TY - JOUR
T1 - Two-loop helicity amplitudes for V+jet production including axial vector couplings to higher orders in ϵ
AU - Gehrmann, Thomas
AU - Jakubčík, Petr
AU - Mella, Cesare Carlo
AU - Syrrakos, Nikolaos
AU - Tancredi, Lorenzo
N1 - Publisher Copyright:
© 2023, The Author(s).
PY - 2023/9
Y1 - 2023/9
N2 - We compute the two-loop Quantum Chromodynamics (QCD) corrections to all partonic channels relevant for the production of an electroweak boson V = Z, W ± , γ * and a jet at hadron colliders. We consider the decay of a vector boson V to three partons V → qq¯ g , V → ggg with a vector and axial vector coupling in both channels, including singlet and non-singlet contributions. For the quark channel, we use a recent tensor decomposition and extend the calculation to O (ϵ 2). For the gluonic channel, we define a new tensor decomposition which allows us to compute the vector and the axial vector amplitudes at once and to perform the computation of the amplitudes to O (ϵ 2). We provide finite remainders of the helicity amplitudes analytically continued to all relevant scattering regions qq¯ → Vg, qg → Vq and gg → Vg. The axial vector contribution to the gluon-induced channel completes the set of two-loop amplitudes for this process, while the extension to O (ϵ 2) represents the first step in the calculation of next-to-next-to-next-to-leading-order (N3LO) QCD corrections to Z+jet production at hadron colliders.
AB - We compute the two-loop Quantum Chromodynamics (QCD) corrections to all partonic channels relevant for the production of an electroweak boson V = Z, W ± , γ * and a jet at hadron colliders. We consider the decay of a vector boson V to three partons V → qq¯ g , V → ggg with a vector and axial vector coupling in both channels, including singlet and non-singlet contributions. For the quark channel, we use a recent tensor decomposition and extend the calculation to O (ϵ 2). For the gluonic channel, we define a new tensor decomposition which allows us to compute the vector and the axial vector amplitudes at once and to perform the computation of the amplitudes to O (ϵ 2). We provide finite remainders of the helicity amplitudes analytically continued to all relevant scattering regions qq¯ → Vg, qg → Vq and gg → Vg. The axial vector contribution to the gluon-induced channel completes the set of two-loop amplitudes for this process, while the extension to O (ϵ 2) represents the first step in the calculation of next-to-next-to-next-to-leading-order (N3LO) QCD corrections to Z+jet production at hadron colliders.
KW - Higher-Order Perturbative Calculations
KW - Scattering Amplitudes
KW - Specific QCD Phenomenology
UR - http://www.scopus.com/inward/record.url?scp=85173925278&partnerID=8YFLogxK
U2 - 10.1007/JHEP09(2023)192
DO - 10.1007/JHEP09(2023)192
M3 - Article
AN - SCOPUS:85173925278
SN - 1126-6708
VL - 2023
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 9
M1 - 192
ER -