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New quantum aspects of a vacuum-dominated universe
General Relativity and Quantum Cosmology · Submitted 28 Mar 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This spatially-flat solution implies an accelerating universe at the present time and gives a good one-parameter fit to high-redshift Type Ia supernovae (SNe-Ia) data, and the present age and energy density of the universe.
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The abstract, sentence by sentence
In a new model that we proposed, nonperturbative vacuum contributions to the effective action of a free quantized massive scalar field lead to a cosmological solution in which the scalar curvature becomes constant after a time $t_j$ (when the redshift $z \sim 1$) that depends on the mass of the scalar field and its curvature coupling. This spatially-flat solution implies an accelerating universe at the present time and gives a good one-parameter fit to high-redshift Type Ia supernovae (SNe-Ia) data, and the present age and energy density of the universe. Here we show that the imaginary part of the nonperturbative curvature term that causes the cosmological acceleration, implies a particle production rate that agrees with predictions of other methods and extends them to non-zero mass fields. The particle production rate is very small after the transition and is not expected to alter the nature of the cosmological solution. We also show that the equation of state of our model undergoes a transition at $t_j$ from an equation of state dominated by non-relativistic pressureless matter (without a cosmological constant) to an effective equation of state of mixed radiation and cosmological constant, and we derive the equation of state of the vacuum. Finally, we explain why nonperturbative vacuum effects of this ultralow-mass particle do not significantly change standard early universe cosmology.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In a new model that we proposed, nonperturbative vacuum contributions to the effective action of a free quantized massive scalar field lead to a cosmological solution in which the scalar curvature becomes constant after a time $t_j$ (when the redshift $z \sim 1$) that depends on the mass of the scalar field and its curvature coupling. | contribution 0.66 | 0.91 | 0.60 | asserted 1.00 |
| s1 | This spatially-flat solution implies an accelerating universe at the present time and gives a good one-parameter fit to high-redshift Type Ia supernovae (SNe-Ia) data, and the present age and energy density of the universe. | result 0.87 | 0.87 | 0.35 | asserted 0.99 |
| s2 | Here we show that the imaginary part of the nonperturbative curvature term that causes the cosmological acceleration, implies a particle production rate that agrees with predictions of other methods and extends them to non-zero mass fields. | result 0.82 | 0.93 | 0.21 | asserted 1.00 |
| s3 | The particle production rate is very small after the transition and is not expected to alter the nature of the cosmological solution. | interpretation 0.61 | 0.79 | 0.08 | hedged possibility 0.50 |
| s4 | We also show that the equation of state of our model undergoes a transition at $t_j$ from an equation of state dominated by non-relativistic pressureless matter (without a cosmological constant) to an effective equation of state of mixed radiation and cosmological constant, and we derive the equation of state of the vacuum. | result 0.89 | 0.96 | 0.16 | asserted 1.00 |
| s5 | Finally, we explain why nonperturbative vacuum effects of this ultralow-mass particle do not significantly change standard early universe cosmology. | interpretation 0.51 | 0.86 | 0.12 | asserted 0.98 |
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Original abstract
In a new model that we proposed, nonperturbative vacuum contributions to the effective action of a free quantized massive scalar field lead to a cosmological solution in which the scalar curvature becomes constant after a time $t_j$ (when the redshift $z \sim 1$) that depends on the mass of the scalar field and its curvature coupling. This spatially-flat solution implies an accelerating universe at the present time and gives a good one-parameter fit to high-redshift Type Ia supernovae (SNe-Ia) data, and the present age and energy density of the universe. Here we show that the imaginary part of the nonperturbative curvature term that causes the cosmological acceleration, implies a particle production rate that agrees with predictions of other methods and extends them to non-zero mass fields. The particle production rate is very small after the transition and is not expected to alter the nature of the cosmological solution. We also show that the equation of state of our model undergoes a transition at $t_j$ from an equation of state dominated by non-relativistic pressureless matter (without a cosmological constant) to an effective equation of state of mixed radiation and cosmological constant, and we derive the equation of state of the vacuum. Finally, we explain why nonperturbative vacuum effects of this ultralow-mass particle do not significantly change standard early universe cosmology.
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References
How the literature uses it
12 arXiv papers cite this in 17 sentences
Papers citing it · 12 sentences without a confident label
Cites it as background 5 papers
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In the VM paradigm, the universe undergoes a rapid transition from a standard Friedman-Lemaître-Robetson-Walker (FLRW) spacetime dominated by cold dark matter to one containing significant contributions of vacuum energy and pressure [ref] .
Touch of Neutrinos on the Vacuum Metamorphosis: is the $H_0$ Solution Back? · Vacuum Metamorphosis Revisited · 0.93
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The Vacuum Metamorphosis (VM) model, inspired on quantum gravitational effects, is based on a late-time gravitational phase transition [ref] .
Minimal dark energy: key to sterile neutrino and Hubble constant tensions? · The Vacuum Metamorphosis model · 0.95
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In addition, the vacuum metamorphosis (VM) [ref] , which has a phase transition in the nature of the vacuum, is also considered in this work.
Comparing dark energy models with current observational data · Introduction · 0.90
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