TY - JOUR
T1 - Dihadron production in DIS at NLO
T2 - the real corrections
AU - Iancu, Edmond
AU - Mulian, Yair
N1 - Funding Information:
We would like to thank Nestor Armesto, Guillaume Beuf, Paul Caucal, Adrian Dumitru, Yuri Kovchegov, Tuomas Lappi, Michael Lublinsky, Cyrille Marquet, Farid Salazar and Pieter Taels for insightful discussions during the gestation of this work. The work of E.I. is supported in part by the Agence Nationale de la Recherche project ANR-16-CE31-0019-01. Y.M acknowledges financial support from Xunta de Galicia (Centro singular de investigación de Galicia accreditation 2019-2022); the “María de Maeztu” Units of Excellence program MDM2016-0692 and the Spanish Research State Agency under project PID2020-119632GB-I00; European Union ERDF; MSCA RISE 823947 ”Heavy ion collisions: collectivity and precision in saturation physics” (HIEIC). This work was also supported under the European Union’s Horizon 2020 research and innovation programme by the European Research Council (ERC, grant agreement No. ERC-2018-ADG-835105 YoctoLHC) and by the STRONG-2020 project (grant agreement No. 824093). The content of this article does not reflect the official opinion of the European Union and responsibility for the information and views expressed therein lies entirely with the authors.
Funding Information:
We would like to thank Nestor Armesto, Guillaume Beuf, Paul Caucal, Adrian Dumitru, Yuri Kovchegov, Tuomas Lappi, Michael Lublinsky, Cyrille Marquet, Farid Salazar and Pieter Taels for insightful discussions during the gestation of this work. The work of E.I. is supported in part by the Agence Nationale de la Recherche project ANR-16-CE31-0019-01. Y.M acknowledges financial support from Xunta de Galicia (Centro singular de investigación de Galicia accreditation 2019-2022); the “María de Maeztu” Units of Excellence program MDM2016-0692 and the Spanish Research State Agency under project PID2020-119632GB-I00; European Union ERDF; MSCA RISE 823947 ”Heavy ion collisions: collectivity and precision in saturation physics” (HIEIC). This work was also supported under the European Union’s Horizon 2020 research and innovation programme by the European Research Council (ERC, grant agreement No. ERC-2018-ADG-835105 YoctoLHC) and by the STRONG-2020 project (grant agreement No. 824093). The content of this article does not reflect the official opinion of the European Union and responsibility for the information and views expressed therein lies entirely with the authors.
Publisher Copyright:
© 2023, The Author(s).
PY - 2023/7/1
Y1 - 2023/7/1
N2 - By using the formalism of the light-cone wave function along with the colour glass condensate effective theory, we consider next-to-leading order (NLO) corrections to the production of a pair of hadrons in electron-proton, or electron-nucleus, collisions at small Bjorken x. To the order of interest, the process involves the fluctuation of a virtual photon into a quark-antiquark pair, followed by the emission of a gluon from either the quark, or the antiquark. For the case of a virtual photon with transverse polarization, we compute the real NLO corrections, where the emitted gluon is present in the final state. We first compute the tree-level cross-section for the production of the quark-antiquark-gluon system and then deduce the real NLO corrections to dihadron production by integrating out the kinematics of the gluon. We verify in detail that, in the limit where the gluon is soft, our calculation reproduces the (real piece of the) B-JIMWLK evolution of the leading-order cross-section for quark-antiquark production. Similarly, in the limit where the gluon is collinear with its emitter, we recover the real terms in the DGLAP evolution of the fragmentation function. The virtual NLO corrections to dihadron production will be presented by one of us in a subsequent publication.
AB - By using the formalism of the light-cone wave function along with the colour glass condensate effective theory, we consider next-to-leading order (NLO) corrections to the production of a pair of hadrons in electron-proton, or electron-nucleus, collisions at small Bjorken x. To the order of interest, the process involves the fluctuation of a virtual photon into a quark-antiquark pair, followed by the emission of a gluon from either the quark, or the antiquark. For the case of a virtual photon with transverse polarization, we compute the real NLO corrections, where the emitted gluon is present in the final state. We first compute the tree-level cross-section for the production of the quark-antiquark-gluon system and then deduce the real NLO corrections to dihadron production by integrating out the kinematics of the gluon. We verify in detail that, in the limit where the gluon is soft, our calculation reproduces the (real piece of the) B-JIMWLK evolution of the leading-order cross-section for quark-antiquark production. Similarly, in the limit where the gluon is collinear with its emitter, we recover the real terms in the DGLAP evolution of the fragmentation function. The virtual NLO corrections to dihadron production will be presented by one of us in a subsequent publication.
KW - Deep Inelastic Scattering or Small-x Physics
KW - Higher-Order Perturbative Calculations
UR - http://www.scopus.com/inward/record.url?scp=85165275230&partnerID=8YFLogxK
U2 - 10.1007/JHEP07(2023)121
DO - 10.1007/JHEP07(2023)121
M3 - Article
AN - SCOPUS:85165275230
SN - 1126-6708
VL - 2023
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 7
M1 - 121
ER -