We compute in the heavy quark effective theory the soft coefficient D_2 entering the resummation of next-to-next-to-leading threshold logarithms for jets initiated by a quark with a small mass compared to the hard scale of the process. We find complete agreement with a previous computation in full QCD. Contrary to our previous guess, this coefficient turns out to be different from that one entering heavy flavor decay or heavy flavor fragmentation
Heavy quark fragmenting jet functions describe the fragmentation of a parton into a jet containing a...
The soft-gluon resummation exponents G^N in moment space are investigated for the quark coefficient ...
I discuss the heavy quark expansion for the inclusive widths of heavy-light hadrons, which predicts ...
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...
We resum to all orders of perturbation theory the invariant mass distribution of jets initiated by m...
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 D(2) entering the resummation of...
AbstractWe compute in the heavy quark effective theory the soft coefficient D2 entering the resummat...
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 D(2) entering the resummation of...
AbstractWe present the calculation of the finite part of the heavy quark impact factor at next-to-le...
We compute in the heavy quark effective theory the soft coefficient D(2) entering the resummation of...
Heavy quark fragmenting jet functions describe the fragmentation of a parton into a jet containing a...
The soft-gluon resummation exponents G^N in moment space are investigated for the quark coefficient ...
I discuss the heavy quark expansion for the inclusive widths of heavy-light hadrons, which predicts ...
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...
We resum to all orders of perturbation theory the invariant mass distribution of jets initiated by m...
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 D(2) entering the resummation of...
AbstractWe compute in the heavy quark effective theory the soft coefficient D2 entering the resummat...
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 D(2) entering the resummation of...
AbstractWe present the calculation of the finite part of the heavy quark impact factor at next-to-le...
We compute in the heavy quark effective theory the soft coefficient D(2) entering the resummation of...
Heavy quark fragmenting jet functions describe the fragmentation of a parton into a jet containing a...
The soft-gluon resummation exponents G^N in moment space are investigated for the quark coefficient ...
I discuss the heavy quark expansion for the inclusive widths of heavy-light hadrons, which predicts ...