Journal of Hebei University(Natural Science Edition) >

2021 , Vol. 41 >Issue 1: 7 - 14

DOI: https://doi.org/10.3969/j.issn.1000-1565.2021.01.002

Higgs mass corrections in the B-LSSM

  • LI Wei ,
  • WANG Yinglong
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  • 1.Key Laboratory of High-Precision Computation and Application of Quantum Field Theory of Hebei Province, College of Physics Science and Technology, Hebei University, Baoding 071002, China; 2.Department of Primary Education, Baoding Preschool Teachers College, Baoding 072750, China

Received date: 2020-07-23

  Online published: 2021-02-05

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Abstract

In the extension of the minimum supersymmetry model with local B-L gauge symmetry(B-LSSM), the Higgs particle mass is corrected by a single circle radiation by the effective potential method, and numerical analysis is carried out. According to the Higgs particle theoretical quality and experimental data further restricting the relevant parameters of B-LSSM and constraining the parameter space, thereby making the parameter space of B-LSSM more complete.

Key words： B-LSSM; Higgs; the effective potential; one-loop radiation

Cite this article

LI Wei , WANG Yinglong . Higgs mass corrections in the B-LSSM[J]. Journal of Hebei University(Natural Science Edition), 2021 , 41(1) : 7 -14 . DOI: 10.3969/j.issn.1000-1565.2021.01.002

References

[1] GEORGES A, BRAD A, JALAL A, et al. Search for the standard model Higgs boson in the H→WW(*)→lνlν decay mode with 4.7/fb of ATLAS data at S1/2=7 TeV [J].Physics Letters B,2012,716:62-81.DOI: 10.1016/j.physletb.2012.08.010.
[2] CHATRCHYAN S, KHACHATRYAM V, TUMASYAM. A, et al. Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC[J].Physics Letters B,2012,716:30-61. DOI: 10.1016/j.physletb.2012.08.021.
[3] GEORGES A, BRAD A, JALAL A, et al. Combined measurement of the Higgs boson mass in pp collisions at S1/2=7and 8 TeV with the ATLAS and CMS experiments[J].Physical Review Letters,2015,114:1-33.DOI:10.1103/PhyRevLett.114.191803.
[4] YANG J L, FENG T F. Lepton-flavor violation and two loop electroweak corrections to(g-2)μ in the B-L symmetric SSM[J].Physical Review D,2019,99:015002-1-18. DOI: 10.1103/PhysRevD.99.015002.
[5] ROSIEK J. Complete set of Feynman rules for the MSSM: Erratum[J].Physical Review D,1990, 41:3464-3501.DOI:10.1103/PhysRevD.41.3464.
[6] BASSO L, STAUB F. Enhancing h→γγ with staus in SUSY models with extended gauge sector[J].Physical Review D,2013,87:015011-1-15.DOI: 10.1103/Phys.Rev.D.87.015011.
[7] AMBROSO M,OVRUTB A. The mass spectra, hierarchy and cosmology of B-L MSSM heterotic compactifications [J].International Journal of Modern Physics A,2010,26:1569-1627.DOI: 10.1142/S0217751X11052943.
[8] PEREZ P F, SPINNER S. The fate of R-parity[J].Physical Review D,2011,83:035004-1-12.DOI: 10.1103/PhysRevD.83.035004.
[9] BARGERV, FILEVIEZ P, SPINNER S. Minimal gauged U(1)(B-L) model with spontaneous R-parity violation[J].Physical Review Letters, 2009,102:181802-1-8.DOI: 10.1103/PhysRevLett.102.181802.
[10] ELSAYED A, KHALIL S,MORETTI S. Higgs mass corrections in the SUSY B-L model with inverse seesaw[J].Physics Letters B,2012,715:208-216.DOI: 10.1016/j.physletb.2012.07.066.
[11] KHALIL S, OKADA H. Dark matter in B-L extended MSSM models[J]. Journal of High Energy Physics, 2009,79:083510-1-9.DOI: 10.1007/JHEP09(2012)054.
[12] AULAKHC S, MELFO A. Seesaw and supersymmetry or exact R-parity[J].PhysicsLettersB, 1999,459:557-562.DOI: 10.1016/S0370-2693(99)00708-X.
[13] DELLE R L, KHALIL S. Naturalness and dark matter in the supersymmetric B-L extension of the standard model[J].Physical Review D, 2017,96:055004-1-16.DOI: 10.1103/PhysRevD.96.055004.
[14] ZHANG H B, FENG T F. Higgs boson mass corrections in the μνSSM with effective potential methods[J].Physical Review D,2017,95:075013-1-12.DOI: 10.1103/PhysRevD.95.075013.
[15] BABUK S, KOLDAC F, MARCH-RUSSELL J. Implications of generalized Z-Z-prime mixing[J].Physical Review D,1998,57:97-114.DOI.10.1103/PhysRevD.57.6788.
[16] HIRSCH M, KLAPDOR-KLEINGROTHAUS H V, KOVALENKO S G. B-L violating masses in softly broken supersymmetry [J]. Physics Letters B,1997,398:311-314.DOI: 10.1016/S0370-2693(97)00234-7.
[17] CAMARGO-MOLINA J E, OLEARY B, POROD W. The stability of R-parity in supersymmetric models extended by U(1)(B-L)[J].Physical Review D,2013,88:015033-1-33.DOI: 10.1103/PhysRevD.88.015033.
[18] DEGASSI G, STEFANO D V. Higgs mass and vacuum stability in the standard model at NNLO[J].Journal of High Energy Physics,2012,12:9-18.DOI: 10.1007/JHEP08(2012)098.
[19] PATRIGNANI C. Review of particle physics [J].Chinese Physics C,2016,40:100001-1-18.DOI: 10.1088/1674-1137/40/10/100001.
[20] GEORGES A, TATEVIK A, BRAD A, et al. Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using 4.7 fb-1 1of S1/2=7 TeV proton-proton collision data[J].Physical Review D,2013,87:012008-1-18.DOI: 10.1103/PhysRevD.87.012008.
[21] CHATR CHYAN S, KHACHATRYAM V, TLIMASYAM A, et al.Search for supersymmetry in hadronic final states using MT2 in pp collisions at S1/2=7 TeV [J].Journal of High Energy Physics,2012,18:89-98.DOI: 10.1007/JHEP10(2012)018.
[22] OZADL O. Mass spectrum and Higgs profile in BLSSM[J].Physical Review D,2016,93:055024-1-14.DOI: 10.1103/PhysRevD.93.055024. (
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