Abstract

In the present paper, we make a detailed analysis for the QCD corrections to the electroweak ρρ parameter by applying the principle of maximum conformality (PMC). As a comparison, we show that under the conventional scale setting, we have Δρ∣N3LO=(8.257−0.012+0.045)×10−3Δρ|_{\rm N^3LO} = \left(8.257^{+0.045}_{-0.012}\right) \times10^{-3} by varying the scale μr∈[Mt/2μ_{r}\in[M_{t}/2, 2Mt]2M_{t}]. By defining a ratio, ΔR=Δρ/3Xt−1ΔR=Δρ/3X_t-1, which shows the relative importance of the QCD corrections, it is found that its scale error is ∼±9%\sim \pm9 \% at the two-loop level, which changes to ∼±4%\sim\pm4\% at the three-loop level and ∼±2.5%\sim \pm 2.5\% at the four-loop level, respectively. These facts well explain why the conventional scale uncertainty constitutes an important error for estimating the ρρ parameter. On the other hand, by applying the PMC scale setting, the four-loop estimation Δρ∣N3LOΔρ|_{\rm N^3LO} shall be almost fixed to 8.228×10−38.228\times10^{-3}, which indicates that the conventional scale error has been eliminated. We observe the pQCD convergence for the ρρ parameter has also been greatly improved due to the elimination of the divergent renormalon terms. As applications of the present QCD improved ρρ parameter, we show the shifts of the WW-boson mass and the effective leptonic weak-mixing angle due to ΔρΔρ can be reduced to δMW∣N3LO=0.7δM_{W}|_{\rm N^3LO} =0.7 MeV and δsin⁡2θeff∣N3LO=−0.4×10−5δ\sin^2θ_{\rm eff}|_{\rm N^3LO}=-0.4\times10^{-5}.

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