Oblique corrections to the W width.

Oblique corrections to the W width.
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W 宽度的倾斜修正。

DOI:
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发表时间:
1993
期刊:
Physical Review D, Particles and fields
影响因子:
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通讯作者:
T. Takeuchi
T. Takeuchi
中科院分区:
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文献类型:
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作者:
J. Rosner;M. Worah;T. Takeuchi

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部分$W$Width to$e的最低阶表达式 U,~Gamma(W o e U)=G_muM_W^3/(6pi_Sqrt{2})$,如果使用测量的$W$质量,则没有来自新物理的倾斜辐射修正。这里$G_MU=(1.16639 PM 0.00002)imes 10^{-5}$GeV/$c^2$是介子衰变常数。对于现值$M_W=(80.14 PM 0.27)$GeV/$c^2$,如果$m_t=140$GeV$/c^2$,则预期为$Gamma(W o e U)=(224.4 PM 2.3)$MeV总宽度$Gamma_{ Mtot}(W)$预计也没有来自新物理的倾斜修正,因此$Gamma_{ M Tot}(W)/Gamma(W o e U)=3+6[1+{α_S(M_W)/pi}]$。目前的数据与这一预测一致。
The lowest-order expression for the partial $W$ width to $e u ,~Gamma (W o e u) = G_mu M_W^3 /(6 pi sqrt{2})$, has no oblique radiative corrections from new physics if the measured $W$ mass is used. Here $G_mu = (1.16639 pm 0.00002) imes 10^{-5}$ GeV/$c^2$ is the muon decay constant. For the present value of $M_W = (80.14 pm 0.27)$ GeV/$c^2$, and with $m_t = 140$ GeV$/c^2$, one expects $Gamma (W o e u) = (224.4 pm 2.3)$ MeV. The total width $Gamma_{ m tot}(W)$ is also expected to lack oblique corrections from new physics, so that $Gamma_{ m tot} (W)/ Gamma (W o e u) = 3 + 6 [1 + {alpha_s (M_W)/pi }]$. Present data are consistent with this prediction.