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Gravitation and cosmology in generalized (1 + 1)-dimensional dilaton gravity
Open accessAbstract
The actions of the `R=T' and string-inspired theories of gravity in (1+1) dimensions are generalized into one single action which is characterized by two functions. We discuss differing interpretations of the matter stress--energy tensor, and show how two such different interpretations can yield two different sets of field equations from this action. The weak-field approximation, post-Newtonian expansion, hydrostatic equilibrium state of a star and two-dimensional cosmology are studied separately by using the two sets of field equations. Some properties in the `R=T' and string-inspired theories are shown to be generic in the theory induced by the generalized action.
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TL;DR
The paper generalizes (1+1)-dimensional dilaton gravity actions, including “R = T” and string-inspired theories, into a single action characterized by two functions \(H(\Phi)\) and \(D(\Phi)\). It studies two possible interpretations of the matter stress-energy tensor, yielding type-I and type-II field equations, and analyzes weak-field, post-Newtonian, stellar-structure, and cosmological consequences.
Key findings
- The generalized action \(S=S_g-S_s\) with \(H(\Phi)\), \(D(\Phi)\), and potential \(V\) yields two sets of field equations: type-I from defining \(T_{\mu\nu}\) as the metric variation of the matter action, and type-II under \(H(\Phi)=kD'(\Phi)\), which incorporates the dilaton variation. Type-II includes both the “R = T” and string-inspired theories; type-I and type-II have the same dynamical properties only if condition (10) holds and the dilaton source vanishes.
- In weak-field calculations, the roles of dilaton and matter sources are interchanged: for type-I, the dilaton perturbation depends only on the matter source while the trace of the metric perturbation depends on both dilaton and matter sources; the reverse occurs for type-II.
- Post-Newtonian expansions can be carried to arbitrary high order for both equation types. Stellar equilibrium reduces to Newton’s equation in the Newtonian limit: for type-I when \([D'(0)]^2/H(0)=2\), and for type-II when \(D'(0)=2k\). The case \(H=0\) is not appropriate for modeling one-dimensional stellar structure.
- Cosmological solutions are given for dust (\(\gamma=1\)) and radiation (\(\gamma=2\)) universes, with radiation-filled solutions generally more complicated. For inflationary exponential expansion, type-I requires \(H(\Phi)\) strictly negative; type-II yields \(D(\Phi)\) functions so complicated that the relevant differential equations appear analytically intractable, leaving numerical solutions as the only practical option.
Methods
- Theoretical analysis of a generalized (1+1)-dimensional dilaton gravity action, varying with respect to the metric and dilaton field, and deriving type-I and type-II field equations under different interpretations of the matter stress-energy tensor.
- Weak-field expansion about a background with conformal transformations and harmonic gauge; post-Newtonian expansion in powers of velocity \(v\); static metric and perfect-fluid stress tensor for stellar structure; Robertson-Walker metric with equation of state \(p=(\gamma-1)\rho\) for cosmology, considering \(\gamma=1,2,0\).
- Computations are carried out without restricting \(D\), \(H\), and \(V\) except for the constraint \(D'(\Phi)\neq 0\); Maple V was used for expansions.
Limitations
- The paper states that ambiguity in interpreting the matter action arises from lack of knowledge of the potential density \(V\), and can only be clarified once \(V\) is explicitly specified; many other interpretations are possible, but only type-I and type-II are considered.
- Type-II equations require \(H\neq 0\); if \(H=0\), only type-I equations are available. The paper also notes that \(H=0\) is not appropriate for modeling one-dimensional stellar structure.
- For inflationary type-II solutions, the derived \(D(\Phi)\) functions make the differential equations analytically intractable, so numerical solutions are the only practical option.
- Evident from the text: the analysis is confined to (1+1)-dimensional models, and many results depend on unspecified characteristic functions \(D\) and \(H\), so no direct (3+1)-dimensional observational predictions are established.
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“If we substitute equations (51) and (52) into the first order expansions, one will easily conclude that 1 Φ (t, x) = 1 Φa . (53”
§ Gravitation and Cosmology in Generalized (1+1)-dimensional dilaton gravity > 3.2.2 Case II:
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“Finally, the remaining equation 2 T 10 = 0 is just trivially satisfied.”
§ Gravitation and Cosmology in Generalized (1+1)-dimensional dilaton gravity > 3.2.2 Case II:
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In the paper
“which has a general solution”
§ Gravitation and Cosmology in Generalized (1+1)-dimensional dilaton gravity > 2.1 Type I Equations
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“As p(x) and p ′ (x) tend to zero in the Newtonian limit, the density ρ(x) goes to zero in this limit.”
§ Gravitation and Cosmology in Generalized (1+1)-dimensional dilaton gravity > 4.1 Type I Equations
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“According to equation ( 12), the dilaton source J is a constant.”
§ Gravitation and Cosmology in Generalized (1+1)-dimensional dilaton gravity > 5.2 Type II Equations
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Citations
Cites
Bondi, S. H. (1974) · Journal of the Franklin Institute · doi:10.1016/0016-0032(74)90062-3 · Cited by 2,968
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Self-citationConservation laws and two-dimensional black holes in dilaton gravity
Mann, R. B. (1993) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.47.4438 · Cited by 143
Self-citationParticle Physics and Cosmology
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Canonical quantization of polyakov's string in arbitrary dimensions
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Research works printed but not linked: 5
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- Torre C G, 1989, Phys. Rev., 40
- Mann R B, 1991, Phys. Rev., 43
- Callan C G, 1992, Phys. Rev., 45
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Cited by
Scalar wave falloff in asymptotically anti–de Sitter backgrounds
Chan, J. S. F., & Mann, R. B. (1997) · Physical Review D · doi:10.1103/physrevd.55.7546 · Cited by 186
Self-citationScalar wave falloff in topological black hole backgrounds
Chan, J. S. F., & Mann, R. B. (1999) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.59.064025 · Cited by 100
Self-citationExact solution for the metric and the motion of two bodies in (1+1)-dimensional gravity
Mann, R. B., & Ohta, T. (1997) · Physical Review D · doi:10.1103/physrevd.55.4723 · Cited by 48
Self-citationSoluble models in two-dimensional dilaton gravity
Fabbri, A., & Russo, J. G. (1996) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.53.6995 · Cited by 48
Canonical reduction of two-dimensional gravity for particle dynamics
Ohta, T., & Mann, R. (1996) · Classical and Quantum Gravity · doi:10.1088/0264-9381/13/9/022 · Cited by 39
Self-citation(1+1) -dimensional entropic gravity
Mann, R. B., & Mureika, J. (2011) · Physics Letters B · doi:10.1016/j.physletb.2011.07.052 · Cited by 37
Self-citationThe Classical Solutions of Two-dimensional Gravity
Schmidt, H. (1999) · General Relativity and Gravitation · doi:10.1023/a:1026708320831 · Cited by 26
Two-dimensional gravitation and sine-Gordon solitons
Stötzel, B. (1995) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.52.2192 · Cited by 23
Canonical reduction of two-dimensional gravity for Particle DynamicsPreprint
Ohta, T., & Mann, R. B. (1996) · Cited by 20
Self-citationN-body gravity and the Schrödinger equation
Farrugia, P.-S., Mann, R. B., & Scott, T. C. (2007) · Classical and Quantum Gravity · doi:10.1088/0264-9381/24/18/006 · Cited by 18
Self-citationExact solutions to the motion of two charged particles in lineal gravity
Mann, R. B., Robbins, D. G., Ohta, T., & Trott, M. (2000) · Nuclear Physics B · doi:10.1016/s0550-3213(00)00537-x · Cited by 17
Self-citationExact solutions of relativistic two-body motion in lineal gravity
Mann, R. B., Robbins, D. G., & Ohta, T. (1999) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.60.104048 · Cited by 15
Self-citationChaos in an exact relativistic three-body self-gravitating system
Burnell, F. J., Malecki, J., Mann, R. B., & Ohta, T. (2004) · Physical Review E · doi:10.1103/physreve.69.016214 · Cited by 14
Self-citationStatistical mechanics of relativistic one-dimensional self-gravitating systems
Mann, R. B., & Chak, P. (2002) · Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics · doi:10.1103/physreve.65.026128 · Cited by 12
Self-citationThree-body dynamics in a(1+1)-dimensional relativistic self-gravitating system
Malecki, J. J., & Mann, R. B. (2004) · Physical Review E · doi:10.1103/physreve.69.066208 · Cited by 10
Self-citationPrimordial black holes in a dimensionally reduced universe
Tzikas, A. G., Nicolini, P., Mureika, J., & Carr, B. J. (2018) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2018/12/033 · Cited by 11
Supergravity from a massive superparticle and the simplest super black hole
Wehlau, M. E., & Mann, R. B. (1998) · Nuclear Physics B · doi:10.1016/s0550-3213(97)00805-5 · Cited by 11
Self-citationPerturbative quantum gravity coupled to particles in (1 + 1) dimensions
Mann, R. B., & Young, M. B. (2007) · Classical and Quantum Gravity · doi:10.1088/0264-9381/24/4/014 · Cited by 9
Self-citationPerturbative Quantum Gravity Coupled to Particles in (1 + 1)-DimensionsPreprint
Mann, R. B., & Young, M. B. (2006) · Cited by 8
Self-citationQuantum field formalism for the higher-derivative nonrelativistic electrodynamics in 1+1 dimensions
Manavella, E. C. (2019) · International Journal of Modern Physics A · doi:10.1142/s0217751x19500507 · Cited by 6
Particles on a circle in canonical lineal gravity
Mann, R. B. (2001) · Classical and Quantum Gravity · doi:10.1088/0264-9381/18/17/306 · Cited by 6
Self-citationChaos in a three-body self-gravitating cosmological spacetime
Koop, M. J., Mann, R. B., & Bachmann, S. (2007) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.76.104051 · Cited by 4
Self-citationChaotic behavior in a charged three-body self-gravitating system
Koop, M. J., Mann, R. B., & Rohanizadegan, M. (2009) · Journal of Mathematical Physics · doi:10.1063/1.3190103 · Cited by 1
Self-citationHiggs boson mass from maximally nonlinear superconductive quantum gravityPreprint
Yepez, J. (2019) · arXiv (Cornell University) · doi:10.48550/arxiv.1907.13427 · Cited by 1
Noncommutative black holes in extended anti-de Sitter phase space
Tzikas, A. G. (2025) · International Journal of Modern Physics D · doi:10.1142/s0218271825500841
Metadata
- Authors
- Chan, J. S. F., & Mann, R. B.
- Affiliations
- University of Waterloo (CA)
- Venue
- Classical and Quantum Gravity
- Publisher
- IOP Publishing
- Published
- 1995-02-01
- Volume
- 12
- Issue
- 2
- Pages
- 351-371
- ISSN
- 0264-9381 (ISSN-L)
- 1361-6382
- OpenAlex
- W2132163639
- Cited by
- 25
- References
- 15
- Citations by year
- 2025: 1 · 2019: 2 · 2018: 1
- FWCI
- 2.76
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Locations
- Classical and Quantum Gravity (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- CERN Document Server (European Organization for Nuclear Research) (submittedVersion)
- arXiv (Cornell University)
- Funders
- Natural Sciences and Engineering Research Council of Canada
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Cosmology and Gravitation Theories
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Black Holes and Theoretical Physics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Relativity and Gravitational Theory
- Keywords
- dilaton gravity, 1+1 dimensional gravity, string-inspired gravity, field equations, weak field approximation, post-Newtonian approximation, hydrostatic equilibrium
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