pith. machine review for the scientific record. sign in

arxiv: 2604.22450 · v1 · submitted 2026-04-24 · 🌀 gr-qc

Recognition: unknown

Exploring Cosmic Evolution in R\'enyi Entropic Cosmology with Constraints from DESI DR2 BAO and GW Data

Authors on Pith no claims yet

Pith reviewed 2026-05-08 10:28 UTC · model grok-4.3

classification 🌀 gr-qc
keywords Rényi entropyentropic cosmologylate-time accelerationDESI BAOgravitational wavesFriedmann equationsquintessencecosmological constraints
0
0 comments X

The pith

Rényi entropic corrections to the Friedmann equations receive a direct constraint on their parameter from late-time acceleration data.

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

The paper tests a cosmological model in which Rényi entropy modifies the standard equations that describe the universe's expansion rate. Using recent baryon acoustic oscillation measurements from DESI DR2 along with other BAO, cosmic chronometer, and gravitational-wave observations, the authors derive bounds on the single free parameter in the model. This parameter value produces accelerated expansion at late times that behaves like quintessence, stays above the phantom divide, and approaches the standard cosmological constant model as the parameter limit is taken. The derived Hubble constant and matter density today fall within current observational ranges. A reader would care because the approach offers an alternative explanation for cosmic acceleration rooted in entropy corrections rather than an added dark-energy component.

Core claim

The Rényi entropic correction supplies a viable description of late-time cosmic acceleration, with the parameter λ tightly bounded by DESI DR2 BAO, P-BAO, CC, and GW data to values that also satisfy Big Bang Nucleosynthesis and baryogenesis limits; the resulting expansion history remains stable, obeys energy conditions, and transitions smoothly to the ΛCDM limit without phantom behavior.

What carries the argument

The Rényi entropic correction added to the Friedmann equations, which introduces the parameter λ that alters the effective energy density and pressure to drive acceleration at late times.

If this is right

  • The model reproduces the observed late-time acceleration with a quintessence-like equation of state.
  • Predicted values of the present Hubble constant and matter density fraction remain consistent with current measurements.
  • The model satisfies standard energy conditions and remains stable against perturbations.
  • Statistical comparisons favor the entropic model as a viable alternative to the standard cosmological constant picture.
  • The derived λ satisfies independent bounds from Big Bang Nucleosynthesis and baryogenesis.

Where Pith is reading between the lines

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

  • If the constraint holds, entropy-based modifications could link late-time acceleration to quantum-information effects without introducing new fields.
  • Future surveys with tighter BAO or gravitational-wave standard-siren measurements could shrink the allowed range for λ further.
  • The approach might be extended to early-universe epochs to test whether the same correction influences inflation or recombination.

Load-bearing premise

The Rényi entropic correction fully accounts for the observed late-time dynamics without hidden degeneracies or unmodeled systematics in the combined datasets.

What would settle it

A future high-precision measurement of the dark-energy equation-of-state parameter that falls below -1 at any redshift, or a Hubble-constant value lying well outside the model's predicted range from the same data combination.

Figures

Figures reproduced from arXiv: 2604.22450 by Kalyan Bhuyan, Kalyan Malakar, Rajdeep Mazumdar.

Figure 1
Figure 1. Figure 1: FIG. 1. The evolution of view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. 2-d contour subplots for the parameters view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. The evolution of the deceleration parameter Vs redshift is illustrated, along with corresponding transition redshift view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Evolution of the effective equation-of-state parameter with redshift for the best-fit parameter values of the given model. view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Evolution of the view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Evolution of the statefinder diagnostic pairs view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. Redshift evolution of the energy conditions for the best-fit model parameter values. view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. The evolution of the perturbations view at source ↗
read the original abstract

We explore a cosmological model based on R\'enyi entropic corrections to the Friedmann equations and constrain it using DESI, P-BAO, CC, and gravitational-wave observations. Unlike earlier works, we obtain a direct and stringent constraint on the R\'enyi parameter $\lambda$ from late-time cosmic acceleration, with the resulting value even satisfying recent Big Bang Nucleosynthesis and baryogenesis bounds. The model predicts values of $H_0$ and $\Omega_{m0}$ that are consistent with current observational data. It provides a successful description of late-time acceleration with a quintessence-like behavior, smoothly approaching the $\Lambda$CDM limit without crossing the phantom divide. Furthermore, the statical comparisons along with the evaluation of energy conditions and stability analyses reinforce its viability as a robust alternative to the standard cosmological model.

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

2 major / 2 minor

Summary. The manuscript develops a cosmological model in which Rényi entropic corrections are added to the Friedmann equations, introducing a single free parameter λ. Using DESI DR2 BAO, P-BAO, cosmic chronometer, and gravitational-wave datasets, the authors perform a joint MCMC fit for λ, H0, and Ωm0, report a best-fit value of λ that satisfies BBN and baryogenesis bounds, and show that the resulting expansion history is quintessence-like, approaches the ΛCDM limit at late times, satisfies energy conditions, and passes statistical model-comparison tests.

Significance. If the reported bound on λ proves robust against parameter degeneracies, the work supplies one of the first direct late-time observational constraints on an entropic-gravity correction, together with explicit checks of energy conditions and stability that are not always performed in similar models. The approach of letting the data drive λ while recovering standard H0 and Ωm0 values is a concrete, falsifiable test of the framework.

major comments (2)
  1. [§4] §4 (MCMC results and posterior plots): the abstract asserts a 'direct and stringent constraint' on λ from late-time data, yet the fit simultaneously varies λ, H0, and Ωm0 on the same DESI DR2 + P-BAO + CC + GW datasets. No correlation matrix, degeneracy diagnostic (e.g., Δχ² when λ is fixed to zero), or conditional posterior is presented; without these the claim that the λ bound is independent rather than a projection along the H0–Ωm0 degeneracy direction cannot be verified.
  2. [§2.2] §2.2 (modified Friedmann equations): the entropic correction is introduced as an additive term to the effective dark-energy density. The paper does not quantify how this term correlates with the standard background parameters in the likelihood; a brief analytic or numerical degeneracy analysis (e.g., the derivative of the Hubble function with respect to λ at fixed H0, Ωm0) would be required to substantiate that the datasets can actually isolate λ.
minor comments (2)
  1. [Abstract] Abstract: 'statical comparisons' should read 'statistical comparisons'.
  2. [Figures/Tables] Figure captions and tables: axis labels and column headings should explicitly state the units and the 1σ/2σ confidence levels used for the reported intervals on λ, H0, and Ωm0.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive and detailed comments, which help clarify the presentation of our MCMC results and the independence of the λ constraint. We address each major point below and will revise the manuscript to incorporate the suggested analyses.

read point-by-point responses
  1. Referee: [§4] §4 (MCMC results and posterior plots): the abstract asserts a 'direct and stringent constraint' on λ from late-time data, yet the fit simultaneously varies λ, H0, and Ωm0 on the same DESI DR2 + P-BAO + CC + GW datasets. No correlation matrix, degeneracy diagnostic (e.g., Δχ² when λ is fixed to zero), or conditional posterior is presented; without these the claim that the λ bound is independent rather than a projection along the H0–Ωm0 degeneracy direction cannot be verified.

    Authors: We acknowledge that the manuscript does not present a correlation matrix or explicit degeneracy diagnostics such as Δχ² for λ fixed to zero. The joint MCMC posterior does show λ constrained away from zero while returning H0 and Ωm0 values consistent with independent data, and the inclusion of gravitational-wave standard sirens provides an additional handle on the expansion history. To substantiate the claim of an independent constraint, the revised version will include the full correlation matrix from the chains and a Δχ² comparison between the free-λ and λ=0 cases. If these diagnostics reveal significant degeneracy, we will also revise the abstract wording accordingly. revision: yes

  2. Referee: [§2.2] §2.2 (modified Friedmann equations): the entropic correction is introduced as an additive term to the effective dark-energy density. The paper does not quantify how this term correlates with the standard background parameters in the likelihood; a brief analytic or numerical degeneracy analysis (e.g., the derivative of the Hubble function with respect to λ at fixed H0, Ωm0) would be required to substantiate that the datasets can actually isolate λ.

    Authors: We agree that an explicit quantification of the correlation is needed. In the revised manuscript we will add both an analytic expression for ∂H(z)/∂λ evaluated at fixed H0 and Ωm0 (derived directly from the modified Friedmann equation) and a numerical evaluation of the likelihood response when λ is varied while holding the background parameters fixed. These additions will demonstrate the independent sensitivity of the late-time datasets to the Rényi term. revision: yes

Circularity Check

1 steps flagged

Fitted H0 and Ωm0 values presented as model predictions after joint fit with λ

specific steps
  1. fitted input called prediction [Abstract]
    "The model predicts values of H0 and Ωm0 that are consistent with current observational data."

    H0 and Ωm0 are fitted jointly with λ to the DESI DR2 BAO, P-BAO, CC, and GW data to obtain the constraint on λ; stating that the model 'predicts' these values therefore restates the best-fit results from the identical fit rather than providing an independent forecast.

full rationale

The paper constrains the Rényi parameter λ from late-time datasets and states that the model then predicts H0 and Ωm0 values consistent with observations. Because these parameters are varied jointly in the fit, the reported 'predictions' are direct outputs of the same parameter estimation rather than independent forecasts. The BBN/baryogenesis consistency check occurs after the fit and does not create circularity. The central constraint on λ retains independent content provided the entropic correction introduces dynamics not fully degenerate with standard parameters, but the presentation of fitted results as predictions constitutes partial circularity per the defined patterns.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The central claim rests on one fitted parameter λ introduced by the Rényi correction and on standard cosmological background assumptions; no new entities are postulated.

free parameters (1)
  • λ (Rényi parameter)
    Single adjustable parameter in the entropic correction to the Friedmann equations, constrained by fitting to late-time acceleration data.
axioms (2)
  • domain assumption Rényi entropy supplies a correction term that modifies the Friedmann equations
    Invoked as the foundational modification for the cosmological model.
  • standard math FLRW metric and standard energy-momentum conservation hold
    Background geometry and conservation laws assumed throughout.

pith-pipeline@v0.9.0 · 5454 in / 1514 out tokens · 59676 ms · 2026-05-08T10:28:54.658467+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

94 extracted references · 91 canonical work pages · 3 internal anchors

  1. [1]

    G., Filippenko, A

    Riess, A. G., et al. (1998). Observational Evidence from Supernovae for an Accelerating Universe and a Cosmological Constant. Astronomical Journal, 116(3), 1009–1038. https://doi.org/10.1086/300499

  2. [2]

    Perlmutter, S., et al. (1999). Measurements ofΩ and Λ from 42 High-Redshift Supernovae.Astrophysical Journal, 517(2), 565–586. https://doi.org/10.1086/307221 19

  3. [3]

    L., Halpern, M., Hinshaw, G., et al

    Bennett, C. L., et al. (2003). First-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Preliminary Maps and Basic Results.Astrophysical Journal Supplement Series , 148, 1–27. https://doi.org/10.1086/377253

  4. [4]

    N., Verde, L., Peiris, H

    Spergel, D. N., et al. (2003). First-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Determination of Cosmological Parameters.Astrophysical Journal Supplement Series , 148, 175–194. https://doi.org/10.1086/377226

  5. [5]

    , keywords =

    Eisenstein, D. J., et al. (2005). Detection of the Baryon Acoustic Peak in the Large-Scale Correlation Function of SDSS Luminous Red Galaxies.Astrophysical Journal, 633(2), 560–574. https://doi.org/10.1086/466512

  6. [6]

    L., & Haiman, Z

    Percival, W. J., et al. (2010). Baryon Acoustic Oscillations in the Sloan Digital Sky Survey Data Release 7 Galaxy Sample. Monthly Notices of the Royal Astronomical Society , 401(4), 2148–2168. https://doi.org/10.1111/j.1365-2966.2009.15812.x

  7. [7]

    Weinberg, S. (1989). The Cosmological Constant Problem. Reviews of Modern Physics , 61(1), 1–23. https://doi.org/10.1103/RevModPhys.61.1

  8. [8]

    Everything You Always Wanted To Know About The Cosmological Constant Problem (But Were Afraid To Ask)

    J. Martin, “Everything You Always Wanted To Know About The Cosmological Constant Problem (But Were Afraid To Ask),”Comptes Rendus Physique 13, 566 (2012), arXiv:1205.3365 [astro-ph.CO]

  9. [9]

    M., Press, W

    Carroll, S. M., Press, W. H., & Turner, E. L. (1992). The Cosmological Constant.Annual Review of Astronomy and Astrophysics, 30, 499–542. https://doi.org/10.1146/annurev.aa.30.090192.002435

  10. [10]

    Sahni, V., & Starobinsky, A. A. (2000). The Case for a Positive CosmologicalΛ-Term. International Journal of Modern Physics D, 9(4), 373–443. https://doi.org/10.1142/S0218271800000542

  11. [11]

    Armendariz-Picon, C., Mukhanov, V., & Steinhardt, P. J. (2000). Dynamical solution to the problem of a small cosmological constant and late-time cosmic acceleration. Phys. Rev. Lett. , 85(21), 4438–4441. https://doi.org/10.1103/PhysRevLett.85.4438

  12. [12]

    Sen, A. (2002). Rolling tachyon. Journal of High Energy Physics , 2002(04), 048. https://doi.org/10.1088/1126- 6708/2002/04/048

  13. [13]

    Khoury, J., & Weltman, A. (2004). Chameleon fields: Awaiting surprises for tests of gravity in space.Phys. Rev. Lett. , 93(17), 171104. https://doi.org/10.1103/PhysRevLett.93.171104

  14. [14]

    Kamenshchik, A., Moschella, U., & Pasquier, V. (2001). An alternative to quintessence.Physics Letters B , 511(2-4), 265–268. https://doi.org/10.1016/S0370-2693(01)00571-8

  15. [15]

    C., Bertolami, O., & Sen, A

    Bento, M. C., Bertolami, O., & Sen, A. A. (2002). Generalized Chaplygin gas, accelerated expansion, and dark energy- matter unification. Phys. Rev. D , 66(4), 043507. https://doi.org/10.1103/PhysRevD.66.043507

  16. [16]

    J. M. Bardeen, B. Carter and S. W. Hawking, The four laws of black hole mechanics,Commun. Math. Phys. 31, 161 (1973). https://doi.org/10.1007/BF01645742

  17. [17]

    J. D. Bekenstein, Black holes and entropy,Phys. Rev. D 7, 2333 (1973). https://doi.org/10.1103/PhysRevD.7.2333

  18. [18]

    S. W. Hawking, Particle creation by black holes, Commun. Math. Phys. 43, 199 (1975). https://doi.org/10.1007/BF02345020

  19. [19]

    Dimensional Reduction in Quantum Gravity

    G. ’t Hooft, Dimensional reduction in quantum gravity, in Salamfestschrift, World Scientific (1993). https://arxiv.org/abs/gr-qc/9310026

  20. [20]

    Susskind, J

    L. Susskind, The world as a hologram,J. Math. Phys. 36, 6377 (1995). https://doi.org/10.1063/1.531249

  21. [21]

    J. M. Maldacena, The largeN limit of superconformal field theories and supergravity,Adv. Theor. Math. Phys. 2, 231 (1998). https://doi.org/10.1023/A:1026654312961

  22. [22]

    Black holes: complementarity vs. firewalls,

    A. Almheiri, D. Marolf, J. Polchinski and J. Sully, Black holes: Complementarity or firewalls?,JHEP 02, 062 (2013). https://doi.org/10.1007/JHEP02(2013)062

  23. [23]

    Jacobson, Phys

    T. Jacobson, Thermodynamics of spacetime: The Einstein equation of state, Phys. Rev. Lett. 75, 1260 (1995). https://doi.org/10.1103/PhysRevLett.75.1260

  24. [24]

    R. G. Cai and S. P. Kim, First law of thermodynamics and Friedmann equations of FRW universe,JHEP 02, 050 (2005). https://doi.org/10.1088/1126-6708/2005/02/050

  25. [25]

    Akbar, R.-G

    M. Akbar and R. G. Cai, Thermodynamic behavior of Friedmann equations at apparent horizon,Phys. Rev. D 75, 084003 (2007). https://doi.org/10.1103/PhysRevD.75.084003

  26. [26]

    Sheykhi, Modified Friedmann equations from generalized entropy,Phys

    A. Sheykhi, Modified Friedmann equations from generalized entropy, Phys. Lett. B 785, 118 (2018). https://doi.org/10.1016/j.physletb.2018.08.018

  27. [27]

    Nojiri, S

    S. Nojiri, S. D. Odintsov and V. K. Oikonomou, Modified gravity theories on a nutshell,Phys. Rept. 692, 1 (2017). https://doi.org/10.1016/j.physrep.2017.06.001

  28. [28]

    Possible generalization of Boltzmann-Gibbs statistics,

    C. Tsallis, Possible generalization of Boltzmann–Gibbs statistics, J. Stat. Phys. 52, 479 (1988). https://doi.org/10.1007/BF01016429

  29. [29]

    Rényi, On measures of entropy and information, inProceedings of the Fourth Berkeley Symposium on Mathematical Statistics and Probability (1961)

    A. Rényi, On measures of entropy and information, inProceedings of the Fourth Berkeley Symposium on Mathematical Statistics and Probability (1961)

  30. [30]

    J. D. Barrow, The area of a rough black hole, Phys. Lett. B 808, 135643 (2020). https://doi.org/10.1016/j.physletb.2020.135643

  31. [31]

    Kaniadakis, Statistical mechanics in the context of special relativity, Physical Review E 66 (5) (Nov

    G. Kaniadakis, Statistical mechanics in the context of special relativity, Phys. Rev. E 66, 056125 (2002). https://doi.org/10.1103/PhysRevE.66.056125 20

  32. [32]

    B. D. Sharma and D. P. Mittal, New non-additive measures of entropy,J. Math. Sci. 10, 28 (1975)

  33. [33]

    Rovelli, Black hole entropy from loop quantum gravity,Phys

    C. Rovelli, Black hole entropy from loop quantum gravity, Phys. Rev. Lett. 77, 3288 (1996). https://doi.org/10.1103/PhysRevLett.77.3288

  34. [34]

    Shankaranarayanan, & Sur, S

    Das, S., S. Shankaranarayanan, & Sur, S. (2008). Power-law corrections to entanglement entropy of horizons. Physical Re- view. D. Particles, Fields, Gravitation, and Cosmology/Physical Review. D, Particles, Fields, Gravitation, and Cosmology, 77(6). doi:10.1103/physrevd.77.064013. ‌

  35. [35]

    Radicella, N., & Pavón, D. (2010). The generalized second law in universes with quantum corrected entropy relations. Physics Letters B, 691(3), 121–126. doi:10.1016/j.physletb.2010.06.019 ‌

  36. [36]

    B., & Solodukhin, S

    Mann, R. B., & Solodukhin, S. N. (1997). Quantum scalar field on a three-dimensional (BTZ) black hole instanton: Heat kernel, effective action, and thermodynamics. Physical Review. D. Particles, Fields, Gravitation, and Cosmology/Physical Review. D. Particles and Fields, 55(6), 3622–3632. doi:10.1103/physrevd.55.3622 ‌

  37. [37]

    Banerjee, R., & Majhi, B. R. (2008). Quantum tunneling and back reaction. Physics Letters B, 662(1), 62–65. doi:10.1016/j.physletb.2008.02.044 ‌

  38. [38]

    Shannon, C. E. (1948). A Mathematical Theory of Communication. Bell System Technical Journal, 27(3), 379–423. doi:10.1002/j.1538-7305.1948.tb01338.x

  39. [39]

    Sheykhi, A., & Sooraki, A. S. (2025). Constraints on Renyi Entropy through Primordial Big-Bang Nucleosynthesis and Baryogenesis. 2507.14250

  40. [40]

    Fazlollahi, H. R. (2023). Rényi entropy correction to expanding universe. The European Physical Journal C, 83(1). doi:10.1140/epjc/s10052-023-11183-w

  41. [41]

    Ghaffari, A

    Ghaffari, S., Ziaie, A. H., Bezerra, V. B., & Moradpour, H. (2019). Inflation in the Rényi cosmology. Modern Physics Letters A, 35(01), 1950341. doi:10.1142/s0217732319503413 ‌

  42. [42]

    Golanbari, T., Saaidi, K., & Karimi, P. (2020). Renyi entropy and the holographic dark energy in flat space time. 2002.04097

  43. [43]

    Pandey, B. (2021). Renyi entropy as a measure of cosmic homogeneity. Journal of Cosmology and Astroparticle Physics, 2021(02), 023–023. doi:10.1088/1475-7516/2021/02/023 ‌

  44. [44]

    Abdul Karimet al.[DESI], Phys

    Abdul Karim, M., Aguilar, J., Ahlen, S., Alam, S., Allen, L., Prieto, C. A., Brieden, S. (2025). DESI DR2 results. II. Measurements of baryon acoustic oscillations and cosmological constraints. Physical Review D, 112(8). https://doi.org/10.1103/tr6y-kpc6

  45. [45]

    A. N. Ormondroyd, W. J. Handley, M. P. Hobson, and A. N. Lasenby.Comparison of Dynamical Dark Energy with ΛCDM in Light of DESI DR2 . arXiv:2503.17342

  46. [46]

    Chaussidon, M

    E. Chaussidon et al.. (2025). Early Time Solution as an Alternative to the Late Time Evolving Dark Energy with DESI DR2 BAO. [arXiv:2503.24343]

  47. [47]

    J., García-García, C., Anton, T., et al

    Wolf, W. J., García-García, C., Anton, T., et al. (2025). Assessing Cosmological Evidence for Nonminimal Coupling.Phys. Rev. Lett., 135(8), 081001. https://doi.org/10.1103/jysf-k72m [arXiv:2504.07679]

  48. [48]

    Paliathanasis, Dark energy within the generalized un- certainty principle in light of DESI DR2, JCAP09, 067, arXiv:2503.20896 [astro-ph.CO]

    A. Paliathanasis. (2025). Dark Energy within the Generalized Uncertainty Principle in Light of DESI DR2 . [arXiv:2503.20896]

  49. [49]

    Rich Abbott et. al. (2021). Open data from the first and second observing runs of Advanced LIGO and Advanced Virgo. SoftwareX, 13, 100658. doi:10.1016/j.softx.2021.100658

  50. [50]

    Rich Abbott et. al. GWTC-3: Compact Binary Coalescences Observed by LIGO and Virgo during the Second Part of the Third Observing Run. Physical Review X, 13(4). doi:10.1103/physrevx.13.041039. ‌

  51. [51]

    Gaztanaga, E., Cabre, A., & Hui, L. (2009). Clustering of Luminous Red Galaxies IV: Baryon Acoustic Peak in the Line- of-Sight Direction and a Direct Measurement of H(z).Monthly Notices of the Royal Astronomical Society , 399, 1663–1680. arXiv:0807.3551

  52. [52]

    Oka, A., Saito, S., Nishimichi, T., Taruya, A., & Yamamoto, K. (2014). Simultaneous constraints on the growth of structure and cosmic expansion from the multipole power spectra of the SDSS DR7 LRG sample.Monthly Notices of the Royal Astronomical Society, 439, 2515–2530. arXiv:1310.2820

  53. [53]

    Wang, Y., et al. (2017). The clustering of galaxies in the completed SDSS-III Baryon Oscillation Spectroscopic Survey: tomographic BAO analysis of DR12 combined sample in configuration space.Monthly Notices of the Royal Astronomical Society, 469(3), 3762–3774. arXiv:1607.03154

  54. [54]

    Chuang, C.-H., & Wang, Y. (2013). Modeling the Anisotropic Two-Point Galaxy Correlation Function on Small Scales and Improved Measurements of H(z), DA(z), andβ(z) from the Sloan Digital Sky Survey DR7 Luminous Red Galaxies. Monthly Notices of the Royal Astronomical Society , 435, 255–262. arXiv:1209.0210

  55. [55]

    Anderson, L., et al. (2014). The clustering of galaxies in the SDSS-III Baryon Oscillation Spectroscopic Survey: baryon acoustic oscillations in the Data Releases 10 and 11 Galaxy samples.Monthly Notices of the Royal Astronomical Society , 441(1), 24–62. arXiv:1312.4877

  56. [56]

    Zhao, G.-B., et al. (2019). The clustering of the SDSS-IV extended Baryon Oscillation Spectroscopic Survey DR14 quasar sample: a tomographic measurement of cosmic structure growth and expansion rate based on optimal redshift weights. 21 Monthly Notices of the Royal Astronomical Society , 482(3), 3497–3513. arXiv:1801.03043

  57. [57]

    Baryon acoustic oscillations in the Ly α forest of BOSS quasars

    Busca, N. G., et al. (2013). Baryon Acoustic Oscillations in the Ly-α forest of BOSS quasars.Astronomy & Astrophysics, 552, A96. arXiv:1211.2616

  58. [58]

    Font-Ribera, A., et al. (2014). Quasar-Lymanα Forest Cross-Correlation from BOSS DR11: Baryon Acoustic Oscillations. Journal of Cosmology and Astroparticle Physics , 2014(05), 027. arXiv:1311.1767

  59. [59]

    du Mas des Bourboux, H., et al. (2017). Baryon acoustic oscillations from the complete SDSS-III Lyα-quasar cross- correlation function at z = 2.4.Astronomy & Astrophysics, 608, A130. arXiv:1708.02225

  60. [60]

    Alam, S., et al. (2017). The clustering of galaxies in the completed SDSS-III Baryon Oscillation Spectroscopic Survey: cosmological analysis of the DR12 galaxy sample.Monthly Notices of the Royal Astronomical Society , 470(3), 2617–2652. arXiv:1607.03155

  61. [61]

    Chuang, C.-H., et al. (2013). The clustering of galaxies in the SDSS-III Baryon Oscillation Spectroscopic Survey: single- probe measurements and the strong power of normalized growth rate on constraining dark energy.Monthly Notices of the Royal Astronomical Society, 433, 3559. arXiv:1303.4486

  62. [62]

    Blake, C., et al. (2012). The WiggleZ Dark Energy Survey: Joint measurements of the expansion and growth history at z < 1. Monthly Notices of the Royal Astronomical Society , 425, 405–414. arXiv:1204.3674

  63. [63]

    Neveux, R., et al. (2020). The completed SDSS-IV extended Baryon Oscillation Spectroscopic Survey: BAO and RSD measurements from the anisotropic power spectrum of the quasar sample between redshift 0.8 and 2.2.Monthly Notices of the Royal Astronomical Society , 499(1), 210–229. arXiv:2007.08999

  64. [64]

    Jimenez, R., & Loeb, A. (2002). Constraining Cosmological Parameters Based on Relative Galaxy Ages. The Astrophysical Journal, 573(1), 37–42. https://doi.org/10.1086/340549

  65. [65]

    Brieden, S., Gil-Marín, H., & Verde, L. (2023). A tale of two (or more) h’s. Journal of Cosmology and Astroparticle Physics, 2023(04), 023. doi:10.1088/1475-7516/2023/04/023 ‌

  66. [66]

    Burnham and David R

    Burnham, K. P., & Anderson, D. R. (2004). Multimodel inference: Understanding AIC and BIC in model selection. Sociological Methods & Research, 33(2), 261–304. https://doi.org/10.1177/0049124104268644

  67. [67]

    Liddle, A. R. (2004). How many cosmological parameters?Monthly Notices of the Royal Astronomical Society , 351(3), L49–L53. astro-ph/0401198

  68. [68]

    Schwarz, G. (1978). Estimating the dimension of a model. The Annals of Statistics , 6(2), 461–464. https://doi.org/10.1214/aos/1176344136

  69. [69]

    Zhang, C., Zhang, H., Yuan, S., Liu, S., Zhang, T.-J., Sun, Y.: Four new observationalH(z) data from luminous red galaxies in the Sloan Digital Sky Survey data release seven.Res. Astron. Astrophys. 14, 1221 (2014).https://doi.org/ 10.1088/1674-4527/14/10/002

  70. [70]

    Simon, J., Verde, L., Jimenez, R.: Constraints on the redshift dependence of the dark energy potential.Phys. Rev. D 71, 123001 (2005). https://doi.org/10.1103/PhysRevD.71.123001

  71. [71]

    Moresco, M., Cimatti, A., Jimenez, R., Pozzetti, L., Zamorani, G., Bolzonella, M., Dunlop, J.C., Lamareille, F., Mignoli, M., Pearce, H., Rosati, P., Stern, D., Verde, L., Zucca, E., Carollo, C.M., Contini, T., Kneib, J.-P., Le Fèvre, O., Lilly, S.J., Mainieri, V.: Improved constraints on the expansion rate of the Universe up toz ∼ 1.1 from the spectrosco...

  72. [72]

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

    Alam, S., Ata, M., Bailey, S.J., Beutler, F., Bizyaev, D., Blazek, J., Bolton, A.S., Brownstein, J.R., Burden, A., Chuang, C.-H., Comparat, J., Cuesta, A.J., Dawson, K.S., Eisenstein, D.J., Escoffier, S., Gil-Marín, H., Grieb, J.N., Hand, N., Ho, S., Kinemuchi, K. et al.: The clustering of galaxies in the completed SDSS-III Baryon Oscillation Spectroscopi...

  73. [73]

    Moresco, M., Pozzetti, L., Cimatti, A., Jimenez, R., Maraston, C., Verde, L., Thomas, D., Citro, A., Tojeiro, R., Wilkinson, D.: A 6% measurement of the Hubble parameter atz ∼ 0.45: direct evidence of the epoch of cosmic re-acceleration.JCAP 2016, 014 (2016).https://doi.org/10.1088/1475-7516/2016/05/014

  74. [74]

    Monthly Notices of the Royal Astronomical Society , author =

    Alam, S., Ata, M., Bailey, S. J., Beutler, F., Dmitry Bizyaev, Blazek, J., ... Kinemuchi, K. (2017). The clustering of galaxies in the completed SDSS-III Baryon Oscillation Spectroscopic Survey: cosmological analysis of the DR12 galaxy sample. Monthly Notices of the Royal Astronomical Society, 470(3), 2617–2652. https://doi.org/10.1093/mnras/stx721

  75. [75]

    , keywords =

    Bautista, J. E., Romain Paviot, Mariana Vargas Magaña, Sylvain, S. Fromenteau, Héctor Gil-Marín, ... Chapman, M. (2020). The completed SDSS-IV extended Baryon Oscillation Spectroscopic Survey: measurement of the BAO and growth rate of structure of the luminous red galaxy sample from the anisotropic correlation function between redshifts 0.6 and 1. 500(1),...

  76. [76]

    J., Hou, J.,

    Neveux, R., Burtin, E., Arnaud de Mattia, Smith, A., Ross, A. J., Hou, J., ... Rossi, G. (2020). The completed SDSS-IV extended Baryon Oscillation Spectroscopic Survey: BAO and RSD measurements from the anisotropic power spectrum of the quasar sample between redshift 0.8 and 2.2. Monthly Notices of the Royal Astronomical Society, 499(1), 210–229. https://...

  77. [77]

    E., Busca, N

    Bautista, J. E., Busca, N. G., Guy, J., Rich, J., Blomqvist, M., du Mas des Bourboux, H., Noterdaeme, P. (2017). Measurementofbaryonacousticoscillationcorrelationsat z = 2.3withSDSSDR12Ly αforests. Astronomy & Astrophysics, 603, A12. https://doi.org/10.1051/0004-6361/201730533

  78. [78]

    G., Guy, J., Rich, J., Pieri, M

    du Mas des Bourboux, H., Le Goff, J.-M., Blomqvist, M., Busca, N. G., Guy, J., Rich, J., Pieri, M. M. (2017). Baryon acous- tic oscillations from the complete SDSS-III Lyα-quasar cross-correlation function at z = 2.4. Astronomy & Astrophysics, 608, A130. https://doi.org/10.1051/0004-6361/201731731

  79. [79]

    and Samushia, Lado and Howlett, Cullan and Percival, Will J

    Ross, A. E., Lado Samushia, Howlett, C., Percival, W. J., Burden, A., & Manera, M. (2015). The clustering of the SDSS DR7 main Galaxy sample – I. A 4 per cent distance measure at z = 0.15. Monthly Notices of the Royal Astronomical Society, 449(1), 835–847. doi:10.1093/mnras/stv154

  80. [80]

    Kazin, Jun Koda, Chris Blake, Nikhil Padmanabhan, Sarah Brough, et al

    Eyal A. Kazin, Jun Koda, Chris Blake, Nikhil Padmanabhan, Sarah Brough, et al. (2014). The WiggleZ Dark Energy Survey: improved distance measurements to z = 1 with reconstruction of the baryonic acoustic feature, Monthly Notices of the Royal Astronomical Society, 441(4), 3524–3542. doi:10.1093/mnras/stu778

Showing first 80 references.