Abstract
Diffractive scattering involves exchange of a pomeron to make a rapidity gap. It is normally assumed that to get a hard scattering in diffraction, one may treat the pomeron as an ordinary particle, which has distributions of gluons and quarks. We show that this is not so: When we use perturbative QCD, there is a breakdown of the factorization theorem. The whole pomeron can initiate the hard scattering, even though it is not point-like. Qualitatively, but not quantitatively, this gives the same effect as a delta-function term in the gluon density in a pomeron.
| Original language | English (US) |
|---|---|
| Pages (from-to) | 161-168 |
| Number of pages | 8 |
| Journal | Physics Letters B |
| Volume | 307 |
| Issue number | 1-2 |
| DOIs | |
| State | Published - Jun 10 1993 |
All Science Journal Classification (ASJC) codes
- Nuclear and High Energy Physics
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