% 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”.

@INBOOK{Mller:902433,
      author       = {Müller, David},
      title        = {{D}ata {C}ollection {S}trategies, {A}nalysis, and
                      {I}nterpretation in {AP}-{XAS}},
      address      = {Washington, DC},
      publisher    = {ACS Publications},
      reportid     = {FZJ-2021-04255},
      isbn         = {9780841298125},
      pages        = {315-331},
      year         = {2021},
      comment      = {Ambient Pressure Spectroscopy in Complex Chemical
                      Environments},
      booktitle     = {Ambient Pressure Spectroscopy in
                       Complex Chemical Environments},
      abstract     = {This chapter will focus on strategies to collect meaningful
                      X-ray absorption data in an ambient medium covering both the
                      hard and soft X-ray regime and how to guide analysis,
                      keeping experimental and physical differences of various
                      strategies in mind. A special interest will be put on how
                      the interaction of primary radiation and signal carriers
                      with the surrounding medium will influence data acquisition
                      and interpretation. Since hard and soft X-rays can be used
                      to probe different electron shells in a material, both
                      experiments can yield important and complementary
                      information. Dipole selection rules lead to vastly different
                      behavior of K- and L-edge XAS of transition metals, for
                      example. In their ambient pressure variants, two major
                      issues (that are fundamentally intertwined) arise when
                      interpreting the data collected from both techniques:
                      Whereas hard X-rays can penetrate condensed matter on a
                      macroscopic scale making true transmission experiments
                      possible, soft X-rays are confined to either electron or
                      fluorescence yield detection modes, the latter suffering
                      from low yields from lighter elements. Those not only pose
                      different experimental challenges to avoid signal loss due
                      to absorption in the reaction medium, but also probe depths
                      of different orders of magnitude.},
      cin          = {PGI-6 / PGI-7},
      cid          = {I:(DE-Juel1)PGI-6-20110106 / I:(DE-Juel1)PGI-7-20110106},
      pnm          = {632 - Materials – Quantum, Complex and Functional
                      Materials (POF4-632)},
      pid          = {G:(DE-HGF)POF4-632},
      typ          = {PUB:(DE-HGF)7},
      url          = {https://juser.fz-juelich.de/record/902433},
}