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Topological Features of the Quantum Vacuum
General Relativity and Quantum Cosmology · Submitted 4 Oct 2018
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This feature that goes beyond general relativity (and unimodular gravity) offers an interpretation of the smallness of the currently observed cosmological constant.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
A central aspect of the cosmological constant problem is to understand why vacuum energy does not gravitate. In order to account for this observation, while allowing for nontrivial dynamics of the quantum vacuum, we motivate a novel background independent theory of gravity. The theory is an extension of unimodular gravity that is described in geometric terms by means of a conformal (light-cone) structure and differential forms of degree one and two. We show that the subset of the classical field equations describing the dynamics of matter degrees of freedom and the conformal structure of spacetime are equivalent to that of unimodular gravity. The sector with vanishing matter fields and flat conformal structure is governed by the field equations of BF theory and contains topological invariants that are influenced by quantum vacuum fluctuations. Perturbative deviations from this sector lead to classical solutions that necessarily display relatively small values of the cosmological constant with respect to the would-be contribution of quantum vacuum fluctuations. This feature that goes beyond general relativity (and unimodular gravity) offers an interpretation of the smallness of the currently observed cosmological constant.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A central aspect of the cosmological constant problem is to understand why vacuum energy does not gravitate. | background 0.99 | 0.05 | 0.03 | asserted 1.00 |
| s1 | In order to account for this observation, while allowing for nontrivial dynamics of the quantum vacuum, we motivate a novel background independent theory of gravity. | contribution 0.95 | 0.71 | 0.07 | asserted 0.66 |
| s2 | The theory is an extension of unimodular gravity that is described in geometric terms by means of a conformal (light-cone) structure and differential forms of degree one and two. | contribution 0.57 | 0.53 | 0.04 | asserted 1.00 |
| s3 | We show that the subset of the classical field equations describing the dynamics of matter degrees of freedom and the conformal structure of spacetime are equivalent to that of unimodular gravity. | result 0.98 | 0.93 | 0.11 | asserted 1.00 |
| s4 | The sector with vanishing matter fields and flat conformal structure is governed by the field equations of BF theory and contains topological invariants that are influenced by quantum vacuum fluctuations. | result 0.80 | 0.78 | 0.08 | asserted 1.00 |
| s5 | Perturbative deviations from this sector lead to classical solutions that necessarily display relatively small values of the cosmological constant with respect to the would-be contribution of quantum vacuum fluctuations. | result 0.99 | 0.84 | 0.48 | asserted 0.99 |
| s6 | This feature that goes beyond general relativity (and unimodular gravity) offers an interpretation of the smallness of the currently observed cosmological constant. | interpretation 1.00 | 0.70 | 0.72 | asserted 0.85 |
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The paper
Original abstract
A central aspect of the cosmological constant problem is to understand why vacuum energy does not gravitate. In order to account for this observation, while allowing for nontrivial dynamics of the quantum vacuum, we motivate a novel background independent theory of gravity. The theory is an extension of unimodular gravity that is described in geometric terms by means of a conformal (light-cone) structure and differential forms of degree one and two. We show that the subset of the classical field equations describing the dynamics of matter degrees of freedom and the conformal structure of spacetime are equivalent to that of unimodular gravity. The sector with vanishing matter fields and flat conformal structure is governed by the field equations of BF theory and contains topological invariants that are influenced by quantum vacuum fluctuations. Perturbative deviations from this sector lead to classical solutions that necessarily display relatively small values of the cosmological constant with respect to the would-be contribution of quantum vacuum fluctuations. This feature that goes beyond general relativity (and unimodular gravity) offers an interpretation of the smallness of the currently observed cosmological constant.
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How the literature uses it
8 arXiv papers cite this in 27 sentences
Papers citing it · 17 sentences without a confident label
Builds on it 2 papers
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In this paper we consider the physics of Dirac fermions charged under the BF gauge group of [ref] , and their impact on the cosmological constant.
Chiral Symmetry and the Cosmological Constant · Introduction · 0.90
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Here, we develop the fundamentals for obtaining a modified gravity theory that is coupled to several gauge fields, extending the approach presented in [ref] to higher order BF theories.
Categorical generalization of BF theory coupled to gravity · Physical applications · 0.99
Cites it as background 5 papers
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Here we review a model presented in [ref] and developed further in [ref] that will provide the background for our analysis.
Black hole and cosmological analysis of BF sequestered gravity · Review of BF-Coupled Gravity · 0.93
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In this section, we give an overview of a model proposed in [ref] that solves aspects of the cosmological constant problem.
Chiral Symmetry and the Cosmological Constant · Non-Renormalization of the cosmological constant in BF-Coupled Gravity · 0.83
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In the field of modified gravity, a new relationship between $BF$ theories and gravity has recently been proposed under the name of $BF$ sequestered gravity, in which Lagrangians for both theories are coupled such that the volume form of spacetime must coincide with the volume form constructed from one of the fields of the $BF$ theory, with this volume form acting as the potential term [ref] .
Categorical generalization of BF theory coupled to gravity · Introduction · 0.80
What it cites · 29 sentences without a confident label
Uses the method or tool of 3 papers
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Let us just quote the results that can be obtained using procedures that are thoroughly described in [ref] , as explained in [ref] .
Heat kernel expansion: user's manual · Semiclassical renormalization group · 0.86
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Let us just quote the results that can be obtained using procedures that are thoroughly described in [ref] , as explained in [ref] .
Sakharov's induced gravity: a modern perspective · Semiclassical renormalization group · 0.86
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Let us just quote the results that can be obtained using procedures that are thoroughly described in [ref] , as explained in [ref] .
Longitudinal diffeomorphisms obstruct the protection of vacuum energy · Semiclassical renormalization group · 0.86
Compares with 9 papers
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These considerations are remarkably similar to Volovik's proposal to understand the value of the cosmological constant as arising from a small displacement with respect to (or perturbative deviation from) the equilibrium state of the universe [ref] .
Gluonic vacuum, q-theory, and the cosmological constant · Perturbations of the quantum vacuum · 0.92
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These considerations are remarkably similar to Volovik's proposal to understand the value of the cosmological constant as arising from a small displacement with respect to (or perturbative deviation from) the equilibrium state of the universe [ref] .
Equilibrium boundary conditions, dynamic vacuum energy, and the Big Bang · Perturbations of the quantum vacuum · 0.92
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These considerations are remarkably similar to Volovik's proposal to understand the value of the cosmological constant as arising from a small displacement with respect to (or perturbative deviation from) the equilibrium state of the universe [ref] .
Dynamic vacuum variable and equilibrium approach in cosmology · Perturbations of the quantum vacuum · 0.92
Cites as background 7 papers
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Let us start with a brief review of the relevant properties of BF theory [ref] , a topological field theory formulated on the principal bundle of a group $G$ over the spacetime manifold $ℳ$.
On the Relations between Gravity and BF Theories · Constructing the action · 0.99
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Let us start with a brief review of the relevant properties of BF theory [ref] , a topological field theory formulated on the principal bundle of a group $G$ over the spacetime manifold $ℳ$.
$BF$ gravity · Constructing the action · 0.99
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Let us start with a brief review of the relevant properties of BF theory [ref] , a topological field theory formulated on the principal bundle of a group $G$ over the spacetime manifold $ℳ$.
Classical general relativity as BF-Plebanski theory with linear constraints · Constructing the action · 0.99
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