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arxiv: 2602.22840 · v2 · submitted 2026-02-26 · 🌌 astro-ph.CO · gr-qc

Recognition: 2 theorem links

· Lean Theorem

Redshift evolution of the Hubble constant: Constraints and new insights from an interacting dark energy model

Authors on Pith no claims yet

Pith reviewed 2026-05-15 19:24 UTC · model grok-4.3

classification 🌌 astro-ph.CO gr-qc
keywords interacting dark energyHubble constantredshift evolutionHubble tensiondark sector interactioncosmological constraintsBAOCMB priors
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The pith

An interacting dark energy model produces a redshift-dependent Hubble constant that decreases at higher redshifts.

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

The paper introduces a modified interacting dark energy model where energy is exchanged between dark energy and dark matter, causing the Hubble constant to vary with redshift rather than remain fixed. Late-universe observations from BAO, cosmic chronometers, and supernovae constrain the interaction parameter alpha to approximately 0.01, supporting a power-law decline in H0 as redshift increases. Adding CMB distance priors tightens the bound on alpha by orders of magnitude because the interaction is suppressed at early times by baryon-photon coupling. This framework supplies a consistent dynamical description of H0 evolution that differs from the constant value assumed in Lambda CDM.

Core claim

In the interacting dark energy framework, energy exchange between dark energy and dark matter induces a redshift dependence of H0 that is parameterized by a single constant alpha. Late-Universe data yield alpha = 0.0107^{+0.0032}_{-0.011}, revealing a decreasing trend of H0 with redshift and supporting power-law evolution beyond Lambda CDM. CMB data further constrain alpha to order 10^{-5} because strong baryon-photon coupling suppresses dark-sector interactions at high redshifts.

What carries the argument

The redshift-dependent Hubble constant induced by dark-sector energy exchange and parameterized by the constant alpha that sets the interaction strength.

If this is right

  • Late-universe data alone favor a small positive alpha indicating H0 decreases with increasing redshift.
  • The model yields a power-law evolution for H0 that differs from the constant value in Lambda CDM.
  • Inclusion of CMB data suppresses the allowed interaction strength at early times due to baryon-photon coupling.
  • The framework supplies a dynamical mechanism capable of describing epoch-dependent H0 measurements.

Where Pith is reading between the lines

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

  • Future surveys at intermediate redshifts could directly test whether the inferred decline in H0 continues or flattens.
  • If the same interaction affects perturbation growth, it might produce observable signatures in large-scale structure that differ from standard predictions.
  • Relaxing the single-parameter assumption to allow redshift-dependent interaction strengths could be confronted with next-generation BAO and supernova samples.

Load-bearing premise

The chosen functional form of the dark-sector interaction is assumed to produce a redshift-dependent Hubble constant that can be captured entirely by fitting one constant alpha to the observations.

What would settle it

A direct measurement of the Hubble constant at redshift around 1 that shows no decline relative to low-redshift values, or that forces alpha to be consistent with zero at high significance, would rule out the model's predicted evolution.

Figures

Figures reproduced from arXiv: 2602.22840 by Fayin Wang, Shuangxi Yi, Xinyi Dai, Yankun Qu, Yicheng Wang, Yupeng Yang.

Figure 1
Figure 1. Figure 1: FIG. 1. 2-D posterior distributions and 1-D marginal [PITH_FULL_IMAGE:figures/full_fig_p005_1.png] view at source ↗
read the original abstract

We develop a modified interacting dark energy (IDE) model to study the redshift evolution of the Hubble constant ($H_0$), in light of the Hubble tension. In this framework, the energy exchange between dark energy and dark matter induces a redshift dependence of $H_0$. We evaluate the model against a comprehensive suite of observations, including baryon acoustic oscillations (BAO) from DESI DR2 and SDSS, cosmic chronometers, type Ia supernovae from the Pantheon sample, and Planck CMB distance priors. Analysis of late-Universe data yields $\alpha = 0.0107^{+0.0032}_{-0.011}$, with the best-fit value on the order of $10^{-2}$, revealing a decreasing trend of $H_0$ with redshift. This supports a power-law evolution beyond $\Lambda$CDM. Incorporating CMB data further tightens the constraint to the order of $10^{-5}$, which we attribute to the suppression of dark-sector interactions at high redshifts, a consequence of the strong baryon--photon coupling. These results indicate that the IDE framework provides a theoretically consistent and observationally viable mechanism for describing the redshift evolution of $H_0$, offering a promising avenue toward alleviating the Hubble tension.

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 paper proposes a modified interacting dark energy (IDE) model in which a constant parameter alpha governs energy exchange between dark energy and dark matter, inducing a redshift-dependent Hubble constant H0. Fits to late-Universe data (DESI DR2 and SDSS BAO, cosmic chronometers, Pantheon SNe) yield alpha = 0.0107^{+0.0032}_{-0.011}, interpreted as a decreasing H0(z) trend beyond LambdaCDM. Adding Planck CMB distance priors suppresses alpha to order 10^{-5}, attributed to baryon-photon coupling at high redshift. The authors conclude that the IDE framework provides a consistent and viable description of H0 evolution and a promising route to alleviating the Hubble tension.

Significance. If the model could be shown to accommodate both early- and late-Universe constraints with a single non-zero alpha that independently predicts the observed H0 discrepancy, the result would be significant for tension-resolution studies. The use of multiple independent late-time datasets is a positive feature. However, the reported suppression of alpha by CMB priors indicates that any apparent alleviation is confined to late-Universe subsets and does not extend to a joint early-late reconciliation.

major comments (3)
  1. [Abstract] Abstract: the claim that the IDE framework offers a promising avenue toward alleviating the Hubble tension is not supported when the full dataset is used, because CMB inclusion drives alpha to ~10^{-5} (consistent with zero interaction), leaving the model unable to maintain a non-zero interaction while satisfying CMB distance priors.
  2. [Abstract] Abstract and results: the redshift trend is obtained by fitting the free parameter alpha to the same observations that are then said to reveal the trend; the evolution is therefore defined by the fit rather than independently predicted, weakening the evidence for a genuine departure from LambdaCDM.
  3. [Abstract] Abstract: the attribution of alpha suppression to baryon-photon coupling at high z requires an explicit quantitative demonstration in the model equations (e.g., the interaction term and its redshift scaling) to show it is not simply an indication that the model fails to reconcile the datasets simultaneously.
minor comments (2)
  1. [Abstract] The abstract provides no derivation details, error budgets, or checks against post-hoc data choices for the reported constraints on alpha.
  2. [Model section] Clarify the precise functional form of the dark-sector interaction that produces the redshift-dependent H0 captured by the single constant alpha.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for the constructive and detailed report. We respond point-by-point to the major comments, clarifying our results and indicating revisions made to the manuscript.

read point-by-point responses
  1. Referee: [Abstract] Abstract: the claim that the IDE framework offers a promising avenue toward alleviating the Hubble tension is not supported when the full dataset is used, because CMB inclusion drives alpha to ~10^{-5} (consistent with zero interaction), leaving the model unable to maintain a non-zero interaction while satisfying CMB distance priors.

    Authors: We agree that CMB distance priors drive alpha to O(10^{-5}), consistent with zero interaction at high redshift. This is expected in our framework because the interaction is physically suppressed early on. The model nevertheless yields a statistically preferred non-zero alpha from late-universe data alone, providing a consistent description of H0(z) evolution in that regime. We have revised the abstract to state that the IDE framework offers a promising description of late-universe H0 evolution and a potential route to understanding the tension when early-universe constraints are considered separately, rather than claiming simultaneous reconciliation. revision: partial

  2. Referee: [Abstract] Abstract and results: the redshift trend is obtained by fitting the free parameter alpha to the same observations that are then said to reveal the trend; the evolution is therefore defined by the fit rather than independently predicted, weakening the evidence for a genuine departure from LambdaCDM.

    Authors: The model with constant alpha predicts a specific functional form for the redshift dependence of the effective Hubble parameter via the interaction term in the continuity equations. The data are used to constrain the single free parameter alpha; the resulting best-fit value being non-zero at ~3 sigma in the late-universe combination demonstrates that the predicted evolution is favored by the observations. This constitutes a test of the model's functional prediction rather than a circular definition of the trend. We have added clarifying text in the results section to emphasize the model's a priori predicted H0(z) form. revision: partial

  3. Referee: [Abstract] Abstract: the attribution of alpha suppression to baryon-photon coupling at high z requires an explicit quantitative demonstration in the model equations (e.g., the interaction term and its redshift scaling) to show it is not simply an indication that the model fails to reconcile the datasets simultaneously.

    Authors: We accept this point and have added an explicit derivation in the model section. Starting from the interaction term Q = 3 alpha H rho_de, we show that the effective coupling is modulated by the baryon-photon fluid's tight coupling at high z, which scales as (1+z)^4 in the early universe and suppresses the dark-sector exchange rate to O(10^{-5}) by z~1100. This quantitative scaling is now presented with the relevant equations, confirming it is a physical feature of the model rather than an ad hoc failure to reconcile datasets. revision: yes

Circularity Check

1 steps flagged

H0(z) redshift trend is produced by fitting the interaction parameter alpha to late-time data under an assumed functional form, reducing the claimed evolution to a fitted output rather than an independent derivation.

specific steps
  1. fitted input called prediction [Abstract (model results paragraph)]
    "Analysis of late-Universe data yields α = 0.0107^{+0.0032}_{-0.011}, with the best-fit value on the order of 10^{-2}, revealing a decreasing trend of H_0 with redshift."

    The model is constructed so that the dark-sector interaction (controlled by alpha) produces redshift-dependent H0 by design. Fitting alpha to the late-time data (BAO, chronometers, supernovae) then 'reveals' the trend, which is therefore the direct statistical output of the fit rather than an a priori prediction or first-principles result.

full rationale

The paper introduces a modified IDE model whose interaction term is parameterized by a constant alpha chosen to induce explicit redshift dependence in H0. Late-Universe observations are then used to constrain alpha, directly yielding the reported decreasing H0(z) trend. This matches the fitted-input-called-prediction pattern: the evolution is not predicted from first principles or external constraints but is defined by the model's ansatz and the fit to the same data. Inclusion of CMB priors drives alpha to ~10^{-5} (consistent with zero), showing the trend is not robust across the full dataset. The central claim of a viable mechanism for H0 evolution therefore rests on the parameterization and fit rather than an independent derivation chain.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim rests on a single fitted interaction strength alpha and the assumption that energy exchange in the dark sector produces a power-law redshift dependence of H0 within standard FLRW cosmology.

free parameters (1)
  • alpha = 0.0107^{+0.0032}_{-0.011}
    Interaction strength parameter whose value is determined by fitting to late-universe observations.
axioms (1)
  • domain assumption Energy is exchanged between dark energy and dark matter while total energy is conserved in the FLRW background
    Core modeling assumption invoked to derive the redshift dependence of H0.

pith-pipeline@v0.9.0 · 5544 in / 1316 out tokens · 24012 ms · 2026-05-15T19:24:34.119875+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

109 extracted references · 109 canonical work pages · 42 internal anchors

  1. [1]

    1999, , 517, 565, 10.1086/307221

    S. Perlmutteret al.(Supernova Cosmology Project), Astrophys. J.517, 565 (1999), arXiv:astro-ph/9812133

  2. [2]

    Discovery of a Supernova Explosion at Half the Age of the Universe and its Cosmological Implications

    S. Perlmutteret al.(Supernova Cosmology Project), Nature391, 51 (1998), arXiv:astro-ph/9712212

  3. [3]

    A. G. Riesset al.(Supernova Search Team), Astron. J. 116, 1009 (1998), arXiv:astro-ph/9805201

  4. [4]

    R. R. Caldwell and M. Doran, Phys. Rev. D69, 103517 (2004), arXiv:astro-ph/0305334

  5. [5]

    Holographic explanation of wide-angle power correlation suppression in the Cosmic Microwave Background Radiation

    Z.-Y. Huang, B. Wang, E. Abdalla, and R.-K. Su, JCAP 05, 013 (2006), arXiv:hep-th/0501059

  6. [6]

    Planck 2015 results. I. Overview of products and scientific results

    R. Adamet al.(Planck), Astron. Astrophys.594, A1 (2016), arXiv:1502.01582 [astro-ph.CO]

  7. [7]

    The clustering of galaxies in the completed SDSS-III Baryon Oscillation Spectroscopic Survey: cosmological analysis of the DR12 galaxy sample

    S. Alamet al.(BOSS), Mon. Not. Roy. Astron. Soc.470, 2617 (2017), arXiv:1607.03155 [astro-ph.CO]

  8. [8]

    The WiggleZ Dark Energy Survey: measuring the cosmic growth rate with the two-point galaxy correlation function

    C. Contreraset al.(WiggleZ), Mon. Not. Roy. Astron. Soc.430, 924 (2013), arXiv:1302.5178 [astro-ph.CO]

  9. [9]

    Cosmological parameters from SDSS and WMAP

    M. Tegmarket al.(SDSS), Phys. Rev. D69, 103501 (2004), arXiv:astro-ph/0310723

  10. [10]

    Alestas, L

    G. Alestas, L. Kazantzidis, and L. Perivolaropoulos, Phys. Rev. D101, 123516 (2020), arXiv:2004.08363 [astro-ph.CO]

  11. [11]

    In the Realm of the Hubble tension $-$ a Review of Solutions

    E. Di Valentino, O. Mena, S. Pan, L. Visinelli, W. Yang, A. Melchiorri, D. F. Mota, A. G. Riess, and J. Silk, Class. Quant. Grav.38, 153001 (2021), arXiv:2103.01183 [astro-ph.CO]

  12. [12]

    A. G. Riesset al., Astrophys. J. Lett.934, L7 (2022), arXiv:2112.04510 [astro-ph.CO]

  13. [14]

    Y. Yang, Y. Wang, and X. Dai, Eur. Phys. J. C85, 224 (2025), arXiv:2502.17792 [astro-ph.CO]

  14. [15]

    Early Dark Energy Can Resolve The Hubble Tension

    V. Poulin, T. L. Smith, T. Karwal, and M. Kamionkowski, Phys. Rev. Lett.122, 221301 (2019), arXiv:1811.04083 [astro-ph.CO]

  15. [16]

    Hu and F.-Y

    J.-P. Hu and F.-Y. Wang, Universe9, 94 (2023), arXiv:2302.05709 [astro-ph.CO]

  16. [17]

    Elizalde, J

    E. Elizalde, J. Gluza, and M. Khurshudyan, (2021), arXiv:2104.01077 [astro-ph.CO]

  17. [18]

    Khurshudyan and E

    M. Khurshudyan and E. Elizalde, Galaxies12, 31 (2024), arXiv:2402.08630 [gr-qc]

  18. [19]

    The CosmoVerse White Paper: Addressing observational tensions in cosmology with systematics and fundamental physics

    E. Di Valentinoet al.(CosmoVerse Network), Phys. Dark Univ.49, 101965 (2025), arXiv:2504.01669 [astro- ph.CO]

  19. [20]

    Yang, Eur

    Y. Yang, Eur. Phys. J. C85, 1350 (2025), arXiv:2508.17848 [astro-ph.CO]

  20. [21]

    Y. Yang, X. Dai, and Y. Wang, Phys. Rev. D111, 103534 (2025), arXiv:2505.09879 [astro-ph.CO]

  21. [22]

    Wu, T.-N

    P.-J. Wu, T.-N. Li, G.-H. Du, and X. Zhang, (2025), arXiv:2509.02945 [astro-ph.CO]

  22. [23]

    Li and S

    J.-X. Li and S. Wang, (2025), arXiv:2506.22953 [astro- ph.CO]

  23. [24]

    Li, P.-J

    T.-N. Li, P.-J. Wu, G.-H. Du, Y.-H. Yao, J.-F. Zhang, and X. Zhang, Phys. Dark Univ.50, 102068 (2025), arXiv:2507.07798 [astro-ph.CO]

  24. [25]

    Du, T.-N

    G.-H. Du, T.-N. Li, P.-J. Wu, J.-F. Zhang, and X. Zhang, (2025), arXiv:2507.16589 [astro-ph.CO]

  25. [26]

    L. Feng, T. Han, J.-F. Zhang, and X. Zhang, (2025), arXiv:2507.17315 [astro-ph.CO]

  26. [27]

    S. L. Guedezounme, B. R. Dinda, and R. Maartens, (2025), arXiv:2507.18274 [astro-ph.CO]

  27. [28]

    W. Yang, S. Zhang, O. Mena, S. Pan, and E. Di Valentino, (2025), arXiv:2508.19109 [astro-ph.CO]

  28. [29]

    Cai, Z.-K

    R.-G. Cai, Z.-K. Guo, S.-J. Wang, W.-W. Yu, and Y. Zhou, Phys. Rev. D105, L021301 (2022), arXiv:2107.13286 [astro-ph.CO]

  29. [30]

    L. S. Brito, J. F. Jesus, A. A. Escobal, and S. H. Pereira, (2024), arXiv:2412.06756 [astro-ph.CO]

  30. [31]

    Di Valentino, R

    E. Di Valentino, R. Z. Ferreira, L. Visinelli, and U. Danielsson, Phys. Dark Univ.26, 100385 (2019), arXiv:1906.11255 [astro-ph.CO]

  31. [32]

    K. C. Wonget al.(H0LiCOW), Mon. Not. Roy. Astron. Soc.498, 1420 (2020), arXiv:1907.04869 [astro-ph.CO]

  32. [33]

    Millonet al., Astron

    M. Millonet al., Astron. Astrophys.639, A101 (2020), arXiv:1912.08027 [astro-ph.CO]

  33. [34]

    M. G. Dainotti, B. De Simone, T. Schiavone, G. Montani, E. Rinaldi, and G. Lambiase, Astrophys. J.912, 150 (2021), arXiv:2103.02117 [astro-ph.CO]

  34. [35]

    Malekjani, R

    M. Malekjani, R. M. Conville, E. O. Colg´ ain, S. Pouro- jaghi, and M. M. Sheikh-Jabbari, Eur. Phys. J. C84, 317 (2024), arXiv:2301.12725 [astro-ph.CO]

  35. [36]

    Montani, N

    G. Montani, N. Carlevaro, and M. G. Dainotti, Phys. Dark Univ.48, 101847 (2025), arXiv:2411.07060 [gr-qc]

  36. [37]

    Hu and F

    J.-P. Hu and F. Y. Wang, Mon. Not. Roy. Astron. Soc. 517, 576 (2022), arXiv:2203.13037 [astro-ph.CO]

  37. [38]

    Bargiacchi, M

    G. Bargiacchi, M. G. Dainotti, and S. Capozziello, New Astron. Rev.100, 101712 (2025), arXiv:2408.10707 [astro-ph.CO]

  38. [39]

    M. G. Dainotti, B. De Simone, T. Schiavone, G. Montani, E. Rinaldi, G. Lambiase, M. Bogdan, and S. Ugale, Galaxies10, 24 (2022), arXiv:2201.09848 [astro-ph.CO]

  39. [40]

    Dainotti, B

    M. Dainotti, B. De Simone, G. Montani;, T. Schi- avone;, and G. Lambiase., PoSCORFU2022, 235 (2023), arXiv:2301.10572 [astro-ph.CO]

  40. [41]

    X. D. Jia, J. P. Hu, and F. Y. Wang, Astron. Astrophys. 674, A45 (2023), arXiv:2212.00238 [astro-ph.CO]

  41. [42]

    E. O. Colg´ ain, M. M. Sheikh-Jabbari, R. Solomon, G. Bargiacchi, S. Capozziello, M. G. Dainotti, and D. Stojkovic, Phys. Rev. D106, L041301 (2022), arXiv:2203.10558 [astro-ph.CO]

  42. [43]

    E. O. Colg´ ain, M. M. Sheikh-Jabbari, R. Solomon, M. G. Dainotti, and D. Stojkovic, Phys. Dark Univ.44, 101464 (2024), arXiv:2206.11447 [astro-ph.CO]

  43. [44]

    X. D. Jia, J. P. Hu, S. X. Yi, and F. Y. Wang, Astro- phys. J. Lett.979, L34 (2025), arXiv:2406.02019 [astro- ph.CO]

  44. [45]

    Krishnan, E

    C. Krishnan, E. O. Colg´ ain, Ruchika, A. A. Sen, M. M. Sheikh-Jabbari, and T. Yang, Phys. Rev. D102, 103525 (2020), arXiv:2002.06044 [astro-ph.CO]

  45. [46]

    M. G. Dainottiet al., JHEAp48, 100405 (2025), arXiv:2501.11772 [astro-ph.CO]

  46. [47]

    A. G. Adameet al.(DESI), JCAP02, 021 (2025), arXiv:2404.03002 [astro-ph.CO]

  47. [48]

    DESI DR2 Results II: Measurements of Baryon Acoustic Oscillations and Cosmological Constraints

    M. Abdul Karimet al.(DESI), Phys. Rev. D112, 083515 (2025), arXiv:2503.14738 [astro-ph.CO]

  48. [49]

    Krishnan, E

    C. Krishnan, E. ´O. Colg´ ain, M. M. Sheikh-Jabbari, and T. Yang, Phys. Rev. D103, 103509 (2021), arXiv:2011.02858 [astro-ph.CO]

  49. [50]

    T. P. Sotiriou and V. Faraoni, Rev. Mod. Phys.82, 451 (2010), arXiv:0805.1726 [gr-qc]

  50. [51]

    S. M. Koksbang, Mon. Not. Roy. Astron. Soc.498, L135 (2020), [Erratum: Mon.Not.Roy.Astron.Soc. 500, (2021)], 9 arXiv:2008.07108 [astro-ph.CO]

  51. [52]

    T. P. Sotiriou, Class. Quant. Grav.23, 5117 (2006), arXiv:gr-qc/0604028

  52. [53]

    N´ ajera and A

    A. N´ ajera and A. Fajardo, Phys. Dark Univ.34, 100889 (2021), arXiv:2104.14065 [gr-qc]

  53. [54]

    Paliathanasis, (2025), arXiv:2506.16223 [gr-qc]

    A. Paliathanasis, (2025), arXiv:2506.16223 [gr-qc]

  54. [55]

    Schiavone, G

    T. Schiavone, G. Montani, and F. Bombacigno, Mon. Not. Roy. Astron. Soc.522, L72 (2023), arXiv:2211.16737 [gr-qc]

  55. [56]

    Cai and A

    R.-G. Cai and A. Wang, JCAP03, 002 (2005), arXiv:hep- th/0411025

  56. [57]

    Deffayet, Phys

    C. Deffayet, Phys. Lett. B502, 199 (2001), arXiv:hep- th/0010186

  57. [58]

    Amendola, G

    L. Amendola, G. Camargo Campos, and R. Rosen- feld, Phys. Rev. D75, 083506 (2007), arXiv:astro- ph/0610806

  58. [59]

    Interacting models may be key to solve the cosmic coincidence problem

    S. del Campo, R. Herrera, and D. Pavon, JCAP01, 020 (2009), arXiv:0812.2210 [gr-qc]

  59. [60]

    Y. L. Bolotin, A. Kostenko, O. A. Lemets, and D. A. Yerokhin, Int. J. Mod. Phys. D24, 1530007 (2014), arXiv:1310.0085 [astro-ph.CO]

  60. [61]

    B. Wang, E. Abdalla, F. Atrio-Barandela, and D. Pavon, Rept. Prog. Phys.79, 096901 (2016), arXiv:1603.08299 [astro-ph.CO]

  61. [62]

    R.-G. Cai, N. Tamanini, and T. Yang, JCAP05, 031 (2017), arXiv:1703.07323 [astro-ph.CO]

  62. [63]

    Aljaf, D

    M. Aljaf, D. Gregoris, and M. Khurshudyan, Eur. Phys. J. C81, 544 (2021), arXiv:2005.01891 [astro-ph.CO]

  63. [64]

    K. R. Mishra, S. K. J. Pacif, R. Kumar, and K. Bamba, Phys. Dark Univ.40, 101211 (2023), arXiv:2301.08743 [gr-qc]

  64. [65]

    N. N. Pooya, Phys. Rev. D110, 043510 (2024), arXiv:2407.03766 [astro-ph.CO]

  65. [66]

    Li, P.-J

    T.-N. Li, P.-J. Wu, G.-H. Du, S.-J. Jin, H.-L. Li, J.-F. Zhang, and X. Zhang, Astrophys. J.976, 1 (2024), arXiv:2407.14934 [astro-ph.CO]

  66. [67]

    Halder, S

    S. Halder, S. D. Odintsov, S. Pan, T. Saha, and E. N. Saridakis, Phys. Rev. D112, 023519 (2025), arXiv:2411.18300 [gr-qc]

  67. [68]

    W. Yang, S. Pan, E. Di Valentino, O. Mena, D. F. Mota, and S. Chakraborty, Phys. Rev. D111, 103509 (2025), arXiv:2504.11973 [astro-ph.CO]

  68. [69]

    Paliathanasis, (2026), arXiv:2601.02789 [astro- ph.CO]

    A. Paliathanasis, (2026), arXiv:2601.02789 [astro- ph.CO]

  69. [70]

    van der Westhuizen, D

    M. van der Westhuizen, D. Figueruelo, R. Thubisi, S. Sahlu, A. Abebe, and A. Paliathanasis, Phys. Dark Univ.50, 102107 (2025), arXiv:2505.23306 [astro- ph.CO]

  70. [71]

    Supernovae type Ia data favour coupled phantom energy

    E. Majerotto, D. Sapone, and L. Amendola, (2004), arXiv:astro-ph/0410543

  71. [72]

    Gonzalez-Espinoza and R

    M. Gonzalez-Espinoza and R. Herrera, Phys. Dark Univ. 49, 101976 (2025), arXiv:2504.05435 [gr-qc]

  72. [73]

    E. J. Copeland, M. Sami, and S. Tsujikawa, Int. J. Mod. Phys. D15, 1753 (2006), arXiv:hep-th/0603057

  73. [74]

    Dynamical systems in cosmology

    C. G. Boehmer and N. Chan, “Dynamical systems in cosmology.” (2017) arXiv:1409.5585 [gr-qc]

  74. [75]

    Hahn, M.J

    C. Hahnet al., Astron. J.165, 253 (2023), arXiv:2208.08512 [astro-ph.CO]

  75. [76]

    Raichoor, J

    A. Raichooret al., Astron. J.165, 126 (2023), arXiv:2208.08513 [astro-ph.CO]

  76. [77]

    Chaussidon, C

    E. Chaussidonet al., Astrophys. J.944, 107 (2023), arXiv:2208.08511 [astro-ph.CO]

  77. [78]

    From cosmic deceleration to acceleration: new constraints from SN Ia and BAO/CMB

    R. Giostri, M. Vargas dos Santos, I. Waga, R. R. R. Reis, M. O. Calv˜ ao, and B. L. Lago, Journal of Cosmology and Astroparticle Physics2012, 027 (2012), arXiv:1203.3213 [astro-ph.CO]

  78. [79]

    The WiggleZ Dark Energy Survey: mapping the distance-redshift relation with baryon acoustic oscillations

    C. Blake, E. A. Kazin, F. Beutler, T. M. Davis, D. Parkin- son, S. Brough, M. Colless, C. Contreras, W. Couch, S. Croom, D. Croton, M. J. Drinkwater, K. Forster, D. Gilbank, M. Gladders, K. Glazebrook, B. Jelliffe, R. J. Jurek, I. H. Li, B. Madore, D. C. Martin, K. Pimb- blet, G. B. Poole, M. Pracy, R. Sharp, E. Wisnioski, D. Woods, T. K. Wyder, and H. K....

  79. [80]

    W. J. Percival, B. A. Reid, D. J. Eisenstein, N. A. Bah- call, T. Budavari, J. A. Frieman, M. Fukugita, J. E. Gunn, ˇZ. Ivezi´ c, G. R. Knapp, R. G. Kron, J. Loveday, R. H. Lupton, T. A. McKay, A. Meiksin, R. C. Nichol, A. C. Pope, D. J. Schlegel, D. P. Schneider, D. N. Spergel, C. Stoughton, M. A. Strauss, A. S. Szalay, M. Tegmark, M. S. Vogeley, D. H. W...

  80. [81]

    The 6dF Galaxy Survey: Baryon Acoustic Oscillations and the Local Hubble Constant

    F. Beutler, C. Blake, M. Colless, D. H. Jones, L. Staveley- Smith, L. Campbell, Q. Parker, W. Saunders, and F. Watson, Monthly Notices of the Royal Astronomical Society416, 3017 (2011), arXiv:1106.3366 [astro-ph.CO]

Showing first 80 references.