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Chiral anomalies and Wilson fermions

Michael Creutz*

  • *Contact author: mike@latticeguy.net

Phys. Rev. D 113, 074516 – Published 21 April, 2026

DOI: https://doi.org/10.1103/pbpl-5wdb

Abstract

The Wilson formulation of fermions in lattice gauge theory provides a unified description of the chiral anomalies in the standard model. The discrete Dirac operator diagonalizes into a series of 2×2 blocks. In each block the possible eigenvalues either form a complex pair or separate into two real eigenvalues that have specific chirality. The collision of these pairs of eigenvalues occurs outside the perturbative region and provides a path between topological sectors.

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References (24)

  1. J. Steinberger, Phys. Rev. 76, 1180 (1949).
  2. S. L. Adler, Phys. Rev. 177, 2426 (1969).
  3. S. L. Adler and W. A. Bardeen, Phys. Rev. 182, 1517 (1969).
  4. J. Bell and R. Jackiw, Nuovo Cimento A 60, 47 (1969).
  5. G. ’t Hooft, Phys. Rev. D 14, 3432 (1976).
  6. J. Smit, Eur. Phys. J. H 50, 5 (2025).
  7. J. Smit, Acta Phys. Pol. B 17, 531 (1986).
  8. P. V. D. Swift, Phys. Lett. 145B, 256 (1984).
  9. J. Smit and J. C. Vink, Nucl. Phys. B286, 485 (1987).
  10. S. Itoh, Y. Iwasaki, and T. Yoshie, Phys. Lett. B 184, 375 (1987).
  11. S. Itoh, Y. Iwasaki, and T. Yoshie, Phys. Rev. D 36, 527 (1987).
  12. M. Creutz, Phys. Rev. D 109, 034514 (2024).
  13. S. Duane, A. Kennedy, B. Pendleton, and D. Roweth, Phys. Lett. B 195, 216 (1987).
  14. K. G. Wilson, Phys. Rev. D 10, 2445 (1974).
  15. W. Pauli and F. Villars, Rev. Mod. Phys. 21, 434 (1949).
  16. Notice an analogy with the connection between the Lorentz group and the group SL(2)C, where vectors also divide into two classes: time- and spacelike.

  17. M. Luscher, J. High Energy Phys. 06 (2000) 028.
  18. M. Creutz, Ann. Phys. (Amsterdam) 326, 911 (2011).
  19. M. Teper, Phys. Lett. 162B, 357 (1985).
  20. H. Neuberger, Phys. Lett. B 417, 141 (1998).
  21. M. Creutz, Nucl. Phys. B, Proc. Suppl. 119, 837 (2003).
  22. This is consistent with the strong gauge group since in SU(3) the product of two triplet representations contains an antitriplet, i.e. 3⊗3=6⊕3¯.

  23. E. Seiler and I. Stamatescu, Phys. Rev. D 25, 2177 (1982).
  24. F. Karsch, E. Seiler, and I. O. Stamatescu, Nucl. Phys. B271, 349 (1986).

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