Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access

Beyond the Dilute Instanton Gas: Resurgence with Exact Saddles in the Double Well

Aurélien Dersy and Matthew D. Schwartz

Phys. Rev. Lett. 137, 181601 – Published 27 October, 2026

DOI: https://doi.org/10.1103/hg9t-ypvf

Abstract

The path-integral approach to the double well has long been limited by the dilute instanton gas approximation. We show that if the finite Euclidean-time structure is taken seriously by using exact saddles, the dilute gas can be sidestepped, allowing the partition function and energy levels to be computed systematically. At each instanton order, the full resurgent structure—which saddles contribute, what asymptotic growth is expected, and how ambiguities cancel—is encoded in a finite-dimensional Picard-Lefschetz contour integral over the quasizero modes with a clear geometric interpretation. Working at finite T is essential: the dilute instanton gas can only access the ground-state splitting, whereas the exact finite-T computation systematically produces the nonperturbative energy splittings for all excited states, including their full dependence on the level number. The key ingredients—Weierstrass elliptic functions for the saddles, Lamé operators for the fluctuations, and Picard-Fuchs equations for the periods—form a coherent mathematical framework that both overlaps and complements that of exact WKB.

View figure in article

Physics Subject Headings (PhySH)

Article Text

References (34)

  1. C. M. Bender and T. T. Wu, Anharmonic oscillator, Phys. Rev. 184, 1231 (1969).
  2. E. Brezin, G. Parisi, and J. Zinn-Justin, Perturbation theory at large orders for potential with degenerate minima, Phys. Rev. D 16, 408 (1977).
  3. A. Voros, The return of the quartic oscillator. The complex WKB method, Ann. Inst. Henri Poincare, Sect. A 39, 211 (1983).
  4. H. Dillinger, E. Delabaere, and F. Pham, Résurgence de Voros et périodes des courbes hyperelliptiques, Ann. Inst. Fourier 43, 163 (1993).
  5. E. Delabaere and F. Pham, Resurgent methods in semi-classical asymptotics, Ann. Inst. Henri Poincaré Phys. Théor. 71, 1 (1999).
  6. G. Álvarez, Langer–Cherry derivation of the multi-instanton expansion for the symmetric double well, J. Math. Phys. (N. Y.) 45, 3095 (2004).
  7. G. V. Dunne and M. Ünsal, Generating nonperturbative physics from perturbation theory, Phys. Rev. D 89, 041701 (2014).
  8. B. Bucciotti, T. Reis, and M. Serone, An anharmonic alliance: Exact WKB meets EPT, J. High Energy Phys. 11 (2023) 124.
  9. G. Basar, G. V. Dunne, and M. Unsal, Quantum geometry of resurgent perturbative/nonperturbative relations, J. High Energy Phys. 05 (2017) 087.
  10. J. Gu and M. Marino, Exact multi-instantons in topological string theory, SciPost Phys. 15, 179 (2023).
  11. A. van Spaendonck and M. Vonk, Exact instanton transseries for quantum mechanics, SciPost Phys. 16, 103 (2024).
  12. E. B. Bogomolny, Calculation of instanton–anti-instanton contributions in quantum mechanics, Phys. Lett. 91B, 431 (1980).
  13. J. Zinn-Justin, Multi-instanton contributions in quantum mechanics, Nucl. Phys. B192, 125 (1981).
  14. J. Zinn-Justin and U. D. Jentschura, Multi-instantons and exact results I: Conjectures, WKB expansions, and instanton interactions, Ann. Phys. (Amsterdam) 313, 197 (2004).
  15. J. Zinn-Justin and U. D. Jentschura, Multi-instantons and exact results II: Specific cases, higher-order effects, and numerical calculations, Ann. Phys. (Amsterdam) 313, 269 (2004).
  16. J. L. Richard and A. Rouet, Complex saddle points in the double well oscillator, Nucl. Phys. B183, 251 (1981).
  17. J. L. Richard and A. Rouet, Complex saddle points versus dilute gas approximation in the double well anharmonic oscillator, Nucl. Phys. 185, 47 (1981).
  18. Y. Tanizaki and T. Koike, Real-time Feynman path integral with Picard-Lefschetz theory and its applications to quantum tunneling, Ann. Phys. (Amsterdam) 351, 250 (2014).
  19. N. Nekrasov, Tying up instantons with anti-instantons, in Ludwig Faddeev Memorial Volume (2018), pp. 351–388, arXiv:1802.04202.
  20. A. Behtash, G. V. Dunne, T. Schaefer, T. Sulejmanpasic, and M. Ünsal, Critical points at infinity, non-Gaussian saddles, and bions, J. High Energy Phys. 06 (2018) 068.
  21. A. Bhattacharya, J. Cotler, A. Dersy, and M. D. Schwartz, Collective coordinate fix in the path integral, Phys. Rev. D 110, 116023 (2024).
  22. The imaginary ambiguity coming from the lateral Borel resummation of the asymptotic expansion of Eq. (18) turns out to be independent of the choice of αmin. The real part of the series does, however, depend on αmin. The choice of Seff(αmin)=0 corresponds to fixing the action gap Seff(T/2)−Seff(αmin)=2SI and sets the Borel singularity at t=2SI.

  23. We also use (det⊥Ok,0)−1/2=ZSHO(det O0/det⊥Ok,0)1/2≈ZSHO12k where the last approximation holds at large T.

  24. D. Dorigoni, An introduction to resurgence, trans-series and alien calculus, Ann. Phys. (Amsterdam) 409, 167914 (2019).
  25. N. Sueishi, S. Kamata, T. Misumi, and M. Ünsal, On exact-WKB analysis, resurgent structure, and quantization conditions, J. High Energy Phys. 12 (2020) 114.
  26. S. Coleman, Aspects of Symmetry: Selected Erice Lectures (Cambridge University Press, Cambridge, England, 1985).
  27. G. ’t Hooft, Computation of the quantum effects due to a four-dimensional pseudoparticle, Phys. Rev. D 14, 3432 (1976); 18, 2199(E) (1978).
  28. G. ’t Hooft, Can we make sense out of quantum chromodynamics?, Subnuclear series 15, 943 (1979).
  29. M. Beneke, Renormalons, Phys. Rep. 317, 1 (1999).
  30. A. Bhattacharya, J. Cotler, A. Dersy, and M. D. Schwartz, Renormalons as saddle points, J. High Energy Phys. 04 (2026) 140.
  31. I. I. Balitsky and A. V. Yung, Instanton molecular vacuum in N=1 supersymmetric quantum mechanics, Nucl. Phys. B274, 475 (1986).
  32. T. C. Kraan and P. van Baal, Periodic instantons with nontrivial holonomy, Nucl. Phys. B533, 627 (1998).
  33. K.-M. Lee and C.-h. Lu, SU(2) calorons and magnetic monopoles, Phys. Rev. D 58, 025011 (1998).
  34. P. C. Argyres and M. Unsal, The semi-classical expansion and resurgence in gauge theories: New perturbative, instanton, bion, and renormalon effects, J. High Energy Phys. 08 (2012) 063.

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation