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Probing the Dense Medium in Cold Nuclei -- Gluon Saturation at small-x. Bowen Xiao (CCNU) Feng Yuan (LBNL). Gluon saturation inevitable at small-x. QCD evolution drives the gluon distribution rising at small-x. BFKL evolution becomes relevant at small-x.
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Probing the Dense Medium in Cold Nuclei-- Gluon Saturation at small-x Bowen Xiao (CCNU) Feng Yuan (LBNL)
QCD evolution drives the gluon distribution rising at small-x
BFKL evolution becomes relevant at small-x • Balitsky-Fadin-Lipatov-Kuraev, 1977-78 • Balitsky-Kovchegov: Non-linear term, 98
QCD Phase structure of cold nuclei • Hard processes probe the kt-dependent gluon distributions directly • Saturation phenomena manifest in the observables • Xiao,Yuan, et al, PRL106, 022301 (2011) PRL105, 062001 (2010)
Conventional gluon distribution • Collins-Soper, 1981 • Gauge link in the adjoint representation
Physical interpretation • Choosing light-cone gauge, with certain boundary condition (either one, but not the principal value) • Gauge link contributions can be dropped • Number density interpretation, and can be calculated from the wave functions of nucleus • McLerran-Venugopalan • Kovchegov-Mueller
Classic YM theory • McLerran-Venugopalan • See also, Kovchegov-Mueller • We can reproduce this gluon distribution using the TMD definition with gauge link contribution, following BJY 02, BHPS 02 • Weizsacker-Williams gluon distribution is the conventional one
DIS dijet probes WW gluons • Hard interaction includes the gluon attachments to both quark and antiquark • The qt dependence is the gluon distribution w/o gauge link contribution at this order
Final state interaction gauge link Dominguez-Xiao-Yuan, 2010 This is exactly the leading order expansion of the gauge link contribution, checked at three-gluon exchange order a a b b
Differential cross section • Rigorous kt-factorization can be built for this process • Initial photon, not hadron • Similar to e+e-, Collins-Soper, 81 • It is also a clean place to study the gluon Sivers function, Vogelsang-Yuan, 07
Golden channel for an EIC • Directly probe the Weizsacker-Williams gluon distribution in nucleus • Factorization is very clear • Various channels within DIS processes • Heavy flavor • Real/virtual photon
Photon-jet correlation probes the dipole gluon distribution • No difference for the Born diagram • Naïve kt-factorization would predict the same qt-dependence
Initial/final state interactions There is no color structure corresponding to this, We have to express the gluon Distribution in the Fundamental representation a b a b
Differential cross section Dominguez-Xiao-Yuan, 2010 • This is the dipole gluon distribution, also called unintegrated gluon distribution
Intuitive explanations • Final state interactions in DIS can be eliminated by choosing the light-cone gauge number density interpretation • Photon-jet correlation have both initial/final state interactions, can not be eliminated by choosing LC gauge there is no number density interpretation dipole gluon distribution
Dijet-correlation at RHIC • Initial state and/or final state interactions Jet 2 Jet 1 Boer-Vogelsang 03 P,ST Standard (naïve) Factorization breaks! Becchetta-Bomhof-Mulders-Pijlman, 04-06 Collins-Qiu 08; Vogelsang-Yuan 08 Rogers-Mulders 10; Xiao-Yuan, 10
Modified factorization • Dilute system on a dense target, in the large Nc limit,
Sudakov (CSS) Resummation • Sudakov double logs can be re-summed in the small-x saturation formalism • Radiated gluon momentum • Soft gluon, α~β<<1 • Collinear gluon, α~1, β<<1 • Small-x collinear gluon, 1-β<<1, α0 • Rapidity divergence Mueller, Xiao, Yuan, PRL110,082301 (2013)
Conclusions: EIC • Great opportunities in nuclear science • Ultimate machine for nucleon spin physics • Unique place to investigate gluon saturation • Potential discovery in BSM physics
Small-x factorization Mueller, 1994 • eikonal approximation in high energy scattering
Splitting function • Dipole amplitude • At one-loop order BK-JIMWLK Y~Log(1/x)