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Space-time superpositions as fluctuating geometries
General Relativity and Quantum Cosmology · Submitted 30 May 2024
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim A detailed analysis in the weak-field limit reveals quantum corrections to Newton's potential in generic semiclassical states, as well as new bounds on quantum fluctuations, implied by the covariance condition, rather than the usual uncertainty principle.
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The abstract, sentence by sentence
Superpositions of black holes can be described geometrically using a combined canonical formulation for space-time and quantum states. A previously introduced black-hole model that includes quantum fluctuations of metric components is shown here to give full access to the corresponding space-time geometry of weak-field gravity in terms of suitable line elements with quantum corrections. These results can be interpreted as providing covariant formulations of the gravitational force implied by a distribution of black holes in superposition. They can also be understood as a distribution of quantum matter constituents in superposition for a single black hole. A detailed analysis in the weak-field limit reveals quantum corrections to Newton's potential in generic semiclassical states, as well as new bounds on quantum fluctuations, implied by the covariance condition, rather than the usual uncertainty principle. These results provide additional control on quantum effects in Newton's potential that can be used in a broad range of predictions to be compared with observations.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Superpositions of black holes can be described geometrically using a combined canonical formulation for space-time and quantum states. | method 0.38 | 0.46 | 0.23 | asserted 0.88 |
| s1 | A previously introduced black-hole model that includes quantum fluctuations of metric components is shown here to give full access to the corresponding space-time geometry of weak-field gravity in terms of suitable line elements with quantum corrections. | contribution 0.48 | 0.84 | 0.39 | asserted 1.00 |
| s2 | These results can be interpreted as providing covariant formulations of the gravitational force implied by a distribution of black holes in superposition. | interpretation 1.00 | 0.72 | 0.24 | hedged possibility 0.86 |
| s3 | They can also be understood as a distribution of quantum matter constituents in superposition for a single black hole. | interpretation 1.00 | 0.59 | 0.10 | hedged possibility 0.60 |
| s4 | A detailed analysis in the weak-field limit reveals quantum corrections to Newton's potential in generic semiclassical states, as well as new bounds on quantum fluctuations, implied by the covariance condition, rather than the usual uncertainty principle. | result 0.98 | 0.90 | 0.40 | asserted 1.00 |
| s5 | These results provide additional control on quantum effects in Newton's potential that can be used in a broad range of predictions to be compared with observations. | interpretation 0.51 | 0.78 | 0.22 | asserted 0.90 |
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The paper
Original abstract
Superpositions of black holes can be described geometrically using a combined canonical formulation for space-time and quantum states. A previously introduced black-hole model that includes quantum fluctuations of metric components is shown here to give full access to the corresponding space-time geometry of weak-field gravity in terms of suitable line elements with quantum corrections. These results can be interpreted as providing covariant formulations of the gravitational force implied by a distribution of black holes in superposition. They can also be understood as a distribution of quantum matter constituents in superposition for a single black hole. A detailed analysis in the weak-field limit reveals quantum corrections to Newton's potential in generic semiclassical states, as well as new bounds on quantum fluctuations, implied by the covariance condition, rather than the usual uncertainty principle. These results provide additional control on quantum effects in Newton's potential that can be used in a broad range of predictions to be compared with observations.
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How the literature uses it
What this paper does with the arXiv papers it cites
What it cites · 22 sentences without a confident label
Uses the method or tool of 1 paper
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Our methods were originally developed in [ref] and evaluated in Schwarzschild-type coordinates.
Quasiclassical solutions for static quantum black holes · Conclusions · 0.96
Compares with 2 papers
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From the first two terms of the expansion, we obtain the solution [equation] To first order in $b/x$, this result is consistent with the corresponding solution derived for Schwarzschild coordinates in [ref] .
Quasiclassical solutions for static quantum black holes · Solutions · 1.00
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Therefore, our quantum corrections are always greater than what is expected from perturbative quantum gravity as derived (with varying results) for instance in [ref] .
Effective Field Theory of Gravity: Leading Quantum Gravitational Corrections to Newtons and Coulombs Law · Effective potentials · 0.95
Cites as background 6 papers
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Recent examples of such studies include [ref] for superpositions of spherically symmetric masses or shells.
Quantum signatures of black hole mass superpositions · Current approaches · 0.89
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Recent examples of such studies include [ref] for superpositions of spherically symmetric masses or shells.
Gravitational quantum switch on a superposition of spherical shells · Current approaches · 0.89
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For instance, various proposals in [ref] analyze potential aspects of quantum superpositions of test-particle states at locations that experience different values of proper time, due to their location in the gravitational potential well of a larger mass.
Quantum clocks observe classical and quantum time dilation · Current approaches · 0.90
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