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Effect of the trace anomaly on the cosmological constant
Open accessAbstract
It has been argued that the quantum (conformal) trace anomaly could potentially provide us with a dynamical explanation of the cosmological constant problem. In this paper, however, we show by means of a semiclassical analysis that the trace anomaly does not affect the cosmological constant. We construct the effective action of the conformal anomaly for flat Friedmann-Lema\^{\i}tre-Robertson-Walker spacetimes consisting of local quadratic geometric curvature invariants. Counterterms are thus expected to influence the numerical value of the coefficients in the trace anomaly and we must therefore allow these parameters to vary. We calculate the evolution of the Hubble parameter in quasi-de Sitter spacetime, where we restrict our Hubble parameter to vary slowly in time, and in Friedmann-Lema\^{\i}tre-Robertson-Walker spacetimes. We show dynamically that a universe consisting of matter with a constant equation of state, a cosmological constant, and the quantum trace anomaly evolves either to the classical de Sitter attractor or to a quantum trace anomaly driven one. When considering the trace anomaly truncated to quasi-de Sitter spacetime, we find a region in parameter space where the quantum attractor destabilizes. When considering the exact expression of the trace anomaly, a stability analysis shows that whenever the trace anomaly driven attractor is stable, the classical de Sitter attractor is unstable, and vice versa. Semiclassically, the trace anomaly does not affect the classical late time de Sitter attractor, and hence it does not solve the cosmological constant problem.
Overview
CoChat Summary
TL;DR
Using a semiclassical analysis, the authors show that the quantum trace anomaly does not affect the late-time effective cosmological constant; the classical de Sitter attractor is not dynamically altered. They derive the anomaly effective action in flat FLRW and find either classical or anomaly-driven attractors depending on parameters, but conclude the trace anomaly does not solve the cosmological constant problem.
Key findings
- The trace anomaly can be generated by an infinite effective action in flat FLRW consisting of local quadratic curvature invariants \(R^2\) and the Gauss-Bonnet term \(E\); counterterms imply the coefficients \(b,b',b''\) are not uniquely fixed, so the authors vary them.
- Late-time asymptotes are a classical de Sitter attractor \(H^0_C\) and a quantum anomaly-driven attractor \(H^0_A\), independent of \(b''\); in the small-\(\lambda\) expansion \(H^0_C \simeq \sqrt{\Lambda/3}[1-8\pi b'\lambda]\) and \(H^0_A \simeq \sqrt{-1/(16\pi G b')-\Lambda/3}\).
- In quasi de Sitter spacetime, both attractors can be stable, but the quantum attractor destabilises when inequality (50) is violated; they illustrate this with \(b''=7b'/6<5b'/6\) for radiation \(w=1/3\), \(\lambda=1/50\), \(b'=-0.015\).
- In exact FLRW spacetimes, stability depends on the sign of \(b''-2b'/3\): if \(>0\), the quantum attractor is stable and the classical de Sitter attractor is unstable; if \(<0\), the classical attractor is stable and the quantum attractor is unstable; at \(b''=2b'/3\), both are stable. The classical attractor shows under-damped oscillations, with frequency independent of the equation of state.
Methods
- Semiclassical effective-field-theory approach: trace of the Einstein field equations plus stress-energy conservation, including matter with constant equation of state \(w>-1\), a cosmological constant, and the trace anomaly.
- Derives the anomaly effective action in flat FLRW from local quadratic curvature invariants \(R^2\) and Gauss-Bonnet \(E\), then studies two regimes: quasi de Sitter spacetime with slowly varying \(H\) and truncated higher derivatives, and exact FLRW spacetime including all higher-derivative contributions via numerical and linear stability analysis.
- Varies the anomaly coefficients \(b,b',b''\) because counterterms can shift their physical values; uses Standard Model values \(N_S=4\), \(N_F=45/2\), \(N_V=12\), with \(b'=-0.015\) and \(\lambda=1/50\) in figures.
Limitations
- Stated: the authors do not consider a new conformal degree of freedom; they do not know whether the truncated quasi de Sitter or exact FLRW treatment is correct, and note that higher-derivative terms may destabilise the system (Ostrogradsky). The quantum attractor is of order the Planck mass, where perturbative general relativity may break down and quantum fluctuations may affect or remove it.
- Stated: the physical coefficients in the trace anomaly have not been measured, so they must be allowed to vary.
- Evident from the text: the analysis assumes flat, homogeneous, isotropic FLRW spacetimes and constant \(w>-1\); stability conclusions depend on the sign of \(b''-2b'/3\) and on \(\lambda\ll 1\).
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In the paper
“The branching point is still given by equation (43) for which we just have to insert b ′′ = 2b ′ /3.”
§ Effect of the Trace Anomaly on the Cosmological Constant > B. Case II: b
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In the paper
“The trace anomaly or the conformal anomaly in four dimensions is in general curved spacetimes given by [6,7,33]: T Q ≡ T µ µ = bF + b ′ E - 2 3 2R + b ′′ 2R ,(2)”
§ Effect of the Trace Anomaly on the Cosmological Constant > II. TRACING THE EINSTEIN FIELD EQUATIONS AND THE TRACE ANOMALY A. The Conformal Anomaly in Four Dimensions in FLRW Spacetimes
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In the paper
“When the above inequality is satisfied, the Hubble parameter in the high energy limit decays exponentially towards the quantum anomaly driven attractor”
§ Effect of the Trace Anomaly on the Cosmological Constant > A. Case I: unrestricted value of b ′′
plainstates a cause- Asserted: passes — The authors put it forward as true.
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In the paper
“When considering the trace anomaly truncated to quasi de Sitter spacetime, we find a region in parameter space where the quantum attractor destabilises.”
§ Effect of the Trace Anomaly on the Cosmological Constant > Abstract
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In the paper
“Because ρ Q can be expressed in a local form, we would like to point out that this yields a local expression for the stressenergy tensor too.”
§ Effect of the Trace Anomaly on the Cosmological Constant > B. The Dynamics driven by the Trace Anomaly
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Metadata
- Authors
- Koksma, J. F., & Prokopec, T.
- Affiliations
- Utrecht University (NL)
- ORCID
- Prokopec, Tomislav
- Venue
- Physical Review D
- Publisher
- American Physical Society (APS)
- Published
- 2008-07-08
- Volume
- 78
- Issue
- 2
- ISSN
- 0556-2821 (ISSN-L)
- 1550-7998
- 1550-2368
- OpenAlex
- W2166561590
- Cited by
- 19
- References
- 61
- Citations by year
- 2025: 1 · 2023: 1 · 2021: 1 · 2020: 2 · 2019: 1 · 2017: 1 · 2015: 2 · 2014: 1 · 2013: 1
- FWCI
- 1.15
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Locations
- Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- Utrecht University Repository (Utrecht University) (submittedVersion, other-oa)
- arXiv (Cornell University)
- Funders
- Universiteit Utrecht
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Cosmology and Gravitation Theories
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Noncommutative and Quantum Gravity Theories
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Black Holes and Theoretical Physics
- Keywords
- trace anomaly, cosmological constant problem, Friedmann-Robertson-Walker spacetime, counterterms, Hubble parameter evolution, de Sitter attractor, attractor stability
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