We present the even-N moments N <= 20 of the fourth-order (N3LO) contribution P (3) gq (x) to the quark-to-gluon splitting function in perturbative QCD. These moments, obtained by analytically computing off-shell operator matrix elements for a general gauge group, agree with all known results, in particular with the moments N <= 10 derived before from structure functions in deep-inelastic scattering. Using the new moments and the available endpoint constraints, we construct approximations for P (3) gq (x) which improve upon those obtained from the lowest five even moments. The remaining uncertainties of this function are now practically irrelevant at momentum fractions x > 0.1. The resulting errors of the convolution of Pgq at N3LO with a typical quark distribution are small at x >= 10−3 and exceed 1% only at x <= 10−4 for a strong coupling as = 0.2. The present results for P (3) gq (x) should thus be sufficient for most collider-physics applications.

Four-loop splitting functions in QCD – The quark-to-gluon case

Falcioni G.
;
2024-01-01

Abstract

We present the even-N moments N <= 20 of the fourth-order (N3LO) contribution P (3) gq (x) to the quark-to-gluon splitting function in perturbative QCD. These moments, obtained by analytically computing off-shell operator matrix elements for a general gauge group, agree with all known results, in particular with the moments N <= 10 derived before from structure functions in deep-inelastic scattering. Using the new moments and the available endpoint constraints, we construct approximations for P (3) gq (x) which improve upon those obtained from the lowest five even moments. The remaining uncertainties of this function are now practically irrelevant at momentum fractions x > 0.1. The resulting errors of the convolution of Pgq at N3LO with a typical quark distribution are small at x >= 10−3 and exceed 1% only at x <= 10−4 for a strong coupling as = 0.2. The present results for P (3) gq (x) should thus be sufficient for most collider-physics applications.
2024
856
138906
138915
https://www.sciencedirect.com/science/article/pii/S0370269324004647
Falcioni G.; Herzog F.; Moch S.; Pelloni A.; Vogt A.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/2021317
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