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@PHDTHESIS{Briskin:301960,
      author       = {Briskin, Gennady M.},
      title        = {{D}iffractive {D}issociation in $ep$ {D}eep {I}nelastic
                      {S}cattering},
      school       = {Tel-Aviv University},
      type         = {Dr.},
      reportid     = {PUBDB-2016-03003, DESY-THESIS-1998-036},
      pages        = {152},
      year         = {1998},
      note         = {Tel-Aviv University, Diss., 1998},
      abstract     = {The deep inelastic diffractive cross section, $d
                      \sigma^D_{\gamma* p\to XN}/dM_x$ , has been measured in the
                      mass range $M_x \leq$15 GeV for $\gamma^* p$ center of mass
                      energies 60 < W < 200 GeV and photon virtualities $Q^2$ = 7
                      to 140 $GeV^2$. For fixed $Q^2$ and $M_x$, the diffractive
                      cross section is found to rise rapidly with W.
                      Parameterizing the $W$ dependence by the form
                      $d\sigma^D_{\gamma* \to XN}$/$dM_x \propto (W^2)$
                      $^{2\overline{\alpha_P} -2}$ the data yielded for the
                      i-averaged Pomeron trajectory a value of
                      $\overline{\alpha_P}$ = 1.135 ±
                      0.008(stat)$^{+0.011}_{-0.030}$(syst). This value for the
                      Pomeron trajectory is larger than $\overline{\alpha_P}$
                      extracted from soft interactions. The IV dependence of the
                      diffractive cross section measured in this analysis is found
                      to be the same as that of the total cross section for
                      scattering of virtual photons on protons. From the measured
                      diffractive cross section the diffractive structure function
                      of the proton $F^{d(3)}_2$ $(\beta$,$x_P$, $Q^2$) has been
                      determined. We find the data to be consistent with the
                      assumption that the diffractive structure function
                      $F^{D(3)}_2$ factorizes according to $x_P$
                      $F^{D(3)}_2$($x_P$, $\beta$, $Q^2$) =
                      ($x_0$/$x_P$)$^nF^{P}_2$ ($\beta$,$Q^2$). They are also
                      consistent with QCD based models which incorporate
                      factorization breaking. The rise of $X_P$ $F^{D(3)}_2$ with
                      decreasing $x_P$ and the weak dependence of $F^P_2$ on $Q^2$
                      suggest a substantial contribution from partonic
                      interactions.},
      keywords     = {thesis (INSPIRE)},
      cin          = {L},
      cid          = {I:(DE-H253)L-20120731},
      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)11},
      doi          = {10.3204/PUBDB-2016-03003},
      url          = {https://bib-pubdb1.desy.de/record/301960},
}