Renormalization scheme dependence of the two-loop QCD corrections to the neutral Higgs-boson masses in the MSSM

被引:42
作者
Borowka, S. [1 ]
Hahn, T. [2 ]
Heinemeyer, S. [3 ]
Heinrich, G. [2 ]
Hollik, W. [2 ]
机构
[1] Univ Zurich, Inst Phys, CH-8057 Zurich, Switzerland
[2] Max Planck Inst Phys & Astrophys, Werner Heisenberg Inst, D-80805 Munich, Germany
[3] CSIC UC, Inst Fis Cantabria, Santander, Spain
来源
EUROPEAN PHYSICAL JOURNAL C | 2015年 / 75卷 / 09期
关键词
SUPERSYMMETRIC STANDARD MODEL; HIGH-PRECISION PREDICTIONS; ON-SHELL RENORMALIZATION; RADIATIVE-CORRECTIONS; COMPLEX MSSM; PROGRAM; SECTOR; FEYNARTS; REGULARIZATION; IMPLEMENTATION;
D O I
10.1140/epjc/s10052-015-3648-6
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
Reaching a theoretical accuracy in the prediction of the lightest MSSM Higgs-boson mass, M-h, at the level of the current experimental precision requires the inclusion of momentum-dependent contributions at the two-loop level. Recently two groups presented the two-loop QCD momentum-dependent corrections to M-h (Borowka et al., Eur Phys J C 74(8): 2994, 2014; Degrassi et al., Eur Phys J C 75(2): 61, 2015), using a hybrid on-shell-(DR) over bar scheme, with apparently different results. We show that the differences can be traced back to a different renormalization of the top-quark mass, and that the claim in Ref. Degrassi et al. (Eur Phys J C 75(2): 61, 2015) of an inconsistency in Ref. Borowka et al. (Eur Phys J C 74(8): 2994, 2014) is incorrect. We furthermore compare consistently the results for M-h obtained with the top-quark mass renormalized on-shell and (DR) over bar. The latter calculation has been added to the FeynHiggs package and can be used to estimate missing higher-order corrections beyond the two-loop level.
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页数:16
相关论文
共 93 条
[1]   Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC [J].
Aad, G. ;
Abajyan, T. ;
Abbott, B. ;
Abdallah, J. ;
Khalek, S. Abdel ;
Abdelalim, A. A. ;
Abdinov, O. ;
Aben, R. ;
Abi, B. ;
Abolins, M. ;
AbouZeid, U. S. ;
Abramowicz, H. ;
Abreu, H. ;
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. ;
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. .
PHYSICS LETTERS B, 2012, 716 (01) :1-29
[2]  
Aad G., ARXIV150307589HEPEX
[3]  
Allanach BC, 2004, J HIGH ENERGY PHYS
[4]  
[Anonymous], ARXIV150302138HEPPH
[5]  
[Anonymous], ATLASCONF2015008
[6]  
[Anonymous], ARXIV14128662HEPEX C
[7]  
[Anonymous], ARXIV150206595HEPPH
[8]  
[Anonymous], EUR PHYS J C
[9]  
[Anonymous], ARXIV14120918HEPPH
[10]  
Asner D. M., ARXIV13100763HEPPH