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@ARTICLE{Hartmann:147324,
      author       = {G. Hartmann$^*$ and F. Hensley and R.-P. Kapsch and B.
                      Poppe and O. Sauer and J. Würfel and K. Zink},
      title        = {[{D}etector {B}ased {D}etermination of {W}ater {A}bsorbed
                      {D}ose {A}ccording to {DIN} 6800 {T}eil 1: {S}uggestion for
                      an {E}xtension of the {F}undamental {F}ormalism].},
      journal      = {Zeitschrift für medizinische Physik},
      volume       = {30},
      number       = {1},
      issn         = {0939-3889},
      address      = {Amsterdam},
      publisher    = {Elsevier, Urban $\&$ Fischer45882},
      reportid     = {DKFZ-2019-02445},
      pages        = {24-39},
      year         = {2020},
      note         = {2020 Feb;30(1):24-39#EA:E040#},
      abstract     = {For any detector to be used for the determination of
                      absorbed dose at the point of measurement in water a basic
                      equation is required to convert the reading of the detector
                      into absorbed dose in water. The German DIN 6800 part 1
                      provides a general formalism for that. A further
                      differentiated formalism applicable to photon dosimetry is
                      suggested in this work. This modified formalism presents the
                      two following still general and at the same time fundamental
                      properties of any dosimetry detector: a) a clear distinction
                      of correction factors with respect to the physical processes
                      involved during the measurement, and b) the fact that the
                      process of energy absorption in the detector is determined
                      by the spectral distribution of the fluence of the secondary
                      charged particles. It is concluded that based on the
                      modified formalism and knowing this spectral distribution
                      within the detector a general method is available with
                      benefits for ionization chambers as well as for any other
                      dosimetry detector and which is applicable at reference as
                      well as non-reference conditions without any preconditions.},
      cin          = {E040},
      ddc          = {610},
      cid          = {I:(DE-He78)E040-20160331},
      pnm          = {315 - Imaging and radiooncology (POF3-315)},
      pid          = {G:(DE-HGF)POF3-315},
      typ          = {PUB:(DE-HGF)16},
      pubmed       = {pmid:31585786},
      doi          = {10.1016/j.zemedi.2019.05.001},
      url          = {https://inrepo02.dkfz.de/record/147324},
}