Abstract: The gauge/gravity duality is used to investigate the imaginary part of the heavy quark potential (defined via the rectangular Wilson loop) in strongly coupled plas-mas. This quantity can be used to estimate the width of heavy quarkonia in a plasma at strong coupling. In this paper the thermal worldsheet fluctuation method, proposed in [J. Noronha and A. Dumitru, Phys. Rev. Lett. 103, 152304 (2009)], is revisited and general conditions for the existence of an imaginary part for the heavy quark potential computed within classical gravity models are obtained. We prove a general result that establishes the connection between this imaginary part of the potential determined holographically and the area law displayed by the Wilson loop i...
Using AdS/CFT, we compute the Fourier space profile of generated by a heavy quark moving through a ...
We compute and study the drag force acting on a heavy quark propagating through the matter produced ...
We study the energy loss of a quark moving in the strongly coupled $\mathcal{N} = 4$ supersymmetric ...
The imaginary part of the heavy quark-antiquark potential experienced by moving heavy quarkonia in s...
From the AdS/CFT correspondence, the effects of charge and finite ’t Hooft coupling correction on th...
The heavy quark potential of a thermal Yang–Mills theory in strong coupling limit is explored in ter...
By the use of the gauge/gravity duality, we calculate the imaginary part of heavy quarkonium potenti...
We study the properties of heavy quarks as probes of strongly coupled plasmas with and without chemi...
We develop a holographic (bottom-up) gravity model for QCD to understand the connection between the ...
In general we can say that the thermal width of quarkonia corresponds to imaginary part of it’s pote...
We study several observables related to heavy quarks in strongly coupled plasmas using the gauge/gra...
In this work I explore theoretical and phenomenological implications of chemical potentials and char...
We analysis physical observables of heavy quarks in gravity models describing strongly coupled non-c...
We study the energy loss of a heavy quark propagating through the matter produced in the collision o...
Abstract We extract the imaginary part of the heavy-quark potential using classical-statistical simu...
Using AdS/CFT, we compute the Fourier space profile of generated by a heavy quark moving through a ...
We compute and study the drag force acting on a heavy quark propagating through the matter produced ...
We study the energy loss of a quark moving in the strongly coupled $\mathcal{N} = 4$ supersymmetric ...
The imaginary part of the heavy quark-antiquark potential experienced by moving heavy quarkonia in s...
From the AdS/CFT correspondence, the effects of charge and finite ’t Hooft coupling correction on th...
The heavy quark potential of a thermal Yang–Mills theory in strong coupling limit is explored in ter...
By the use of the gauge/gravity duality, we calculate the imaginary part of heavy quarkonium potenti...
We study the properties of heavy quarks as probes of strongly coupled plasmas with and without chemi...
We develop a holographic (bottom-up) gravity model for QCD to understand the connection between the ...
In general we can say that the thermal width of quarkonia corresponds to imaginary part of it’s pote...
We study several observables related to heavy quarks in strongly coupled plasmas using the gauge/gra...
In this work I explore theoretical and phenomenological implications of chemical potentials and char...
We analysis physical observables of heavy quarks in gravity models describing strongly coupled non-c...
We study the energy loss of a heavy quark propagating through the matter produced in the collision o...
Abstract We extract the imaginary part of the heavy-quark potential using classical-statistical simu...
Using AdS/CFT, we compute the Fourier space profile of generated by a heavy quark moving through a ...
We compute and study the drag force acting on a heavy quark propagating through the matter produced ...
We study the energy loss of a quark moving in the strongly coupled $\mathcal{N} = 4$ supersymmetric ...