The dynamics of heavy quarkonium systems in the strong coupling regime reduces to a quantum mechanical problem with a number of potentials which may be organized in powers of 1 / m , m being the heavy quark mass. The potentials must be calculated nonperturbatively, for instance, in lattice QCD. It is well known that the long-distance behavior of the static ( 1 / m 0 ) potential is well reproduced by an effective string theory. We show that this effective string theory, if correct, should also reproduce the long-distance behavior of all 1 / m suppressed potentials. We demonstrate the practical usefulness of this result by finding a suitable parameterization of the recently calculated 1 / m potential. We also calculate the 1 / m 2 velocity-de...
We present our calculation of the non-relativistic corrections to the heavy quark-antiquark potentia...
We present our calculation of the non-relativistic corrections to the heavy quark-antiquark potentia...
We use Dual QCD to derive an effective potential to order (quark mass)-2 for a constituent quark and...
The dynamics of heavy quarkonium systems in the strong coupling regime reduces to a quantum mechanic...
The dynamics of heavy quarkonium systems in the strong coupling regime reduces to a quantum mechanic...
The effective string picture of confinement is used to derive theoretical predictions for the interq...
Expressions for the potentials appearing in the nonrelativistic effective field theory description o...
The effective string picture of confinement is used to derive theoretical predictions for the interq...
The subleading term of the heavy quark potential (the analogue of the Luscher term) is computed in a...
The imaginary part of the effective heavy-quark potential can be related to the total in-medium deca...
We study the ''effective string picture'' of confinement, deriving theoretical predictions for the i...
Screening effects from sea pairs on the quark-antiquark static potential are analyzed phenomenologic...
Screening effects from sea pairs on the quark-antiquark static potential are analyzed phenomenologic...
Abstract We consider the $${\mathcal {O}}(1/m)$$ O(1/m) and the spin-independent momentum-dependent ...
We present our calculation of the non-relativistic corrections to the heavy quark-antiquark potentia...
We present our calculation of the non-relativistic corrections to the heavy quark-antiquark potentia...
We present our calculation of the non-relativistic corrections to the heavy quark-antiquark potentia...
We use Dual QCD to derive an effective potential to order (quark mass)-2 for a constituent quark and...
The dynamics of heavy quarkonium systems in the strong coupling regime reduces to a quantum mechanic...
The dynamics of heavy quarkonium systems in the strong coupling regime reduces to a quantum mechanic...
The effective string picture of confinement is used to derive theoretical predictions for the interq...
Expressions for the potentials appearing in the nonrelativistic effective field theory description o...
The effective string picture of confinement is used to derive theoretical predictions for the interq...
The subleading term of the heavy quark potential (the analogue of the Luscher term) is computed in a...
The imaginary part of the effective heavy-quark potential can be related to the total in-medium deca...
We study the ''effective string picture'' of confinement, deriving theoretical predictions for the i...
Screening effects from sea pairs on the quark-antiquark static potential are analyzed phenomenologic...
Screening effects from sea pairs on the quark-antiquark static potential are analyzed phenomenologic...
Abstract We consider the $${\mathcal {O}}(1/m)$$ O(1/m) and the spin-independent momentum-dependent ...
We present our calculation of the non-relativistic corrections to the heavy quark-antiquark potentia...
We present our calculation of the non-relativistic corrections to the heavy quark-antiquark potentia...
We present our calculation of the non-relativistic corrections to the heavy quark-antiquark potentia...
We use Dual QCD to derive an effective potential to order (quark mass)-2 for a constituent quark and...