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20022008
most citedNon-thermal fixed points: effective weak-coupling for strongly correlated systems far from equilibrium

275 citations

Showing 2008Show all

23 papers · 1 filter

hep-ph200893 cited

Beyond the rainbow: effects from pion back-coupling

Christian S. Fischer, Richard Williams

We investigate hadronic unquenching effects in light quarks and mesons. To this end we take into account the back-coupling of the pion onto the quark propagator within the non-pert…

nucl-th20081 cited

Reply to the Comment on 'Pygmy dipole response of proton-rich argon nuclei in random-phase approximation and no-core shell model'

C. Barbieri, E. Caurier, K. Langanke +1

We respond to a Comment on our recent paper (Phys.Rev.C77:024304,2008) by Paar (arXiv:0803.0274).

math.NT2008

Faltings heights of CM cycles and derivatives of L-functions

Jan Hendrik Bruinier, Tonghai Yang

We study the Faltings height pairing of arithmetic Heegner divisors and CM cycles on Shimura varieties associated to orthogonal groups. We compute the Archimedian contribution to t…

nucl-th200824 cited

Statistical hadronization of charm: from FAIR to the LHC

A. Andronic, P. Braun-Munzinger, K. Redlich +1

We discuss the production of charmonium in nuclear collisions within the framework of the statistical hadronization model. We demonstrate that the model reproduces very well the av…

astro-ph2008107 cited

Influence of light nuclei on neutrino-driven supernova outflows

A. Arcones, G. Martinez-Pinedo, E. O'Connor +4

We study the composition of the outer layers of a protoneutron star and show that light nuclei are present in substantial amounts. The composition is dominated by nucleons, deutero…

cond-mat.supr-con200888 cited

Superconductivity phase diagrams of electron doped cuprates R(2-x)CexCuO4 (R = La, Pr, Nd, Sm, and Eu)

Y. Krockenberger, J. Kurian, A. Winkler +3

The superconductivity phase diagrams of electron doped cuprates of the form R(2-x)CexCuO4 (with R= La, Pr, Nd, Sm, and Eu) have been determined for cerium compositions 0 < x < 0.36…