Leading neutron production in $e^{+}p$ collisions at HERA

Abstract

The production of neutrons carrying at least 20% of the proton beam energy ($\xl > 0.2$) in $e^{+}p$ collisions has been studied with the ZEUS detector at HERA for a wide range of $Q^2$, the photon virtuality, from photoproduction to deep inelastic scattering. The neutron-tagged cross section, $ep\to e^{\prime }Xn$, is measured relative to the inclusive cross section, $ep\to e^{\prime }X$, thereby reducing the systematic uncertainties. For $\xl >$ 0.3, the rate of neutrons in photoproduction is about half of that measured in hadroproduction, which constitutes a clear breaking of factorisation. There is about a 20% rise in the neutron rate between photoproduction and deep inelastic scattering, which may be attributed to absorptive rescattering in the ${\hat{I}}^{3}p$ system. For $0.64 < \xl < 0.82$, the rate of neutrons is almost independent of the Bjorken scaling variable $x$ and $Q^2$. However, at lower and higher $\xl$ values, there is a clear but weak dependence on these variables, thus demonstrating the breaking of limiting fragmentation. The neutron-tagged structure function, ${{F}^{\rm\tiny LN(3)}_2}(x,Q^2,\xl)$, rises at low values of $x$ in a way similar to that of the inclusive \ff of the proton. The total ${\hat{I}}^3\ddot{I}€$ cross section and the structure function of the pion, $F^{\ddot{I}}{€}_2(x_{\ddot{I}}€,Q^2)$ where $x_π= x/(1-\xl)$, have been determined using a one-pion-exchange model, up to uncertainties in the normalisation due to the poorly understood pion flux. At fixed $Q^2$, $F^{\ddot{I}}{€}_2$ has approximately the same $x$ dependence as $F_2$ of the proton.

61 pages, 19 figures