Spin asymmetry at large x_F and k_T

TL;DR

This paper proposes that large single spin asymmetries at high x_F and k_T in pion production result from soft-hard interaction coherence, which is maintained under specific kinematic conditions, explaining experimental observations.

Contribution

It introduces a coherence mechanism linking soft interactions with hard scattering to explain large spin asymmetries at high x_F and k_T.

Findings

Large dynamic phases in production amplitudes

Helicity flip contributions are unsuppressed at high x_F and k_T

Coherence effects similar to those in Drell-Yan observed

Abstract

We suggest that the large single spin asymmetries observed at high momentum fractions x_F and transverse momenta k_T of the pion in p^\uparrow p -> \pi(x_F,k_T)+X arise from the coherence of the soft interactions with the hard parton scattering process. Such coherence can be maintained if x_F -> 1 as k_T -> \infty, while k_T^2(1-x_F) ~ \Lambda_{QCD}^2 stays fixed. Analogous coherence effects have been seen experimentally in the Drell-Yan process at high x_F. We find that the p^\uparrow p -> \pi X production amplitudes have large dynamic phases and that helicity flip contributions are unsuppressed in this limit, giving rise to potentially large single spin asymmetries.