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- Brookhaven National LaboratoryUS24 papers
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- Centre National de la Recherche ScientifiqueFR15 papers
- Columbia UniversityUS14 papers
- Commissariat à l'Énergie Atomique et aux Énergies AlternativesFR13 papers
- Ruhr University BochumDE13 papers
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- Johannes Gutenberg University MainzDE12 papers
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- Helsinki Institute of PhysicsFI11 papers
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- University of BonnDE11 papers
9 papers · 2 filters
New developments in PJFry
Jochem Fleischer, Tord Riemann, Valery Yundin
We report on recent progress in numerical evaluation of one loop tensor integrals. A public C++ package PJFry implementing algorithms from arXiv:1009.4436 and its extension to hexa…
Quark number susceptibilities from resummed perturbation theory
Jens O. Andersen, Sylvain Mogliacci, Nan Su +1
We evaluate the second and fourth order quark number susceptibilities in hot QCD using two variations of resummed perturbation theory. On one hand, we carry out a one-loop calculat…
Charmonium dissociation and heavy quark transport in hot quenched lattice QCD
H. -T. Ding, A. Francis, O. Kaczmarek +3
We study the properties of charmonium states at finite temperature in quenched lattice QCD on large and fine isotropic lattices. We perform a detailed analysis of charmonium correl…
Computing the temperature dependence of effective CP violation in the standard model
Tomas Brauner, Olli Taanila, Anders Tranberg +1
CP violation in the standard model originates from the Cabibbo-Kobayashi-Maskawa mixing matrix. Upon integrating all fermions out of the theory, its effects are captured by a serie…
Heavy quark chemical equilibration rate as a transport coefficient
D. Bodeker, M. Laine
Motivated by indications that heavy (charm and bottom) quarks interact strongly at temperatures generated in heavy ion collision experiments, we suggest a non-perturbative definiti…
A brief overview of hard-thermal-loop perturbation theory
Nan Su
The poor convergence of quantum field theory at finite temperature has been one of the main obstacles in the practical applications of thermal QCD for decades. Here we briefly revi…