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Slightly Bimetric Gravitation
General Relativity and Quantum Cosmology · Submitted 16 Jan 2001
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The theories are equivalent to generally covariant theories with an arbitrary cosmological constant and an arbitrarily coupled scalar field, which can serve as an inflaton or dark matter.
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The abstract, sentence by sentence
The inclusion of a flat metric tensor in gravitation permits the formulation of a gravitational stress-energy tensor and the formal derivation of general relativity from a linear theory in flat spacetime. Building on the works of Kraichnan and Deser, we present such a derivation using universal coupling and gauge invariance. Next we slightly weaken the assumptions of universal coupling and gauge invariance, obtaining a larger ``slightly bimetric'' class of theories, in which the Euler-Lagrange equations depend only on a curved metric, matter fields, and the determinant of the flat metric. The theories are equivalent to generally covariant theories with an arbitrary cosmological constant and an arbitrarily coupled scalar field, which can serve as an inflaton or dark matter. The question of the consistency of the null cone structures of the two metrics is addressed. A difficulty for Logunov's massive gravitation on this front is noted.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The inclusion of a flat metric tensor in gravitation permits the formulation of a gravitational stress-energy tensor and the formal derivation of general relativity from a linear theory in flat spacetime. | background 1.00 | 0.12 | 0.12 | asserted 0.92 |
| s1 | Building on the works of Kraichnan and Deser, we present such a derivation using universal coupling and gauge invariance. | contribution 0.76 | 0.83 | 0.05 | asserted 0.99 |
| s2 | Next we slightly weaken the assumptions of universal coupling and gauge invariance, obtaining a larger ``slightly bimetric'' class of theories, in which the Euler-Lagrange equations depend only on a curved metric, matter fields, and the determinant of the flat metric. | contribution 0.97 | 0.94 | 0.24 | asserted 1.00 |
| s3 | The theories are equivalent to generally covariant theories with an arbitrary cosmological constant and an arbitrarily coupled scalar field, which can serve as an inflaton or dark matter. | result 0.76 | 0.81 | 0.60 | asserted 0.94 |
| s4 | The question of the consistency of the null cone structures of the two metrics is addressed. | contribution 0.93 | 0.67 | 0.03 | unclear 0.68 |
| s5 | A difficulty for Logunov's massive gravitation on this front is noted. | result 0.53 | 0.52 | 0.03 | asserted 0.92 |
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The paper
Original abstract
The inclusion of a flat metric tensor in gravitation permits the formulation of a gravitational stress-energy tensor and the formal derivation of general relativity from a linear theory in flat spacetime. Building on the works of Kraichnan and Deser, we present such a derivation using universal coupling and gauge invariance. Next we slightly weaken the assumptions of universal coupling and gauge invariance, obtaining a larger ``slightly bimetric'' class of theories, in which the Euler-Lagrange equations depend only on a curved metric, matter fields, and the determinant of the flat metric. The theories are equivalent to generally covariant theories with an arbitrary cosmological constant and an arbitrarily coupled scalar field, which can serve as an inflaton or dark matter. The question of the consistency of the null cone structures of the two metrics is addressed. A difficulty for Logunov's massive gravitation on this front is noted.
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References
How the literature uses it
10 arXiv papers cite this in 23 sentences
Papers citing it · 19 sentences without a confident label
Builds on it 1 paper
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Furthermore, it represents a generalisation of the result shown in [ref] of the appearance of a global degree of freedom because here we have not specified any particular action to obtain [ref] , thus showing that the appearance of a global degree of freedom is in fact a generic property of TDiff symmetric teleparallel theories, as already noticed in e.g. [ref] .
A class of ghost-free theories in symmetric teleparallel geometry · Symmetries · 0.87
Cites it as support 2 papers
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Improper conservation laws follow [ref] : the stress-energy tensor is a piece vanishing on-shell and a curl.
Einstein's Equations for Spin $2$ Mass $0$ from Noether's Converse Hilbertian Assertion · Aristotle on Inferring from Improper Conservation Laws to Einstein's Equations · 0.96
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The massless spin $2$ derivations of Einstein's equations from flat space-time would eventually [ref] show why it might not be unreasonable to favor universal forces even given Einstein's equations because it isn't implausible that gravity would act in just that way without any peculiar premises.
Kant, Schlick and Friedman on Space, Time and Gravity in Light of Three Lessons from Particle Physics · Lindemann's Challenge, Answered · 0.96
Cites it as background 1 paper
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Our HBP has ties with other attempts in the literature to construct special relativistic theories of gravitation [ref] .
Cone hierarchy and the screening of matter by gravity · Introduction · 0.88
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