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slac-pub-2605 - SLAC - Stanford University

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-43-<br />

(8) Some of the most important tests of QCD involve real photons. In<br />

contrast to vector-meson dominance ideas , point-like interactions are predicted<br />

to dominate the hadronic interactions of on-shell photons in large momenta<br />

transfer reactions C511. This feature is particularly clear in the QCD<br />

predictions for the two-photon inclusive [52] and exclusive processes [5]<br />

yy + jet+jet and yy + 6, and the photon structure function at large momentum<br />

transfer. Higher twist terms should be relatively less important in photon<br />

reactions compared to hadron reactions.<br />

(9) The generation of hadron multiplicity is not completely understood<br />

in QCD. However a number of features are anticipated which appear to differ<br />

strongly from parton model expectations: For example, in QCD (a) the final<br />

state multiplicity reflects the color separation set up in the collision [53];<br />

this is believed to even hold in low pT hadron collisions since the basic<br />

interactions involve color exchange; (b) the evolution in space-time corres-<br />

ponds to an inside-outside cascade -- the slowest hadrons are created first;<br />

(c) the final state multiplicity in the Drell-Yan process AB -+ !LzX is expected<br />

to reflect the creation of 3c and 3: spectator systems at the moment of<br />

annihilation C531; and (d) the multiplicity of gluon jets and other color<br />

octet systems should reflect its higher color charge relative to color triplet<br />

systems C531. It is clear that QCD provides a novel perspective for multi-<br />

particle phenomena.<br />

(10) Another critical testing ground of QCD dynamics is the study of<br />

quark and gluon interactions in nuclear targets c551. For example, consider<br />

the Drell-Yan process pU + u+u-X. If the factorization theorem for inclusive<br />

reactions is correct the cross section at large pair mass Q is given by the<br />

convolution of the anti-proton structure function G- -(x ,Q) with the nuclear<br />

qlp a<br />

distribution function G q/U%‘Q) -- which for large Q2 is -AGqjN$ ,Q) .<br />

Thus the factorization theorem predicts no absorption of the constituents<br />

of the anti-proton despite the fact that the F suffers repeated inelastic<br />

collisions in its passage through the nuclear volume! If this is really

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