TY - JOUR
T1 - Forward trijet production in proton–nucleus collisions
AU - Iancu, Edmond
AU - Mulian, Yair
N1 - Funding Information:
We would like to thank M. Lublinsky, C. Marquet, and A. H. Mueller for useful discussions. The work of Y.M. was in part supported by the 2016–2017 Chateaubriand fellowship of the French embassy in Israel. This work is supported in part by the Agence Nationale de la Recherche project ANR-16-CE31-0019-01 .
Publisher Copyright:
© 2019 Elsevier B.V.
PY - 2019/5/1
Y1 - 2019/5/1
N2 - Using the formalism of the light-cone wave function in perturbative QCD together with the hybrid factorization, we compute the cross-section for three particle production at forward rapidities in proton–nucleus collisions. We focus on the quark channel, in which the three produced partons — a quark accompanied by a gluon pair, or two quarks plus one antiquark — are all generated via two successive splittings starting with a quark that was originally collinear with the proton. The three partons are put on-shell by their scattering off the nuclear target, described as a Lorentz-contracted “shockwave”. The three-parton component of the quark light-cone wave function that we compute on this occasion is also an ingredient for other interesting calculations, like the next-to-leading order correction to the cross-section for the production of a pair of jets.
AB - Using the formalism of the light-cone wave function in perturbative QCD together with the hybrid factorization, we compute the cross-section for three particle production at forward rapidities in proton–nucleus collisions. We focus on the quark channel, in which the three produced partons — a quark accompanied by a gluon pair, or two quarks plus one antiquark — are all generated via two successive splittings starting with a quark that was originally collinear with the proton. The three partons are put on-shell by their scattering off the nuclear target, described as a Lorentz-contracted “shockwave”. The three-parton component of the quark light-cone wave function that we compute on this occasion is also an ingredient for other interesting calculations, like the next-to-leading order correction to the cross-section for the production of a pair of jets.
KW - Color glass condensate
KW - Multiparticle production
KW - Proton–nucleus collisions
UR - http://www.scopus.com/inward/record.url?scp=85062391502&partnerID=8YFLogxK
U2 - 10.1016/j.nuclphysa.2019.02.003
DO - 10.1016/j.nuclphysa.2019.02.003
M3 - Article
AN - SCOPUS:85062391502
SN - 0375-9474
VL - 985
SP - 66
EP - 127
JO - Nuclear Physics A
JF - Nuclear Physics A
ER -