7 research outputs found
Nonperturbative and perturbative aspects of photo- and electroproduction of vector mesons
We discuss various aspects of vector meson production, first analysing the
interplay between perturbative and nonperturbative aspects of the QCD
calculation. Using a general method adapted to incorporate both perturbative
and nonpertubative aspects, we show that nonperturbative effects are important
for all experimentally available values of the photon virtuality Q2. We compare
the huge amount of experimental information now available with our theoretical
results obtained using a specific nonperturbative model without free
parameters, showing that quite simple features are able to explain the data.Comment: 19 page
The XMM-Newton Serendipitous Survey: I - The role of XMM-Newton Survey Science Centre
This paper describes the performance of XMM-Newton for serendipitous surveys and summarises the scope and potential of the XMM-Newton Serendipitous Survey. The role of the Survey Science Centre (SSC) in the XMM-Newton project is outlined. The SSC's follow-up and identification programme for the XMM-Newton serendipitous survey is described together with the presentation of some of the first results
Muoproduction of J / psi and the gluon distribution of the nucleon
Ashman J, Badelek B, Baum G, et al. Muoproduction of J/Psi and the gluon distribution of the nucleon. Z.Phys. C. 1992;56(1):21-28
Elastic and Proton-Dissociative Photoproduction of Mesons at HERA
Cross sections for elastic and proton-dissociative photoproduction of J/Ï mesons are measured with the H1 detector in positron-proton collisions at HERA. The data were collected at ep centre-of-mass energies sââ318 GeV and sââ225 GeV , corresponding to integrated luminosities of L=130 pbâ1 and L=10.8 pbâ1 , respectively. The cross sections are measured as a function of the photon-proton centre-of-mass energy in the range 25<W Îłp <110 GeV. Differential cross sections dÏ/dt, where t is the squared four-momentum transfer at the proton vertex, are measured in the range |t|<1.2 GeV2 for the elastic process and |t|<8 GeV2 for proton dissociation. The results are compared to other measurements. The W Îłp and t-dependences are parametrised using phenomenological fits