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@ARTICLE{Brandelik:321196,
      author       = {Brandelik, R. and Braunschweig, W. and Martyn, H.-U. and
                      Sander, H. G. and Schmitz, D. and Sturm, W. and Wallraff, W.
                      and Cords, D. and Felst, R. and Fries, R. and Gadermann, E.
                      and Hultschig, H. and Joos, P. and Koch, W. and Kötz, U.
                      and Krehbiel, H. and Kreinick, D. and Lynch, H. L. and
                      McNeely, W. A. and Moffeit, K. C. and Notz, D. and Rüsch,
                      R. and Schliwa, M. and Wilk, B. H. and Wolf, G. and
                      Grindhammer, G. and Ludwig, J. and Mess, K. H. and Petersen,
                      A. and Poelz, G. and Ringel, J. and Römer, O. and
                      Sauerberg, K. and Schmüser, P. and De Boer, W. and
                      Buschhorn, G. and Fues, W. and Von Gagern, Ch. and
                      Gunderson, B. and Kotthaus, R. and Lierl, H. and Oberlack,
                      H. and Orito, S. and Suda, T. and Totsuka, Y. and Yamada,
                      S.},
      collaboration = {{DASP Collaboration}},
      title        = {{O}n the origin of inclusive electron events in
                      $e^+$$e^−$ annihilation between 3.6 and 5.2 {G}$e{V}$},
      journal      = {Physics letters / B},
      volume       = {70},
      number       = {1},
      issn         = {0370-2693},
      address      = {Amsterdam},
      publisher    = {North-Holland Publ.},
      reportid     = {PUBDB-2017-02466, DESY-77-036},
      pages        = {125 - 131},
      year         = {1977},
      abstract     = {The multiplicity distribution of inclusive electron events
                      above 4 GeV cm energy shows two distinct classes of events:
                      two prong no photon and high multiplicity events. If the
                      high multiplicity events are attributed to the semi-leptonic
                      decay of charmed particles the two prong no photon events
                      must come from the weak decay of a different type of
                      particle. The charged K to π ratio was measured for these
                      events. The average number of charged kaons is 0.07 ± 0.06
                      per two prong event and 0.90 ± 0.18 per multiprong event.
                      Thus the weak current responsible for the low multiplicity
                      events has a small coupling to strange particles.},
      cin          = {DESY(-2012)},
      ddc          = {530},
      cid          = {$I:(DE-H253)DESY_-2012_-20170516$},
      pnm          = {899 - ohne Topic (POF3-899)},
      pid          = {G:(DE-HGF)POF3-899},
      experiment   = {EXP:(DE-MLZ)NOSPEC-20140101},
      typ          = {PUB:(DE-HGF)29 / PUB:(DE-HGF)16},
      UT           = {WOS:A1977DV04400032},
      doi          = {10.1016/0370-2693(77)90360-4},
      url          = {https://bib-pubdb1.desy.de/record/321196},
}