We resum to all orders of perturbation theory the invariant mass distribution of jets initiated by massive quarks. We find that the inclusion of mass terms, in the N-moment space, results in the universal factor delta_N(Q^2;m^2), taking into account dead-cone effects in gluon emission, which multiplies the massless jet distribution function J_N(Q^2). The variable N is rescaled by the mass correction parameter r = m^2/Q^2 c l nu decay spectra or the inclusion of beauty mass effects in t --> b W decays, are briefly sketched
We construct jet observables for energetic top quarks that can be used to determine a short distance...
We construct jet observables for energetic top quarks that can be used to determine a short-distance...
After giving their general expressions valid at all x, double differential 1-particle inclusive dist...
We resum the invariant mass distribution of jets initiated by massive quarks in next-to-leading loga...
We resum the invariant mass distribution of jets initiated by massive quarks in next-to-leading loga...
AbstractWe resum the invariant mass distribution of jets initiated by massive quarks in next-to-lead...
Abstract We resum the invariant mass distribution of jets initiated by massive quarks in next-to-le...
We resum the invariant mass distribution of jets initiated by massive quarks in next-to-leading loga...
We resum the invariant mass distribution of jets initiated by massive quarks in next-to-leading loga...
We resum the invariant mass distribution of jets initiated by massive quarks in next-to-leading loga...
We resum the invariant mass distribution of jets initiated by massive quarks in next-to-leading loga...
We compute in the heavy quark effective theory the soft coefficient D_2 entering the resummation of ...
We compute in the heavy quark effective theory the soft coefficient D2 entering the resummation of n...
AbstractWe compute in the heavy quark effective theory the soft coefficient D2 entering the resummat...
The resummed invariant mass distribution evaluated to all orders of perturbation theory for jets ini...
We construct jet observables for energetic top quarks that can be used to determine a short distance...
We construct jet observables for energetic top quarks that can be used to determine a short-distance...
After giving their general expressions valid at all x, double differential 1-particle inclusive dist...
We resum the invariant mass distribution of jets initiated by massive quarks in next-to-leading loga...
We resum the invariant mass distribution of jets initiated by massive quarks in next-to-leading loga...
AbstractWe resum the invariant mass distribution of jets initiated by massive quarks in next-to-lead...
Abstract We resum the invariant mass distribution of jets initiated by massive quarks in next-to-le...
We resum the invariant mass distribution of jets initiated by massive quarks in next-to-leading loga...
We resum the invariant mass distribution of jets initiated by massive quarks in next-to-leading loga...
We resum the invariant mass distribution of jets initiated by massive quarks in next-to-leading loga...
We resum the invariant mass distribution of jets initiated by massive quarks in next-to-leading loga...
We compute in the heavy quark effective theory the soft coefficient D_2 entering the resummation of ...
We compute in the heavy quark effective theory the soft coefficient D2 entering the resummation of n...
AbstractWe compute in the heavy quark effective theory the soft coefficient D2 entering the resummat...
The resummed invariant mass distribution evaluated to all orders of perturbation theory for jets ini...
We construct jet observables for energetic top quarks that can be used to determine a short distance...
We construct jet observables for energetic top quarks that can be used to determine a short-distance...
After giving their general expressions valid at all x, double differential 1-particle inclusive dist...