Recognition: unknown
Four-Loop Gluon Anomalous Dimension of General Lorentz Spin: Transcendental Part
Pith reviewed 2026-05-07 15:56 UTC · model grok-4.3
The pith
The zeta(3) contribution to the four-loop gluon anomalous dimension gamma_gg^(3)(N) is constructed in analytic form for arbitrary Lorentz spin N.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We construct the contribution proportional to zeta(3) to the four-loop anomalous dimension gamma_gg^(3)(N) of the twist-two gluon operator for arbitrary N in the singlet sector by applying the Lenstra-Lenstra-Lovasz algorithm to available low-N moments, exploiting generalized Gribov-Lipatov reciprocity and new self-tuning relations for the singlet anomalous dimension matrix, and injecting information from N=1 and N=4 supersymmetric Yang-Mills theories; we also give the rational contribution with color factor C_F^2 n_f^2. Exact pieces of the four-loop splitting function P_gg^(3)(x) obtained via inverse Mellin transformation reduce theoretical uncertainties in the scaling violations of parton
What carries the argument
The Lenstra-Lenstra-Lovasz lattice reduction algorithm applied to low-N moments of the anomalous dimension, augmented by generalized Gribov-Lipatov reciprocity and self-tuning relations for the singlet sector.
If this is right
- Exact transcendental and rational contributions to the four-loop splitting function P_gg^(3)(x) become available for the gluon channel.
- Theoretical uncertainties on the scale evolution of parton distribution functions in QCD are reduced.
- The method supplies a template that can be repeated for other color structures or higher transcendental weights at four loops.
- The resulting splitting functions can be inserted directly into global PDF fits and DGLAP evolution codes.
Where Pith is reading between the lines
- If the reciprocity relations continue to hold, the same lattice-reduction approach could isolate the zeta(5) or higher-weight terms at four loops or beyond.
- Numerical lattice or Monte-Carlo evaluations of moments at moderate N could provide an immediate cross-check of the constructed expression.
- The results improve the precision frontier for predictions of scaling violations at the LHC and future colliders.
Load-bearing premise
Generalized Gribov-Lipatov reciprocity and the new self-tuning relations for the singlet anomalous dimension matrix remain valid at four loops so that supersymmetric Yang-Mills information can be used without uncontrolled errors.
What would settle it
An independent four-loop computation of the anomalous dimension at a sufficiently high specific N (such as N=12) that yields a zeta(3) coefficient differing from the analytic expression obtained here.
read the original abstract
We consider the anomalous dimension $\gamma_{gg}^{(3)}(N)$ of the twist-two gluon operator of arbitrary Lorentz spin $N$ in the quark flavor singlet sector of a general gauge theory at four loops and construct its contribution proportional to $\zeta(3)$ in analytic form by applying the Lenstra-Lenstra-Lov\'{a}sz algorithm to the available low-$N$ moments. We exploit generalized Gribov-Liptov reciprocity, establish new self-tuning relations for the anomalous dimension matrix of the singlet sector, and inject information from $\mathcal{N}=1,4$ supersymmetric Yang-Mills theories. We also present the contribution to the rational part of $\gamma_{gg}^{(3)}(N)$ with color factor $C_F^2n_f^2$. Exact contributions to the four-loop splitting function $P_{gg}^{(3)}(x)$ hence resulting via inverse Mellin transformation help us to reduce theoretical uncertainties in scaling violations of parton distribution functions in QCD.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript computes the contribution proportional to ζ(3) to the four-loop gluon anomalous dimension γ_gg^(3)(N) for arbitrary Lorentz spin N in the quark flavor singlet sector. This is achieved by applying the Lenstra-Lenstra-Lovász (LLL) algorithm to low-N moments, while exploiting generalized Gribov-Lipatov reciprocity, establishing new self-tuning relations for the singlet anomalous dimension matrix, and incorporating information from N=1 and N=4 supersymmetric Yang-Mills theories. Additionally, the rational part with color factor C_F² n_f² is presented, leading to exact contributions to the four-loop splitting function P_gg^(3)(x) via inverse Mellin transform.
Significance. If the results hold, this provides valuable analytic expressions for higher-order QCD corrections to anomalous dimensions and splitting functions. Such results are significant for reducing theoretical uncertainties in the evolution of parton distribution functions, which is crucial for precision phenomenology at colliders like the LHC. The combination of moment-based reconstruction with symmetry relations and SUSY inputs represents a powerful approach in the field.
major comments (3)
- [Section describing the LLL ansatz construction] The completeness of the basis of possible transcendental structures (products of harmonic sums and zeta values) used in the LLL reconstruction must be explicitly demonstrated. An incomplete basis risks producing a compact but incorrect analytic form that fits the given moments but does not represent the true expression.
- [Section on self-tuning relations] The newly established self-tuning relations for the anomalous dimension matrix are load-bearing for constraining the ansatz. Their derivation should be shown to be independent of the low-N moment data used in the reconstruction to avoid potential circularity.
- [Discussion of generalized reciprocity] The extension of generalized Gribov-Lipatov reciprocity to four loops is assumed; a clear statement or proof of its validity in this context is needed, as it underpins the reduction of the parameter space for the ζ(3) term.
minor comments (2)
- [Abstract] The abstract mentions 'exact contributions' but the main result is only the ζ(3) part plus one rational term; clarify the scope of what is fully determined.
- [Notation] Ensure consistent use of superscripts for loop order and subscripts for color factors throughout the manuscript.
Simulated Author's Rebuttal
We thank the referee for the positive evaluation of our work and the insightful comments. We respond to each major comment in turn below.
read point-by-point responses
-
Referee: The completeness of the basis of possible transcendental structures (products of harmonic sums and zeta values) used in the LLL reconstruction must be explicitly demonstrated. An incomplete basis risks producing a compact but incorrect analytic form that fits the given moments but does not represent the true expression.
Authors: We will revise the manuscript to include a more explicit demonstration of the basis completeness in the section describing the LLL ansatz. The basis is constructed from all terms allowed by the weight and the known analytic properties of the anomalous dimensions at lower orders. We have performed checks by extending the basis with additional structures, which result in inconsistent systems for the given moments, indicating that the chosen basis is complete within the constraints. A full mathematical proof of completeness is not feasible without the exact result, but this is the standard approach used in similar reconstructions in the literature. revision: yes
-
Referee: The newly established self-tuning relations for the anomalous dimension matrix are load-bearing for constraining the ansatz. Their derivation should be shown to be independent of the low-N moment data used in the reconstruction to avoid potential circularity.
Authors: The self-tuning relations are derived purely from the general properties of the singlet sector anomalous dimension matrix and do not depend on the low-N moments. We will add an appendix with the full derivation, which starts from the definition of the evolution operator and the required algebraic constraints on the matrix elements. This ensures there is no circularity in the application to the LLL reconstruction. revision: yes
-
Referee: The extension of generalized Gribov-Lipatov reciprocity to four loops is assumed; a clear statement or proof of its validity in this context is needed, as it underpins the reduction of the parameter space for the ζ(3) term.
Authors: We will include a clear statement in the revised manuscript explaining that the generalized reciprocity is extended based on its established validity through three loops and its consistency with the supersymmetric Yang-Mills theories considered. While a rigorous proof at four loops is not provided here, as it would require a separate investigation, the assumption is validated by the agreement with independent results in the N=4 SYM limit. We believe this addresses the concern. revision: partial
Circularity Check
No significant circularity detected; reconstruction uses independent inputs.
full rationale
The paper's central step applies the LLL algorithm to independently computed low-N moments (presumed external) to recover the analytic zeta(3) contribution, after constraining the ansatz via generalized Gribov-Lipatov reciprocity and newly established self-tuning relations. Supersymmetric Yang-Mills information is injected from external sources. No quoted equation or self-citation chain reduces the final analytic form to a tautological fit of the same data by construction; the low-N moments and SYM inputs remain independent benchmarks, and the result is presented as an interpolation whose validity can be checked via inverse Mellin transform against higher-N behavior. This is the normal, non-circular case for moment-based reconstructions.
Axiom & Free-Parameter Ledger
axioms (3)
- domain assumption Generalized Gribov-Lipatov reciprocity holds for the four-loop gluon anomalous dimension
- domain assumption Self-tuning relations exist for the singlet-sector anomalous dimension matrix at four loops
- domain assumption Results from N=1 and N=4 supersymmetric Yang-Mills theories can be directly injected into QCD expressions
Forward citations
Cited by 1 Pith paper
-
Properties and implications of the four-loop non-singlet splitting functions in QCD
Four-loop non-singlet QCD splitting functions are verified for consistency and used to finalize analytical forms for the gluon virtual anomalous dimension and N^4LL threshold resummation coefficients, revealing a new ...
Reference graph
Works this paper leans on
-
[1]
for all N, we may thus analytically reconstruct tr ˆγ(3) ζ3 from the known Mellin moments ofγ (3) gg,ζ 3 [34, 39, 43, 46] and so obtainγ (3) gg,ζ 3 = tr ˆγ(3) ζ3 −γ (3)+ ns,ζ3 −γ (3) ps,ζ3 for allN. 3 The sought-aftern 1 f andn 0 f terms ofγ (3) gg,ζ 3 come with color factorsn f C 3 F ,n f CAC 2 F ,n f C 2 ACF ,n f C 3 A, nf d(4) RA/na,C 4 A, andd (4) AA/...
2019
-
[2]
and similar contributions toγ (3) ps withC ACF n2 f [36] andγ (3) gq withC ACF n2 f [38]. Such terms do not yet appear inγ (2) ij [20–25], but were already observed at two loops in the coefficient functions of inclusive deep-inelastic scattering (DIS) by photon exchange [87, 88]. They emerge from D−2S−2(N−2) forN= 2 and allow us to predict that γ(3) gg,ra...
-
[3]
J. D. Bjorken and E. A. Paschos, Inelastic Electron- Proton andγ-Proton Scattering and the Structure of the Nucleon, Phys. Rev.185, 1975–1982 (1969) doi:10.1103/PhysRev.185.1975
-
[4]
H. Fritzsch, M. Gell-Mann, and H. Leutwyler, Advan- tages of the color octet gluon picture, Phys. Lett. B47, 365–368 (1973) doi:10.1016/0370-2693(73)90625-4
-
[5]
V. N. Gribov and L. N. Lipatov, Deep inelasticepscatter- ing in perturbation theory, Yad. Fiz.15, 781–807 (1972) [Sov. J. Nucl. Phys.15, 438–450 (1972)]
1972
-
[6]
V. N. Gribov and L. N. Lipatov,e +e−-pair annihilation and deep inelasticepscattering in perturbation theory, Yad. Fiz.15, 1218–1237 (1972) [Sov. J. Nucl. Phys.15, 675–684 (1972)]
1972
-
[7]
G. Altarelli and G. Parisi, Asymptotic freedom in par- ton language, Nucl. Phys. B126, 298–318 (1977). doi:10.1016/0550-3213(77)90384-4
-
[8]
Yu. L. Dokshitzer, Calculation of the structure functions for deep inelastic scattering ande +e− annihilation by perturbation theory in Quantum Chromodynamics, Zh. Eksp. Teor. Fiz.73, 1216–1240 (1977) [Sov. Phys. JETP 46, 641–653 (1977)]
1977
-
[9]
J. C. Collins, D. E. Soper, and G. Sterman, Factorization of Hard Processes in QCD, Adv. Ser. Direct. High Energy Phys.5, 1–91 (1989) doi:10.1142/9789814503266 0001 [arXiv:hep-ph/0409313 [hep-ph]]
-
[10]
On consistency of the interacting (anti)holomorphic higher-spin sector
S. Alekhin, M. V. Garzelli, S. Moch, and O. Zenaiev, De- termination of the strong coupling from high-energy data, Eur. Phys. J. C86(2026) 161 doi:10.1140/epjc/s10052- 026-15403-x [arXiv:2510.21435 [hep-ph]]
-
[11]
S. Alekhin and S. Moch, Heavy-quark deep-inelastic scattering with a running mass, Phys. Lett. B 699(2011) 345–353 doi:10.1016/j.physletb.2011.04.026 [arXiv:1011.5790 [hep-ph]]
-
[12]
S. Alekhin, K. Daum, K. Lipka and S. Moch, Deter- mination of the charm-quark mass in the MS scheme using charm production data from deep inelastic scat- tering at HERA, Phys. Lett. B718(2012) 550– 557 doi:10.1016/j.physletb.2012.11.010 [arXiv:1209.0436 [hep-ph]]
-
[13]
D. J. Gross and F. Wilczek, Asymptotically Free Gauge Theories. I, Phys. Rev. D8, 3633–3652 (1973) doi:10.1103/PhysRevD.8.3633
-
[14]
D. J. Gross and F. Wilczek, Asymptotically free gauge theories. II, Phys. Rev. D9, 980–993 (1974) doi:10.1103/PhysRevD.9.980
-
[15]
E. G. Floratos, D. A. Ross, and C. T. Sachrajda, Higher-order effects in asymptotically free gauge theo- ries: The anomalous dimensions of Wilson operators, Nucl. Phys. B129, 66–88 (1977);139, 545–546(E) (1978) doi: 10.1016/0550-3213(77)90020-7; doi:10.1016/0550- 3213(78)90367-X
-
[19]
W. Furmanski and R. Petronzio, Singlet parton densities beyond leading order, Phys. Lett. B97, 437–442 (1980) doi:10.1016/0370-2693(80)90636-X
-
[21]
S. A. Larin, P. Nogueira, T. van Ritbergen, and J. A. M. Vermaseren, The 3-loop QCD calculation of the moments of deep inelastic structure functions, Nucl. Phys. B492, 338–378 (1997) doi:10.1016/S0550- 3213(97)80038-7 [arXiv:hep-ph/9605317 [hep-ph]]
-
[22]
S. Moch, J. A. M. Vermaseren, and A. Vogt, The three-loop splitting functions in QCD: the non- singlet case, Nucl. Phys. B688, 101–134 (2004) doi:10.1016/j.nuclphysb.2004.03.030 [hep-ph/0403192]
-
[23]
A. Vogt, S. Moch, and J. A. M. Vermaseren, The three-loop splitting functions in QCD: the sin- glet case, Nucl. Phys. B691, 129–181 (2004) doi:10.1016/j.nuclphysb.2004.04.024 [hep-ph/0404111]
-
[24]
J. Ablinger, A. Behring, J. Bl¨ umlein, A. De Freitas, A. von Manteuffel, and C. Schneider, The 3-loop pure sin- glet heavy flavor contributions to the structure function F2(x, Q2) and the anomalous dimension, Nucl. Phys. B 890, 48–151 (2014) doi:10.1016/j.nuclphysb.2014.10.008 [arXiv:1409.1135 [hep-ph]]
-
[25]
J. Bl¨ umlein, P. Marquard, C. Schneider, and K. Sch¨ onwald, The three-loop unpolarized and po- larized non-singlet anomalous dimensions from off shell operator matrix elements, Nucl. Phys. B971, 115542 (2021) doi:10.1016/j.nuclphysb.2021.115542 [arXiv:2107.06267 [hep-ph]]
-
[26]
J. Bl¨ umlein, P. Marquard, C. Schneider, and K. Sch¨ onwald, The massless three-loop Wilson coefficients for the deep-inelastic structure func- tionsF 2,F L,xF 3 andg 1, JHEP11, 156 (2022) doi:10.1007/JHEP11(2022)156 [arXiv:2208.14325 [hep- ph]]
-
[27]
T. Gehrmann, A. von Manteuffel, and T. Z. Yang, Renormalization of twist-two operators in covariant gauge to three loops in QCD, JHEP04, 041 (2023) doi:10.1007/JHEP04(2023)041 [arXiv:2302.00022 [hep- ph]]
-
[28]
J. A. Gracey, Anomalous dimension of non-singlet Wil- son operators atO(1/N f) in deep inelastic scattering, Phys. Lett. B322, 141–146 (1994) doi:10.1016/0370- 2693(94)90502-9 [arXiv:hep-ph/9401214 [hep-ph]]
-
[29]
V. N. Velizhanin, Four loop anomalous dimension of the second moment of the non-singlet twist-2 op- erator in QCD, Nucl. Phys. B860, 288–294 (2012) doi:10.1016/j.nuclphysb.2012.03.006 [arXiv:1112.3954 [hep-ph]]
-
[30]
V. N. Velizhanin, Four-loop anomalous dimension of the third and fourth moments of the nonsinglet twist-2 op- erator in QCD, Int. J. Mod. Phys. A35, 2050199 (2020) doi:10.1142/S0217751X20501997 [arXiv:1411.1331 [hep- ph]]
-
[31]
J. Davies, A. Vogt, B. Ruijl, T. Ueda, and J. A. M. Ver- maseren, Large-n f contributions to the four-loop splitting functions in QCD, Nucl. Phys. B915, 335–362 (2017) doi:10.1016/j.nuclphysb.2016.12.012 [arXiv:1610.07477 [hep-ph]]
-
[32]
S. Moch, B. Ruijl, T. Ueda, J. A. M. Vermaseren, and A. Vogt, Four-loop non-singlet splitting functions in the planar limit and beyond, JHEP10, 041 (2017) doi:10.1007/JHEP10(2017)041 [arXiv:1707.08315 [hep- ph]]
-
[33]
J. Davies and A. Vogt, Absence ofπ 2 terms in physical anomalous dimensions in DIS: Veri- fication and resulting predictions, Phys. Lett. B 776, 189–194 (2018) doi:10.1016/j.physletb.2017.11.036 [arXiv:1711.05267 [hep-ph]]
-
[34]
S. Moch, B. Ruijl, T. Ueda, J. A. M. Vermaseren, and A. Vogt, On quartic colour factors in splitting functions and the gluon cusp anomalous dimension, Phys. Lett. B 782, 627–632 (2018) doi:10.1016/j.physletb.2018.06.017 [arXiv:1805.09638 [hep-ph]]
-
[35]
G. Das, S. Moch, and A. Vogt, Approximate four- loop QCD corrections to the Higgs-boson production cross section, Phys. Lett. B807, 135546 (2020) doi:10.1016/j.physletb.2020.135546 [arXiv:2004.00563 [hep-ph]]
-
[36]
S. Moch, B. Ruijl, T. Ueda, J. A. M. Ver- maseren, and A. Vogt, Low moments of the four- loop splitting functions in QCD, Phys. Lett. B 825, 136853 (2022) doi:10.1016/j.physletb.2021.136853 [arXiv:2111.15561 [hep-ph]]
-
[37]
G. Falcioni, F. Herzog, S. Moch, and A. Vogt, Four-loop splitting functions in QCD – The quark- quark case, Phys. Lett. B842, 137944 (2023) doi:10.1016/j.physletb.2023.137944 [arXiv:2302.07593 [hep-ph]]
-
[38]
T. Gehrmann, A. von Manteuffel, V. Sotnikov, and T.-Z. Yang, CompleteN 2 f contributions to four-loop pure-singlet splitting functions, JHEP01, 029 (2024) doi:10.1007/JHEP01(2024)029 [arXiv:2308.07958 [hep- ph]]
-
[39]
G. Falcioni, F. Herzog, S. Moch, and A. Vogt, Four-loop splitting functions in QCD – The gluon- to-quark case, Phys. Lett. B846, 138215 (2023) doi:10.1016/j.physletb.2023.138215 [arXiv:2307.04158 [hep-ph]]
-
[40]
G. Falcioni, F. Herzog, S. Moch, J. Vermaseren, and A. Vogt, The double fermionic contribution to the four- loop quark-to-gluon splitting function, Phys. Lett. B 848, 138351 (2024) doi:10.1016/j.physletb.2023.138351 [arXiv:2310.01245 [hep-ph]]
-
[41]
S. Moch, B. Ruijl, T. Ueda, J. Vermaseren, and A. Vogt, Additional moments andx-space approximations of four-loop splitting functions in QCD, Phys. Lett. B 849, 138468 (2024) doi:10.1016/j.physletb.2024.138468 [arXiv:2310.05744 [hep-ph]]
-
[42]
T. Gehrmann, A. von Manteuffel, V. Sotnikov, and T.-Z. Yang, TheN f C 3 F contribution to the non-singlet splitting function at four-loop order, Phys. Lett. B 849, 138427 (2024) doi:10.1016/j.physletb.2023.138427 [arXiv:2310.12240 [hep-ph]]
-
[43]
G. Falcioni, F. Herzog, S. Moch, A. Pelloni, and A. Vogt, Four-loop splitting functions in QCD – The quark-to-gluon case,” Phys. Lett. B856, 138906 (2024) 7 doi:10.1016/j.physletb.2024.138906 [arXiv:2404.09701 [hep-ph]]
-
[44]
G. Falcioni, F. Herzog, S. Moch, and S. Van Thuren- hout, Constraints for twist-two alien operators in QCD, JHEP11, 080 (2024) doi:10.1007/JHEP11(2024)080 [arXiv:2409.02870 [hep-ph]]
-
[45]
G. Falcioni, F. Herzog, S. Moch, A. Pelloni, and A. Vogt, Four-loop splitting functions in QCD – the gluon-gluon case –, Phys. Lett. B860, 139194 (2025) doi:10.1016/j.physletb.2024.139194 [arXiv:2410.08089 [hep-ph]]
-
[46]
B. A. Kniehl and V. N. Velizhanin, Four-Loop Anomalous Dimension of Flavor Nonsinglet Twist- Two Operator of General Lorentz Spin in QCD: ζ(3) Term, Phys. Rev. Lett.134, 131901 (2025) doi:10.1103/PhysRevLett.134.131901 [arXiv:2503.20422 [hep-ph]]
-
[47]
B. A. Kniehl, S. Moch, V. N. Velizhanin, and A. Vogt, Flavor Nonsinglet Splitting Functions at Four Loops in QCD: Fermionic Contributions, Phys. Rev. Lett.135, 071902 (2025) doi:10.1103/hkg5-88hr [arXiv:2505.09381 [hep-ph]]
-
[48]
G. Falcioni, F. Herzog, S. Moch, A. Pelloni, and A. Vogt, Additional results on the four-loop flavour- singlet splitting functions in QCD, Phys. Lett. B 875, 140278 (2026) doi:10.1016/j.physletb.2026.140278 [arXiv:2512.10783 [hep-ph]]
-
[49]
B. A. Kniehl and V. N. Velizhanin, Four-loop anomalous dimension of flavor non-singlet quark operator of twist two and Lorentz spinNfor general gauge group: tran- scendental part, submitted to Nucl. Phys. B
-
[50]
The four-loop non-singlet splitting functions in QCD
T. Gehrmann, A. von Manteuffel, V. Sotnikov, and T. Yang, The four-loop non-singlet splitting functions in QCD, [arXiv:2604.09534 [hep-ph]]
work page internal anchor Pith review Pith/arXiv arXiv
-
[51]
M. Jamin and R. Miravitllas, Absence of even- integerζ-function values in Euclidean physical quan- tities in QCD, Phys. Lett. B779, 452–455 (2018) doi:10.1016/j.physletb.2018.02.030 [arXiv:1711.00787 [hep-ph]]
-
[52]
P. A. Baikov and K. G. Chetyrkin, The struc- ture of generic anomalous dimensions and no-πtheo- rem for massless propagators, JHEP06, 141 (2018) doi:10.1007/JHEP06(2018)141 [arXiv:1804.10088 [hep- ph]]
-
[53]
J. A. M. Vermaseren, Harmonic sums, Mellin transforms and integrals, Int. J. Mod. Phys. A14(1999) 2037–2076 doi:10.1142/S0217751X99001032 [arXiv:hep-ph/9806280 [hep-ph]]
-
[54]
A. K. Lenstra, H. W. Lenstra, and L. Lov´ asz, Factoring polynomials with rational coefficients, Math. Ann.261, 515–534 (1982) doi:10.1007/BF01457454
-
[55]
Albrech, D
M. Albrech, D. Cad´ e, X. Pujol, and D. Stehl´ e (The FPLLL development team),fplll, a lattice reduction library, 2016, available at https://github.com/fplll/fplll
2016
-
[56]
V. N. Velizhanin, Six-loop anomalous dimension of twist-three operators inN= 4 SYM, JHEP11, 129 (2010) doi:10.1007/JHEP11(2010)129 [arXiv:1003.4717 [hep-th]]
-
[57]
V. N. Velizhanin, Twist-2 at five loops: wrapping cor- rections without wrapping computations, JHEP06, 108 (2014) doi:10.1007/JHEP06(2014)108 [arXiv:1311.6953 [hep-th]]
-
[58]
C. Marboe, V. Velizhanin, and D. Volin, Six-loop anomalous dimension of twist-two operators in pla- narN= 4 SYM theory, JHEP07, 084 (2015) doi:10.1007/JHEP07(2015)084 [arXiv:1412.4762 [hep- th]]
-
[59]
C. Marboe and V. Velizhanin, Twist-2 at seven loops in planarN= 4 SYM theory: full re- sult and analytic properties, JHEP11, 013 (2016) doi:10.1007/JHEP11(2016)013 [arXiv:1607.06047 [hep- th]]
-
[60]
B. A. Kniehl and V. N. Velizhanin, Nonplanar cusp and transcendental anomalous dimension at four loops inN= 4 supersymmetric Yang- Mills theory, Phys. Rev. Lett.126, 061603 (2021) doi:10.1103/PhysRevLett.126.061603 [arXiv:2010.13772 [hep-th]]
-
[61]
B. A. Kniehl and V. N. Velizhanin, Non-planar uni- versal anomalous dimension of twist-two operators with general Lorentz spin at four loops inN= 4 SYM theory, Nucl. Phys. B968, 115429 (2021) doi:10.1016/j.nuclphysb.2021.115429 [arXiv:2103.16420 [hep-th]]
- [62]
-
[63]
B. A. Kniehl and V. N. Velizhanin, Anomalous dimen- sions of twist-two operators in extendedN= 2 and N= 4 super Yang-Mills theories, Nucl. Phys. B1001, 116511 (2024) doi:10.1016/j.nuclphysb.2024.116511 [arXiv:2312.05888 [hep-th]]
-
[64]
B. A. Kniehl and V. N. Velizhanin, Nonplanar four-loop anomalous dimensions of twist-two oper- ators inN= 4 supersymmetric Yang-Mills theory: Higher moment, general result, and cusp anoma- lous dimension, Phys. Rev. D111, L061902 (2025) doi:10.1103/PhysRevD.111.L061902 [arXiv:2409.09463 [hep-th]]
-
[65]
V. N. Velizhanin, Three loop anomalous di- mension of the non-singlet transversity opera- tor in QCD, Nucl. Phys. B864, 113–140 (2012) doi:10.1016/j.nuclphysb.2012.06.010 [arXiv:1203.1022 [hep-ph]]
-
[66]
Sun Tzu Suan Ching, 3rd to 5th century AD, see,e.g., D. E. Knuth, The Art of Computer Programming, vol. 1: Fundamental Algorithms, 3rd ed., Adison–Wesley, Read- ing, Massachusetts, 1997
1997
-
[67]
S. Moch, J. A. M. Vermaseren, and A. Vogt, The three-Loop splitting functions in QCD: The helicity- dependent case, Nucl. Phys. B889, 351–400 (2014) doi:10.1016/j.nuclphysb.2014.10.016 [arXiv:1409.5131 [hep-ph]]
-
[68]
Yu. L. Dokshitzer, G. Marchesini, and G. P. Salam, Revisiting parton evolution and the large- xlimit, Phys. Lett. B634, 504–507 (2006) doi:10.1016/j.physletb.2006.02.023 [arXiv:hep- ph/0511302 [hep-ph]]
-
[69]
Yu. L. Dokshitzer and G. Marchesini,N= 4 SUSY Yang-Mills: Three loops made simple(r), Phys. Lett. B 646, 189–201 (2007) doi:10.1016/j.physletb.2007.01.016 [arXiv:hep-th/0612248 [hep-th]]
-
[70]
B. Basso and G. P. Korchemsky, Anomalous dimensions of high-spin operators beyond the leading order, Nucl. Phys. B775, 1–30 (2007) doi:10.1016/j.nuclphysb.2007.03.044 [arXiv:hep- th/0612247 [hep-th]]. 8
-
[71]
D. J. Gross and F. Wilczek, Ultraviolet Behavior of Non- Abelian Gauge Theories, Phys. Rev. Lett.30(1973) 1343–1346 doi:10.1103/PhysRevLett.30.1343
-
[72]
H. D. Politzer, Reliable Perturbative Results for Strong Interactions?, Phys. Rev. Lett.30(1973) 1346–1349 doi:10.1103/PhysRevLett.30.1346
-
[73]
D. R. T. Jones, Two-loop diagrams in Yang-Mills the- ory, Nucl. Phys. B75(1974) 531–538 doi:10.1016/0550- 3213(74)90093-5
-
[74]
W. E. Caswell, Asymptotic Behavior of Non-Abelian Gauge Theories to Two-Loop Order, Phys. Rev. Lett. 33(1974) 244–246 doi:10.1103/PhysRevLett.33.244
-
[75]
O. V. Tarasov, A. A. Vladimirov, and A. Yu. Zharkov, The gell-mann-low function of QCD in the three- loop approximation, Phys. Lett. B93(1980) 429–432 doi:10.1016/0370-2693(80)90358-5
-
[76]
S. A. Larin and J. A. M. Vermaseren, The three-loop QCDβ-function and anomalous dimensions, Phys. Lett. B303(1993) 334–336 doi:10.1016/0370-2693(93)91441- O [arXiv:hep-ph/9302208 [hep-ph]]
-
[77]
T. van Ritbergen, J. A. M. Vermaseren, and S. A. Larin, The four-loopβ-function in quantum chromodynamics, Phys. Lett. B400, 379–384 (1997) doi:10.1016/S0370- 2693(97)00370-5 [arXiv:hep-ph/9701390 [hep-ph]]
-
[78]
K. G. Chetyrkin, Four-loop renormalization of QCD: Full set of renormalization constants and anomalous dimensions, Nucl. Phys. B710, 499–510 (2005) doi:10.1016/j.nuclphysb.2005.01.011 [arXiv:hep- ph/0405193 [hep-ph]]
-
[79]
Czakon, The four-loop QCDβ-function and anomalous dimensions, Nucl
M. Czakon, The four-loop QCDβ-function and anomalous dimensions, Nucl. Phys. B710, 485–498 (2005) doi:10.1016/j.nuclphysb.2005.01.012 [arXiv:hep- ph/0411261 [hep-ph]]
-
[80]
T. Luthe, A. Maier, P. Marquard, and Y. Schr¨ oder, Towards the five-loop Beta function for a general gauge group, JHEP07, 127 (2016) doi:10.1007/JHEP07(2016)127 [arXiv:1606.08662 [hep- ph]]
-
[81]
P. A. Baikov, K. G. Chetyrkin, and J. H. K¨ uhn, Five-Loop Running of the QCD Coupling Con- stant, Phys. Rev. Lett.118, 082002 (2017) doi:10.1103/PhysRevLett.118.082002 [arXiv:1606.08659 [hep-ph]]
-
[82]
The five- loop beta function of Yang-Mills theory with fermions,
F. Herzog, B. Ruijl, T. Ueda, J. A. M. Vermaseren, and A. Vogt, The five-loop beta function of Yang- Mills theory with fermions, JHEP02, 090 (2017) doi:10.1007/JHEP02(2017)090 [arXiv:1701.01404 [hep- ph]]
-
[83]
The five-loop Beta function for a general gauge group and anomalous dimensions beyond Feynman gauge,
T. Luthe, A. Maier, P. Marquard, and Y. Schr¨ oder, The five-loop Beta function for a general gauge group and anomalous dimensions beyond Feynman gauge, JHEP10, 166 (2017) doi:10.1007/JHEP10(2017)166 [arXiv:1709.07718 [hep-ph]]
-
[84]
H. Chen, T.-Z. Yang, H.-X. Zhu, and Y.-J. Zhu, Ana- lytic continuation and reciprocity relation for collinear splitting in QCD, Chin. Phys. C45(2021) 043101 doi:10.1088/1674-1137/abde2d [arXiv:2006.10534 [hep- ph]]
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.