Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data

Collaboration
Jul, 1998
46 pages
Published in:
  • Eur.Phys.J.C 6 (1999) 43-66
e-Print:
Report number:
  • DESY-98-084,
  • ANL-HEP-PR-98-98
Experiments:

Citations per year

19982005201220192025010203040
Abstract:
The DIS diffractive cross section, dσγpXNdiff/dMXd\sigma^{diff}_{\gamma^* p \to XN}/dM_X, has been measured in the mass range MX<15M_X < 15 GeV for γp\gamma^*p c.m. energies 60<W<20060 < W < 200 GeV and photon virtualities Q2=7Q^2 = 7 to 140 GeV2^2. For fixed Q2Q^2 and MXM_X, the diffractive cross section rises rapidly with WW, dσγpXNdiff(MX,W,Q2)/dMXWadiffd\sigma^{diff}_{\gamma^*p \to XN}(M_X,W,Q^2)/dM_X \propto W^{a^{diff}} with adiff=0.507±0.034(stat)0.046+0.155(syst)a^{diff} = 0.507 \pm 0.034 (stat)^{+0.155}_{-0.046}(syst) corresponding to a tt-averaged pomeron trajectory of \bar{\alphapom} = 1.127 \pm 0.009 (stat)^{+0.039}_{-0.012} (syst) which is larger than \bar{\alphapom} observed in hadron-hadron scattering. The WW dependence of the diffractive cross section is found to be the same as that of the total cross section for scattering of virtual photons on protons. The data are consistent with the assumption that the diffractive structure function F2D(3)F^{D(3)}_2 factorizes according to \xpom F^{D(3)}_2 (\xpom,\beta,Q^2) = (x_0/ \xpom)^n F^{D(2)}_2(\beta,Q^2). They are also consistent with QCD based models which incorporate factorization breaking. The rise of \xpom F^{D(3)}_2 with decreasing \xpom and the weak dependence of F2D(2)F^{D(2)}_2 on Q2Q^2 suggest a substantial contribution from partonic interactions.
Note:
  • 46 pages including 14 figures Report-no: DESY 98-084
  • positron p: colliding beams
  • positron p: deep inelastic scattering
  • photon: diffraction
  • exchange: pomeron
  • p: diffraction
  • diffraction: structure function
  • cross section: energy dependence
  • cross section: mass
  • momentum transfer dependence
  • ZEUS
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