Vector Meson Production

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    Elastic vector meson production from ep collisions involve the exchange of a colour singlet object which is emitted by the proton. Of special interest are processes with a hard scale such as

    the mass MV of a heavy vector meson, 

    the virtuality Q2 of the photon in a deep inelastic scattering process, or 

    the squared four-momentum transfer t of the colour singlet exchange.

    Such processes allow perturbative QCD calculations to be compared with the measurements and therefore give new information on colour singlet exchange as well as on the proton and the vector meson. 
The figure shows a compilation of the measurements of the total photoproduction cross section sigmagamma-p and elastic vector meson cross sections sigmagamma-pV up to the production of Upsilon as a function of the photon--proton center-of-mass energy W=root(sgamma-p). 
    The measured total cross section is at large center-of-mass energies compatible with a slowly rising distribution as 

    sigmagamma-p ~ sepsilon

    with epsilon ~ 0.095+- 0.002. The optical theorem relates the total cross section to the imaginary part of the amplitude of forward elastic scattering. Therefore, elastic vector meson cross sections should rise with approximately twice the power:

    sigmagamma-pV ~ s2epsilon.

    Photoproduction of light vector mesons (rho, omega, phi) show an increase in the production that is compatible with this prediction. However, photoproduction of the heavy J/psi mesons exhibit a stronger dependence on the center-of-mass energy with epsilon ~ 0.2. In the following results from processes involving a hard scale as defined above, are shown.  

Rho Meson

The figure shows the measurement of the rho meson production cross section as a function of Q2. In contrast to the parton density of virtual photons, the rho cross section falls steeply which implies that the time to develop a hadronic bound state from the quark-antiquark pair of the photon diminishes as Q2 increases.  
    At fixed Q2, the energy dependence of the rho cross section has been measured:  
In the figure the measured energy dependence of sigmagamma-pV was expressed in terms of the intercept parameter alpha(0). The scale was here chosen to be the photon virtuality Q2. The intercept is found to increase with increasing scale. 
    A similar energy dependence is observed in this vector meson production and in the inclusive deep inelastic scattering processes . This is suggestive of sensitivity of the vector meson data to the gluon distribution of the proton.

    For a discussion of the t distribution see below.  

J/Psi Meson

The figure shows the J/psi production cross section as a function of the photon--proton center-of-mass energy W= root(sgamma*p). 
    The measurements can be described by perturbative QCD calculations which use existing parameterizations of the gluon distributions in the proton. The calculations use the square of the gluon density to account for the colour neutrality of the exchanged object. Therefore, the comparisons of the data with the calculations give a highly sensitive measure of the gluons in the proton. A further component of the calculations is the mechanism for formation of the vector meson such that the comparisons to the data give new information also on this part of the process. 

t distribution

    The t distribution at small momentum transfer from the proton gives a measure of the size of the interaction region which is quantified by exponential fits to the data:

    exp( - b t )  
In the figure, the fitted b parameters is shown for rho meson production. The scale was chosen to be the photon virtuality Q2.  
    With increasing scale, the data tend to approach a value of b ~ 4 GeV-2 which corresponds to the size of the proton. The size of the quark-antiquark state is therefore small compared to that of the proton and probes the proton at small distances. Note that the b parameter measured for the photoproduction of J/psi mesons is already at b ~ 4 GeV-2 and indicates the small size of the charm-anticharm object in the interaction with the proton. 
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last updated by H1 webmaster on 19/05/98