001 | 141403 | ||
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037 | _ | _ | |a FZJ-2013-06583 |
082 | _ | _ | |a 530 |
100 | 1 | _ | |a Bali, G. S. |0 P:(DE-HGF)0 |b 0 |
111 | 2 | _ | |a 10th Conference on Quark Confinement and the Hadron Spectrum (Confinement X) |w Germany |c Munich |d 2012-10-08 - 2012-10-12 |g Confinement X |
245 | _ | _ | |a Thermodynamic properties of QCD in external magnetic fields |
260 | _ | _ | |a Trieste |c 2013 |b SISSA |
300 | _ | _ | |a 198 |
336 | 7 | _ | |a Contribution to a conference proceedings |b contrib |m contrib |0 PUB:(DE-HGF)8 |s 1389853530_19613 |2 PUB:(DE-HGF) |
336 | 7 | _ | |a Conference Paper |0 33 |2 EndNote |
336 | 7 | _ | |a CONFERENCE_PAPER |2 ORCID |
336 | 7 | _ | |a Output Types/Conference Paper |2 DataCite |
336 | 7 | _ | |a conferenceObject |2 DRIVER |
336 | 7 | _ | |a INPROCEEDINGS |2 BibTeX |
520 | _ | _ | |a We consider the effect of strong external electromagnetic fields on thermodynamic observables in QCD, through lattice simulations with 1+1+1 flavors of staggered quarks at physical quark masses. Continuum extrapolated results are presented for the light quark condensates and for their tensor polarizations, as functions of the temperature and the magnetic field. We find the light condensates to undergo inverse magnetic catalysis in the transition region, in a manner that the transition temperature decreases with growing magnetic field. We also compare the results to other approaches and lattice simulations. Furthermore, we relate the tensor polarization to the spin part of the magnetic susceptibility of the QCD vacuum, and show that this contribution is diamagnetic. |
536 | _ | _ | |a 411 - Computational Science and Mathematical Methods (POF2-411) |0 G:(DE-HGF)POF2-411 |c POF2-411 |x 0 |f POF II |
588 | _ | _ | |a Dataset connected to arXivarXiv |
700 | 1 | _ | |a Bruckmann, F. |0 P:(DE-HGF)0 |b 1 |
700 | 1 | _ | |a Constantinou, M. |0 P:(DE-HGF)0 |b 2 |
700 | 1 | _ | |a Costa, M. |0 P:(DE-HGF)0 |b 3 |
700 | 1 | _ | |a Endrodi, G. |0 P:(DE-HGF)0 |b 4 |
700 | 1 | _ | |a Fodor, Z. |0 P:(DE-HGF)0 |b 5 |
700 | 1 | _ | |a Katz, S. D. |0 P:(DE-HGF)0 |b 6 |
700 | 1 | _ | |a Krieg, S. |0 P:(DE-Juel1)132171 |b 7 |
700 | 1 | _ | |a Panagopoulos, H. |0 P:(DE-HGF)0 |b 8 |
700 | 1 | _ | |a Schafer, A. |0 P:(DE-HGF)0 |b 9 |
700 | 1 | _ | |a Szabo, K. K. |0 P:(DE-HGF)0 |b 10 |
773 | _ | _ | |0 PERI:(DE-600)2642026-0 |x 1824-8039 |t Proceedings of Science |p 197 |v Confinement X |
856 | 4 | _ | |u http://pos.sissa.it/archive/conferences/171/197/Confinement%20X_197.pdf |
909 | _ | _ | |p VDB |o oai:juser.fz-juelich.de:141403 |
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910 | 1 | _ | |a Forschungszentrum Jülich GmbH |0 I:(DE-588b)5008462-8 |k FZJ |b 7 |6 P:(DE-Juel1)132171 |
913 | 2 | _ | |a DE-HGF |b Key Technologies |l Supercomputing & Big Data |1 G:(DE-HGF)POF3-510 |0 G:(DE-HGF)POF3-511 |2 G:(DE-HGF)POF3-500 |v Computational Science and Mathematical Methods |x 0 |
913 | 1 | _ | |a DE-HGF |b Schlüsseltechnologien |l Supercomputing |1 G:(DE-HGF)POF2-410 |0 G:(DE-HGF)POF2-411 |2 G:(DE-HGF)POF2-400 |v Computational Science and Mathematical Methods |x 0 |4 G:(DE-HGF)POF |3 G:(DE-HGF)POF2 |
914 | 1 | _ | |y 2013 |
915 | _ | _ | |a Peer Review unknown |0 StatID:(DE-HGF)0040 |2 StatID |
920 | _ | _ | |l yes |
920 | 1 | _ | |0 I:(DE-Juel1)JSC-20090406 |k JSC |l Jülich Supercomputing Center |x 0 |
980 | _ | _ | |a contrib |
980 | _ | _ | |a VDB |
980 | _ | _ | |a UNRESTRICTED |
980 | _ | _ | |a I:(DE-Juel1)JSC-20090406 |
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