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@ARTICLE{Knie:192588,
      author       = {Knie, A. and Ilchen, M. and Schmidt, Ph. and Reiß, Ph. and
                      Ozga, C. and Kambs, B. and Hans, A. and Müglich, N. and
                      Galitskiy, S. A. and Glaser, L. and Walter, P. and Viefhaus,
                      J. and Ehresmann, A. and Demekhin, Ph. V.},
      title        = {{A}ngle-resolved study of resonant {A}uger decay and
                      fluorescence emission processes after core excitations of
                      the terminal and central nitrogen atoms in
                      ${\mathrm{{N}}}_{2}\mathrm{{O}}$},
      journal      = {Physical review / A},
      volume       = {90},
      number       = {1},
      issn         = {1050-2947},
      address      = {College Park, Md.},
      publisher    = {APS},
      reportid     = {PUBDB-2014-04170},
      pages        = {013416},
      year         = {2014},
      abstract     = {Angular distributions of the N2O+(X) and N2O+(A)
                      photoelectrons were measured as functions of the
                      exciting-photon energy with small bandwidth in the vicinity
                      of the resonant Nt(1s→π∗), Nt(1s→σ∗), and
                      Nc(1s→π∗) core excitations of N2O. For selected
                      exciting-photon energies in this range, angular distribution
                      parameters of the N2O+(A→X) fluorescence were also
                      determined. These data are interpreted by ab initio
                      calculations. Long-range exciting-photon energy dependencies
                      of the photoelectron angular distribution parameters
                      βeX(ω) and βeA(ω), recorded vibrationally unresolved,
                      are attributed to an electronic state interference between
                      the direct and the different resonant amplitudes for the
                      population of the final ionic states. In addition to that,
                      strong influence of lifetime vibrational interference is
                      identified in the observed dispersion of the vibrationally
                      resolved fluorescence angular distribution parameter
                      β2XA(ω) across the electronic resonances.},
      cin          = {DOOR / FS-PE / Eur.XFEL / FS-SCS},
      ddc          = {530},
      cid          = {I:(DE-H253)HAS-User-20120731 / I:(DE-H253)FS-PE-20120731 /
                      $I:(DE-H253)Eur_XFEL-20120731$ / I:(DE-H253)FS-SCS-20131031},
      pnm          = {DORIS Beamline BW3 (POF2-54G13)},
      pid          = {G:(DE-H253)POF2-BW3-20130405},
      experiment   = {EXP:(DE-H253)D-BW3-20150101},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000339093200007},
      doi          = {10.1103/PhysRevA.90.013416},
      url          = {https://bib-pubdb1.desy.de/record/192588},
}