Single Spin Asymmetry in transverse polarized proton production and lambda production in Semi-Inclusive DIS at twist-3

TL;DR

This paper investigates single spin asymmetries in semi-inclusive deep inelastic scattering, focusing on twist-3 distributions and twist-2 fragmentation functions, providing theoretical calculations and predictions for experiments at JLab and COMPASS.

Contribution

It presents a detailed analysis of the role of twist-3 distributions and twist-2 fragmentation functions in single spin asymmetries, with model calculations and experimental predictions.

Findings

Asymmetry can probe the distribution function h and fragmentation function H_1 in proton production.

Lambda production asymmetry can access f^⊥ and D_{1T}^⊥ functions at JLab.

Predicted asymmetries at JLab and COMPASS offer experimental tests for twist-3 and twist-2 functions.

Abstract

We study the single spin asymmetry in the transversely polarized proton production and the lambda hyperon production in semi-inclusive deep inelastic scattering with a $\sin \phi_{S_h}$ modulation, in which $S_h$ is the azimuthal angle of the transverse spin of the final hadron. The theoretical interpretation for the asymmetry is presented as the convolution of the twist-3 quark transverse momentum dependent distributions and twist-2 fragmentation functions. We investigate the role of the twist-3 distribution functions $h(x, p_T^2)$, $f^\perp(x, p_T^2)$ and $g^\perp(x, p_T^2)$ and the twist-2 fragmentation functions $H_1(x, k_T^2)$, $D_{1T}^\perp(x, k_T^2)$ and $G_{1T}(x, k_T^2)$ in this asymmetry. Using spectator model, we compute these distribution and fragmentation functions and estimate the $\sin \phi_{S_h}$ asymmetry for the proton production as well as for the lambda production at JLab with a 12 $\mathrm{GeV}$ electron beam. The asymmetry at the COMPASS kinematics is also predicted. By comparing different sources for the asymmetry, we conclude that it is feasible to access the distribution function $h$ and the fragmentation function $H_1$ through measuring the asymmetry in the proton production, whereas the $f^\perp \,D_{1T}^\perp$ term might be probed in the lambda production at JLab 12 GeV.