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@ARTICLE{OlmosdeLeon:35853,
      author       = {Olmos de Leon, V. and Wissmann, F. and Achenbach, P. and
                      Ahrens, J. and Arends, H. J. and Beck, R. and Harty, P. D.
                      and Hejny, V. and Jennewein, P. and Kotulla, M. and Krusche,
                      B. and Kuhr, V. and Leukel, R. and MacGeorge, J. C. and
                      Metag, V. and Novotny, R. and Polonski, A. and Rambo, F. and
                      Schmidt, A. and Schumacher, M. and Siodlaczek, U. and
                      Ströher, H. and Thomas, A. and Weiß, J. and Wolf, M.},
      title        = {{L}ow-energy compton scattering and the polarizabilities of
                      the proton},
      journal      = {The European physical journal / A},
      volume       = {10},
      issn         = {1434-6001},
      address      = {Berlin},
      publisher    = {Springer},
      reportid     = {PreJuSER-35853},
      pages        = {207},
      year         = {2001},
      note         = {Record converted from VDB: 12.11.2012},
      abstract     = {Differential cross-sections for Compton scattering from the
                      proton hal e been measured at the MAMI tagged photon
                      facility using the TAPS setup. The data cover an angular
                      range of theta (lab)(gamma) = 59 degrees -155 degrees and
                      photon energies ranging from 55 MeV to 165 MeV. Our results
                      are in good agreement with those from previous experiments,
                      but yield higher precision. Using dispersion relations the
                      proton polarizabilities have been determined to be
                      <(<alpha>)over bar> = [11.9 +/- 0.5(stat.) -/+ 1.3(syst.)
                      +/- 0.3(mod.)] (.) 10(-4) fm(3) and <(<beta>)over bar> =
                      [1.2 +/- 0.7(stat.) +/- 0.3(syst). +/- 0.4(mod.))] (.)
                      10(-4) fm(3). These results confirm the Baldin sum rule
                      which was re-evaluated to be <(<alpha>)over bar> +
                      <(<beta>)over bar> = [13.8 +/- 0.4] 10(-4) fm(3). We can
                      also conclude that there is no significant additional
                      asymptotic contribution to the backward spin polarizability
                      gamma (pi) beyond the t-channel pi (0)-exchange.},
      keywords     = {J (WoSType)},
      cin          = {IKP-2},
      ddc          = {530},
      cid          = {I:(DE-Juel1)VDB24},
      pnm          = {Mittelenergiephysik},
      pid          = {G:(DE-Juel1)FUEK38},
      shelfmark    = {Physics, Nuclear / Physics, Particles $\&$ Fields},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000168527600012},
      url          = {https://juser.fz-juelich.de/record/35853},
}