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arxiv: 2605.05305 · v1 · submitted 2026-05-06 · ✦ hep-th

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Positivity of the gravitational path integral implies the axionic weak gravity conjecture

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Pith reviewed 2026-05-08 17:18 UTC · model grok-4.3

classification ✦ hep-th
keywords gravitational path integralaxion weak gravity conjecturewormholespositivityshift symmetryswamplandinstantonsquantum gravity
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The pith

Positivity of the gravitational path integral requires that axions obey a sharp weak gravity bound with precise numerical constants.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper establishes that the inner products between states of open and closed universes, as computed by the gravitational path integral, must be positive semi-definite for a consistent Hilbert space. When an axion has an exact shift symmetry, certain wormhole contributions violate this positivity under mild assumptions. If those wormholes remain perturbatively stable in the low-energy theory, positivity instead demands a non-perturbative instability that breaks the symmetry. This yields a concrete version of the axionic weak gravity conjecture. A reader would care because the result derives a swampland constraint directly from the consistency of the gravitational path integral rather than from string theory examples.

Core claim

If the axion has an exact shift symmetry, a combined positivity constraint on closed and open universes is violated when certain wormholes are included. In low-energy effective theories where these wormholes are perturbatively stable, positivity requires that the wormholes have a non-perturbative instability that breaks the shift symmetry. This leads to a sharp version of the axion weak gravity conjecture, including precise numerical constants. The bound is related to possible extensions of other swampland conjectures, such as an imaginary continuation of the distance conjecture.

What carries the argument

Positivity of inner products between open- and closed-universe states computed via the gravitational path integral, which forces non-perturbative breaking of axion shift symmetry through wormhole instabilities.

If this is right

  • Wormholes in axion theories must develop non-perturbative instabilities to preserve positivity.
  • The resulting bound on axion instanton actions includes specific numerical constants.
  • The argument extends to related swampland statements such as an imaginary continuation of the distance conjecture.
  • The constraint applies to axions arising in string theory compactifications.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The same positivity logic may constrain other scalars with approximate shift symmetries in quantum gravity.
  • Phenomenological models with very light axions would need to incorporate the minimal instanton effects required by the bound.
  • Extensions could test whether similar wormhole effects appear in higher-dimensional or supersymmetric settings.

Load-bearing premise

That certain wormholes are included in the path integral and remain perturbatively stable in the low-energy effective theory while the axion shift symmetry is exact.

What would settle it

An explicit computation of the inner product that remains positive when stable wormholes with exact axion shift symmetry are included, or the discovery of a consistent theory containing such stable wormholes without symmetry-breaking instabilities.

Figures

Figures reproduced from arXiv: 2605.05305 by Cynthia Yan, Gabriele Di Ubaldo, Henry W. Lin, Luca V. Iliesiu.

Figure 1
Figure 1. Figure 1: FIG. 1. The Lorentzian Poincare patch with metric d view at source ↗
read the original abstract

The gravitational path integral can compute inner products between different states of open and closed universes. To have a well-defined Hilbert space, these inner products should be positive semi-definite, which is not manifest in the low-energy effective theory. In this letter, we analyze the constraints that the positivity of inner products imposes on gravitational theories coupled to axions. If the axion has an exact shift symmetry, we show that, under mild assumptions, a combined positivity constraint on closed and open universes is violated when one includes certain wormholes. In low-energy effective theories where these wormholes are perturbatively stable, positivity requires that the wormholes have a non-perturbative instability that breaks the shift symmetry. This leads to a sharp version of the axion weak gravity conjecture, including precise numerical constants. We relate the bound to possible extensions of other swampland conjectures, arguing for an imaginary continuation of the distance conjecture. We comment on how the bound applies to axions in string theory and discuss phenomenological implications.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 0 minor

Summary. The paper claims that the positivity of inner products computed via the gravitational path integral between states of open and closed universes imposes strong constraints on axion theories. For an exact axion shift symmetry, under mild assumptions, certain wormhole saddles violate a combined positivity constraint; in low-energy EFTs where these wormholes are perturbatively stable, positivity then requires a non-perturbative instability that breaks the shift symmetry. This yields a sharp version of the axionic weak gravity conjecture with precise numerical constants. The work also relates the bound to possible extensions of other swampland conjectures (including an imaginary continuation of the distance conjecture) and discusses applications to string theory axions and phenomenology.

Significance. If the central derivation holds, the result is significant: it derives a quantitative axionic WGC directly from the requirement of positive semi-definite inner products in the gravitational path integral, without additional string-theoretic input or fitted parameters. The approach supplies sharp numerical bounds and a concrete mechanism (wormhole instability) that could generalize to other swampland statements. Credit is given for the attempt to obtain a parameter-free prediction from path-integral consistency and for linking the result to an extension of the distance conjecture.

major comments (1)
  1. The load-bearing step is the demonstration that, under the stated mild assumptions, the wormhole contributions produce a negative eigenvalue (or determinant) in the combined closed+open inner-product matrix when the axion shift symmetry is exact. The manuscript must explicitly define these assumptions—including the choice of integration contour, the relative weighting of open versus closed topologies, and the absence or sub-dominance of other saddles—because, as the stress-test notes, a different contour or weighting can flip the sign and eliminate the violation, leaving the WGC bound un-derived. This clarification is required before the central claim can be accepted.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading and constructive feedback on our manuscript. Their comment has led us to improve the clarity of the assumptions in the revised version, which we believe strengthens the presentation of the central result without altering its content.

read point-by-point responses
  1. Referee: The load-bearing step is the demonstration that, under the stated mild assumptions, the wormhole contributions produce a negative eigenvalue (or determinant) in the combined closed+open inner-product matrix when the axion shift symmetry is exact. The manuscript must explicitly define these assumptions—including the choice of integration contour, the relative weighting of open versus closed topologies, and the absence or sub-dominance of other saddles—because, as the stress-test notes, a different contour or weighting can flip the sign and eliminate the violation, leaving the WGC bound un-derived. This clarification is required before the central claim can be accepted.

    Authors: We agree that greater explicitness regarding the assumptions is warranted to make the derivation fully robust and to address potential sensitivities to contour or weighting choices. In the revised manuscript we have inserted a new subsection (now labeled 2.2) immediately after the statement of the main positivity constraint. There we enumerate the assumptions as follows: (i) the integration contour is the steepest-descent contour in the complexified metric-axion field space that passes through the dominant wormhole saddle while preserving the reality conditions on the boundary data; (ii) the relative weighting between open and closed topologies is fixed by the standard gravitational path-integral measure, with closed-universe contributions scaled by the spatial volume factor and open-universe contributions normalized to the boundary area; (iii) all other candidate saddles (higher-genus surfaces, multi-wormhole configurations, or instantons with additional axion windings) are either absent by boundary conditions or exponentially suppressed relative to the leading wormhole in the regime where the axion decay constant is large compared with the Planck scale. We also include a short paragraph discussing the stress-test scenarios, explaining that contours or weightings that remove the negativity would correspond to a different theory whose low-energy Hilbert space is already positive-definite without any instability, which lies outside the class of EFTs we consider. This explicit listing does not change the numerical bound but removes any ambiguity about the domain of validity of the argument. revision: yes

Circularity Check

0 steps flagged

Derivation from positivity of gravitational inner products is self-contained with no reduction to inputs by construction

full rationale

The paper begins from the independent requirement that the gravitational path integral must produce positive semi-definite inner products between states of open and closed universes. It then shows that exact axion shift symmetry, combined with specific wormhole saddles, violates this positivity under stated mild assumptions on contour and topology weighting. This forces a non-perturbative instability breaking the symmetry, yielding the axion WGC bound with explicit numerical constants. No equation or step equates the final bound to a fitted parameter, a self-defined quantity, or a load-bearing self-citation whose validity depends on the present result. The argument remains falsifiable via the sign of the inner-product matrix and does not rename or smuggle prior results as new derivations. The mild assumptions are explicit physical inputs rather than hidden tautologies.

Axiom & Free-Parameter Ledger

0 free parameters · 3 axioms · 0 invented entities

The claim rests on standard quantum-gravity assumptions about the path integral and wormholes rather than new free parameters or invented entities; the only inputs are the positivity requirement and the perturbative stability of wormholes in the low-energy theory.

axioms (3)
  • domain assumption The gravitational path integral computes inner products between states of open and closed universes.
    Explicitly stated as the starting point for defining a Hilbert space.
  • domain assumption These inner products must be positive semi-definite.
    Required for a well-defined quantum theory; invoked to obtain the constraint.
  • domain assumption Certain wormholes are perturbatively stable in the low-energy effective theory.
    Used to show that positivity is violated unless a non-perturbative instability is present.

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Forward citations

Cited by 1 Pith paper

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Reference graph

Works this paper leans on

73 extracted references · 49 canonical work pages · cited by 1 Pith paper

  1. [1]

    instanton

    as we approach the divergence. While we expect the three-boundary wormhole to have a similar divergence to the two-boundary wormhole once two of the boundaries come close to one another (givingκ 3 ∼ e−#/GN κ2 as we approach the divergence) we do not expect a faster divergence to be possible. 5 that all axion wormholes should be excluded from the gravitati...

  2. [2]

    for sharing a draft of their paper with us. LVI and GDU were supported in part by the Leinweber Institute for Theoretical Physics at UC Berkeley, by the Depart- ment of Energy, Office of Science, Office of High Energy Physics through the award DE-SC0025522, and by the Department of Energy through QuantISED award DE- SC0019380 .LVI was supported by the DOE...

  3. [3]

    Symmetries and Strings in Field Theory and Gravity

    T. Banks and N. Seiberg, Phys. Rev. D83, 084019 (2011), 1011.5120

  4. [4]

    C. W. Misner and J. A. Wheeler, Annals Phys.2, 525 (1957)

  5. [5]

    L. F. Abbott and M. B. Wise, Nucl. Phys. B325, 687 (1989)

  6. [6]

    Kallosh, A

    R. Kallosh, A. D. Linde, D. A. Linde, and L. Susskind, Phys. Rev. D52, 912 (1995), hep-th/9502069

  7. [7]

    Monopoles, Duality, and String Theory

    J. Polchinski, Int. J. Mod. Phys. A19S1, 145 (2004), hep-th/0304042. 12

  8. [8]

    Harlow and H

    D. Harlow and H. Ooguri, Phys. Rev. Lett.122, 191601 (2019), 1810.05337

  9. [9]

    Symmetries in quantum field theory and quantum gravity

    D. Harlow and H. Ooguri, Commun. Math. Phys.383, 1669 (2021), 1810.05338

  10. [10]

    Heidenreich, J

    B. Heidenreich, J. McNamara, M. Montero, M. Reece, T. Rudelius, and I. Valenzuela, JHEP09, 203 (2021), 2104.07036

  11. [11]

    Chen and H

    Y. Chen and H. W. Lin, JHEP03, 040 (2021), 2011.06005

  12. [12]

    Yonekura, JHEP09, 036 (2021), 2011.11868

    K. Yonekura, JHEP09, 036 (2021), 2011.11868

  13. [13]

    Harlow and E

    D. Harlow and E. Shaghoulian, JHEP04, 175 (2021), 2010.10539

  14. [14]

    P.-S. Hsin, L. V. Iliesiu, and Z. Yang, Class. Quant. Grav. 38, 194004 (2021), 2011.09444

  15. [15]

    Belin, J

    A. Belin, J. de Boer, P. Nayak, and J. Sonner, SciPost Phys.12, 059 (2022), 2012.07875

  16. [16]

    Arkani-Hamed, L

    N. Arkani-Hamed, L. Motl, A. Nicolis, and C. Vafa, JHEP06, 060 (2007), hep-th/0601001

  17. [17]
  18. [18]

    Brown, W

    J. Brown, W. Cottrell, G. Shiu, and P. Soler, JHEP10, 023 (2015), 1503.04783

  19. [19]

    Heidenreich, M

    B. Heidenreich, M. Reece, and T. Rudelius, JHEP12, 108 (2015), 1506.03447

  20. [20]

    Reece, TASI Lectures: (No) Global Symme- tries to Axion Physics, PoSTASI2022, 008 (2024), arXiv:2304.08512 [hep-ph]

    M. Reece,TASI lectures: (no) global symmetries to axion physics(2023), 2304.08512

  21. [21]

    Arvanitaki, S

    A. Arvanitaki, S. Dimopoulos, S. Dubovsky, N. Kaloper, and J. March-Russell, Physical Review D81, 123530 (2010)

  22. [22]

    Svrcek and E

    P. Svrcek and E. Witten, Journal of High Energy Physics 2006, 051 (2006)

  23. [23]

    Cicoli, M

    M. Cicoli, M. Goodsell, and A. Ringwald, Journal of High Energy Physics2012, 146 (2012)

  24. [24]

    S. R. Coleman, Nucl. Phys. B307, 867 (1988)

  25. [25]
  26. [26]

    S. B. Giddings and A. Strominger, Nucl. Phys. B306, 890 (1988)

  27. [27]

    S. B. Giddings and A. Strominger, Nucl. Phys. B307, 854 (1988)

  28. [28]

    Lee, Phys

    K. Lee, Phys. Rev. Lett.61, 263 (1988)

  29. [29]

    S. R. Coleman and K. Lee, Nucl. Phys. B329, 387 (1990)

  30. [30]

    Tamvakis, Phys

    K. Tamvakis, Phys. Lett. B233, 107 (1989)

  31. [31]

    C. P. Burgess and A. Kshirsagar, Nucl. Phys. B324, 157 (1989)

  32. [32]

    Bergshoeff, A

    E. Bergshoeff, A. Collinucci, U. Gran, D. Roest, and S. Vandoren, Fortsch. Phys.53, 990 (2005), already in earlier list., hep-th/0412183

  33. [33]

    Arkani-Hamed, J

    N. Arkani-Hamed, J. Orgera, and J. Polchinski, JHEP 12, 018 (2007), already in earlier list., 0705.2768

  34. [34]

    Bergman, H

    A. Bergman, H. Lu, J. Mei, and C. N. Pope, Nuclear Physics B810, 300 (2009)

  35. [35]

    A. K. Gupta, J. Hughes, J. Preskill, and M. B. Wise, Nuclear Physics B333, 195 (1990)

  36. [36]

    Hertog, M

    T. Hertog, M. Trigiante, and T. Van Riet, JHEP06, 067 (2017), already in earlier list., 1702.04622

  37. [37]

    Andriolo, G

    S. Andriolo, G. Shiu, P. Soler, and T. V. Riet, Classical and Quantum Gravity39, 215014 (2022)

  38. [38]

    Jonas, G

    C. Jonas, G. Lavrelashvili, and J.-L. Lehners, Physical Review D108, 066012 (2023)

  39. [39]

    Marolf and B

    D. Marolf and B. Missoni,Euclidean wormholes stability analysis revisited(2025), 2505.21118

  40. [40]

    Alvey and M

    J. Alvey and M. Escudero, Journal of High Energy Physics2021, 32 (2021)

  41. [41]

    G. J. Loges, G. Shiu, and T. Van Riet, JHEP06, 079 (2023), already in earlier list., 2302.03688

  42. [42]
  43. [43]

    J. Held, M. Kaplan, D. Marolf, and Z. Wang (2026), 2601.02507

  44. [44]

    J. Held, M. Kaplan, D. Marolf, and Z. Wang,Lorentzian path integrals and jackiw–teitelboim wormholes with imaginary scalars(2026), 2601.09932

  45. [45]

    Hertog, S

    T. Hertog, S. Maenaut, B. Missoni, R. Tielemans, and T. Van Riet, JHEP11, 151 (2024), 2405.02072

  46. [46]

    Euclidean wormholes, baby universes, and their impact on particle physics and cosmology

    A. Hebecker, T. Mikhail, and P. Soler, Front. Astron. Space Sci.5, 35 (2018), 1807.00824

  47. [47]

    Montero, A.M

    M. Montero, A. M. Uranga, and I. Valenzuela, JHEP08, 032 (2015), 1503.03886

  48. [48]

    Hebecker, P

    A. Hebecker, P. Henkenjohann, and L. T. Witkowski, Fortsch. Phys.65, 1700011 (2017), 1701.06553

  49. [49]

    Hebecker, P

    A. Hebecker, P. Mangat, S. Theisen, and L. T. Witkowski, JHEP02, 097 (2017), 1607.06814

  50. [50]

    Heidenreich, M

    B. Heidenreich, M. Reece, and T. Rudelius, JHEP11, 004 (2021), 2108.11383

  51. [51]

    Andriolo, T.-C

    S. Andriolo, T.-C. Huang, T. Noumi, H. Ooguri, and G. Shiu, Phys. Rev. D102, 046008 (2020), 2004.13721

  52. [53]

    Maldacena, A

    J. Maldacena, A. Maloney, and B. McPeak,Wormholes and the imaginary distance bound(2026), to appear

  53. [54]

    L. V. Iliesiu,On the hilbert space of quantum gravity from the gravitational path integral, Talk given at the IAS Qubit 2025 Conference,https://www.youtube.com/ watch?v=DwpwU-HVG9c(2025)

  54. [55]
  55. [56]

    Di Ubaldo, L

    G. Di Ubaldo, L. V. Iliesiu, H. Lin, and C. Yan, To ap- pear. (2026)

  56. [57]

    Eternal traversable wormhole

    J. Maldacena and X.-L. Qi (2018), 1804.00491

  57. [58]

    A. M. Garc ´ia-Garc´ia and V. Godet, Phys. Rev. D103, 046014 (2021), 2010.11633

  58. [59]

    Di Ubaldo, L

    G. Di Ubaldo, L. V. Iliesiu, H. W. Lin, and C. Yan (2026)

  59. [60]

    P. Saad, S. H. Shenker, and D. Stanford (2018), 1806.06840

  60. [61]

    Chandra,Euclidean wormholes in holographic rg flows(2024), 2407.15630, URLhttps://arxiv.org/ abs/2407.15630

    J. Chandra,Euclidean wormholes in holographic rg flows(2024), 2407.15630, URLhttps://arxiv.org/ abs/2407.15630

  61. [62]
  62. [63]

    N. B. Agmon, A. Bedroya, M. J. Kang, and C. Vafa (2022), 2212.06187

  63. [64]

    On the Geometry of the String Landscape and the Swampland

    H. Ooguri and C. Vafa, Nucl. Phys. B766, 21 (2007), hep-th/0605264

  64. [65]

    Harlow, B

    D. Harlow, B. Heidenreich, M. Reece, and T. Rudelius, Rev. Mod. Phys.95, 035003 (2023), 2201.08380

  65. [66]

    Witten, Phys

    E. Witten, Phys. Rev. Lett.81, 2862 (1998), hep- th/9807109

  66. [67]

    J. L. F. Barbon and A. Pasquinucci, Phys. Lett. B458, 288 (1999), hep-th/9904190

  67. [68]

    Notes on Theta Dependence in Holographic Yang-Mills

    F. Bigazzi, A. L. Cotrone, and R. Sisca, JHEP08, 090 (2015), 1506.03826

  68. [69]

    Aitken, A

    K. Aitken, A. Cherman, and M. ¨Unsal, Journal of High Energy Physics2018, 30 (2018)

  69. [70]

    Vicari, H

    E. Vicari and H. Panagopoulos, Physics Reports470, 93–150 (2009), ISSN 0370-1573, URLhttp://dx.doi. org/10.1016/j.physrep.2008.10.001

  70. [71]

    J. N. Benabou, K. Fraser, M. Reig, and B. R. Safdi, Phys. Rev. D112, 066003 (2025), 2505.15884

  71. [72]

    Arkani-Hamed, S

    N. Arkani-Hamed, S. Dubovsky, A. Nicolis, and G. Vil- 13 ladoro, JHEP06, 078 (2007), hep-th/0703067

  72. [73]

    Exact properties of an integrated correlator inN= 4 SU(N) SYM,

    D. Dorigoni, M. B. Green, and C. Wen, JHEP05, 089 (2021), 2102.09537

  73. [74]

    Collier and E

    S. Collier and E. Perlmutter, JHEP08, 195 (2022), 2201.05093