The naive time-reversal-odd (``T-odd'') parton distribution h₁^⊥, the so-called Boer-Mulders function, for both up (u) and down (d) quarks is considered in the diquark spectator model. While the results of different articles in the literature suggest that the signs of the Boer-Mulders function in semi-inclusive deep inelastic scattering (SIDIS) for both flavors u and d are the same and negative, a previous calculation in the diquark spectator model found that h₁^⊥(u) and h₁^⊥(d) have different signs. The flavor dependence is of significance for the analysis of the azimuthal cos(2φ) asymmetries in unpolarized SIDIS and Drell-Yan processes, as well as for the overall physical understanding of the distribution of transversely polarized quarks in unpolarized nucleons. We find substantial differences with previous work. In particular, we obtain half and first moments of the Boer-Mulders function that are negative over the full range in Bjorken x for both the u and d quarks. In conjunction with the Collins function, we then predict the cos(2φ) azimuthal asymmetry for π⁺ and π^- in this framework. We also find that the Sivers u and d quarks are negative and positive, respectively. As a by-product of the formalism, we calculate the chiral-odd but ``T-even'' function h1L^⊥, which allows us to present a prediction for the single-spin asymmetry AUL^sin(2φ) for a longitudinally polarized target in SIDIS.
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Gamberg et al. (2008) studied this question.
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