H. Liang

Next-to-leading order QCD predictions for Z

A bstractWe calculate the complete next-to-leading order (NLO) QCD corrections to the Z0H0 production in association with a jet at the LHC. We study the impacts of the NLO QCD radiative corrections to the integrated and differential cross sections and the dependence of the cross section on the factorization/renormalization scale. We present the transverse momentum distributions of the final Z0-, Higgs-boson and leading-jet. We find that the NLO QCD corrections significantly modify the physical observables, and obviously reduce the scale uncertainty of the LO cross section. The QCD K-factors can be 1.183 and 1.180 at the

Pair production of charged Higgs bosons in gluon - gluon collisions

\sqrt {s} = {14}

Probing flavor-changing interactions in photon-photon collisions

TeV and

Associated production of a graviton with an e+ e-pair via photon-photon collisions at a linear collider

\sqrt {s} = {7}

The Effects of the little Higgs models on t anti-t h0 production via gamma gamma collision at linear colliders

TeV LHC respectively, when we adopt the inclusive event selection scheme with

SUSY charged Higgs boson pair production via gluon-gluon collisions

p_{T,j}^{cut} = {5}0

Pair production of charged Higgs bosons from bottom-quark fusion

GeV, mH = 120 GeV and μ = μr = μf = μ0 ≡

Revisiting the QCD Corrections to the R-Parity Violating Processes pp̄/pp → eμ + X

\frac{1}{2}\left( {{m_Z} + {m_H}} \right)

Top-quark pair production via polarized and unpolarized protons in the supersymmetric QCD

. Furthermore, we make the comparison between the two scale choices, μ = μ0 and μ = μ1 =

Full one-loop electroweak and NLO QCD corrections to the associated production of chargino and neutralino at hadron colliders

\frac{1}{2}\left( {E_T^Z + E_T^H + \sum\nolimits_j {E_T^{jet}} } \right)