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On "New Massive" 4D Gravity
High Energy Physics - Theory · Submitted 7 Feb 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We construct a four-dimensional (4D) gauge theory that propagates, unitarily, the five polarization modes of a massive spin-2 particle.
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The abstract, sentence by sentence
We construct a four-dimensional (4D) gauge theory that propagates, unitarily, the five polarization modes of a massive spin-2 particle. These modes are described by a "dual" graviton gauge potential and the Lagrangian is 4th-order in derivatives. As the construction mimics that of 3D "new massive gravity", we call this 4D model (linearized) "new massive dual gravity". We analyse its massless limit, and discuss similarities to the Eddington-Schroedinger model.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We construct a four-dimensional (4D) gauge theory that propagates, unitarily, the five polarization modes of a massive spin-2 particle. | contribution 1.00 | 0.95 | 0.72 | asserted 1.00 |
| s1 | These modes are described by a "dual" graviton gauge potential and the Lagrangian is 4th-order in derivatives. | method 0.51 | 0.80 | 0.13 | asserted 1.00 |
| s2 | As the construction mimics that of 3D "new massive gravity", we call this 4D model (linearized) "new massive dual gravity". | contribution 0.51 | 0.66 | 0.14 | asserted 0.99 |
| s3 | We analyse its massless limit, and discuss similarities to the Eddington-Schroedinger model. | contribution 0.83 | 0.87 | 0.07 | asserted 0.74 |
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The paper
Original abstract
We construct a four-dimensional (4D) gauge theory that propagates, unitarily, the five polarization modes of a massive spin-2 particle. These modes are described by a "dual" graviton gauge potential and the Lagrangian is 4th-order in derivatives. As the construction mimics that of 3D "new massive gravity", we call this 4D model (linearized) "new massive dual gravity". We analyse its massless limit, and discuss similarities to the Eddington-Schroedinger model.
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References
How the literature uses it
17 arXiv papers cite this in 33 sentences
Papers citing it · 24 sentences without a confident label
Builds on it 2 papers
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Here we generalize the linearized version of the 3D [ref] and 4D [ref] models to arbitrary dimensions by using a rank-3 tensor which satisfies $Ω_μνρ= - Ω_μρν$ and is traceless $η^μνΩ_μνρ=0$.
A note on linearized "New Massive Gravity" in arbitrary dimensions · Introduction · 1.00
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Finally, the total action reads S[φ_μ_1⋯μ_d-2,ν]=S_B[φ_μ_1⋯μ_d-2,ν] -m^2 S_E[φ_μ_1⋯μ_d-2,ν] , and it generalizes the NMG actions [ref] to arbitrary dimensions.
Higher-derivative massive actions from dimensional reduction · General $d$ dimensions · 0.95
Uses its method or tool 1 paper
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Inspired by [ref] we use the Levi-Civita symbol and define the linear change of variables
A note on linearized "New Massive Gravity" in arbitrary dimensions · Recovering “New Massive” 3D and 4D Gravity · 0.85
Compares with it 1 paper
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The result for the parity-odd model is similar to what happens for the 3D TMG model while the result for the parity-even model resembles the parity-even cases in 3D [ref] and 4D [ref] .
On Topologically Massive Spin-2 Gauge Theories beyond Three Dimensions · Discussion · 0.99
Cites it as background 4 papers
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In three dimensions, the most interesting theory in this context is the Bergshoeff-Hohm-Townsend (BHT) gravity [ref] , whose generalization to four-dimensional space-time has been proposed in [ref] .
Softly higher-derivative massive gravity · Introduction · 0.88
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This realm of research has uncovered many interesting aspects such as its interplay with the physics of diffeomorphism violation [ref] , extra dimensions [ref] , the Stückelberg trick [ref] , linearized [ref] vs. nonlinear massive gravity [ref] , the helicity decomposition of the metric perturbation [ref] , and the Ostrogradsky formalism as well as ghost states [ref] .
Modified-gravity theories with nondynamical background fields · Introduction · 0.99
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other three-dimensional theories studied in recent years [ref] .
Super-renormalizable Multidimensional Quantum Gravity · APPENDIX: 3D HIGHER-DERIVATIVE QUANTUM GRAVITY · 0.92
What it cites · 11 sentences without a confident label
Builds on 2 papers
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In this paper we have constructed a 4D analog of the linearized 3D massive gravity theory known as “new massive gravity” (NMG) [ref] .
Massive Gravity in Three Dimensions · Conclusions · 0.94
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This 3D model was analysed in a different way in [ref] , and here we adapt this analysis to the 4D case.
Massive 3D Supergravity · Massless limit of NMDG · 0.89
Compares with 1 paper
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A discontinuity of this sort was to be expected because a similar discontinuity in the number of propagated modes occurs in the massless limit of the 3D NMG, which is what one finds by an application to the Lagrangian ([ref]) of the reduction/truncation procedure of subsection [ref]; i.e. the “pure” fourth-order 3D Lagrangian analysed by Deser [ref] .
Ghost-free, finite, fourth order D=3 (alas) gravity · Massless limit of NMDG · 0.82
Cites as background 2 papers
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This possibility has implications for cosmology that have motivated many recent models of “massive gravity”; see [ref] for a recent review.
Theoretical Aspects of Massive Gravity · Introduction · 0.98
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Other “exotic” Lorentz representations were explored in [ref] , and the topic has been reconsidered more recently in the context of string/M-theory dualities, see, e.g. [ref] .
Duality in Gravity and Higher Spin Gauge Fields · Introduction · 0.93
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