- Open Access
Scalar amplitudes from fiber bundle geometry
Phys. Rev. D 113, 076005 – Published 6 April, 2026
DOI: https://doi.org/10.1103/qxwr-1vs6
Abstract
We compute tree-level -point scattering amplitudes in scalar field theories in terms of geometric invariants on a fiber bundle. All 0- and 2-derivative interactions are incorporated into a metric on this bundle. The on-shell amplitudes can be efficiently pieced together from covariant Feynman rules, and we present a general closed formula for obtaining the -point amplitude in this way. The covariant Feynman rules themselves can be derived using a generalization of the normal coordinate expansion of the fiber bundle metric. We demonstrate the efficiency of this approach by computing the covariant Feynman rules up to points, from which one can obtain the full amplitudes using our general formula. The formalism offers a prototype for obtaining geometric amplitudes in theories with higher-derivative interactions, by passing from the fiber bundle to its jet bundles.
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References (51)
- K. Meetz, J. Math. Phys. (N.Y.) 10, 589 (1969).
- G. Ecker and J. Honerkamp, Nucl. Phys. B35, 481 (1971).
- G. A. Vilkovisky, Nucl. Phys. B234, 125 (1984).
- J. Honerkamp, Nucl. Phys. B36, 130 (1972).
- L. Tataru, Phys. Rev. D 12, 3351 (1975).
- L. Alvarez-Gaume, D. Z. Freedman, and S. Mukhi, Ann. Phys. (N.Y.) 134, 85 (1981).
- L. Alvarez-Gaume and D. Z. Freedman, Commun. Math. Phys. 80, 443 (1981).
- M. K. Gaillard, Nucl. Phys. B268, 669 (1986).
- R. Alonso, E. E. Jenkins, and A. V. Manohar, Phys. Lett. B 754, 335 (2016).
- R. Alonso, E. E. Jenkins, and A. V. Manohar, J. High Energy Phys. 08 (2016) 101.
- T. Cohen, N. Craig, X. Lu, and D. Sutherland, J. High Energy Phys. 03 (2021) 237.
- T. Cohen, N. Craig, X. Lu, and D. Sutherland, J. High Energy Phys. 12 (2021) 003.
- R. Alonso and M. West, Phys. Rev. D 105, 096028 (2022).
- R. Alonso, arXiv:2307.14301.
- K. Finn, S. Karamitsos, and A. Pilaftsis, Eur. Phys. J. C 81, 572 (2021).
- A. Helset, E. E. Jenkins, and A. V. Manohar, Phys. Rev. D 106, 116018 (2022).
- B. Assi, A. Helset, A. V. Manohar, J. Pagès, and C.-H. Shen, J. High Energy Phys. 11 (2023) 201.
- V. Gattus and A. Pilaftsis, Phys. Rev. D 110, 105006 (2024).
- B. Assi, A. Helset, J. Pagès, and C.-H. Shen, J. High Energy Phys. 12 (2025) 082.
- N. Craig, I.-K. Lee, and Y.-T. Lee, J. High Energy Phys. 02 (2026) 044.
- C. Cheung, A. Helset, and J. Parra-Martinez, J. High Energy Phys. 04 (2022) 011.
- C. Cheung, A. Helset, and J. Parra-Martinez, Phys. Rev. D 106, 045016 (2022).
- M. Derda, A. Helset, and J. Parra-Martinez, J. High Energy Phys. 06 (2024) 133.
- T. Cohen, I. Fadakar, A. Helset, and F. Nardi, J. High Energy Phys. 08 (2025) 140.
- R. Alonso and M. West, Phys. Lett. B 841, 137937 (2023).
- A. Helset, E. E. Jenkins, and A. V. Manohar, J. High Energy Phys. 02 (2023) 063.
- E. E. Jenkins, A. V. Manohar, L. Naterop, and J. Pagès, J. High Energy Phys. 02 (2024) 131.
- E. E. Jenkins, A. V. Manohar, L. Naterop, and J. Pagès, J. High Energy Phys. 12 (2023) 165.
- P. Aigner, L. Bellafronte, E. Gendy, D. Haslehner, and A. Weiler, J. High Energy Phys. 07 (2025) 167.
- X.-X. Li, X. Lu, and Z. Zhang, J. High Energy Phys. 08 (2025) 102.
- K. Finn, S. Karamitsos, and A. Pilaftsis, Phys. Rev. D 102, 045014 (2020).
- T. Cohen, N. Craig, X. Lu, and D. Sutherland, Phys. Rev. Lett. 130, 041603 (2023).
- T. Cohen, X. Lu, and D. Sutherland, J. High Energy Phys. 06 (2024) 149.
- T. Cohen, X. Lu, and Z. Zhang, Phys. Rev. D 111, 085012 (2025).
- T. Cohen, X.-X. Li, and Z. Zhang, J. High Energy Phys. 02 (2026) 076.
- N. Craig, Y.-T. Lee, X. Lu, and D. Sutherland, J. High Energy Phys. 11 (2023) 069.
- N. Craig and Y.-T. Lee, Phys. Rev. Lett. 132, 061602 (2024).
- M. Alminawi, I. Brivio, and J. Davighi, J. Phys. A 57, 435401 (2024).
- G. Ecker and J. Honerkamp, Phys. Lett. 42B, 253 (1972).
- J. Honerkamp, F. Krause, and M. Scheunert, Nucl. Phys. B69, 618 (1974).
- M. Alminawi, arXiv:2510.24866.
If the vacuum is , selects the pure linear term in the field transformation. Indeed field redefinitions that leave both the vacuum and the mass spectrum invariant are of the type .
- J. S. R. Chisholm, Nucl. Phys. 26, 469 (1961).
- S. Kamefuchi, L. O’Raifeartaigh, and A. Salam, Nucl. Phys. 28, 529 (1961).
- D. Kreimer and K. Yeats, Math. Phys. Anal. Geom. 20, 16 (2017).
- P.-H. Balduf, Math. Phys. Anal. Geom. 23, 33 (2020).
To see how covariance of on implies covariance of on , consider a change of section that can be captured by a fiber-preserving diffeomorphism on : , where , also known as a nonderivative field redefinition [38]. Under the metric is pulled back while the vector fields on which we evaluate it are pushed forward, and is covariant.
- U. Muller, C. Schubert, and A. E. M. van de Ven, Gen. Relativ. Gravit. 31, 1759 (1999).
- R. Nagai, M. Tanabashi, K. Tsumura, and Y. Uchida, Phys. Rev. D 100, 075020 (2019).
- D. Skinner, Lecture Notes, Part III of the Mathematical Tripos (University of Cambridge, Cambridge, United Kingdom, 2018), p. 16.
- J. M. Martín-García, D. Yllanes et al., www.xAct.es.