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

被引:8
作者
Falcioni, G. [1 ,2 ]
Herzog, F. [3 ]
Moch, S. [4 ]
Pelloni, A. [5 ]
Vogt, A. [6 ]
机构
[1] Univ Torino, Dipartimento Fis, Via Pietro Giuria 1, I-10125 Turin, Italy
[2] Univ Zurich, Phys Inst, Winterthurerstr 190, CH-8057 Zurich, Switzerland
[3] Univ Edinburgh, Higgs Ctr Theoret Phys, Sch Phys & Astron, Edinburgh EH9 3FD, Scotland
[4] Hamburg Univ, Inst Theoret Phys 2, Luruper Chaussee 149, D-22761 Hamburg, Germany
[5] Swiss Fed Inst Technol, Inst Theoret Phys, CH-8093 Zurich, Switzerland
[6] Univ Liverpool, Dept Math Sci, Liverpool L69 3BX, England
关键词
ANOMALOUS DIMENSIONS; WILSON OPERATORS; RENORMALIZATION; GAUGE; COEFFICIENT;
D O I
10.1016/j.physletb.2024.138906
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present the even-N moments N <= 20 of the fourth-order ((NLO)-L-3) contribution P-gq((3))(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-gq((3))(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 (NLO)-L-3 with a typical quark distribution are small at x greater than or similar to 10(-3) and exceed 1% only at x less than or similar to 10(-4) for a strong coupling alpha(s )= 0.2. The present results for P-gq((3))(x) should thus be sufficient for most collider-physics applications.
引用
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页数:10
相关论文
共 57 条
[1]   On the next-to-next-to-leading order evolution of flavour-singlet fragmentation functions [J].
Almasy, A. A. ;
Moch, S. ;
Vogt, A. .
NUCLEAR PHYSICS B, 2012, 854 (01) :133-152
[2]   Generalized double-logarithmic large-x resummation in inclusive deep-inelastic scattering [J].
Almasy, A. A. ;
Soar, G. ;
Vogt, A. .
JOURNAL OF HIGH ENERGY PHYSICS, 2011, (03)
[3]   Higgs Boson Gluon-Fusion Production in QCD at Three Loops [J].
Anastasiou, Charalampos ;
Duhr, Claude ;
Dulat, Falko ;
Herzog, Franz ;
Mistlberger, Bernhard .
PHYSICAL REVIEW LETTERS, 2015, 114 (21)
[4]   A STUDY OF A POSSIBLE QUARK-GLUON SYMMETRY IN QCD [J].
ANTONIADIS, I ;
FLORATOS, EG .
NUCLEAR PHYSICS B, 1981, 191 (01) :217-226
[5]   The structure of generic anomalous dimensions and no-π theorem for massless propagators [J].
Baikov, P. A. ;
Chetyrkin, K. G. .
JOURNAL OF HIGH ENERGY PHYSICS, 2018, (06)
[6]  
BLUMLEIN J, 1999, PHYS REV D, V60, DOI DOI 10.1103/PHYSREVD.60.014018
[7]  
Caola F., 2021, Snowmass
[8]   SMALL-X BEHAVIOR OF INITIAL STATE RADIATION IN PERTURBATIVE QCD [J].
CATANI, S ;
FIORANI, F ;
MARCHESINI, G .
NUCLEAR PHYSICS B, 1990, 336 (01) :18-85
[9]   INFRARED R-OPERATION AND ULTRAVIOLET COUNTERTERMS IN THE MS-SCHEME [J].
CHETYRKIN, KG ;
TKACHOV, FV .
PHYSICS LETTERS B, 1982, 114 (05) :340-344
[10]   R-STAR-OPERATION CORRECTED [J].
CHETYRKIN, KG ;
SMIRNOV, VA .
PHYSICS LETTERS B, 1984, 144 (5-6) :419-424