Table 15.

Electroweak input parameters, in the $G_{\mathit{\mu }}$ scheme, for the NC and CC Drell–Yan pp and deep inelastic ep scattering cross-section calculations, see text. Standard Model parameters are taken from Refs. [39, 100], except $\mathrm{\Gamma }(W\to \ell \mathit{\nu })$. The $V_{ij}$ symbols denote the elements of the CKM matrix. The parameters below the line, the weak mixing angle ${sin}^2{\mathit{\theta }}_{\mathrm{W}}$, the fine-structure constant ${\mathit{\alpha }}_{G_{\mathit{\mu }}}$, and the vector couplings of up-type quarks $v_u$, down-type quarks $v_d$, and charged leptons $v_{\ell }$ to the Z boson, are calculated at tree level from the ones above

$m_Z$	91.1876 $\text{GeV}$	$|V_{ud}|$	0.97427
${\mathrm{\Gamma }}_Z$	2.4949 $\text{GeV}$	$|V_{us}|$	0.22534
$\mathrm{\Gamma }(Z\to \ell \ell )$	0.08400 $\text{GeV}$	$|V_{ub}|$	0.00351
$m_W$	80.385 $\text{GeV}$	$|V_{cd}|$	0.22520
${\mathrm{\Gamma }}_W$	2.0906 $\text{GeV}$	$|V_{cs}|$	0.97344
$\mathrm{\Gamma }(W\to \ell \mathit{\nu })$	0.22727 $\text{GeV}$	$|V_{cb}|$	0.0412
$m_H$	125 $\text{GeV}$	$|V_{td}|$	0.00867
$m_t$	173.5 $\text{GeV}$	$|V_{ts}|$	0.0404
$G_{\mathrm{F}}$	$1.1663787\times {10}^{-5}$ $\text{GeV}$ ${}^{-2}$	$|V_{tb}|$	0.999146
${sin}^2{\mathit{\theta }}_{\mathrm{W}}$	0.222897
${\mathit{\alpha }}_{G_{\mathit{\mu }}}$	$7.562396\times {10}^{-3}$
$v_u$	0.405607
$v_d$	−0.702804
$v_{\ell }$	−0.108411