Spin-flip gluon GTMD at small-
arXiv:2312.04132 · doi:10.1103/PhysRevD.109.074039
Abstract
Until recently the spin-flip processes in the deep inelastic scatterings are thought to be suppressed in the high energy. We found a positive intercept for the spin-flip generalized transverse momentum-dependent parton distribution (GTMDs) as, \begin{eqnarray} {\rm Re}(F_{1,2}) \sim \left(\frac{1}{x}\right)^{{\bar α}_s\left(4\ln2-8/3\right)} \left(\cos 3ϕ_{kΔ} +\cos ϕ_{kΔ}\right). \nonumber \end{eqnarray} This is done by analytically solving the integro-differential evolution equation for , recently proposed by Hatta and Zhou, in the dilute regime. Interestingly, the surviving solution corresponds to conformal spin and carries an explicit azimuthal dependence. As the imaginary part of , is related to the spin-dependent odderon or gluon Siver function and scales as , the positive intercept for , implies that it is expected to dominate over the gluon Siver function in the small- limit - and may directly impact the modeling of unpolarised GTMDs and associated spin-flip processes.
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Cited by in corpus (3)
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