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@ARTICLE{Stephan:20163,
      author       = {Stephan, E. and Kistryn, S. and Kalantar-Nayestanaki, N.
                      and Biegun, A. and Bodek, K. and Ciepal, I. and Deltuva, A.
                      and Eslami-Kalantari, M. and Fonseca, A. C. and Gasparic, I.
                      and Golak, J. and Jamroz, B. and Joulaeizadeh, L. and
                      Kamada, H. and Kis, M. and Klos, B. and Kozela, A. and
                      Mahjour-Shafiei, M. and Mardanpour, H. and Messchendorp, J.
                      and Micherdzinska, A. and Moeini, H. and Nogga, A. and
                      Ramazani-Moghaddam-Arani, A. and Skibinski, R. and Sworst,
                      R. and Witala, H. and Zejma, J.},
      title        = {{V}ector and {T}ensor {A}nalyzing {P}owers in
                      {D}euteron-{P}roton {B}reakup},
      journal      = {Journal of physics / Conference Series},
      volume       = {295},
      issn         = {1742-6588},
      address      = {Bristol},
      publisher    = {IOP Publ.},
      reportid     = {PreJuSER-20163},
      pages        = {012119},
      year         = {2011},
      note         = {Record converted from VDB: 12.11.2012},
      abstract     = {Vector and tensor analyzing powers of the breakup reaction
                      at 130 and 100 MeV deuteron beam energies have been measured
                      at KVI Groningen with the use of the detection systems
                      covering large fractions of the phase space. The high
                      precision data are compared to the theoretical predictions
                      based on various approaches to describe the three nucleon
                      (3N) system dynamics. Theoretical predictions describe very
                      well the vector analyzing power data, with no need to
                      include any three-nucleon force effects fo r these
                      observables. The tensor analyzing powers can be also very
                      well reproduced by calculations in most of the studied
                      region, but locally certain discrepancies are observed. At
                      130 MeV for Axy such discrepancies usually appear, or are
                      enhanced, when mo del 3N forces (3NFs), TM99 or Urbana IX,
                      are included. Problems of all theoretical approaches with
                      describing Axx and Ayy are limited to very small regions of
                      the phase space, usually characterized with the lowest
                      relative energies of the two protons. Pre dicted effects of
                      3NFs are much lower at 100 MeV, therefore at this energy
                      equally good consistency between the data and the
                      calculations is obtained with or without 3NFs.},
      cin          = {IKP-3},
      ddc          = {530},
      cid          = {I:(DE-Juel1)IKP-3-20111104},
      pnm          = {Physik der Hadronen und Kerne},
      pid          = {G:(DE-Juel1)FUEK413},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000297031400044},
      doi          = {10.1088/1742-6596/295/1/012119},
      url          = {https://juser.fz-juelich.de/record/20163},
}