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Enhanced Higgs pair production from higgsino decay at the HL-LHC
The scenario of multi-sector SUSY breaking predicts pseudo-goldstinos which are not absorbed by the gravitino and their mass can be as low as <math altimg="si1.svg"><mi mathvariant="script">O</mi><mo stretchy="false">(</mo><mn>0.1<...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2022
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/j.nuclphysb.2022.115912 http://cds.cern.ch/record/2802166 |
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author | Dai, Jianpeng Liu, Tao Wang, Daohan Yang, Jin Min |
author_facet | Dai, Jianpeng Liu, Tao Wang, Daohan Yang, Jin Min |
author_sort | Dai, Jianpeng |
collection | CERN |
description | The scenario of multi-sector SUSY breaking predicts pseudo-goldstinos which are not absorbed by the gravitino and their mass can be as low as <math altimg="si1.svg"><mi mathvariant="script">O</mi><mo stretchy="false">(</mo><mn>0.1</mn><mo stretchy="false">)</mo></math> GeV. Since the interactions of pseudo-goldstinos are not so weak as gravitino, a produced higgsino can decay to a pseudo-goldstino plus a Higgs boson insider the detector at the LHC, and thus the higgsino pair production can lead to the signal of Higgs pair plus missing energy. For the scenario of natural SUSY which requires rather light higgsinos, such events may sizably outnumber the Higgs pair events predicted by the SM and be accessible at the HL-LHC (14 TeV with a luminosity of 3 <math altimg="si168.svg"><msup><mrow><mi mathvariant="normal">ab</mi></mrow><mrow><mo linebreak="badbreak" linebreakstyle="after">−</mo><mn>1</mn></mrow></msup></math>). In this work we examine the observability of such Higgs pair plus missing energy from the decay of light higgsinos produced at the HL-LHC. Considering three channels of the Higgs-pair decay (<math altimg="si3.svg"><mi>b</mi><mi>b</mi><mi>W</mi><msup><mrow><mi>W</mi></mrow><mrow><mo>⁎</mo></mrow></msup></math>, <math altimg="si4.svg"><mi>b</mi><mi>b</mi><mi>γ</mi><mi>γ</mi></math>, <math altimg="si5.svg"><mi>b</mi><mi>b</mi><mi>b</mi><mi>b</mi></math>), our detailed Monte Carlo simulations for the signal and backgrounds show that the best channel is <math altimg="si6.svg"><mi>b</mi><mi>b</mi><mi>b</mi><mi>b</mi><mo linebreak="goodbreak" linebreakstyle="after">+</mo><mspace width="0.25em"/><mo stretchy="false">/</mo><msub><mrow><mi>E</mi></mrow><mrow><mi>T</mi></mrow></msub></math>, whose statistical significance can reach 2σ level for a light higgsino allowed by current experiments. This is over the SM Higgs pair result which is about 1.8σ. |
id | cern-2802166 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2022 |
record_format | invenio |
spelling | cern-28021662023-10-25T02:35:36Zdoi:10.1016/j.nuclphysb.2022.115912http://cds.cern.ch/record/2802166engDai, JianpengLiu, TaoWang, DaohanYang, Jin MinEnhanced Higgs pair production from higgsino decay at the HL-LHCParticle Physics - ExperimentParticle Physics - PhenomenologyThe scenario of multi-sector SUSY breaking predicts pseudo-goldstinos which are not absorbed by the gravitino and their mass can be as low as <math altimg="si1.svg"><mi mathvariant="script">O</mi><mo stretchy="false">(</mo><mn>0.1</mn><mo stretchy="false">)</mo></math> GeV. Since the interactions of pseudo-goldstinos are not so weak as gravitino, a produced higgsino can decay to a pseudo-goldstino plus a Higgs boson insider the detector at the LHC, and thus the higgsino pair production can lead to the signal of Higgs pair plus missing energy. For the scenario of natural SUSY which requires rather light higgsinos, such events may sizably outnumber the Higgs pair events predicted by the SM and be accessible at the HL-LHC (14 TeV with a luminosity of 3 <math altimg="si168.svg"><msup><mrow><mi mathvariant="normal">ab</mi></mrow><mrow><mo linebreak="badbreak" linebreakstyle="after">−</mo><mn>1</mn></mrow></msup></math>). In this work we examine the observability of such Higgs pair plus missing energy from the decay of light higgsinos produced at the HL-LHC. Considering three channels of the Higgs-pair decay (<math altimg="si3.svg"><mi>b</mi><mi>b</mi><mi>W</mi><msup><mrow><mi>W</mi></mrow><mrow><mo>⁎</mo></mrow></msup></math>, <math altimg="si4.svg"><mi>b</mi><mi>b</mi><mi>γ</mi><mi>γ</mi></math>, <math altimg="si5.svg"><mi>b</mi><mi>b</mi><mi>b</mi><mi>b</mi></math>), our detailed Monte Carlo simulations for the signal and backgrounds show that the best channel is <math altimg="si6.svg"><mi>b</mi><mi>b</mi><mi>b</mi><mi>b</mi><mo linebreak="goodbreak" linebreakstyle="after">+</mo><mspace width="0.25em"/><mo stretchy="false">/</mo><msub><mrow><mi>E</mi></mrow><mrow><mi>T</mi></mrow></msub></math>, whose statistical significance can reach 2σ level for a light higgsino allowed by current experiments. This is over the SM Higgs pair result which is about 1.8σ.The scenario of multi-sector SUSY breaking predicts pseudo-goldstinos which are not absorbed by the gravitino and their mass can be as low as O(0.1) GeV. Since the interactions of pseudo-goldstinos are not so weak as gravitino, a produced higgsino can decay to a pseudo-goldstino plus a Higgs boson insider the detector at the LHC, and thus the higgsino pair production can lead to the signal of Higgs pair plus missing energy. For the scenario of natural SUSY which requires rather light higgsinos, such events may sizably outnumber the Higgs pair events predicted by the SM and be accessible at the HL-LHC (14 TeV with a luminosity of 3 ab−1). In this work we examine the observability of such Higgs pair plus missing energy from the decay of light higgsinos produced at the HL-LHC. Considering three channels of the Higgs-pair decay (bbWW⁎, bbγγ, bbbb), our detailed Monte Carlo simulations for the signal and backgrounds show that the best channel is bbbb+/ET, whose statistical significance can reach 2σ level for a light higgsino allowed by current experiments. This is over the SM Higgs pair result which is about 1.8σ.The scenario of multi-sector SUSY breaking predicts pseudo-goldstinos which are not absorbed by the gravitino and their mass can be as low as ${{\cal O} (0.1)}$ GeV. Since the interactions of pseudo-goldstinos are not so weak as gravitino, a produced higgsino can decay to a pseudo-goldstino plus a Higgs boson insider the detector at the LHC, and thus the higgsino pair production can lead to the signal of Higgs pair plus missing energy. For the scenario of natural SUSY which requires rather light higgsinos, such events may sizably outnumber the Higgs pair events predicted by the SM and be accessible at the HL-LHC (14 TeV with a luminosity of 3~$\rm{ab}^{-1}$). In this work we examine the observability of such Higgs pair plus missing energy from the decay of light higgsinos produced at the HL-LHC. Considering three channels of the Higgs-pair decay ($bbWW^*$, $bb\gamma\gamma$, $bbbb$), our detailed Monte Carlo simulations for the signal and backgrounds show that the best channel is $bbbb+\textrm{E\!\!\!\! \!\slash}_T$, whose statistical significance can reach $2\sigma$ level for a light higgsino allowed by current experiments. This is over the SM Higgs pair result which is about $1.8\sigma$.arXiv:2202.03258oai:cds.cern.ch:28021662022-02-07 |
spellingShingle | Particle Physics - Experiment Particle Physics - Phenomenology Dai, Jianpeng Liu, Tao Wang, Daohan Yang, Jin Min Enhanced Higgs pair production from higgsino decay at the HL-LHC |
title | Enhanced Higgs pair production from higgsino decay at the HL-LHC |
title_full | Enhanced Higgs pair production from higgsino decay at the HL-LHC |
title_fullStr | Enhanced Higgs pair production from higgsino decay at the HL-LHC |
title_full_unstemmed | Enhanced Higgs pair production from higgsino decay at the HL-LHC |
title_short | Enhanced Higgs pair production from higgsino decay at the HL-LHC |
title_sort | enhanced higgs pair production from higgsino decay at the hl-lhc |
topic | Particle Physics - Experiment Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/j.nuclphysb.2022.115912 http://cds.cern.ch/record/2802166 |
work_keys_str_mv | AT daijianpeng enhancedhiggspairproductionfromhiggsinodecayatthehllhc AT liutao enhancedhiggspairproductionfromhiggsinodecayatthehllhc AT wangdaohan enhancedhiggspairproductionfromhiggsinodecayatthehllhc AT yangjinmin enhancedhiggspairproductionfromhiggsinodecayatthehllhc |