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The quantum realm of the "Little Sibling" of the Big Rip singularity
General Relativity and Quantum Cosmology · Submitted 24 Sep 2015
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We conclude that in all the cases analysed the DW condition can be verified, which might be an indication that the LSBR can be avoided or smoothed in the quantum approach.
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The abstract, sentence by sentence
We analyse the quantum behaviour of the "Little Sibling" of the Big Rip singularity (LSBR) [1]. The quantisation is carried within the geometrodynamical approach given by the Wheeler--DeWitt (WDW) equation. The classical model is based on a Friedmann--Lema\^{i}tre--Robertson--Walker Universe filled by a perfect fluid that can be mapped to a scalar field with phantom character. We analyse the WDW equation in two setups. In the first step, we consider the scale factor as the single degree of freedom, which from a classical perspective parametrises both the geometry and the matter content given by the perfect fluid. We then solve the WDW equation within a WKB approximation, for two factor ordering choices. On the second approach, we consider the WDW equation with two degrees of freedom: the scale factor and a scalar field. We solve the WDW equation, with the Laplace--Beltrami factor-ordering, using a Born--Oppenheimer approximation. In both approaches, we impose the DeWitt (DW) condition as a potential criterion for singularity avoidance. We conclude that in all the cases analysed the DW condition can be verified, which might be an indication that the LSBR can be avoided or smoothed in the quantum approach.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We analyse the quantum behaviour of the "Little Sibling" of the Big Rip singularity (LSBR) [1]. | contribution 0.99 | 0.92 | 0.02 | asserted 0.86 |
| s1 | The quantisation is carried within the geometrodynamical approach given by the Wheeler--DeWitt (WDW) equation. | method 0.99 | 0.75 | 0.02 | asserted 1.00 |
| s2 | The classical model is based on a Friedmann--Lema\^{i}tre--Robertson--Walker Universe filled by a perfect fluid that can be mapped to a scalar field with phantom character. | method 0.90 | 0.29 | 0.02 | asserted 1.00 |
| s3 | We analyse the WDW equation in two setups. | method 0.91 | 0.88 | 0.01 | asserted 0.89 |
| s4 | In the first step, we consider the scale factor as the single degree of freedom, which from a classical perspective parametrises both the geometry and the matter content given by the perfect fluid. | method 0.99 | 0.48 | 0.01 | asserted 1.00 |
| s5 | We then solve the WDW equation within a WKB approximation, for two factor ordering choices. | method 0.99 | 0.96 | 0.02 | asserted 0.99 |
| s6 | On the second approach, we consider the WDW equation with two degrees of freedom: the scale factor and a scalar field. | method 0.96 | 0.85 | 0.02 | asserted 0.97 |
| s7 | We solve the WDW equation, with the Laplace--Beltrami factor-ordering, using a Born--Oppenheimer approximation. | method 0.99 | 0.95 | 0.02 | asserted 1.00 |
| s8 | In both approaches, we impose the DeWitt (DW) condition as a potential criterion for singularity avoidance. | method 0.98 | 0.94 | 0.04 | asserted 0.73 |
| s9 | We conclude that in all the cases analysed the DW condition can be verified, which might be an indication that the LSBR can be avoided or smoothed in the quantum approach. | interpretation 0.74 | 0.93 | 0.97 | hedged possibility 0.63 |
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Original abstract
We analyse the quantum behaviour of the "Little Sibling" of the Big Rip singularity (LSBR) [1]. The quantisation is carried within the geometrodynamical approach given by the Wheeler--DeWitt (WDW) equation. The classical model is based on a Friedmann--Lema\^{i}tre--Robertson--Walker Universe filled by a perfect fluid that can be mapped to a scalar field with phantom character. We analyse the WDW equation in two setups. In the first step, we consider the scale factor as the single degree of freedom, which from a classical perspective parametrises both the geometry and the matter content given by the perfect fluid. We then solve the WDW equation within a WKB approximation, for two factor ordering choices. On the second approach, we consider the WDW equation with two degrees of freedom: the scale factor and a scalar field. We solve the WDW equation, with the Laplace--Beltrami factor-ordering, using a Born--Oppenheimer approximation. In both approaches, we impose the DeWitt (DW) condition as a potential criterion for singularity avoidance. We conclude that in all the cases analysed the DW condition can be verified, which might be an indication that the LSBR can be avoided or smoothed in the quantum approach.
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References
How the literature uses it
12 arXiv papers cite this in 21 sentences
Papers citing it · 18 sentences without a confident label
Compares with it 1 paper
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This is in strike difference to what happens in GR in presence of a BR singularity induced by a phantom minimally coupled scalar field where $G^AB$ has a positive signature [ref] .
$f(R)$ quantum cosmology: avoiding the Big Rip · Modified Wheeler–DeWitt equation · 1.00
Cites it as background 2 papers
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Examples of these models can be found, for instance, in references [ref] .
Classical and quantum $f(R)$ cosmology: The big rip, the little rip and the little sibling of the big rip · Modified Wheeler-DeWitt · 0.81
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This abrupt event has been well studied in [ref] and dubbed as Little Sibling of the Big Rip since it smooths the big rip singularity in the future.
Smoothing the $H_0$ tension with a dynamical dark energy model · introduction · 0.93
What it cites · 25 sentences without a confident label
Uses the method or tool of 1 paper
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Using the WKB (Wentzel, Kramers, Brillouin) approximation method at first order, which is enough to ensure that the DW condition is satisfied; i.e. $Ψ(u)$ vanishes for $u→∞$, the wave function of the universe can be described by [ref]
Quantisation of the holographic Ricci dark energy model · First quantisation procedure ($aĤ(a,π̂_a)ψ(a)=0$) · 0.87
Cites as background 13 papers
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This future event is what we refer as “Little Sibling” of the Big Rip singularity [ref] .
The little sibling of the big rip singularity · The Little Sibling of the Big Rip event: review · 0.80
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This second case, it what we named the Big Démarrage, it results from a phantom fluid leading to a cosmic expansion that starts with infinite acceleration [ref] .].
On the quantum fate of singularities in a dark-energy dominated universe · Introduction · 0.83
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Some works have applied the methods of quantum cosmology to the classical models leading to these DE related singularities [ref] .
Does loop quantum cosmology replace the big rip singularity by a non-singular bounce? · Introduction · 0.84
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