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Nothing really matters
Open accessAbstract
We study non-perturbative instabilities of AdS spacetime in General Relativity with a cosmological constant in arbitrary dimensions. In this simple setup we explicitly construct a class of gravitational instantons generalizing Witten’s bubble of nothing. We calculate the corresponding Euclidean action and show that its change is finite. The expansion of these bubbles is described by a lower-dimensional de Sitter geometry within a non- compact foliation of the background spacetime. Moreover we discuss the existence of covariantly constant spinors as a possible topological obstruction for such decays to occur. This mechanism is further connected to the stability of supersymmetric vacua in string theory.
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Overview
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TL;DR
The paper constructs gravitational instantons generalizing Witten’s bubble of nothing in (D+1)-dimensional General Relativity with a cosmological constant, describing non-perturbative decay of constant-curvature vacua via expanding bubbles with dS_d × S^{D-d-1} surfaces. It computes finite Euclidean-action bounces, shows exponential suppression in the semiclassical regime, and discusses covariantly constant spinors as a topological obstruction that can stabilize the vacuum.
Key findings
- The construction generalizes Witten’s 5d Kaluza-Klein bubble to (D+1)-dimensional vacua of the form (3.1), with consistency conditions \(L_{dS_d}=1\), \(L_{S^{D-d-1}}=L_{dS_d}\sqrt{(D-d-2)/(d-1)}\), \(d\ge2\), \(D=d+2\). The Euclidean black-hole metric (3.4) is smooth when \(\ell_{KK}^2=4(D-2)f(\rho_0)^2/(d-1)\) (3.6); for \(\Lambda\le0\) it is non-singular for \(\rho\in(\rho_0,+\infty)\), while \(\Lambda>0\) is excluded because the Euclidean geometry has no asymptotic region.
- The bounce is finite. For zero curvature, \(\Delta S_E^{(\Lambda=0)}\) is given by (3.15); for \(D=4,d=3\) it reduces to Witten’s result \(\Delta S_E=\pi R^2/(4G_N^{(4)})\) (2.6), and scales as \(\Delta S_E^{(\Lambda=0)}\propto (R/\ell_{Pl})^{D-1}\) (3.17). For \(\Lambda<0\), \(\Delta S_E^{(\Lambda<0)}\) is given by (3.18), with scaling (3.19); the decay rate is exponentially suppressed whenever the semiclassical approximation is valid.
- The decay changes topology: the vacuum is foliated by \(S^1\times S^{d-1}\times S^{D-d-1}\), while near the bubble the instanton has topology \(R^2\times S^{d-1}\times S^{D-d-1}\). Covariantly constant spinors require \(\alpha=0\), whereas the unique spin structures on spheres require \(\alpha=\pi\); hence the instanton does not contribute to the path integral for theories with covariantly constant spinors, so suitable fermion boundary conditions can “cure” the instability.
- Appendix B shows the bubble decay can be captured by a tunneling scalar field in one lower dimension via Kaluza-Klein reduction.
Methods
- Theoretical construction: double analytic continuation of non-extremal black holes in (D+1)-dimensional GR with \(\Lambda\), using Wick rotation and continuing \(S^d\to dS^d\) to obtain the instanton geometry (3.7). The Hamilton-Jacobi formulation is used to recast the coupled second-order equations into first-order conditions without supersymmetry.
- Euclidean action analysis: computes \(S_E=S_{E,\text{bulk}}+S_{E,\text{GHY}}\) and the bounce \(\Delta S_E=S_E|_{\text{inst}}-S_E|_{\text{false}}\), evaluating bulk and boundary contributions separately for zero and non-zero curvature.
- No empirical data or sample; the work is an analytic study in arbitrary dimensions, with smoothness and consistency conditions imposed on the solutions.
Limitations
- Stated: the semiclassical approximation is trusted only for \(R\) large compared to the Planck length \(\ell_{Pl}\). For \(\Lambda>0\), the Euclidean geometry does not have an asymptotic region due to a zero in \(f(\rho)\) and the static patch, so the paper specializes to \(\Lambda\le0\).
- Stated: the interpretation of asymptotically AdS decay in holography remains an open problem; it is unknown how to interpret the decay in the dual field theory or whether the decay invalidates the holographic correspondence.
- Text-evident: no explicit string-theory embedding or dual field theory computation is performed; extension to fully stringy decays is left for future work, and the analysis is classical/Euclidean rather than a full quantum-gravity treatment.
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In the paper
“At the surface ρ = R the KK direction, φ pinches off to zero size, so that the interior of the bubble is dubbed”
§ Nothing really matters > JHEP08(2020)040
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“The fact that this decay will happen with probability equal to one in an infinite volume of space can be seen by computing a finite difference in Euclidean actions”
- Also stated in: § JHEP08(2020)040 · plain
“∆S E = πR 2 4 G (4) N .”
§ Nothing really matters > JHEP08(2020)040
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In the paper
“the (ρ, τ )-plane parametrizes the exterior region of a hyperbola of radius R.This hyperbola is exactly a de Sitter manifold dS 3 which describes a bubble expanding under constant proper acceleration.”
§ Nothing really matters > JHEP08(2020)040
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“In this simple setup we explicitly construct a class of gravitational instantons generalizing Witten's bubble of nothing.”
§ Nothing really matters > Abstract
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None of the sources cited for this claim have been checked yet.
In the paper
“In this section we extend the analysis of [3] to a larger class of instabilities in constant curvature vacuum solutions in (D + 1)-dimensional General Relativity [47].”
§ Nothing really matters > 3 Bubbles of nothing and vacuum decay
What the sources say
- Not checked — no full text of the sourcecites [3] E. Witten, Instability of the Kaluza-Klein vacuum, Nucl. Phys. B 195 (1982) 481 [INSPIRE]. source
- Not checked yetcites [47] M. Godazgar and H.S. Reall, Algebraically special axisymmetric solutions of the higher-dimensional vacuum Einstein equation, Class. Quant. Grav. 26 (2009) 165009 [arXiv:0904.4368] [INSPIRE]. source
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Citations
Cites
The cosmological constant problem
Weinberg, S. (1989) · Reviews of Modern Physics · doi:10.1103/revmodphys.61.1 · Cited by 7,341 · cited 1×
“populate different corners of a landscape is a crucial component of the anthropic solution of the cosmological constant problem [31].”
BackgroundAnti-de Sitter space, thermal phase transition, and confinement in gauge theories
Witten, E. (1998) · Advances in Theoretical and Mathematical Physics · doi:10.4310/atmp.1998.v2.n3.a3 · Cited by 3,915
de Sitter vacua in string theory
Shamit Kachru, A., Каллош, Р., Linde, A. D., & Trivedi, S. P. (2003) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.68.046005 · Cited by 3,816
Fate of the false vacuum: Semiclassical theory
Coleman, S. (1977) · Physical Review D · doi:10.1103/physrevd.15.2929 · Cited by 2,552
Constraints on supersymmetry breaking
Witten, E. (1982) · Nuclear Physics B · doi:10.1016/0550-3213(82)90071-2 · Cited by 1,960
Gravitational effects on and of vacuum decay
Coleman, S., & De Luccia, F. (1980) · Physical Review D · doi:10.1103/physrevd.21.3305 · Cited by 1,537 · cited 1×
“Writ large, the possible instanton decay channels can be grouped as Coleman-de Luccia tunnelling of a scalar field [1], the nucleation of charged membranes via the Brown-Teitelboim mechanism [2], and the decay of spacetime itself through Witten’s bubble of nothing [3].”
BackgroundA new proof of the positive energy theorem
Witten, E. (1981) · Communications in Mathematical Physics · doi:10.1007/bf01208277 · Cited by 1,163
The string landscape, black holes and gravity as the weakest force
Arkani-Hamed, N., Motl, L., Nicolis, A., & Vafa, C. (2007) · Journal of High Energy Physics · doi:10.1088/1126-6708/2007/06/060 · Cited by 1,052
The Swampland: Introduction and Review
Palti, E. (2019) · Fortschritte der Physik · doi:10.1002/prop.201900037 · Cited by 908
On the proof of the positive mass conjecture in general relativity
Schoen, R., & Yau, S.-T. (1979) · Communications in Mathematical Physics · doi:10.1007/bf01940959 · Cited by 870
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Metadata
- Authors
- Dibitetto, G., Petri, N., & Schillo, M.
- Affiliations
- Universidad de Oviedo (ES)
- Uppsala University (SE)
- Corresponding author
- Schillo, Marjorie
- ORCID
- Petri, Nicolò
- Venue
- Journal of High Energy Physics
- Published
- 2020-08-10
- Volume
- 2020
- Issue
- 8
- ISSN
- 1029-8479 (ISSN-L)
- OpenAlex
- W3004464755
- Semantic Scholar
- 2e3d43a3fc01c8c44f995b86aae64c8862c3ed0f
- Cited by
- 45
- References
- 64
- Citations by year
- 2026: 7 · 2025: 3 · 2024: 9 · 2023: 4 · 2022: 11 · 2021: 6 · 2020: 4
- FWCI
- 2.43
- Type
- journal article
- Language
- en
- Open access
- diamond
- doi.org
- Locations
- Journal of High Energy Physics (publishedVersion, cc-by)
- arXiv (Cornell University) (submittedVersion)
- Uppsala University Publications (Uppsala University) (submittedVersion, other-oa)
- Cineca Institutional Research Information System (Tor Vergata University) (submittedVersion)
- DOAJ (DOAJ: Directory of Open Access Journals) (submittedVersion, cc-by-sa)
- arXiv (Cornell University)
- Funders
- Vetenskapsrådet
- Türkiye Bilimsel ve Teknolojik Araştırma Kurumu (116F137)
- Topics
- 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
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Noncommutative and Quantum Gravity Theories
- Keywords
- AdS spacetime, gravitational instantons, bubble of nothing, Euclidean action, de Sitter geometry, topological obstructions, supersymmetric vacua, string theory, cosmological constant, higher-dimensional gravity
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