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@ARTICLE{Buchmuller:419176,
      author       = {Buchmuller, Wilfried and Dierigl, Markus and Tatsuta,
                      Yoshiyuki},
      title        = {{M}agnetized orbifolds and localized flux},
      journal      = {Annals of physics},
      volume       = {401},
      issn         = {0003-4916},
      address      = {Amsterdam [u.a.]},
      publisher    = {Elsevier},
      reportid     = {PUBDB-2019-00958, DESY-18-167. arXiv:1810.06362},
      pages        = {91 - 115},
      year         = {2019},
      note         = {© Elsevier Inc.; Final published version in progress; Post
                      referee fulltext in progress; Embargo 12 months from
                      publication},
      abstract     = {Magnetized orbifolds play an important role in
                      compactifications of string theories and higher-dimensional
                      field theories to four dimensions. Magnetic flux leads to
                      chiral fermions, it can be a source of supersymmetry
                      breaking and it is an important ingredient of moduli
                      stabilization. Flux quantization on orbifolds is subtle due
                      to the orbifold singularities. Generically, Wilson line
                      integrals around these singularities are non-trivial, which
                      can be interpreted as localized flux. As a consequence, flux
                      densities on orbifolds can take the same values as on tori.
                      We determine the transition functions for the flux vector
                      bundle on the orbifold and the related twisted boundary
                      conditions of zero-mode wave functions. We also construct
                      “untwisted” zero-mode functions that are obtained for
                      singular vector fields related to the Green’s function on
                      a torus, and we discuss the connection between zeros of the
                      wave functions and localized flux. Twisted and untwisted
                      zero-mode functions are related by a singular gauge
                      transformation.},
      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},
      UT           = {WOS:000460082400005},
      eprint       = {1810.06362},
      howpublished = {arXiv:1810.06362},
      archivePrefix = {arXiv},
      SLACcitation = {$\%\%CITATION$ = $arXiv:1810.06362;\%\%$},
      doi          = {10.1016/j.aop.2018.12.006},
      url          = {https://bib-pubdb1.desy.de/record/419176},
}