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Recent developments in the treatment of a system of heavy quarks close to their production threshold are discussed. Particular emphasis is put on the next-to-next-to-next-to-leading order (N$^3$LO) corrections to the energy levels and the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Matthias Steinhauser

We summarize calculations of the cross section for top quark production at hadron colliders within the context of perturbative quantum chromodynamics, including resummation of the effects of initial-state soft gluon radiation to all orders…

High Energy Physics - Phenomenology · Physics 2007-05-23 Edmond L. Berger , Harry Contopanagos

We present updated predictions for the total cross section of top-quark pair production at Tevatron and LHC. For the LHC we also provide results at sqrt(s) = 10 TeV, in view of the anticipated run in 2008 and quote numbers for the…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Moch , P. Uwer

Differential distributions for heavy quark production depend on the heavy quark mass and other momentum scales, which can yield additional large logarithms and inhibit accurate predictions. Logarithms involving the heavy quark mass can be…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. M. Nadolsky , N. Kidonakis , F. I. Olness , C. -P. Yuan

We use the QCD sum rule approach to calculate the splitting between vector and pseudoscalar mesons containing one light and one heavy quark, and the kinetic energy of the heavy quark. Our result for the splitting induced by the…

High Energy Physics - Phenomenology · Physics 2011-01-25 P. Ball , V. M. Braun

We propose a scheme to measure quantum Stokes parameters, their fluctuations and correlations. The proposal involves measurements of intensities and intensity- intensity correlations for suitably defined modes, which can be produced by a…

Quantum Physics · Physics 2015-06-26 G. S. Agarwal , S. Chaturvedi

We present a status report of a variety of projects related to heavy quark production and parton distributions for the Tevatron Run II.

High Energy Physics - Phenomenology · Physics 2007-05-23 R. Demina , S. Keller , M. Krämer , S. Kretzer , R. Martin , F. I. Olness , R. J. Scalise , D. E. Soper , W. -K. Tung , N. Varelas , U. K. Yang

The study of the properties of the top quark is one of the main goals of the Large Hadron Collider (LHC) physics program. The experimental precision expected at the LHC requires the calculation of several top-quark related observables…

High Energy Physics - Phenomenology · Physics 2014-11-20 R. Bonciani , A. Ferroglia

Heavy quarks are copiously produced in two-photon collisions at $e^+e^-$ colliders. The theoretical predictions including QCD radiative corrections are compared to recent experimental data on $\gamma\gamma$ production of charm quarks at…

High Energy Physics - Phenomenology · Physics 2007-05-23 Michael Krämer

We calculate the heavy quarkonium production in double pomeron exchange processes in perturbative QCD by using two-gluon exchange model. For the $P$-wave $\chi_J$ productions, we find $\chi_1$ and $\chi_2$ production amplitudes which vanish…

High Energy Physics - Phenomenology · Physics 2009-11-07 Feng Yuan

I present a review of selected topics in the computation of heavy flavour cross sections in photon-hadron collisions.

High Energy Physics - Phenomenology · Physics 2009-10-31 S. Frixione

Vector meson production in ultra-peripheral collisions of heavy ions at LHC is calculated in VDM and color dipole approaches.

High Energy Physics - Phenomenology · Physics 2007-06-12 Yu. P. Ivanov , B. Z. Kopeliovich , I. Schmidt

Conventional perturbative QCD calculations on the production of a heavy quark ``$H$'' consist of two contrasting approaches: the usual QCD parton formalism uses the zero-mass approximation ($m_H=0$) once above threshold, and treats $H$ just…

High Energy Physics - Phenomenology · Physics 2009-10-30 Wu-Ki Tung

Data from LEP2 on hadron production in gamma gamma interactions at high pT exceed the predictions of QCD by about an order of magnitude. The amplitude for the process is asymptotically proportional to the sum of the squares of the charges…

High Energy Physics - Phenomenology · Physics 2009-02-16 Philip Yock

The exclusive processes are considered, where a point-like source of heavy quark-antiquark pairs $Q \bar Q$, e.g. their electromagnetic current, produces a pair consisting of a heavy quarkoniumlike exotic meson (tetraquark) or baryon…

High Energy Physics - Phenomenology · Physics 2016-11-02 M. B. Voloshin

We calculate the coupling constants between the light vector mesons and heavy mesons within the framework of the light-cone QCD sum rule in the leading order of heavy quark effective theory. The sum rules are very stable with the variations…

High Energy Physics - Phenomenology · Physics 2009-08-09 Peng-Zhi Huang , Liang Zhang , Shi-Lin Zhu

We present the joint threshold and recoil resummed transverse momentum distributions for heavy quark hadroproduction, at next-to-leading logarithmic accuracy. We exhibit their dependence on the production channel and the color…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Banfi , E. Laenen

Several methodologies are developed for large-scale atomistic simulations with fully quantum mechanical description of electron systems. The important methodological concepts are (i) generalized Wannier state, (ii) Krylov subspace and (iii)…

Materials Science · Physics 2007-05-23 Takeo Hoshi

We describe a next-to-leading-order calculation of the fully exclusive parton cross section for the photoproduction of heavy quarks. We use our result to compute quantities of interest for current fixed-target experiments. We discuss…

High Energy Physics - Phenomenology · Physics 2011-01-25 S. Frixione , M. Mangano , P. Nason , G. Ridolfi

We present a study of heavy quarkonium production in hard diffractive process by the Pomeron exchange for Tevatron and LHC energies. The numerical results are computed using recent experimental determination of the diffractive parton…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. V. T. Machado
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