Abstract

Factorization of short- and long-distance interactions is severely broken in hard diffractive hadronic collisions. Interaction with the spectator partons leads to an interplay between soft and hard scales, which results in a leading twist behavior of the cross section, on the contrary to the higher twist predicted by factorization. This feature is explicitly demonstrated for diffractive radiation of abelian (Drell-Yan, gauge bosons, Higgs) and non-abelian (heavy flavors) particles.

Highlights

  • QCD factorization in inclusive processes is nowadays one of the most powerful and frequently used theoretical tools [1]

  • In the dipole representation hard diffraction of a hadron comes from the difference between elastic amplitudes of hadronic states with and without a hard fluctuation, Ahdi f f ∝ σqq(R + r) − σqq(R) ∝ rR ∼ 1/Q, (1)

  • The leading twist behavior 1/m2Q of the diffractive cross section is confirmed by CDF data, as is demonstrated in Fig. 6, right panel

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Summary

QCD factorization in diffraction

QCD factorization in inclusive processes is nowadays one of the most powerful and frequently used theoretical tools [1]. Were known, one could predict any hard diffractive hadronic reaction. In the dipole representation hard diffraction of a hadron comes from the difference between elastic amplitudes of hadronic states with and without a hard fluctuation, Ahdi f f ∝ σqq(R + r) − σqq(R) ∝ rR ∼ 1/Q,. Where σqq(R) is the total dipole-nucleon cross section [9]; R characterises the hadronic size, while small r ∼ 1/Q R is related to the hard process [10, 11]. Such a mild Q-dependence contradicts factorization prediction, based on the DIS relation, Adi f f ∝ σqq(r) ∝ r2 ∼ 1/Q2,.

Drell-Yan reaction: annihilation or bremsstrahlung?
Diffractive Z and W production
Diffractive heavy flavor production
Diffractive Higgsstrahlung
Findings
Summary

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