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  • Open Access

Nonperturbative S-Matrix Renormalization

Laurent Freidel1,*, José Padua-Argüelles1,2,†, Susanne Schander1,‡, and Marc Schiffer3,§

  • 1Perimeter Institute, 31 Caroline Street North, Waterloo, Ontario, N2L 2Y5, Canada
  • 2Department of Physics and Astronomy, University of Waterloo, 200 University Avenue West, Waterloo, Ontario, N2L 3G1, Canada
  • 3High Energy Physics Department, Institute for Mathematics, Astrophysics, and Particle Physics, Radboud University, Nijmegen, The Netherlands

  • *Contact author: lfreidel@pitp.ca
  • †Contact author: jpaduaarguelles@pitp.ca
  • ‡Contact author: sschander@pitp.ca
  • §Contact author: marc.schiffer@ru.nl

Phys. Rev. Lett. 136, 251602 – Published 24 June, 2026

DOI: https://doi.org/10.1103/jxcl-q2vt

Abstract

We propose a renormalization group flow equation for a functional that generates S-matrix elements and which captures similarities to the well-known Wetterich and Polchinski equations. While the latter ones, respectively, involve the effective action and Schwinger functional, which are genuine off-shell objects, the presented flow equation has the advantage of working more directly with observables, i.e., scattering amplitudes. Compared to the Wetterich equation, our flow equation also greatly simplifies the notion of going on shell, in the sense of satisfying the quantum equations of motion. In addition, unlike the Wetterich equation, it is polynomial and does not require a Hessian inversion. The approach is a promising direction for nonperturbative quantum field theories, allowing one to work more directly with scattering amplitudes.

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References (44)

  1. S. Kamefuchi, L. O’Raifeartaigh, and A. Salam, Change of variables and equivalence theorems in quantum field theories, Nucl. Phys. 28, 529 (1961).
  2. J. Chisholm, Change of variables in quantum field theories, Nucl. Phys. 26, 469 (1961).
  3. C. Arzt, Reduced effective Lagrangians, Phys. Lett. B 342, 189 (1995).
  4. For early reference on the S-matrix and renormalization in string theory see Refs. [5, 6].

  5. T. Banks and E. J. Martinec, The renormalization group and string field theory, Nucl. Phys. B294, 733 (1987).
  6. J. Hughes, J. Liu, and J. Polchinski, Virasoro-Shapiro from Wilson, Nucl. Phys. B316, 15 (1989).
  7. J. Polchinski, Renormalization and effective Lagrangians, Nucl. Phys. B231, 269 (1984).
  8. C. Wetterich, Exact evolution equation for the effective potential, Phys. Lett. B 301, 90 (1993).
  9. T. R. Morris, The exact renormalization group and approximate solutions, Int. J. Mod. Phys. A 09, 2411 (1994).
  10. U. Ellwanger, Flow equations for N point functions and bound states, Z. Phys. C 62, 503 (1994).
  11. N. Dupuis, L. Canet, A. Eichhorn, W. Metzner, J. M. Pawlowski, M. Tissier, and N. Wschebor, The nonperturbative functional renormalization group and its applications, Phys. Rep. 910, 1 (2021).
  12. W.-j. Fu, C. Huang, J. M. Pawlowski, and Y.-y. Tan, Four-quark scatterings in QCD I, SciPost Phys. 14, 069 (2023).
  13. W.-j. Fu, C. Huang, J. M. Pawlowski, and Y.-y. Tan, Four-quark scatterings in QCD II, SciPost Phys. 17, 148 (2024).
  14. F. Ihssen, J. M. Pawlowski, F. R. Sattler, and N. Wink, Towards quantitative precision in functional QCD I, Phys. Rev. D 113, 094038 (2026).
  15. W.-j. Fu, C. Huang, J. M. Pawlowski, Y.-y. Tan, and L.-j. Zhou, Four-quark scatterings in QCD III, Phys. Rev. D 112, 054047 (2025).
  16. T. Draper, B. Knorr, C. Ripken, and F. Saueressig, Finite quantum gravity amplitudes: No strings attached, Phys. Rev. Lett. 125, 181301 (2020).
  17. T. Draper, B. Knorr, C. Ripken, and F. Saueressig, Graviton-mediated scattering amplitudes from the quantum effective action, J. High Energy Phys. 11 (2020) 136.
  18. Á. Pastor-Gutiérrez, J. M. Pawlowski, M. Reichert, and G. Ruisi, e+e−→μ+μ− in the asymptotically safe standard model, Phys. Rev. D 111, 106005 (2025).
  19. J. Fehre, D. F. Litim, J. M. Pawlowski, and M. Reichert, Lorentzian quantum gravity and the graviton spectral function, Phys. Rev. Lett. 130, 081501 (2023).
  20. I. Y. Aref’eva, A. A. Slavnov, and L. D. Faddeev, Generating functional for the S-matrix in gauge-invariant theories, Teor. Mat. Fiz. 21, 311 (1974).
  21. A. Jevicki and C.-k. Lee, The S matrix generating functional and effective action, Phys. Rev. D 37, 1485 (1988).
  22. The boundary term ensures that on-shell variations of the action are compatible with Dirichlet boundary conditions.

  23. More precisely for a functional F[φ] we adopt the “tensorial” notation F(L)[φ] to encode all “components” F(L)[φ]z1…zL≔δδφ(z1)⋯δδφ(zL)F[φ].As is customary, for small L, we may occasionally denote the number of derivatives with a corresponding number of primes. So, for example, F(2)[φ]=F′′[φ].

    With this notation, index contractions correspond to spacetime integrals. E.g., Tr(F′′[φ0])=∫δδφ(z)δδφ(z)F[φ]|φ=φ0.

  24. V. P. Nair, Quantum Field Theory. A Modern Perspective (Springer, New York, 2004).
  25. See Supplemental Material at http://link.aps.org/supplemental/10.1103/jxcl-q2vt for some details on the derivation of Eq. (5), and for details on the relation to other functional equations.
  26. We caution that the argument relies on the LSZ formalism, which might break down in the presence of long-range interactions [27].

  27. L. Lippstreu, Analytic properties of infrared-finite amplitudes in theories with long-range forces, arXiv:2505.04702.
  28. D. Jain, S. Kundu, S. Minwalla, O. Parrikar, S. G. Prabhu, and P. Shrivastava, The S-matrix and boundary correlators in flat space, J. High Energy Phys. 02 (2026) 151.
  29. S. Kim, P. Kraus, R. Monten, and R. M. Myers, S-matrix path integral approach to symmetries and soft theorems, J. High Energy Phys. 10 (2023) 036.
  30. S. Floerchinger, Analytic continuation of functional renormalization group equations, J. High Energy Phys. 05 (2012) 021.
  31. E. Manrique, S. Rechenberger, and F. Saueressig, Asymptotically safe Lorentzian gravity, Phys. Rev. Lett. 106, 251302 (2011).
  32. J. Fehre, D. F. Litim, J. M. Pawlowski, and M. Reichert, Lorentzian quantum gravity and the graviton spectral function, Phys. Rev. Lett. 130, 081501 (2023).
  33. E. D’Angelo, N. Drago, N. Pinamonti, and K. Rejzner, An algebraic QFT approach to the Wetterich equation on Lorentzian manifolds, Ann. Henri Poincare 25, 2295 (2024).
  34. E. D’Angelo, Asymptotic safety in Lorentzian quantum gravity, Phys. Rev. D 109, 066012 (2024).
  35. F. Saueressig and J. Wang, Foliated asymptotically safe gravity: Lorentzian signature fluctuations from the Wick rotation, Phys. Rev. D 111, 106007 (2025).
  36. J. M. Pawlowski, Aspects of the functional renormalisation group, Ann. Phys. (Amsterdam) 322, 2831 (2007).
  37. H. Gies, Introduction to the functional RG and applications to gauge theories, Lect. Notes Phys. 852, 287 (2012).
  38. F. Ihssen and J. M. Pawlowski, Functional flows for complex effective actions, SciPost Phys. 15, 074 (2023).
  39. F. J. Wegner, Some invariance properties of the renormalization group, J. Phys. C 7, 2098 (1974).
  40. J. Pawlowski and S. Ray (to be published).
  41. R. E. Cutkosky, Singularities and discontinuities of Feynman amplitudes, J. Math. Phys. (N.Y.) 1, 429 (1960).
  42. M. Becker and M. Reuter, Background independent field quantization with sequences of gravity-coupled approximants, Phys. Rev. D 102, 125001 (2020).
  43. L. Freidel, J. Kowalski-Glikman, R. G. Leigh, and D. Minic, Vacuum energy density and gravitational entropy, Phys. Rev. D 107, 126016 (2023).
  44. R. Ferrero and R. Percacci, The cosmological constant problem and the effective potential of a gravity-coupled scalar, J. High Energy Phys. 09 (2024) 074.

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