{"title":"4 τ衰变通道中NMSSM次轻标量希格斯态的LHC信号","authors":"M. Almarashi","doi":"10.1155/2021/5569862","DOIUrl":null,"url":null,"abstract":"<jats:p>We study the <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M2\">\n <msub>\n <mrow>\n <mi>a</mi>\n </mrow>\n <mrow>\n <mn>1</mn>\n </mrow>\n </msub>\n <msub>\n <mrow>\n <mi>a</mi>\n </mrow>\n <mrow>\n <mn>1</mn>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> and <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M3\">\n <mi>Z</mi>\n <msub>\n <mrow>\n <mi>a</mi>\n </mrow>\n <mrow>\n <mn>1</mn>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> decay channels of the next-to-lightest CP-even Higgs boson <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M4\">\n <msub>\n <mrow>\n <mi>h</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> of the NMSSM at the LHC, where the <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M5\">\n <msub>\n <mrow>\n <mi>h</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> is produced in gluon fusion. It is found that while the <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M6\">\n <msub>\n <mrow>\n <mi>h</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> discovery is impossible through the latter channel, the former one in the <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M7\">\n <mn>4</mn>\n <mi>τ</mi>\n </math>\n </jats:inline-formula> final state is a promising channel to discover the <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M8\">\n <msub>\n <mrow>\n <mi>h</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> with masses up to around 250 GeV at the LHC. Such a discovery of the <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M9\">\n <msub>\n <mrow>\n <mi>h</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> is mostly accompanied with a light <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M10\">\n <msub>\n <mrow>\n <mi>a</mi>\n </mrow>\n <mrow>\n <mn>1</mn>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula>, which is a clear evidence for distinguishing the NMSSM from the MSSM since such a light <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M11\">\n <msub>\n <mrow>\n <mi>a</mi>\n </mrow>\n <mrow>\n <mn>1</mn>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> is impossible in the MSSM.</jats:p>","PeriodicalId":7498,"journal":{"name":"Advances in High Energy Physics","volume":" ","pages":""},"PeriodicalIF":1.5000,"publicationDate":"2021-03-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":"{\"title\":\"LHC Signals of the Next-to-Lightest Scalar Higgs State of the NMSSM in the \\n 4\\n τ\\n Decay Channel\",\"authors\":\"M. Almarashi\",\"doi\":\"10.1155/2021/5569862\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<jats:p>We study the <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M2\\\">\\n <msub>\\n <mrow>\\n <mi>a</mi>\\n </mrow>\\n <mrow>\\n <mn>1</mn>\\n </mrow>\\n </msub>\\n <msub>\\n <mrow>\\n <mi>a</mi>\\n </mrow>\\n <mrow>\\n <mn>1</mn>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> and <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M3\\\">\\n <mi>Z</mi>\\n <msub>\\n <mrow>\\n <mi>a</mi>\\n </mrow>\\n <mrow>\\n <mn>1</mn>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> decay channels of the next-to-lightest CP-even Higgs boson <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M4\\\">\\n <msub>\\n <mrow>\\n <mi>h</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> of the NMSSM at the LHC, where the <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M5\\\">\\n <msub>\\n <mrow>\\n <mi>h</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> is produced in gluon fusion. It is found that while the <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M6\\\">\\n <msub>\\n <mrow>\\n <mi>h</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> discovery is impossible through the latter channel, the former one in the <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M7\\\">\\n <mn>4</mn>\\n <mi>τ</mi>\\n </math>\\n </jats:inline-formula> final state is a promising channel to discover the <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M8\\\">\\n <msub>\\n <mrow>\\n <mi>h</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> with masses up to around 250 GeV at the LHC. Such a discovery of the <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M9\\\">\\n <msub>\\n <mrow>\\n <mi>h</mi>\\n </mrow>\\n <mrow>\\n <mn>2</mn>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> is mostly accompanied with a light <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M10\\\">\\n <msub>\\n <mrow>\\n <mi>a</mi>\\n </mrow>\\n <mrow>\\n <mn>1</mn>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula>, which is a clear evidence for distinguishing the NMSSM from the MSSM since such a light <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M11\\\">\\n <msub>\\n <mrow>\\n <mi>a</mi>\\n </mrow>\\n <mrow>\\n <mn>1</mn>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> is impossible in the MSSM.</jats:p>\",\"PeriodicalId\":7498,\"journal\":{\"name\":\"Advances in High Energy Physics\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":1.5000,\"publicationDate\":\"2021-03-31\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"3\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advances in High Energy Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1155/2021/5569862\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, PARTICLES & FIELDS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advances in High Energy Physics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1155/2021/5569862","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, PARTICLES & FIELDS","Score":null,"Total":0}
引用次数: 3
摘要
我们研究a 1 a1和Z a 1LHC的NMSSM的次轻CP甚至希格斯玻色子h2的衰变通道,其中h2是在胶子融合中产生的。研究发现,尽管通过后一个信道不可能发现h2,前一个处于4τ终态的通道是发现h2的一个很有前途的通道质量高达250左右 LHC的GeV。H2的这种发现大多伴随着一种曙光a 1,这是区分NMSSM和MSSM的明确证据,因为在MSSM中这种光a1是不可能的。
LHC Signals of the Next-to-Lightest Scalar Higgs State of the NMSSM in the
4
τ
Decay Channel
We study the and decay channels of the next-to-lightest CP-even Higgs boson of the NMSSM at the LHC, where the is produced in gluon fusion. It is found that while the discovery is impossible through the latter channel, the former one in the final state is a promising channel to discover the with masses up to around 250 GeV at the LHC. Such a discovery of the is mostly accompanied with a light , which is a clear evidence for distinguishing the NMSSM from the MSSM since such a light is impossible in the MSSM.
期刊介绍:
Advances in High Energy Physics publishes the results of theoretical and experimental research on the nature of, and interaction between, energy and matter. Considering both original research and focussed review articles, the journal welcomes submissions from small research groups and large consortia alike.