2021
DOI: 10.1103/physrevd.104.054023
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Twist-3 gluon fragmentation contribution to polarized hyperon production in unpolarized proton-proton collision

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Cited by 12 publications
(13 citation statements)
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“…We work in the hadron frame in which the momenta of the initial proton and the virtual photon are collinear [10]. Following the formalism developed for 𝑝 𝑝 β†’ Ξ› ↑ 𝑋 in [6], we could obtain the LO cross section as…”
Section: Twist-3 Gluon Ffs Contribution To the Cross Sectionmentioning
confidence: 99%
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“…We work in the hadron frame in which the momenta of the initial proton and the virtual photon are collinear [10]. Following the formalism developed for 𝑝 𝑝 β†’ Ξ› ↑ 𝑋 in [6], we could obtain the LO cross section as…”
Section: Twist-3 Gluon Ffs Contribution To the Cross Sectionmentioning
confidence: 99%
“…S 1,2,3,4 = sin Ξ¨ 𝑠 and S 8,9 = cos Ξ¨ 𝑠 , where Ξ¨ 𝑠 denotes the azimuthal angle of the transverse spin vector of the final hyperon. According to the formalism developed in [6], intrinsic, kinematical, and the dynamical twist-3 FFs as well as the derivative of kinematical FFs appear in the cross section. By using the QCD equation-of-motion relations and the Lorentz invariance relations [9], one can eliminate the intrinsic FF, Ξ” Ĝ3 T (𝑧), and the derivative of the kinematical FFs, πœ• Ĝ (1) 𝑇 (𝑧)/πœ• (1/𝑧) and πœ•Ξ” Δ€ (1) 𝑇 (𝑧)/πœ• (1/𝑧), in favor of the other twist-3 FFs.…”
Section: Pos(panic2021)370mentioning
confidence: 99%
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“…Derivation of the twist-3 cross sections for SSAs required lots of technical development. By now the collinear twist-3 formalism for all kinds of the twist-3 distribution functions (DFs) and the fragmentation functions (FFs) has been well established in the leading order (LO) with respect to the QCD coupling constant [5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20]. Those functions are, in general, not independent from each other but obey some constraint relations based on the operator identities.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, we study the transverse polarization of hyperons produced in semi-inclusive deep inelastic scattering (SIDIS), ep β†’ eΞ› ↑ X, in the LO collinear twist-3 factorization. As for the case of pp β†’ Ξ› ↑ X [20,[27][28][29][30], two kinds of the twist-3 cross sections contribute. One is from the twist-3 DF in unpolarized proton combined with the "transversity" FF for the polarized Ξ›.…”
Section: Introductionmentioning
confidence: 99%