ﻻ يوجد ملخص باللغة العربية
In this paper, we carry out the next-to-leading-order (NLO) studies on $Z to Upsilon(1S)+g+g$ via the color-singlet (CS) $bbar{b}$ state. We find the newly calculated NLO QCD corrections to this process can significantly influence its leading-order (LO) results, and greatly improve the dependence on the renormalization scale. By including the considerable feeddown contributions, the branching ratio $mathcal{B}_{Z to Upsilon(1S)+g+g}$ is predicted to be $(0.56 sim 0.95)times 10^{-6}$, which can reach up to $19% sim 31%$ of the LO predictions given by the CS dominant process $Z to Upsilon(1S)+b+bar{b}$. Moreover, $Z to Upsilon(1S)+g+g$ also seriously affect the CS predictions on the $Upsilon(1S)$ energy distributions, especially when $z$ is relatively small. In summary, for the inclusive $Upsilon(1S)$ productions in $Z$ decay, besides $Z to Upsilon(1S)+b+bar{b}$, the gluon radiation process $Z to Upsilon(1S)+g+g$ can provide indispensable contributions as well.
We present a first analysis of parton-to-pion fragmentation functions at next-to-next-to-leading order accuracy in QCD based on single-inclusive pion production in electron-positron annihilation. Special emphasis is put on the technical details neces
Applying the nonrelativistic quantum chromodynamics factorization formalism to the $Upsilon(1S,2S,3S)$ hadroproduction, a complete analysis on the polarization parameters $lambda_{theta}$, $lambda_{thetaphi}$, $lambda_{phi}$ for the production are pr
The reaction pp/pbar p -> t tbar jet+X is an important background process for Higgs boson searches in the mass range below 200 GeV. Apart from that it is also an ideal laboratory for precision measurements in the top quark sector. Both applications r
The leading order hadronic contribution to the muon magnetic moment anomaly, $a^{HAD}_mu$, is determined entirely in the framework of QCD. The result in the light-quark sector, in units of $10^{-10}$, is $a^{HAD}_mu|_{uds} =686 pm 26$, and in the hea
We determine an approximate expression for the O(alpha_s^3) contribution chi_2 to the kernel of the BFKL equation, which includes all collinear and anticollinear singular contributions. This is derived using recent results on the relation between the