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Non-Trivial Vacua in Higher-Derivative Gravitation
High Energy Physics - Theory · Submitted 26 Sep 1995
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim For general fourth-order theories, described by actions which are general functions of the scalar curvature, the Ricci tensor and the full Riemann tensor, it is shown that the higher-derivative theories may have multiple stable vacua.
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The abstract, sentence by sentence
A discussion of an extended class of higher-derivative classical theories of gravity is presented. A procedure is given for exhibiting the new propagating degrees of freedom, at the full non-linear level, by transforming the higher-derivative action to a canonical second-order form. For general fourth-order theories, described by actions which are general functions of the scalar curvature, the Ricci tensor and the full Riemann tensor, it is shown that the higher-derivative theories may have multiple stable vacua. The vacua are shown to be, in general, non-trivial, corresponding to deSitter or anti-deSitter solutions of the original theory. It is also shown that around any vacuum the elementary excitations remain the massless graviton, a massive scalar field and a massive ghost-like spin-two field. The analysis is extended to actions which are arbitrary functions of terms of the form $\nabla^{2k}R$, and it is shown that such theories also have a non-trivial vacuum structure.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A discussion of an extended class of higher-derivative classical theories of gravity is presented. | contribution 0.79 | 0.76 | 0.04 | asserted 0.71 |
| s1 | A procedure is given for exhibiting the new propagating degrees of freedom, at the full non-linear level, by transforming the higher-derivative action to a canonical second-order form. | method 0.98 | 0.91 | 0.07 | asserted 0.99 |
| s2 | For general fourth-order theories, described by actions which are general functions of the scalar curvature, the Ricci tensor and the full Riemann tensor, it is shown that the higher-derivative theories may have multiple stable vacua. | result 0.99 | 0.91 | 0.43 | hedged possibility 0.81 |
| s3 | The vacua are shown to be, in general, non-trivial, corresponding to deSitter or anti-deSitter solutions of the original theory. | result 0.95 | 0.91 | 0.28 | asserted 1.00 |
| s4 | It is also shown that around any vacuum the elementary excitations remain the massless graviton, a massive scalar field and a massive ghost-like spin-two field. | result 1.00 | 0.91 | 0.15 | asserted 1.00 |
| s5 | The analysis is extended to actions which are arbitrary functions of terms of the form $\nabla^{2k}R$, and it is shown that such theories also have a non-trivial vacuum structure. | result 0.52 | 0.92 | 0.16 | asserted 1.00 |
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The paper
Original abstract
A discussion of an extended class of higher-derivative classical theories of gravity is presented. A procedure is given for exhibiting the new propagating degrees of freedom, at the full non-linear level, by transforming the higher-derivative action to a canonical second-order form. For general fourth-order theories, described by actions which are general functions of the scalar curvature, the Ricci tensor and the full Riemann tensor, it is shown that the higher-derivative theories may have multiple stable vacua. The vacua are shown to be, in general, non-trivial, corresponding to deSitter or anti-deSitter solutions of the original theory. It is also shown that around any vacuum the elementary excitations remain the massless graviton, a massive scalar field and a massive ghost-like spin-two field. The analysis is extended to actions which are arbitrary functions of terms of the form $\nabla^{2k}R$, and it is shown that such theories also have a non-trivial vacuum structure.
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References
How the literature uses it
15 arXiv papers cite this in 34 sentences
Papers citing it · 25 sentences without a confident label
Uses its method or tool 1 paper
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Following the steps in Refs. [ref] , we perform an expansion of Eq. [ref] up to second order in curvature invariants around a MS solution to study the excitations of the theory around such background.
Higher-order theories of gravity: diagnosis, extraction and reformulation via non-metric extra degrees of freedom · The expansion procedure · 1.00
Compares with it 1 paper
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Then it can be shown that at the bilinear level the linearisation of the theory over a maximally symmetric spacetime will be the same as the theory obtained in [ref] ,
Generalized modified gravity with the second order acceleration equation · weak field limit · 0.87
Cites it as support 2 papers
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Assuming auxiliary fields enter algebraically and $f”(R)>0$, these operations commute at the action level; any ordering yields the same reduced bulk action up to total–derivative boundary terms (Fig. [ref]) [ref] .
Universal Nonminimal Coupling-to-Starobinsky Matching and a Single-Field Attractor · Off–shell commutativity and universality · 0.96
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Regarding these kinds of corrections, it has been shown, both at the level of the equations of motion [ref] , and of the action [ref] , that an ETG of the type [equation] can in general be rewritten as a theory describing a set of scalar fields non-minimally coupled to standard GR.
Higher-order theories of gravity: diagnosis, extraction and reformulation via non-metric extra degrees of freedom · General higher-order theories · 0.98
Cites it as background 3 papers
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More generally, the global stability (i.e., the absence of runaway solutions) and the local stability (i.e., the identification of Lyapunov stable vacua) of Quadratic Gravity are yet to be determined, see also [ref] .
Nonlinear Evolution of Quadratic Gravity in 3+1 Dimensions · Outlook · 0.92
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This method has been widely used in many contexts [ref] .
Higher-order theories of gravity: diagnosis, extraction and reformulation via non-metric extra degrees of freedom · Auxiliary fields method · 0.80
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Perhaps the most fruitful area of their application is cosmology, e.g. in [ref] , where the scalar field is often employed as a quintessence field to drive accelerating phases of the universe; scalar-tensor theories naturally appear in brane-world scenarios [ref] , or arise as equivalent formulations of $f(R)$ gravity theories with Ricci scalar corrections [ref] .
Brans-Dicke geometry · Introduction · 0.98
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