% 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”.

@ARTICLE{Ye:137994,
      author       = {Ye, Q. J. and Hartmann, M. and Chiladze, D. and Dymov, S.
                      and Dzyuba, A. and Gao, H. and Gebel, R. and Hejny, V. and
                      Kacharava, A. and Lorentz, B. and Mchedlishvili, D. and
                      Merzliakov, S. and Mielke, M. and Mikirtytchiants, S. and
                      Ohm, H. and Papenbrock, M. and Polyanskiy, A. and Serdyuk,
                      V. and Stein, H. J. and Trusov, S. and Valdau, Yu. and
                      Wilkin, C. and Wüstner, P. and Stroeher, Hans},
      title        = {{P}roduction of ${K}^{+}{K}^{−}$ pairs in proton-proton
                      collisions below the ϕ meson threshold},
      journal      = {Physical review / C},
      volume       = {87},
      number       = {6},
      issn         = {0556-2813},
      address      = {Woodbury, NY},
      publisher    = {Inst.},
      reportid     = {FZJ-2013-04279},
      pages        = {065203},
      year         = {2013},
      note         = {*Brief entry*},
      abstract     = {The pp -> ppK+K- reaction was measured below the phi
                      threshold at a beam energy of 2.568 GeV using the COSY-ANKE
                      magnetic spectrometer. By assuming that the four-body phase
                      space is distorted only by the product of two-body final
                      state interactions, fits to a variety of one-dimensional
                      distributions permit the evaluation of differential and
                      total cross sections. The shapes of the distributions in the
                      Kp and Kpp invariant masses are reproduced only if the K-p
                      interaction is even stronger than that found at higher
                      energy. The cusp effect in the K+K- distribution at the
                      K0K0bar threshold is much more clear and some evidence is
                      also found for coupling between the K-p and K0bar n
                      channels. However, the energy dependence of the total cross
                      section cannot be reproduced by considering only a simple
                      product of such pair-wise final state interactions.},
      keywords     = {channel cross section: energy dependence (INSPIRE) / K- p:
                      scattering length (INSPIRE) / K: pair production (INSPIRE) /
                      threshold (INSPIRE) / p p: exclusive reaction (INSPIRE) /
                      final-state interaction (INSPIRE) / cusp effect (INSPIRE) /
                      ANKE (INSPIRE) / K+ K-: mass spectrum (INSPIRE) / mass
                      spectrum: (2p K-) (INSPIRE) / Lambda(1405) (INSPIRE) /
                      Juelich COSY PS (INSPIRE) / experimental results (INSPIRE) /
                      p p --> 2p K+ K- (INSPIRE) / 2.568 GeV-kin (INSPIRE)},
      cin          = {IKP-2 / IKP-4 / ZEA-2},
      ddc          = {530},
      cid          = {I:(DE-Juel1)IKP-2-20111104 / I:(DE-Juel1)IKP-4-20111104 /
                      I:(DE-Juel1)ZEA-2-20090406},
      pnm          = {531 - Hadron Structure and Dynamics (HSD) (POF2-531) / 53G
                      - COSY (POF2-53G32)},
      pid          = {G:(DE-HGF)POF2-531 / G:(DE-HGF)POF2-53G32},
      typ          = {PUB:(DE-HGF)16},
      eprint       = {1302.7210},
      howpublished = {arXiv:1302.7210},
      archivePrefix = {arXiv},
      SLACcitation = {$\%\%CITATION$ = $arXiv:1302.7210;\%\%$},
      UT           = {WOS:000320279400002},
      doi          = {10.1103/PhysRevC.87.065203},
      url          = {https://juser.fz-juelich.de/record/137994},
}