- Editors' Suggestion
- Open Access
One-Loop QCD Function as an Index
Phys. Rev. Lett. 136, 211601 – Published 29 May, 2026
DOI: https://doi.org/10.1103/5kd5-3724
Abstract
In this Letter, we show that the one-loop QCD function can be obtained from an index theorem on twistor space. This is achieved by recalling that the angle of self-dual gauge theory flows according the one-loop function. Rewriting self-dual gauge theory as a holomorphic theory on twistor space this flow can be computed as the anomaly to scale invariance. The one-loop Weyl anomaly coefficient can be recovered similarly.
Physics Subject Headings (PhySH)
Article Text
Supplemental Material
References (51)
- H. D. Politzer, Phys. Rev. Lett. 30, 1346 (1973).
- D. J. Gross and F. Wilczek, Phys. Rev. D 8, 3633 (1973).
- L. F. Abbott, Nucl. Phys. B185, 189 (1981).
- L. F. Abbott, Acta Phys. Pol. B 13, 33 (1982).
- G. Chalmers and W. Siegel, Phys. Rev. D 54, 7628 (1996).
- A. Losev, I. Polyubin, and A. Rosly, J. High Energy Phys. 02 (2018) 041.
- T. Schäfer and E. V. Shuryak, Rev. Mod. Phys. 70, 323 (1998).
The flow of was computed by a direct Feynman diagram analysis in [6].
- G. ’t Hooft, Phys. Rev. D 14, 3432 (1976); 18, 2199(E) (1978).
- A. I. Vainshtein, V. I. Zakharov, V. A. Novikov, and M. A. Shifman, Sov. Phys. Usp. 25, 195 (1982).
- L. S. Brown and D. B. Creamer, Phys. Rev. D 18, 3695 (1978).
- N. K. Nielsen and B. Schroer, Nucl. Phys. B127, 493 (1977).
- M. F. Atiyah and I. M. Singer, Ann. Math. 93, 119 (1971).
- D. Quillen, Funct. Anal. Appl. 19, 31 (1985).
- J.-M. Bismut and D. S. Freed, Commun. Math. Phys. 106, 159 (1986).
- R. S. Ward, Phys. Lett. 61A, 81 (1977).
- M. Atiyah, N. Hitchin, V. Drinfeld, and Y. I. Manin, Phys. Lett. 65A, 185 (1978).
- A. S. Schwarz, Commun. Math. Phys. 155, 249 (1993).
- A. Borel and J.-P. Serre, Bull. Soc. Math. Fr. 86, 97 (1958).
- F. Hirzebruch, A. Borel, and R. Schwarzenberger, Topological Methods in Algebraic Geometry (Springer Berlin-Heidelberg-New York, 1966), Vol. 175.
- A. Grothendieck et al., Lecture Notes in Mathematics (Springer-Verlag, Berlin-New York, 1971), Vol. 225.
- D. S. Freed, Surveys Diff. Geom. 22, 125 (2017).
- G. Doran, R. Monteiro, and S. Wikeley, J. High Energy Phys. 07 (2024) 139.
For example, the portion of the quantum effective action of a 4D field theory determined by the trace anomaly can be described by a dimension zero scalar field coupling to curvatures [25]. This is reminiscent of the Green-Schwarz mechanism for twistorial anomalies [25][26].
- R. J. Riegert, Phys. Lett. 134B, 56 (1984).
- K. J. Costello, arXiv:2111.08879.
- S. M. Christensen and M. J. Duff, Nucl. Phys. B154, 301 (1979).
- D. M. Capper and M. J. Duff, Nuovo Cimento A 23, 173 (1974).
- M. J. Duff, Nucl. Phys. B125, 334 (1977).
- M. J. Duff, Classical Quantum Gravity 11, 1387 (1994).
- G. W. Gibbons and S. W. Hawking, Phys. Lett. 78B, 430 (1978).
- N. J. Hitchin, Math. Proc. Cambridge Philos. Soc. 85, 465 (1979).
- R. Penrose, Gen. Relativ. Gravit. 7, 31 (1976).
- See Supplemental Material at http://link.aps.org/supplemental/10.1103/5kd5-3724 for details of the index computation for the Weyl anomaly, and for the contributions of a range of massless fields to the gravitational anomaly on twistor space. Supplemental Material includes Refs. [35–39].
- E. S. Fradkin and A. A. Tseytlin, Nucl. Phys. B203, 157 (1982).
- E. S. Fradkin and A. A. Tseytlin, Phys. Lett. B 110, 117 (1982); 126B (1983).
- E. S. Fradkin and A. A. Tseytlin, Phys. Lett. 134B, 187 (1984).
- E. Witten, Commun. Math. Phys. 252, 189 (2004).
- N. Berkovits and E. Witten, J. High Energy Phys. 08 (2004) 009.
- W. E. Caswell, Phys. Rev. Lett. 33, 244 (1974).
- D. R. T. Jones, Nucl. Phys. B75, 531 (1974).
- D. R. T. Jones, Nucl. Phys. B87, 127 (1975).
The two-loop flow of the canonical coupling also receives contributions from Yukawa couplings which are difficult to incorporate on twistor space [44, 45].
- D. R. T. Jones, Phys. Rev. D 25, 581 (1982).
- M. E. Machacek and M. T. Vaughn, Nucl. Phys. B222, 83 (1983).
- V. A. Novikov, M. A. Shifman, A. I. Vainshtein, and V. I. Zakharov, Phys. Lett. 166B, 329 (1986).
- N. Arkani-Hamed and H. Murayama, J. High Energy Phys. 06 (2000) 030.
- C. LeBrun, J. Diff. Geom. 34, 223 (1991).
- R. Bittleston, A. Sharma, and D. Skinner, Commun. Math. Phys. 403, 1543 (2023).
Although we note that the twistorial anomaly coefficient is proportional to the one-loop vacuum energy [51]. It is not clear to us if also has a space-time avatar.
- L. Boyle and N. Turok, arXiv:2110.06258.