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Top-Quark Decay at Next-to-Next-to-Next-to-Leading Order in QCD

Long Chen, Xiang Chen, Xin Guan, Yan-Qing Ma

Abstract

We present the first complete high-precision QCD corrections to the inclusive decay width $\mathrmΓ_t$, the $W$-helicity fractions $f_{\mathrm{L,R,0}}$ and semi-inclusive distributions for the top-quark decay process $t \rightarrow b + W^+ + X_{\mathrm{\tiny QCD}}$ at NNNLO in the strong coupling constant $α_s$. In particular, the pure NNNLO QCD correction decreases the $\mathrmΓ_t$ by about $0.8\%$ of the previous NNLO result at the top-quark pole mass scale, exceeding the error estimated by the usual scale-variation prescription. After taking into account all sources of errors, we get $\mathrmΓ_t = 1.3148^{+0.003}_{-0.005} + 0.027\,(m_t - 172.69)\,\text{GeV} $, the error of which meets the request by future colliders. On the other hand, the NNNLO QCD effects on $f_{\mathrm{L,R,0}}$ are found to be much smaller, at the level of one per-mille for the dominating $f_{0}$, predestining them to act as precision observables for the top-quark decay process.

Top-Quark Decay at Next-to-Next-to-Next-to-Leading Order in QCD

Abstract

We present the first complete high-precision QCD corrections to the inclusive decay width , the -helicity fractions and semi-inclusive distributions for the top-quark decay process at NNNLO in the strong coupling constant . In particular, the pure NNNLO QCD correction decreases the by about of the previous NNLO result at the top-quark pole mass scale, exceeding the error estimated by the usual scale-variation prescription. After taking into account all sources of errors, we get , the error of which meets the request by future colliders. On the other hand, the NNNLO QCD effects on are found to be much smaller, at the level of one per-mille for the dominating , predestining them to act as precision observables for the top-quark decay process.
Paper Structure (9 equations, 2 figures)

This paper contains 9 equations, 2 figures.

Figures (2)

  • Figure 1: The scale dependence of the fixed-order results for $\mathrm{\Gamma}_t$ in $\mu/m_t \in [0.1, 1]$
  • Figure 2: The $W$-energy distribution in $t$-quark decay observed in the $t$-quark rest frame.