Measurement of the Diffractive Cross Section in Deep Inelastic Scattering
arXiv:hep-ex/9602010 · doi:10.1007/s002880050118
Abstract
Diffractive scattering of , where is either a proton or a nucleonic system with ~GeV has been measured in deep inelastic scattering (DIS) at HERA. The cross section was determined by a novel method as a function of the c.m. energy between 60 and 245~GeV and of the mass of the system up to 15~GeV at average values of 14 and 31~GeV. The diffractive cross section is, within errors, found to rise linearly with . Parameterizing the dependence by the form $dσ^{diff}/dM_X \propto (W^2)^{(2\overline{\mbox{$α_{_{I\hspace{-0.2em}P}}$}} -2)}$ the DIS data yield for the pomeron trajectory $\overline{\mbox{$α_{_{I\hspace{-0.2em}P}}$}} = 1.23 \pm 0.02(stat) \pm 0.04 (syst)$ averaged over in the measured kinematic range assuming the longitudinal photon contribution to be zero. This value for the pomeron trajectory is substantially larger than $\overline{\mbox{$α_{_{I\hspace{-0.2em}P}}$}}$ extracted from soft interactions. The value of $\overline{\mbox{$α_{_{I\hspace{-0.2em}P}}$}}$ measured in this analysis suggests that a substantial part of the diffractive DIS cross section originates from processes which can be described by perturbative QCD. From the measured diffractive cross sections the diffractive structure function of the proton $F^{D(3)}_2(β,Q^2, \mbox{$x_{_{I\hspace{-0.2em}P}}$})$ has been determined, where is the momentum fraction of the struck quark in the pomeron. The form $F^{D(3)}_2 = constant \cdot (1/ \mbox{$x_{_{I\hspace{-0.2em}P}}$})^a$ gives a good fit to the data in all and intervals with $a = 1.46 \pm 0.04 (stat) \pm
45 pages, including 16 figures
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