Abstract
We study the process γA →qq¯ g + X in the Color Glass Condensate (CGC) effective theory. After obtaining the cross section, we consider two kinematic limits which are encompassed in our result. In the so-called correlation limit, the vector sum of the transverse momenta of the three outgoing particles is small with respect to the individual transverse momenta; the cross section then simplifies considerably and can be written in a factorized form, sensitive to both the unpolarized and linearly-polarized Weizsäcker-Williams transverse momentum dependent gluon distribution function (gluon TMD). The second limit of the CGC cross section that we consider is the dilute limit, which we obtain after performing a weak-field expansion; we recover a typical linear-regime expression, involving a single unintegrated gluon distribution function. Using numerical simulations of the small-x QCD evolution of the TMDs, we investigate the rapidity dependence of the cross section in the correlation limit.
| Original language | English |
|---|---|
| Article number | 143 |
| Journal | Journal of High Energy Physics |
| Volume | 2020 |
| Issue number | 7 |
| DOIs | |
| Publication status | Published - 1 Jul 2020 |
Keywords
- Heavy Ion Phenomenology
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