Recently, it has been shown, contrary to previous beliefs, that the k(perp)-distribution of quarks in a transversely polarized proton can be asymmetric. This "Sivers effect" had already been used to explain transverse single spin asymmetry (SSA) observed in inclusive pion production p(uparrow) p --> pi X and pbar(uparrow) p --> pi X. In such channels, however, other mechanisms, such as the "Collins effect" (a k(perp)-asymmetric fragmentation of a transversely polarized quark into pions), may generate SSA. The Sivers asymmetry is used here to compute the SSA in Drell-Yan processes; in this case, by considering the differential cross section in the lepton-pair invariant mass, rapidity, and transverse momentum, other mechanisms that may originate SSA cannot contribute. Estimates for BNL RHIC experiments are given.
Transverse single spin asymmetries in Drell-Yan processes
D'ALESIO, UMBERTO;
2003-01-01
Abstract
Recently, it has been shown, contrary to previous beliefs, that the k(perp)-distribution of quarks in a transversely polarized proton can be asymmetric. This "Sivers effect" had already been used to explain transverse single spin asymmetry (SSA) observed in inclusive pion production p(uparrow) p --> pi X and pbar(uparrow) p --> pi X. In such channels, however, other mechanisms, such as the "Collins effect" (a k(perp)-asymmetric fragmentation of a transversely polarized quark into pions), may generate SSA. The Sivers asymmetry is used here to compute the SSA in Drell-Yan processes; in this case, by considering the differential cross section in the lepton-pair invariant mass, rapidity, and transverse momentum, other mechanisms that may originate SSA cannot contribute. Estimates for BNL RHIC experiments are given.
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