% IMPORTANT: The following is UTF-8 encoded.  This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.

@ARTICLE{Borsnyi:201101,
      author       = {Borsányi, Szabolcs and Fodor, Zoltán and Hoelbling,
                      Christian and Katz, Sándor D. and Krieg, Stefan and Ratti,
                      Claudia and Szabó, Kálmán K.},
      title        = {{I}s there still any {T} c mystery in lattice {QCD}?
                      {R}esults with physical masses in the continuum limit {III}},
      journal      = {Journal of high energy physics},
      volume       = {2010},
      number       = {9},
      issn         = {1029-8479},
      address      = {Berlin},
      publisher    = {Springer},
      reportid     = {FZJ-2015-03406},
      pages        = {73},
      year         = {2010},
      abstract     = {The present paper concludes our investigations on the QCD
                      cross-over transition temperatures with 2+1 staggered
                      flavours and one-link stout improvement. We extend our
                      previous two studies [Phys. Lett. B643 (2006) 46, JHEP
                      0906:088 (2009)] by choosing even finer lattices (N t = 16)
                      and we work again with physical quark masses. The new
                      results on this broad cross-over are in complete agreement
                      with our earlier ones. We compare our findings with the
                      published results of the hotQCD collaboration. All these
                      results are confronted with the predictions of the Hadron
                      Resonance Gas model and Chiral Perturbation Theory for
                      temperatures below the transition region. Our results can be
                      reproduced by using the physical spectrum in these analytic
                      calculations. The findings of the hotQCD collaboration can
                      be recovered by using a distorted spectrum which takes into
                      account lattice discretization artifacts and heavier than
                      physical quark masses. This analysis provides a simple
                      explanation for the observed discrepancy in the transition
                      temperatures between our and the hotQCD collaborations.},
      cin          = {JSC},
      ddc          = {530},
      cid          = {I:(DE-Juel1)JSC-20090406},
      pnm          = {411 - Computational Science and Mathematical Methods
                      (POF2-411)},
      pid          = {G:(DE-HGF)POF2-411},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000282371300042},
      doi          = {10.1007/JHEP09(2010)073},
      url          = {https://juser.fz-juelich.de/record/201101},
}