Photon and graviton mass limits
Open accessAbstract
Efforts to place limits on deviations from canonical formulations of electromagnetism and gravity have probed length scales increasing dramatically over time. Historically, these studies have passed through three stages: (1) testing the power in the inverse-square laws of Newton and Coulomb, (2) seeking a nonzero value for the rest mass of photon or graviton, and (3) considering more degrees of freedom, allowing mass while preserving explicit gauge or general-coordinate invariance. Since the previous review the lower limit on the photon Compton wavelength has improved by four orders of magnitude, to about one astronomical unit, and rapid current progress in astronomy makes further advance likely. For gravity there have been vigorous debates about even the concept of graviton rest mass. Meanwhile there are striking observations of astronomical motions that do not fit Einstein gravity with visible sources. ``Cold dark matter'' (slow, invisible classical particles) fits well at large scales. ``Modified Newtonian dynamics'' provides the best phenomenology at galactic scales. Satisfying this phenomenology is a requirement if dark matter, perhaps as invisible classical fields, could be correct here too. ``Dark energy'' might be explained by a graviton-mass-like effect, with associated Compton wavelength comparable to the radius of the visible universe. Significant mass limits are summarized in a table.
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m_A ≡ ξ^{1/2} can be interpreted as the rest mass of photons.
“When ξ is positive, this equation is equivalent to the Proca equation [34-36] and m A ≡ ξ 1 / 2 can be interpreted as the rest mass of photons.”
From Electrodynamics on cosmological scales (2016) · cites this paper as [36]
“Photon mass from the Proca equation” (pp. 5–6) says that Proca’s modification can give the photon a nonzero rest mass. The passages do not define ξ or establish that √ξ is that mass, so the specific identification is not supported by our copy. (LLM, conf=0.82)
Experimental — accuracy not yet measuredWhen ξ is positive, equation (10) is equivalent to the Proca equation.
“When ξ is positive, this equation is equivalent to the Proca equation [34-36] and m A ≡ ξ 1 / 2 can be interpreted as the rest mass of photons.”
From Electrodynamics on cosmological scales (2016) · cites this paper as [36]
Section B (p. 5) describes the Proca modification of Maxwell’s equations as giving the photon a nonzero rest mass. The equations in our copy are not decoded, however, and the text does not identify the citing paper’s equation (10) or its parameter ξ. It therefore supports the general Proca–photon-mass connection, but not the stated equivalence under ξ > 0. (LLM, conf=0.84)
Experimental — accuracy not yet measuredIf longitudinal photons interact with matter sufficiently weakly or do not interact with matter at all, we still get g = 2 and the Stephan-Boltzmann law remains valid.
“If they interact with matter sufficiently weak or do not interact with matter at all, we still get g = 2 and the Stephan-Boltzmann law remains valid [35, 36, 58].”
From Electrodynamics on cosmological scales (2016) · cites this paper as [36]
Section II.F (p. 12) says that, with local charge conservation, longitudinal-photon coupling is suppressed as photon mass approaches zero and observable electromagnetic phenomena remain continuous in that limit. This supports the weak-interaction premise, but the paper also says a photon with nonzero mass has three polarization degrees of freedom; it does not state that g = 2 or address the Stefan–Boltzmann law. (LLM, conf=0.84)
Experimental — accuracy not yet measuredThere is no observational or experimental evidence for gauge invariance of electromagnetic fields in a curved spacetime with a nonvanishing Ricci curvature.
“We also remark that there is no observational or experimental evidence for gauge invariance of electromagnetic fields in a curved spacetime with a nonvanishing Ricci curvature.”
From Electrodynamics on cosmological scales (2016) · cites this paper as [36]
The discussion of gauge invariance (p. 9) calls the symmetry unobservable, but does not assess observational or experimental evidence for electromagnetic gauge invariance in curved spacetime. Searches for Ricci curvature and tests in curved spacetime found no passage addressing the claim’s specific setting. (LLM, conf=0.73)
Experimental — accuracy not yet measured
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Sorted by citations
Electrodynamics on cosmological scales
Li, L.-X. (2016) · General Relativity and Gravitation · doi:10.1007/s10714-016-2028-3 · Cited by 5 · see citing works
- Authors
- Goldhaber, A. S., & Nieto, M. M.
- Affiliations
- State University of New York (US)
- Venue
- Reviews of Modern Physics
- Publisher
- American Physical Society (APS)
- Published
- 2010-03-23
- Volume
- 82
- Issue
- 1
- Pages
- 939-979
- ISSN
- 0034-6861 (ISSN-L)
- 1539-0756
- OpenAlex
- W2076997212
- Cited by
- 445
- References
- 295
- Citations by year
- 2026: 14 · 2025: 33 · 2024: 22 · 2023: 25 · 2022: 20 · 2021: 16 · 2020: 19 · 2019: 28 · 2018: 28 · 2017: 35 · 2016: 50 · 2015: 30 · 2014: 29 · 2013: 30 · 2012: 24
- FWCI
- 15.19
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Locations
- Reviews of Modern Physics (publishedVersion)
- arXiv (Cornell University) (publishedVersion)
- arXiv (Cornell University)
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Cosmology and Gravitation Theories
- Physical Sciences › Physics and Astronomy › Statistical and Nonlinear Physics › Noncommutative and Quantum Gravity Theories
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Relativity and Gravitational Theory
- Keywords
- photon mass, graviton mass, modified gravity, Compton wavelength, dark matter, MOND, dark energy, gauge invariance, general coordinate invariance, cosmological constraints
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