DOI 10.1007/s100520000510
Analytic coupling and Sudakov effects in exclusive processes: pion and form factors
N.G. Stefanis1 - W. Schroers2 - H.-Ch. Kim3
1 Institut für Theoretische Physik II, Ruhr-Universität Bochum, 44780 Bochum, Germany
2 Fachbereich Physik, Universität Wuppertal, 42097 Wuppertal, Germany
3 Department of Physics, Pusan National University, Pusan 609-735, Republic of Korea
Received: 19 May 2000 / Revised version: 16 August 2000 /
Published online: 13 November 2000 - © Springer-Verlag 2000
Abstract
We develop and discuss in technical detail an infrared-finite
factorization and optimized renormalization scheme for calculating
exclusive processes, which enables the inclusion of transverse
degrees of freedom without entailing suppression of calculated
observables, like form factors. This is achieved by employing an
analytic, i.e., infrared stable, running strong-coupling
which removes the Landau singularity at
by a minimum power-behaved
correction.
The ensuing contributions to the cusp anomalous dimension -
related to the Sudakov form factor - and to the quark anomalous
dimension - which controls evolution - lead to an enhancement at high
Q2 of the hard part of exclusive amplitudes, calculated in
perturbative QCD, while simultaneously improving its scaling behavior.
The phenomenological implications of this framework are analyzed by
applying it to the pion's electromagnetic form factor, including
the NLO contribution to the hard-scattering amplitude, and also
to the pion-photon transition at LO. For the pion wave function,
an improved ansatz of the Brodsky-Huang-Lepage type is employed,
which includes an effective (constituent-like) quark mass,
mq=0.33GeV. Predictions for both
form factors are presented and
compared to the experimental data, applying Brodsky-Lepage-Mackenzie
commensurate scale setting. We find that the perturbative hard part
prevails at momentum transfers above about 20GeV2, while at
lower Q2 values the pion form factor is dominated by Feynman-type
contributions. The theoretical prediction for the
form factor indicates that the true
pion distribution amplitude may be somewhat broader than the asymptotic
one.
Copyright Società Italiana di Fisica, Springer-Verlag 2000