A Lagrangean and a set of Feynman rules are presented for Non-Relativistic QCD with manifest power counting in the heavy quark velocity $v$. A régime is identified in which energies and momenta are of order $Mv$. It is neither identical to the ultrasoft régime corresponding to radiative processes with energies and momenta of order $Mv^2$, nor to the potential régime with on shell quarks and gluons providing the Coulomb binding. In this soft régime, gluons are on shell, and the quark propagator becomes static. Examples show that it contributes to one- and two-loop corrections of scattering and production amplitudes near threshold. The results are readily generalised to any effective field theory with more than one low energy scale
We employ a nonrelativistic version of QCD (NRQCD) to study heavy quark-antiquark bound states in th...
Non-relativistic bound states have two low energy scales, a soft scale mu_S of order mv and an ultra...
There are indications of a faith transition in QCD: The strong coupling may freeze at a sufficiently...
We review some recent developments on non-relativistic effective field theories for heavy quark-anti...
A new derivation of the effective lagrangian for non-relativistic quantum chromodynamics and the hea...
A solution to the Schrodinger equation for the nonrelativistic Green function which is used for desc...
We discuss the matching conditions and renormalization group evolution of non-relativistic QCD. A va...
In the framework of the QCD effective field theory called potential Non-Relativistic QCD, we explore...
An overview of recent theoretical progress on Non-Relativistic QCD and related effective theories is...
We discuss the form and construction of general color singlet heavy particle-antiparticle pair produ...
In this letter we address issues involved in quarkonium production near the boundaries of phase spac...
In this letter we address issues involved in quarkonium production near the boundaries of phase spac...
Starting from the NRQCD Lagrangian the heavy quark-antiquark potential is written in terms of field ...
In this talk I review some recent applications of NRQCD. I first discuss the unquenched NRQCD lattic...
We analyse the possible existence of non-perturbative contributions in heavy \bar Q Q systems (\bar ...
We employ a nonrelativistic version of QCD (NRQCD) to study heavy quark-antiquark bound states in th...
Non-relativistic bound states have two low energy scales, a soft scale mu_S of order mv and an ultra...
There are indications of a faith transition in QCD: The strong coupling may freeze at a sufficiently...
We review some recent developments on non-relativistic effective field theories for heavy quark-anti...
A new derivation of the effective lagrangian for non-relativistic quantum chromodynamics and the hea...
A solution to the Schrodinger equation for the nonrelativistic Green function which is used for desc...
We discuss the matching conditions and renormalization group evolution of non-relativistic QCD. A va...
In the framework of the QCD effective field theory called potential Non-Relativistic QCD, we explore...
An overview of recent theoretical progress on Non-Relativistic QCD and related effective theories is...
We discuss the form and construction of general color singlet heavy particle-antiparticle pair produ...
In this letter we address issues involved in quarkonium production near the boundaries of phase spac...
In this letter we address issues involved in quarkonium production near the boundaries of phase spac...
Starting from the NRQCD Lagrangian the heavy quark-antiquark potential is written in terms of field ...
In this talk I review some recent applications of NRQCD. I first discuss the unquenched NRQCD lattic...
We analyse the possible existence of non-perturbative contributions in heavy \bar Q Q systems (\bar ...
We employ a nonrelativistic version of QCD (NRQCD) to study heavy quark-antiquark bound states in th...
Non-relativistic bound states have two low energy scales, a soft scale mu_S of order mv and an ultra...
There are indications of a faith transition in QCD: The strong coupling may freeze at a sufficiently...