo stretchy=\\\"false\\\">)</e:mo><e:mi>D</e:mi></e:msub></e:math> into a non-Abelian gauge structure not too far above the TeV scale based on the renormalization-group equation running of the <i:math xmlns:i=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><i:mi>U</i:mi><i:mo stretchy=\\\"false\\\">(</i:mo><i:mn>1</i:mn><i:msub><i:mo stretchy=\\\"false\\\">)</i:mo><i:mi>D</i:mi></i:msub></i:math> gauge coupling is potentially indicative of an enlarged group linking together the visible and dark sectors. The gauge group <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><m:mi>G</m:mi><m:mo>=</m:mo><m:mi>S</m:mi><m:mi>U</m:mi><m:mo stretchy=\\\"false\\\">(</m:mo><m:mn>3</m:mn><m:msub><m:mo stretchy=\\\"false\\\">)</m:mo><m:mi>c</m:mi></m:msub><m:mo>×</m:mo><m:mi>S</m:mi><m:mi>U</m:mi><m:mo stretchy=\\\"false\\\">(</m:mo><m:mn>3</m:mn><m:msub><m:mo stretchy=\\\"false\\\">)</m:mo><m:mi>L</m:mi></m:msub><m:mo>×</m:mo><m:mi>U</m:mi><m:mo stretchy=\\\"false\\\">(</m:mo><m:mn>1</m:mn><m:msub><m:mo stretchy=\\\"false\\\">)</m:mo><m:mi>A</m:mi></m:msub><m:mo>×</m:mo><m:mi>U</m:mi><m:mo stretchy=\\\"false\\\">(</m:mo><m:mn>1</m:mn><m:msub><m:mo stretchy=\\\"false\\\">)</m:mo><m:mi>B</m:mi></m:msub><m:mo>=</m:mo><m:msub><m:mn>3</m:mn><m:mi>c</m:mi></m:msub><m:msub><m:mn>3</m:mn><m:mi>L</m:mi></m:msub><m:msub><m:mn>1</m:mn><m:mi>A</m:mi></m:msub><m:msub><m:mn>1</m:mn><m:mi>B</m:mi></m:msub></m:math> is perhaps the simplest setup wherein the SM and dark interactions are partially unified in a non-Abelian fashion that is not a simple product group of the form <w:math xmlns:w=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><w:mi>G</w:mi><w:mo>=</w:mo><w:msub><w:mi>G</w:mi><w:mi>SM</w:mi></w:msub><w:mo>×</w:mo><w:msub><w:mi>G</w:mi><w:mi>D</w:mi></w:msub></w:math> encountered frequently in earlier work. The present paper describes the implications and phenomenology of this type of setup. <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\":\"40 1\",\"pages\":\"\"},\"PeriodicalIF\":5.3000,\"publicationDate\":\"2025-04-14\",\"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.111.075018\",\"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.111.075018","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}
Toward UV models of kinetic mixing and portal matter. VII. A light dark photon in the 3c3L1A1B model
The kinetic mixing (KM) portal, by which the Standard Model (SM) photon mixes with a light dark photon arising from a new U(1)D gauge group, allows for the possibility of viable scenarios of sub-GeV thermal dark matter with appropriately suppressed couplings to the SM. This KM can only occur if particles having both SM and dark quantum numbers, here termed portal matter, also exist. The presence of such types of states and the strong suggestion of a need to embed U(1)D into a non-Abelian gauge structure not too far above the TeV scale based on the renormalization-group equation running of the U(1)D gauge coupling is potentially indicative of an enlarged group linking together the visible and dark sectors. The gauge group G=SU(3)c×SU(3)L×U(1)A×U(1)B=3c3L1A1B is perhaps the simplest setup wherein the SM and dark interactions are partially unified in a non-Abelian fashion that is not a simple product group of the form G=GSM×GD encountered frequently in earlier work. The present paper describes the implications and phenomenology of this type of setup. 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.