W+W-H production through bottom quarks fusion at hadron colliders

被引:1
作者
Agrawal, Pankaj [1 ,2 ]
Das, Biswajit [1 ,2 ]
机构
[1] Inst Phys, Bhubaneswar 751005, India
[2] Homi Bhabha Natl Inst, Training Sch Complex, Mumbai 400094, Maharashtra, India
关键词
CROSS-SECTIONS; AMPLITUDES; ALGORITHM; SCHEME;
D O I
10.1016/j.physletb.2021.136461
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
With the standard model working well in describing the collider data, the focus is now on determining the standard model parameters as well as for any hint of deviation. In particular, the determination of the couplings of the Higgs boson with itself and with other particles of the model is important to better understand the electroweak symmetry breaking sector of the model. In this letter, we look at the process pp -> WWH, in particular through the fusion of bottom quarks. Due to the non-negligible coupling of the Higgs boson with the bottom quarks, there is a dependence on the WWHHcoupling in this process. This sub-process receives the largest contribution when the Wbosons are longitudinally polarized. We compute one-loop QCD corrections to various final states with polarized Wbosons. We find that the corrections to the final state with the longitudinally polarized Wbosons are large. It is shown that the measurement of the polarization of the Wbosons can be used as a tool to probe the WWHHcoupling in this process. We also examine the effect of varying WWHHcoupling in the.-framework. (C) 2021 The Author(s). Published by Elsevier B.V.
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页数:9
相关论文
共 40 条
[1]  
Aaboud M, 2019, EUR PHYS J C, V79, DOI 10.1140/epjc/s10052-019-7027-6
[2]   Measurement of the W boson polarization in top quark decays with the ATLAS detector [J].
Aad, G. ;
Abbott, B. ;
Abdallah, J. ;
Khalek, S. Abdel ;
Abdelalim, A. A. ;
Abdinov, O. ;
Abi, B. ;
Abolins, M. ;
AbouZeid, O. S. ;
Abramowicz, H. ;
Abreu, H. ;
Acerbi, E. ;
Acharya, B. S. ;
Adamczyk, L. ;
Adams, D. L. ;
Addy, T. N. ;
Adelman, J. ;
Adomeit, S. ;
Adragna, P. ;
Adye, T. ;
Aefsky, S. ;
Aguilar-Saavedra, J. A. ;
Agustoni, M. ;
Aharrouche, M. ;
Ahlen, S. P. ;
Ahles, F. ;
Ahmad, A. ;
Ahsan, M. ;
Aielli, G. ;
Akdogan, T. ;
Akesson, T. P. A. ;
Akimoto, G. ;
Akimov, A. V. ;
Akiyama, A. ;
Alam, M. S. ;
Alam, M. A. ;
Albert, J. ;
Albrand, S. ;
Aleksa, M. ;
Aleksandrov, I. N. ;
Alessandria, F. ;
Alexa, C. ;
Alexander, G. ;
Alexandre, G. ;
Alexopoulos, T. ;
Alhroob, M. ;
Aliev, M. ;
Alimonti, G. ;
Alison, J. ;
Allbrooke, B. M. M. .
JOURNAL OF HIGH ENERGY PHYSICS, 2012, (06)
[3]  
Aad G., 2021, J HIGH ENERGY PHYS, V2021
[4]   Production of two photons and a jet through gluon fusion [J].
Agrawal, P ;
Ladinsky, G .
PHYSICAL REVIEW D, 2001, 63 (11)
[5]   Determining the shape of the Higgs potential at future colliders [J].
Agrawal, Pankaj ;
Saha, Debashis ;
Xu, Ling-Xiao ;
Yu, Jiang-Hao ;
Yuan, C-P .
PHYSICAL REVIEW D, 2020, 101 (07)
[6]   Divector boson plus jet production via gluon fusion at hadron colliders [J].
Agrawal, Pankaj ;
Shivaji, Ambresh .
PHYSICAL REVIEW D, 2012, 86 (07)
[7]   The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations [J].
Alwall, J. ;
Frederix, R. ;
Frixione, S. ;
Hirschi, V. ;
Maltoni, F. ;
Mattelaer, O. ;
Shao, H. -S. ;
Stelzer, T. ;
Torrielli, P. ;
Zaro, M. .
JOURNAL OF HIGH ENERGY PHYSICS, 2014, (07)
[8]  
[Anonymous], ARXIV190713168
[9]   Gluon fusion and b(b)over-bar corrections to HW+W-/HZZ production in the POWHEG-BOX [J].
Baglio, Julien .
PHYSICS LETTERS B, 2017, 764 :54-59
[10]   Next-to-leading order QCD corrections to associated production of a SM Higgs boson with a pair of weak bosons in the POWHEG-BOX [J].
Baglio, Julien .
PHYSICAL REVIEW D, 2016, 93 (05)