We consider the problem of including a finite number of scattering centers in dynamical energy loss and classical DGLV formalism. Previously, either one or an infinite number of scattering centers were considered in energy loss calculations, while attempts to relax such approximations were largely inconclusive or incomplete. In reality, however, the number of scattering centers is generally estimated to be 4-5 at RHIC and the LHC, making the above approximations (a priori) inadequate and this theoretical problem significant for QGP tomography. We derived explicit analytical expressions for dynamical energy loss and DGLV up to the $4^{th}$ order in opacity, resulting in complex mathematical expressions that were, to our knowledge, obtained f...
Heavy quark medium induced radiative energy loss is derived to all orders in opacity, $(L/\lambda_g)...
We calculate the contribution from the $q \bar q g$ state production to the diffractive cross sectio...
The transverse momentum broadening coefficient $\hat{q}$ receives both soft, classical and radiative...
We provide the first calculation of two-gluon production at mid-rapidity in ultra-peripheral collisi...
International audienceWe calculate the fully differential medium-induced radiative spectrum at next-...
We perform a global analysis of experimental data on jet quenching for heavy flavors for scenarios w...
The predicted quenching of jets in A + A at RHIC energies has been discovered by STAR and PHENIX in ...
We predict heavy quark production cross sections in Deep Inelastic Scattering at high energy by appl...
AbstractInteractions of high momentum partons with Quark–Gluon Plasma created in relativistic heavy-...
We apply the Low's theorem to soft gluon emission from heavy quark scattering in the nonperturbative...
Energetic partons traveling in a strongly interacting medium lose energy by emitting radiation and t...
We study within the light-cone path integral approach the induced gluon emission from a fast quark p...
Heavy quarks created in heavy-ion collisions serve as an excellent probe of the produced quark-gluon...
We compute the in-medium jet broadening $\langle p_\perp^2\rangle$ to leading order in energy in the...
With the QGP opacity computed perturbatively and with the global entropy constraints imposed by the ...
Heavy quark medium induced radiative energy loss is derived to all orders in opacity, $(L/\lambda_g)...
We calculate the contribution from the $q \bar q g$ state production to the diffractive cross sectio...
The transverse momentum broadening coefficient $\hat{q}$ receives both soft, classical and radiative...
We provide the first calculation of two-gluon production at mid-rapidity in ultra-peripheral collisi...
International audienceWe calculate the fully differential medium-induced radiative spectrum at next-...
We perform a global analysis of experimental data on jet quenching for heavy flavors for scenarios w...
The predicted quenching of jets in A + A at RHIC energies has been discovered by STAR and PHENIX in ...
We predict heavy quark production cross sections in Deep Inelastic Scattering at high energy by appl...
AbstractInteractions of high momentum partons with Quark–Gluon Plasma created in relativistic heavy-...
We apply the Low's theorem to soft gluon emission from heavy quark scattering in the nonperturbative...
Energetic partons traveling in a strongly interacting medium lose energy by emitting radiation and t...
We study within the light-cone path integral approach the induced gluon emission from a fast quark p...
Heavy quarks created in heavy-ion collisions serve as an excellent probe of the produced quark-gluon...
We compute the in-medium jet broadening $\langle p_\perp^2\rangle$ to leading order in energy in the...
With the QGP opacity computed perturbatively and with the global entropy constraints imposed by the ...
Heavy quark medium induced radiative energy loss is derived to all orders in opacity, $(L/\lambda_g)...
We calculate the contribution from the $q \bar q g$ state production to the diffractive cross sectio...
The transverse momentum broadening coefficient $\hat{q}$ receives both soft, classical and radiative...