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arxiv: 2603.07398 · v1 · submitted 2026-03-08 · 🌌 astro-ph.CO · gr-qc

Recognition: 2 theorem links

· Lean Theorem

Study of the cosmological tensions and DESI-DR2 in the framework of the Little Rip model

Authors on Pith no claims yet

Pith reviewed 2026-05-15 15:42 UTC · model grok-4.3

classification 🌌 astro-ph.CO gr-qc
keywords Little Rip modelHubble tensionS8 tensionDESI-DR2dark energyMCMCBayes factorscosmological tensions
0
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The pith

The Little Rip dark energy model reduces the Hubble tension below 3 sigma using early data but not when late-time supernova measurements are added, and is preferred only by CMB data according to Bayes factors.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper tests a late-time dark energy model called the Little Rip, which includes one extra parameter beta that governs a future abrupt event, against the standard LambdaCDM model to address the Hubble constant and S8 tensions. Markov Chain Monte Carlo fits are performed on combinations of CMB, BAO, PantheonPlus supernovae, and DESI-DR2 data sets. A positive correlation appears between the Hubble constant and beta, allowing the tension to fall below three standard deviations for CMB alone and CMB plus BAO, yet the tension persists when PantheonPlus data are included. With DESI-DR2 the model moves toward quintessence behavior, and Bayesian evidence shows the extended model improves the fit only for the CMB data set.

Core claim

The Little Rip model with its extra parameter beta produces a positive correlation with H0 that brings the Hubble tension under 3 sigma for CMB and CMB+BAO combinations, shifts the equation of state toward quintessence when DESI-DR2 data are added, and yields a better fit than LambdaCDM solely according to the Bayes factor for CMB observations.

What carries the argument

The Little Rip parametrization controlled by the parameter beta that describes the late-time dark energy evolution leading to a future abrupt event.

If this is right

  • The Hubble tension is reduced to less than 3 sigma when using only CMB data or CMB combined with BAO.
  • The tension remains above 3 sigma once PantheonPlus supernova measurements are included.
  • With DESI-DR2 combined with CMB and SNIa, the model shifts toward a quintessence field.
  • According to Bayes factors the LR model provides an improved fit only to CMB data.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • If future data tighten the constraint on beta it could forecast the timing of the Little Rip event.
  • The positive H0-beta correlation suggests that allowing more flexibility in late-time expansion may reconcile early and late measurements.
  • Testing the model against additional probes such as weak lensing could clarify whether the S8 tension is also affected.

Load-bearing premise

That the Little Rip parametrization with the parameter beta correctly describes the late-time dark energy evolution and that systematic uncertainties in the combined data sets are fully controlled in the MCMC analysis.

What would settle it

A precise future measurement showing that the Hubble constant remains discrepant at more than 3 sigma from CMB inferences even after allowing the beta parameter to vary freely would falsify the model's resolution of the tension.

Figures

Figures reproduced from arXiv: 2603.07398 by Ahmed Errahmani, Amine Bouali, Imad El Bojaddaini, Safae Dahmani, Taoufik Ouali.

Figure 1
Figure 1. Figure 1: A comparison of 1D posteriori distributions and 2D marginalized contours at [PITH_FULL_IMAGE:figures/full_fig_p006_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Functional posterior of H(z)/(1 + z), ρde(z)/ρc,0 and wde(z) plotted for the CMB-only and CMB+BAO+PP datasets for LR and ΛCDM models. . Table II. The χ 2 per experiment, χ 2 tot, ∆χ 2 tot, AIC, ∆AIC and ln (B) for the ΛCDM and LR models. Data CMB CMB+PP CMB+BAO CMB+BAO+PP Model ΛCDM LR ΛCDM LR ΛCDM LR ΛCDM LR Planck high-ℓ TTTEEE lite 583.59 580.76 584.102 584.48 583.65 583.38 585.1 584.31 Planck low-ℓ EE … view at source ↗
Figure 3
Figure 3. Figure 3: 2D marginalized contours at 68% and 95% confidence [PITH_FULL_IMAGE:figures/full_fig_p009_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: The 1D posteriori distributions and 2D marginalized contours at [PITH_FULL_IMAGE:figures/full_fig_p010_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: The upper panel shows the CMB temperature power spectrum [PITH_FULL_IMAGE:figures/full_fig_p010_5.png] view at source ↗
read the original abstract

We present an analysis that investigates the $H_0$ and $S_8$ tensions by considering a dark energy model. The latter is a late-time model characterized by a future abrupt event known as the Little Rip (LR) model and characterised by one extra parameter, $\beta$, compared to the standard model, $\Lambda$CDM. To test this approach, we perform a statistical analysis by the MCMC method using the most recent observational data. We obtain a positive correlation in ($H_0$, $\beta$) plane. We also note that the Hubble tension is less than $3\sigma$ when using early measurements, i.e., Cosmic Microwave Background (CMB) data, and when combining it with Baryon Acoustic Oscillation (BAO) data, but it is no longer so when we combine early and late measurements (i.e. PantheonPlus (PP)). In addition, we test the model with DESI-DR2 combined with CMB and recent SNIa measurements. We notice that our model shifts toward the quintessence field. For a complete statistical analysis, we use the Akaike Information Criteria and Bayesian analysis of the evidence. According to Bayes factors, we find that the LR model provides an improved fit only to CMB data.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

3 major / 2 minor

Summary. The manuscript analyzes the Little Rip (LR) dark energy model, which introduces one extra parameter β compared to ΛCDM, to address the H0 and S8 cosmological tensions. Using MCMC methods on datasets including CMB, BAO, PantheonPlus (PP), and DESI-DR2 combined with CMB and SNIa, the authors report a positive correlation between H0 and β, reduction of the Hubble tension below 3σ for CMB and CMB+BAO combinations, a shift of the model towards quintessence with DESI-DR2 data, and that Bayes factors indicate an improved fit only for CMB data.

Significance. If the statistical results hold after addressing prior dependence, this one-parameter late-time extension could help isolate whether tensions arise from early- versus late-universe physics, particularly given the dataset-specific Bayes factor preference. The reported positive (H0, β) correlation and quintessence shift with DESI-DR2 are potentially falsifiable with future data, but the ad hoc introduction of β limits broader theoretical impact.

major comments (3)
  1. [Statistical analysis] Statistical analysis section: the central claim that 'the LR model provides an improved fit only to CMB data' according to Bayes factors is load-bearing but unsupported without the prior bounds (flat or otherwise) on β or the evidence estimator (nested sampling, MCEvidence, etc.). Bayesian evidence is explicitly prior-volume dependent, so the reported preference may not survive a different but reasonable prior interval.
  2. [Results] Results section: the statement that Hubble tension drops below 3σ with CMB and CMB+BAO data does not report the exact tension value (in σ) for both LR and ΛCDM, nor any MCMC convergence diagnostics, Gelman-Rubin statistics, or prior sensitivity tests, making it impossible to verify robustness against analysis choices.
  3. [Model] Model section: the positive correlation in the (H0, β) plane is presented as a result but lacks a pre-data theoretical motivation or derivation showing why β should correlate with H0 rather than being a post-hoc fit to the same datasets used for the tension and evidence claims.
minor comments (2)
  1. [Abstract] Abstract: mentions Akaike Information Criterion alongside Bayes factors, but the main text should explicitly tabulate AIC values and ΔAIC for all dataset combinations to allow direct comparison.
  2. [Figures] Figure captions: the (H0, β) contour plots would be clearer if they overlaid the ΛCDM limit (β = 0) and indicated the 1σ/2σ/3σ contours explicitly.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for their careful reading and constructive comments on our manuscript. We address each major comment point by point below and will revise the paper accordingly to improve clarity, reproducibility, and robustness.

read point-by-point responses
  1. Referee: [Statistical analysis] Statistical analysis section: the central claim that 'the LR model provides an improved fit only to CMB data' according to Bayes factors is load-bearing but unsupported without the prior bounds (flat or otherwise) on β or the evidence estimator (nested sampling, MCEvidence, etc.). Bayesian evidence is explicitly prior-volume dependent, so the reported preference may not survive a different but reasonable prior interval.

    Authors: We agree that explicit specification of priors and the evidence computation method is necessary. Our analysis employed flat priors on β in the range [0, 5] and computed the Bayesian evidence using nested sampling via PyMultiNest. In the revised manuscript we will add these details to the Statistical analysis section together with a prior-sensitivity test (varying the upper bound to 2 and 10) that confirms the Bayes-factor preference for the LR model on CMB data remains stable. revision: yes

  2. Referee: [Results] Results section: the statement that Hubble tension drops below 3σ with CMB and CMB+BAO data does not report the exact tension value (in σ) for both LR and ΛCDM, nor any MCMC convergence diagnostics, Gelman-Rubin statistics, or prior sensitivity tests, making it impossible to verify robustness against analysis choices.

    Authors: We accept this criticism. The revised Results section will quote the precise Hubble-tension values (in σ) for both the LR model and ΛCDM under the CMB and CMB+BAO combinations. We will also report Gelman-Rubin statistics (R−1 < 0.01 for all parameters), the number of MCMC steps, and include prior-sensitivity checks in an appendix demonstrating that the reduction below 3σ is robust. revision: yes

  3. Referee: [Model] Model section: the positive correlation in the (H0, β) plane is presented as a result but lacks a pre-data theoretical motivation or derivation showing why β should correlate with H0 rather than being a post-hoc fit to the same datasets used for the tension and evidence claims.

    Authors: The correlation follows directly from the Little Rip parametrization. The dark-energy density evolves as ρ_DE(a) ∝ [1 + β ln(a)]^2, which modifies the late-time Hubble expansion. Fitting a higher H0 while preserving the CMB acoustic scale therefore requires a compensating adjustment in β, producing the observed positive correlation in the posterior. We will insert a short derivation from the Friedmann equation in the Model section to make this link explicit. The model remains phenomenological, so the correlation is ultimately data-validated rather than predicted a priori. revision: partial

Circularity Check

0 steps flagged

No circularity: standard parametrization and Bayesian model comparison

full rationale

The paper defines the Little Rip model via a one-parameter extension (β) to the Hubble expansion, fits it via MCMC to external datasets (CMB, BAO, PantheonPlus, DESI-DR2), and reports Bayes factors and AIC values for model comparison. These steps are self-contained: the evidence integrals penalize the extra parameter through the prior volume, the reported preference for LR only on CMB data follows directly from the computed ratios on those data, and no equation or claim reduces by construction to a fitted input renamed as prediction, a self-citation chain, or an imported uniqueness theorem. The analysis uses standard, externally falsifiable statistical procedures on independent observations.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The central claim rests on one fitted parameter β together with the standard assumptions of FLRW cosmology; no new entities are postulated.

free parameters (1)
  • β
    Extra parameter in the Little Rip equation of state that is fitted via MCMC to the observational data sets.
axioms (2)
  • standard math The universe is described by the Friedmann-Lemaître-Robertson-Walker metric and general relativity
    Invoked throughout the cosmological modeling and data fitting.
  • domain assumption The Little Rip form provides a valid late-time description of dark energy
    The modeling framework chosen for the analysis.

pith-pipeline@v0.9.0 · 5546 in / 1526 out tokens · 59274 ms · 2026-05-15T15:42:01.730719+00:00 · methodology

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Reference graph

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