We calculate the cross section of a pion diffraction dissociation in two je
ts with large transverse momenta originating from a hard gluon exchange bet
ween the pion constituents. To the leading logarithmic accuracy tin energy)
, the contribution coming From small transverse separations between the qua
rk and the antiquark in the pion acquires the expected factorized form, the
longitudinal momentum distribution of the jets being proportional to the p
ion distribution amplitude. The hard gluon exchange can in this case be con
sidered as a part of the unintegrated gluon distribution. Beyond the leadin
g logarithms tin energy) this proportionality does not hold. Moreover, the
collinear factorization appears to be broken by the end-point singularities
. Remarkably enough, the longitudinal momentum distribution of the jets for
the non-factorizable contribution is calculable, and turns out to be the s
ame as for the factorizable contribution with the asymptotic pion distribut
ion amplitude. (C) 2001 Elsevier Science B.V. All rights reserved.