Abstract:This article presents results for the last unknown two-loop contributions to the Z-boson partial widths and Z-peak cross-section. These are the so-called bosonic electroweak two-loop corrections, where "bosonic" refers to diagrams without closed fermion loops. Together with the corresponding results for the Z-pole asymmetries A l , A b , which have been presented earlier, this completes the theoretical description of Z-boson precision observables at full two-loop precision within the Standard Model. The calcul… Show more
“…In this study, we have presented some phenomenologically useful applications of the recently completed electroweak two-loop calculation of Z-boson vertex corrections [36,37]. The work collects multi-year efforts of several groups for predictions of the EWPOs related to the Z peak up to electroweak full two-loop accuracy, supplemented by leading QCD higher-order terms.…”
Section: Discussionmentioning
confidence: 99%
“…Results for the partial and total Z widths, branching ratios and σ 0 had including the full two-loop corrections have first been published in Ref. [37]. They can be expressed in simple parameterization formulae, which are adequate for most phenomenological applications.…”
Section: )mentioning
confidence: 99%
“…• Complete one-loop corrections [23], which have been re-computed for this work, and full two-loop [33,35,37] electroweak corrections;…”
Section: )mentioning
confidence: 99%
“…We reproduced by an independent calculation the contribution of the bosonic electroweak two-loop corrections using the methods of Ref. [37]. The corrections can be expressed in terms of a weak form factor ∆κ (α 2 ,bos) , where…”
Section: Asymmetries and Effective Weak Mixing Anglesmentioning
confidence: 99%
“…After several papers on approximate/partial higher-order corrections, the complete two-loop weak corrections were determined in a series of papers from 2004 to 2018 [27][28][29][30][31][32][33][34][35][36][37]. The correct formulation of the interplay of the 2→2 loop corrections with higher order real QED corrections in the S-matrix approach, also called un-folding of the effective 2→2 Born terms from the realistic 2→n observables, is a topic on its own.…”
We present Standard Model predictions for the complete set of phenomenologically relevant electroweak precision pseudo-observables related to the Zboson: the leptonic and bottom-quark effective weak mixing angles sin 2 θ eff , sin 2 θ b eff , the Z-boson partial decay widths Γ f , where f indicates any charged lepton, neutrino and quark flavor (except for the top quark), as well as the total Z decay width Γ Z , the branching ratios R , R c , R b , and the hadronic cross section σ 0 had . The input parameters are the masses M Z , M H and m t , and the couplings α s , α. The scheme dependence due to the choice of M W or its alternative G µ as a last input parameter is also discussed. Recent substantial technical progress in the calculation of Minkowskian massive higher-order Feynman integrals allows the calculation of the complete electroweak two-loop radiative corrections to all the observables mentioned. QCD contributions are included appropriately. Results are provided in terms of simple and convenient parameterization formulae whose coefficients have been determined from the full numerical multi-loop calculation. The size of the missing electroweak three-loop or QCD higher-order corrections is estimated. We briefly comment on the prospects for their calculation. Finally, direct predictions for the Zf f vector and axial-vector form-factors are given, including a discussion of separate order-by-order contributions.
“…In this study, we have presented some phenomenologically useful applications of the recently completed electroweak two-loop calculation of Z-boson vertex corrections [36,37]. The work collects multi-year efforts of several groups for predictions of the EWPOs related to the Z peak up to electroweak full two-loop accuracy, supplemented by leading QCD higher-order terms.…”
Section: Discussionmentioning
confidence: 99%
“…Results for the partial and total Z widths, branching ratios and σ 0 had including the full two-loop corrections have first been published in Ref. [37]. They can be expressed in simple parameterization formulae, which are adequate for most phenomenological applications.…”
Section: )mentioning
confidence: 99%
“…• Complete one-loop corrections [23], which have been re-computed for this work, and full two-loop [33,35,37] electroweak corrections;…”
Section: )mentioning
confidence: 99%
“…We reproduced by an independent calculation the contribution of the bosonic electroweak two-loop corrections using the methods of Ref. [37]. The corrections can be expressed in terms of a weak form factor ∆κ (α 2 ,bos) , where…”
Section: Asymmetries and Effective Weak Mixing Anglesmentioning
confidence: 99%
“…After several papers on approximate/partial higher-order corrections, the complete two-loop weak corrections were determined in a series of papers from 2004 to 2018 [27][28][29][30][31][32][33][34][35][36][37]. The correct formulation of the interplay of the 2→2 loop corrections with higher order real QED corrections in the S-matrix approach, also called un-folding of the effective 2→2 Born terms from the realistic 2→n observables, is a topic on its own.…”
We present Standard Model predictions for the complete set of phenomenologically relevant electroweak precision pseudo-observables related to the Zboson: the leptonic and bottom-quark effective weak mixing angles sin 2 θ eff , sin 2 θ b eff , the Z-boson partial decay widths Γ f , where f indicates any charged lepton, neutrino and quark flavor (except for the top quark), as well as the total Z decay width Γ Z , the branching ratios R , R c , R b , and the hadronic cross section σ 0 had . The input parameters are the masses M Z , M H and m t , and the couplings α s , α. The scheme dependence due to the choice of M W or its alternative G µ as a last input parameter is also discussed. Recent substantial technical progress in the calculation of Minkowskian massive higher-order Feynman integrals allows the calculation of the complete electroweak two-loop radiative corrections to all the observables mentioned. QCD contributions are included appropriately. Results are provided in terms of simple and convenient parameterization formulae whose coefficients have been determined from the full numerical multi-loop calculation. The size of the missing electroweak three-loop or QCD higher-order corrections is estimated. We briefly comment on the prospects for their calculation. Finally, direct predictions for the Zf f vector and axial-vector form-factors are given, including a discussion of separate order-by-order contributions.
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