{"title":"强子对撞机上的 tt¯H 相互作用和 T-odd 相关性","authors":"Apurba Tiwari, Sudhir Kumar Gupta","doi":"10.1088/1361-6471/ad2276","DOIUrl":null,"url":null,"abstract":"We explore <inline-formula>\n<tex-math>\n<?CDATA ${ \\mathcal C }P$?>\n</tex-math>\n<mml:math overflow=\"scroll\"><mml:mi mathvariant=\"script\">C</mml:mi><mml:mi>P</mml:mi></mml:math>\n<inline-graphic xlink:href=\"jpgad2276ieqn3.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>-violation effects of Higgs-top interactions in the associated production of a Higgs boson with top-pair in the dileptonic decay modes of top-quark originating from proton proton collisions <inline-formula>\n<tex-math>\n<?CDATA ${pp}\\to t\\bar{t}H\\to ({l}^{+}{\\nu }_{l}b)({l}^{-}\\bar{{\\nu }_{l}}\\bar{b})H$?>\n</tex-math>\n<mml:math overflow=\"scroll\"><mml:mi mathvariant=\"italic\">pp</mml:mi><mml:mo>→</mml:mo><mml:mi>t</mml:mi><mml:mover accent=\"true\"><mml:mi>t</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mi>H</mml:mi><mml:mo>→</mml:mo><mml:mo stretchy=\"false\">(</mml:mo><mml:msup><mml:mi>l</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msub><mml:mi>ν</mml:mi><mml:mi>l</mml:mi></mml:msub><mml:mi>b</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mo stretchy=\"false\">(</mml:mo><mml:msup><mml:mi>l</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mover accent=\"true\"><mml:msub><mml:mi>ν</mml:mi><mml:mi>l</mml:mi></mml:msub><mml:mo>¯</mml:mo></mml:mover><mml:mover accent=\"true\"><mml:mi>b</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mo stretchy=\"false\">)</mml:mo><mml:mi>H</mml:mi></mml:math>\n<inline-graphic xlink:href=\"jpgad2276ieqn4.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> at NLO in QCD matched to parton shower via T-odd observables using momenta of various particles involved in the process. In particular, we predict the constraints on the <inline-formula>\n<tex-math>\n<?CDATA ${ \\mathcal C }P$?>\n</tex-math>\n<mml:math overflow=\"scroll\"><mml:mi mathvariant=\"script\">C</mml:mi><mml:mi>P</mml:mi></mml:math>\n<inline-graphic xlink:href=\"jpgad2276ieqn5.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>-violating <inline-formula>\n<tex-math>\n<?CDATA $t\\bar{t}H$?>\n</tex-math>\n<mml:math overflow=\"scroll\"><mml:mi>t</mml:mi><mml:mover accent=\"true\"><mml:mi>t</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mi>H</mml:mi></mml:math>\n<inline-graphic xlink:href=\"jpgad2276ieqn6.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> coupling obtained through the production asymmetries associated with the T-odd observables in the dileptonic decay channel of the <inline-formula>\n<tex-math>\n<?CDATA $t\\bar{t}$?>\n</tex-math>\n<mml:math overflow=\"scroll\"><mml:mi>t</mml:mi><mml:mover accent=\"true\"><mml:mi>t</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math>\n<inline-graphic xlink:href=\"jpgad2276ieqn7.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> pair for the Large hadron collider (LHC) with centre-of-mass energy of 13 TeV and an integrated luminosity of 139 fb<sup>−1</sup>. We also present the corresponding limits for future hadron colliders, namely the High Luminosity LHC (HL-LHC) and the Future Circular Collider (FCC-hh). Our estimates of the <inline-formula>\n<tex-math>\n<?CDATA $t\\bar{t}H$?>\n</tex-math>\n<mml:math overflow=\"scroll\"><mml:mi>t</mml:mi><mml:mover accent=\"true\"><mml:mrow><mml:mi>t</mml:mi></mml:mrow><mml:mrow><mml:mo>¯</mml:mo></mml:mrow></mml:mover><mml:mi>H</mml:mi></mml:math>\n<inline-graphic xlink:href=\"jpgad2276ieqn8.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> interaction strength reveal that the upper bound on pseudoscalar coupling <italic toggle=\"yes\">c</italic>\n<sub>\n<italic toggle=\"yes\">p</italic>\n</sub> corresponding to the largest asymmetry would be of about 1.57 × 10<sup>−2</sup> at 2<italic toggle=\"yes\">σ</italic> C.L. for <italic toggle=\"yes\">c</italic>\n<sub>\n<italic toggle=\"yes\">s</italic>\n</sub> = 1 at the LHC with <inline-formula>\n<tex-math>\n<?CDATA $\\sqrt{S}$?>\n</tex-math>\n<mml:math overflow=\"scroll\"><mml:msqrt><mml:mi>S</mml:mi></mml:msqrt></mml:math>\n<inline-graphic xlink:href=\"jpgad2276ieqn9.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>=13 TeV for an integrated luminosity of 139 fb<sup>−1</sup>. The respective limits for HL-LHC and FCC-hh with the projected Luminosities of 3 ab<sup>−1</sup> and 30 ab<sup>−1</sup> are found to be to 2.7 × 10<sup>−3</sup> and 1.3 × 10<sup>−4</sup> respectively at 2<italic toggle=\"yes\">σ</italic> C.L.","PeriodicalId":16766,"journal":{"name":"Journal of Physics G: Nuclear and Particle Physics","volume":"22 1","pages":""},"PeriodicalIF":3.4000,"publicationDate":"2024-02-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"tt¯H Interactions and T-odd Correlations at Hadron Colliders\",\"authors\":\"Apurba Tiwari, Sudhir Kumar Gupta\",\"doi\":\"10.1088/1361-6471/ad2276\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We explore <inline-formula>\\n<tex-math>\\n<?CDATA ${ \\\\mathcal C }P$?>\\n</tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:mi mathvariant=\\\"script\\\">C</mml:mi><mml:mi>P</mml:mi></mml:math>\\n<inline-graphic xlink:href=\\\"jpgad2276ieqn3.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula>-violation effects of Higgs-top interactions in the associated production of a Higgs boson with top-pair in the dileptonic decay modes of top-quark originating from proton proton collisions <inline-formula>\\n<tex-math>\\n<?CDATA ${pp}\\\\to t\\\\bar{t}H\\\\to ({l}^{+}{\\\\nu }_{l}b)({l}^{-}\\\\bar{{\\\\nu }_{l}}\\\\bar{b})H$?>\\n</tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:mi mathvariant=\\\"italic\\\">pp</mml:mi><mml:mo>→</mml:mo><mml:mi>t</mml:mi><mml:mover accent=\\\"true\\\"><mml:mi>t</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mi>H</mml:mi><mml:mo>→</mml:mo><mml:mo stretchy=\\\"false\\\">(</mml:mo><mml:msup><mml:mi>l</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msub><mml:mi>ν</mml:mi><mml:mi>l</mml:mi></mml:msub><mml:mi>b</mml:mi><mml:mo stretchy=\\\"false\\\">)</mml:mo><mml:mo stretchy=\\\"false\\\">(</mml:mo><mml:msup><mml:mi>l</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mover accent=\\\"true\\\"><mml:msub><mml:mi>ν</mml:mi><mml:mi>l</mml:mi></mml:msub><mml:mo>¯</mml:mo></mml:mover><mml:mover accent=\\\"true\\\"><mml:mi>b</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mo stretchy=\\\"false\\\">)</mml:mo><mml:mi>H</mml:mi></mml:math>\\n<inline-graphic xlink:href=\\\"jpgad2276ieqn4.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> at NLO in QCD matched to parton shower via T-odd observables using momenta of various particles involved in the process. In particular, we predict the constraints on the <inline-formula>\\n<tex-math>\\n<?CDATA ${ \\\\mathcal C }P$?>\\n</tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:mi mathvariant=\\\"script\\\">C</mml:mi><mml:mi>P</mml:mi></mml:math>\\n<inline-graphic xlink:href=\\\"jpgad2276ieqn5.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula>-violating <inline-formula>\\n<tex-math>\\n<?CDATA $t\\\\bar{t}H$?>\\n</tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:mi>t</mml:mi><mml:mover accent=\\\"true\\\"><mml:mi>t</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mi>H</mml:mi></mml:math>\\n<inline-graphic xlink:href=\\\"jpgad2276ieqn6.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> coupling obtained through the production asymmetries associated with the T-odd observables in the dileptonic decay channel of the <inline-formula>\\n<tex-math>\\n<?CDATA $t\\\\bar{t}$?>\\n</tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:mi>t</mml:mi><mml:mover accent=\\\"true\\\"><mml:mi>t</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math>\\n<inline-graphic xlink:href=\\\"jpgad2276ieqn7.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> pair for the Large hadron collider (LHC) with centre-of-mass energy of 13 TeV and an integrated luminosity of 139 fb<sup>−1</sup>. We also present the corresponding limits for future hadron colliders, namely the High Luminosity LHC (HL-LHC) and the Future Circular Collider (FCC-hh). Our estimates of the <inline-formula>\\n<tex-math>\\n<?CDATA $t\\\\bar{t}H$?>\\n</tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:mi>t</mml:mi><mml:mover accent=\\\"true\\\"><mml:mrow><mml:mi>t</mml:mi></mml:mrow><mml:mrow><mml:mo>¯</mml:mo></mml:mrow></mml:mover><mml:mi>H</mml:mi></mml:math>\\n<inline-graphic xlink:href=\\\"jpgad2276ieqn8.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> interaction strength reveal that the upper bound on pseudoscalar coupling <italic toggle=\\\"yes\\\">c</italic>\\n<sub>\\n<italic toggle=\\\"yes\\\">p</italic>\\n</sub> corresponding to the largest asymmetry would be of about 1.57 × 10<sup>−2</sup> at 2<italic toggle=\\\"yes\\\">σ</italic> C.L. for <italic toggle=\\\"yes\\\">c</italic>\\n<sub>\\n<italic toggle=\\\"yes\\\">s</italic>\\n</sub> = 1 at the LHC with <inline-formula>\\n<tex-math>\\n<?CDATA $\\\\sqrt{S}$?>\\n</tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:msqrt><mml:mi>S</mml:mi></mml:msqrt></mml:math>\\n<inline-graphic xlink:href=\\\"jpgad2276ieqn9.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula>=13 TeV for an integrated luminosity of 139 fb<sup>−1</sup>. The respective limits for HL-LHC and FCC-hh with the projected Luminosities of 3 ab<sup>−1</sup> and 30 ab<sup>−1</sup> are found to be to 2.7 × 10<sup>−3</sup> and 1.3 × 10<sup>−4</sup> respectively at 2<italic toggle=\\\"yes\\\">σ</italic> C.L.\",\"PeriodicalId\":16766,\"journal\":{\"name\":\"Journal of Physics G: Nuclear and Particle Physics\",\"volume\":\"22 1\",\"pages\":\"\"},\"PeriodicalIF\":3.4000,\"publicationDate\":\"2024-02-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Physics G: Nuclear and Particle Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1088/1361-6471/ad2276\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics G: Nuclear and Particle Physics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1088/1361-6471/ad2276","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
tt¯H Interactions and T-odd Correlations at Hadron Colliders
We explore CP-violation effects of Higgs-top interactions in the associated production of a Higgs boson with top-pair in the dileptonic decay modes of top-quark originating from proton proton collisions pp→tt¯H→(l+νlb)(l−νl¯b¯)H at NLO in QCD matched to parton shower via T-odd observables using momenta of various particles involved in the process. In particular, we predict the constraints on the CP-violating tt¯H coupling obtained through the production asymmetries associated with the T-odd observables in the dileptonic decay channel of the tt¯ pair for the Large hadron collider (LHC) with centre-of-mass energy of 13 TeV and an integrated luminosity of 139 fb−1. We also present the corresponding limits for future hadron colliders, namely the High Luminosity LHC (HL-LHC) and the Future Circular Collider (FCC-hh). Our estimates of the tt¯H interaction strength reveal that the upper bound on pseudoscalar coupling cp corresponding to the largest asymmetry would be of about 1.57 × 10−2 at 2σ C.L. for cs = 1 at the LHC with S=13 TeV for an integrated luminosity of 139 fb−1. The respective limits for HL-LHC and FCC-hh with the projected Luminosities of 3 ab−1 and 30 ab−1 are found to be to 2.7 × 10−3 and 1.3 × 10−4 respectively at 2σ C.L.
期刊介绍:
Journal of Physics G: Nuclear and Particle Physics (JPhysG) publishes articles on theoretical and experimental topics in all areas of nuclear and particle physics, including nuclear and particle astrophysics. The journal welcomes submissions from any interface area between these fields.
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