2011
DOI: 10.1063/1.3567157
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A spatially homogeneous and isotropic Einstein–Dirac cosmology

Abstract: Abstract. We consider a spatially homogeneous and isotropic cosmological model where Dirac spinors are coupled to classical gravity. For the Dirac spinors we choose a Hartree-Fock ansatz where all one-particle wave functions are coherent and have the same momentum. If the scale function is large, the universe behaves like the classical Friedmann dust solution. If however the scale function is small, quantum effects lead to oscillations of the energy-momentum tensor. It is shown numerically and proven analytica… Show more

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Cited by 4 publications
(6 citation statements)
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“…Let us briefly discuss the qualitative dependence of the bounce on the free parameters R max , R qu , λ, and φ of our model (for a detailed analysis we refer to [4]). First of all, the probability of preventing the crunch can be increased by choosing |w 1 (R max )| smaller.…”
Section: Quantum Oscillations Preventing the Big Crunchmentioning
confidence: 99%
See 3 more Smart Citations
“…Let us briefly discuss the qualitative dependence of the bounce on the free parameters R max , R qu , λ, and φ of our model (for a detailed analysis we refer to [4]). First of all, the probability of preventing the crunch can be increased by choosing |w 1 (R max )| smaller.…”
Section: Quantum Oscillations Preventing the Big Crunchmentioning
confidence: 99%
“…If R min > 0, the big crunch is avoided and R "bounces back," whereas in the case R min = 0 the big crunch appears despite the quantum effects. Considering the phase φ as unknown, one can give the result of Let us briefly discuss the qualitative dependence of the bounce on the free parameters R max , R qu , λ, and φ of our model (for a detailed analysis we refer to [4]). First of all, the probability of preventing the crunch can be increased by choosing |w 1 (R max )| smaller.…”
Section: Quantum Oscillations Preventing the Big Crunchmentioning
confidence: 99%
See 2 more Smart Citations
“…This assumption is reasonable because we cannot expect the WKB approximation to hold near the singularities (in particular because "quantum oscillations" become relevant; see [15]). Under this assumption, the estimate (5.15) can be translated to a relative error of the order O((mR max ) − 1 5 ).…”
Section: Example: a Closed Friedmann-robertson-walker Universementioning
confidence: 99%