TY - JOUR
T1 - J/ψ meson production in SIDIS
T2 - matching high and low transverse momentum
AU - Boer, Daniël
AU - D’Alesio, Umberto
AU - Murgia, Francesco
AU - Pisano, Cristian
AU - Taels, Pieter
N1 - Publisher Copyright:
© 2020, The Author(s).
PY - 2020/9/1
Y1 - 2020/9/1
N2 - We consider the transverse momentum spectrum and the cos 2ϕ azimuthal distribution of J/ψ mesons produced in semi-inclusive, deep-inelastic electron-proton scattering, where the electron and the proton are unpolarized. At low transverse momentum, we propose factorized expressions in terms of transverse momentum dependent gluon distributions and shape functions. We show that our formulae, at the order αs, correctly match with the collinear factorization results at high transverse momentum. The latter are computed at the order αs2 in the framework of nonrelativistic QCD (NRQCD), with the inclusion of the intermediate 3S1[1] color-singlet Fock state, as well as the subleading color-octet ones that are relatively suppressed by a factor v4 in the NRQCD velocity parameter v. We show that the 1S0[8] and 3PJ[8] (J = 0, 1, 2) contributions diverge in the small transverse momentum region and allow us to determine the perturbative tails of the shape functions, which carry the same quantum numbers. These turn out to be identical, except for the overall magnitude given by the appropriate NRQCD long distance matrix element.
AB - We consider the transverse momentum spectrum and the cos 2ϕ azimuthal distribution of J/ψ mesons produced in semi-inclusive, deep-inelastic electron-proton scattering, where the electron and the proton are unpolarized. At low transverse momentum, we propose factorized expressions in terms of transverse momentum dependent gluon distributions and shape functions. We show that our formulae, at the order αs, correctly match with the collinear factorization results at high transverse momentum. The latter are computed at the order αs2 in the framework of nonrelativistic QCD (NRQCD), with the inclusion of the intermediate 3S1[1] color-singlet Fock state, as well as the subleading color-octet ones that are relatively suppressed by a factor v4 in the NRQCD velocity parameter v. We show that the 1S0[8] and 3PJ[8] (J = 0, 1, 2) contributions diverge in the small transverse momentum region and allow us to determine the perturbative tails of the shape functions, which carry the same quantum numbers. These turn out to be identical, except for the overall magnitude given by the appropriate NRQCD long distance matrix element.
KW - Deep Inelastic Scattering (Phenomenology)
KW - QCD Phenomenology
UR - http://www.scopus.com/inward/record.url?scp=85090296984&partnerID=8YFLogxK
U2 - 10.1007/JHEP09(2020)040
DO - 10.1007/JHEP09(2020)040
M3 - Article
AN - SCOPUS:85090296984
VL - 2020
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
SN - 1126-6708
IS - 9
M1 - 40
ER -