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Classical and quantum $f(R)$ cosmology: The big rip, the little rip and the little sibling of the big rip

General Relativity and Quantum Cosmology · Submitted 22 Jun 2021

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim In this review, we discuss the classical and quantum occurrence of these riplike events in the scheme of metric $f(R)$ theories of gravity.

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arXiv ID2106.12050 (version 2)
Pith IDET2AARF4, Pith's permanent record of this paper and its review
CitationMariam Bouhmadi-L\'opez, Prado Mart\'in-Moruno, Teodor Borislavov Vasilev. "Classical and quantum $f(R)$ cosmology: The big rip, the little rip and the little sibling of the big rip." arXiv:2106.12050 (2021). https://pith.science/paper/ET2AARF4
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What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.11 · human participants 0.01 · controlled comparison 0.03 · randomized assignment 0.01 · states quantitative result 0.03 · compares with prior results 0.16 · mentions code or data availability 0.02.

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arXiv listing abstract v2. Results and the main claim are underlined; .

The big rip, the little rip and the little sibling of the big rip are cosmological doomsdays predicted by some phantom dark energy models that could describe the future evolution of our Universe. When the universe evolves towards either of these future cosmic events all bounded structures and, ultimately, space-time itself are ripped apart. Nevertheless, it is commonly belief that quantum gravity effects may smooth or even avoid these classically predicted singularities. In this review, we discuss the classical and quantum occurrence of these riplike events in the scheme of metric $f(R)$ theories of gravity. The quantum analysis is performed in the framework of $f(R)$ quantum geometrodynamics. In this context, we analyse the fulfilment of the DeWitt criterion for the avoidance of these singular fates.

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What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 The big rip, the little rip and the little sibling of the big rip are cosmological doomsdays predicted by some phantom dark energy models that could describe the future evolution of our Universe. background 1.00 0.04 0.05 hedged possibility 0.88
s1 When the universe evolves towards either of these future cosmic events all bounded structures and, ultimately, space-time itself are ripped apart. background 1.00 0.05 0.04 asserted 0.99
s2 Nevertheless, it is commonly belief that quantum gravity effects may smooth or even avoid these classically predicted singularities. background 0.98 0.03 0.05 hedged possibility 0.96
s3 In this review, we discuss the classical and quantum occurrence of these riplike events in the scheme of metric $f(R)$ theories of gravity. contribution 1.00 0.71 0.07 asserted 0.86
s4 The quantum analysis is performed in the framework of $f(R)$ quantum geometrodynamics. method 0.99 0.76 0.04 asserted 0.98
s5 In this context, we analyse the fulfilment of the DeWitt criterion for the avoidance of these singular fates. method 0.85 0.88 0.06 asserted 0.60

What kind of paper the classifier reports this is: review 1.00 · evidence from literature 0.66.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

The big rip, the little rip and the little sibling of the big rip are cosmological doomsdays predicted by some phantom dark energy models that could describe the future evolution of our Universe. When the universe evolves towards either of these future cosmic events all bounded structures and, ultimately, space-time itself are ripped apart. Nevertheless, it is commonly belief that quantum gravity effects may smooth or even avoid these classically predicted singularities. In this review, we discuss the classical and quantum occurrence of these riplike events in the scheme of metric $f(R)$ theories of gravity. The quantum analysis is performed in the framework of $f(R)$ quantum geometrodynamics. In this context, we analyse the fulfilment of the DeWitt criterion for the avoidance of these singular fates.

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2 arXiv papers cite this in 2 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 1 sentence without a confident label

Cites it as background 1 paper

What it cites · 133 sentences without a confident label

Builds on 2 papers
Uses the method or tool of 1 paper
Uses data or values from 3 papers
  • [H] Best fit found in reference [ref] for the phantom DE models discussed in Section [ref], where $A$ is dimensionless for the case of the BR, and has units of inverse of meter and inverse of square meter for the LR and LSBR models, respectively.

    Cosmological constraints of phantom dark energy models · Cosmological Constraints · 0.99

  • The present concentrations of matter and dark energy are roughly $Ω_M,0=0.315$ and $Ω_DE,0=0.685$, respectively, whereas the contribution of radiation to the total content of the universe is negligible at the present time [ref] .

    Planck 2015 results. XIII. Cosmological parameters · A Phantom Dark-Energy Universe · 0.95

  • The present concentrations of matter and dark energy are roughly $Ω_M,0=0.315$ and $Ω_DE,0=0.685$, respectively, whereas the contribution of radiation to the total content of the universe is negligible at the present time [ref] .

    Planck 2018 results. VI. Cosmological parameters · A Phantom Dark-Energy Universe · 0.95

Compares with 3 papers
  • Thus, for the avoidance of the BR singularity, for instance, we found our approximations to the wave function of the universe to be legit only for very tiny values of the parameter $A$, indeed smaller even than those found in reference [ref] where a strong ansatz was imposed on the possible values of $w$.

    Cosmological constraints of phantom dark energy models · Conclusions · 0.91

  • Please note that this behavior was also found in reference [ref] , where it was dubbed “grand rip” (see type $-$1 singularities in reference [ref] ).

    Grand Rip and Grand Bang/Crunch cosmological singularities · A Phantom Dark-Energy Universe · 0.95

  • Please note that this behavior was also found in reference [ref] , where it was dubbed “grand rip” (see type $-$1 singularities in reference [ref] ).

    Initial directional singularity in inflationary models · A Phantom Dark-Energy Universe · 0.95

Cites as support 3 papers
  • It should be noted, however, that even though these abrupt events take place at the infinite distant future, bounded structures are destroyed in a finite time [ref] .

    The Little Rip · Introduction · 0.96

  • It should be noted, however, that even though these abrupt events take place at the infinite distant future, bounded structures are destroyed in a finite time [ref] .

    The little sibling of the big rip singularity · Introduction · 0.96

  • More importantly, some of these models have been shown to be compatible with the current observational data, see, for instance, reference [ref] .

    Cosmological constraints of phantom dark energy models · Conclusions · 0.98

Cites as background 61 papers

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