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@ARTICLE{Horsley:297562,
      author       = {Horsley, R. and Nakamura, Y. and Perlt, H. and Pleiter, D.
                      and Rakow, P. E. L. and Schierholz, G. and Schiller, A. and
                      Stokes, R. and Stüben, H. and Young, R. D. and Zanotti, J.
                      M.},
      title        = {{QED} effects in the pseudoscalar meson sector},
      journal      = {Journal of high energy physics},
      volume       = {2016},
      number       = {4},
      issn         = {1029-8479},
      address      = {Berlin},
      publisher    = {Springer},
      reportid     = {PUBDB-2016-01915, DESY-15-158. ADP-15-30-T932.
                      EDINBURGH-2015-20. LIVERPOOL-LTH-1055. arXiv:1509.00799},
      pages        = {93},
      year         = {2016},
      abstract     = {In this paper we present results on the pseudoscalar meson
                      masses from a fully dynamical simulation of QCD+QED,
                      concentrating particularly on violations of isospin
                      symmetry. We calculate the π +-π 0 splitting and also look
                      at other isospin violating mass differences. We have
                      presented results for these isospin splittings in [1]. In
                      this paper we give more details of the techniques employed,
                      discussing in particular the question of how much of the
                      symmetry violation is due to QCD, arising from the different
                      masses of the u and d quarks, and how much is due to QED,
                      arising from the different charges of the quarks. This
                      decomposition is not unique, it depends on the
                      renormalisation scheme and scale. We suggest a
                      renormalisation scheme in which Dashen’s theorem for
                      neutral mesons holds, so that the electromagnetic
                      self-energies of the neutral mesons are zero, and discuss
                      how the self-energies change when we transform to a scheme
                      such as M S, in which Dashen’s theorem for neutral mesons
                      is violated.},
      cin          = {T},
      ddc          = {530},
      cid          = {I:(DE-H253)T-20120731},
      pnm          = {611 - Fundamental Particles and Forces (POF3-611)},
      pid          = {G:(DE-HGF)POF3-611},
      experiment   = {EXP:(DE-MLZ)NOSPEC-20140101},
      typ          = {PUB:(DE-HGF)16},
      eprint       = {1509.00799},
      howpublished = {arXiv:1509.00799},
      archivePrefix = {arXiv},
      SLACcitation = {$\%\%CITATION$ = $arXiv:1509.00799;\%\%$},
      UT           = {WOS:000374340400004},
      doi          = {10.1007/JHEP04(2016)093},
      url          = {https://bib-pubdb1.desy.de/record/297562},
}