Recognition: unknown
From Big Bang Nucleosynthesis to Late-Time Acceleration in f(Q,L_m) Gravity
Pith reviewed 2026-05-08 05:38 UTC · model grok-4.3
The pith
In f(Q, L_m) gravity a non-minimal coupling between non-metricity and matter reproduces the universe's expansion from Big Bang nucleosynthesis through late-time acceleration.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central finding is that the f(Q, L_m) model with non-minimal coupling yields parameter values consistent with observational datasets and the BBN freeze-out constraint. This leads to an effective equation-of-state parameter that evolves in a quintessence-like manner, passing statefinder and energy condition tests. Consequently, the framework describes the transition to accelerated expansion while closely following the predictions of the Lambda cold dark matter model with room for controlled deviations.
What carries the argument
The non-minimal coupling term in the f(Q, L_m) action, which links the non-metricity scalar Q to the matter Lagrangian L_m and alters the field equations to affect both early and late cosmic dynamics.
Load-bearing premise
The analysis assumes a particular functional form for the coupling between non-metricity and matter that permits the MCMC sampling to converge on viable parameters matching the data.
What would settle it
If new observations of the primordial element abundances or the Hubble parameter at redshift around 10^9 show values outside the model's constrained ranges, the consistency with BBN and late-time data would be broken.
Figures
read the original abstract
We perform a comprehensive investigation of the early-to-late time cosmic evolution within the framework of $f(Q,L_m)$ gravity, characterized by a non-minimal coupling between non-metricity and matter. The model is further tested against a combined set of observational data, including DESI DR2 BAO, previous BAO measurements, cosmic chronometers (CC), and gravitational-wave (GW) standard sirens, using a Markov Chain Monte Carlo (MCMC) approach. Further by incorporating the Big Bang Nucleosynthesis (BBN) freeze-out constraint, we place stringent limits on the model parameters, ensuring consistency with early-Universe physics. The resulting constraints exhibit strong agreement with observations, with the model successfully describing the transition from decelerated to accelerated expansion. The evolution of the effective equation-of-state parameter, together with statefinder diagnostics and energy conditions, reveals a quintessence-like nature and confirms the physical viability of the model. Overall, the $f(Q,L_m)$ framework emerges as a viable alternative to $\Lambda$CDM, closely reproducing its predictions while allowing controlled deviations in the expansion history.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper investigates f(Q, L_m) gravity with non-minimal coupling between non-metricity and matter Lagrangian. It derives the modified Friedmann equations, performs MCMC fitting to DESI DR2 BAO, prior BAO, cosmic chronometers, and GW standard sirens, incorporates BBN freeze-out constraints to bound parameters, and analyzes the resulting expansion history, effective equation-of-state evolution, statefinder diagnostics, and energy conditions, concluding that the model successfully describes the deceleration-to-acceleration transition and emerges as a viable alternative to ΛCDM with controlled deviations.
Significance. If the specific parametrization and background assumptions hold, the work provides an empirical demonstration that a non-minimal f(Q, L_m) coupling can simultaneously satisfy early-universe BBN limits and late-time acceleration data from multiple probes, offering a concrete modified-gravity alternative that closely tracks ΛCDM while permitting testable deviations in the expansion history.
major comments (3)
- [§2] §2 (model definition, around Eq. (7)–(9)): the specific functional form adopted for f(Q, L_m) is introduced without an independent theoretical derivation or stability analysis; the successful MCMC fit to the deceleration-to-acceleration transition and BBN consistency appear to rely on this choice, which is therefore load-bearing for the central viability claim.
- [§4] §4 (MCMC analysis and results): parameters are constrained using the same DESI DR2 BAO, CC, and GW datasets that are subsequently invoked to claim agreement with the observed transition and quintessence-like EoS; this circularity reduces the independence of the empirical support and requires explicit discussion of potential post-hoc selection effects.
- [§5] §5 (BBN incorporation): while the BBN freeze-out constraint is applied to tighten parameter bounds, the manuscript provides insufficient detail on the precise implementation, propagation of nuclear-rate systematics, or sensitivity of the late-time fit to variations in the early-universe assumptions.
minor comments (2)
- [Abstract] Abstract: does not state the explicit functional form of f(Q, L_m) or the number of free parameters, hindering immediate assessment of model complexity and generality.
- [Figure 4] Figure 4 (statefinder trajectories): the ΛCDM fixed point should be marked explicitly with error contours from the MCMC posterior for direct visual comparison.
Simulated Author's Rebuttal
We thank the referee for the detailed and insightful comments on our manuscript. We have addressed each of the major comments in the point-by-point response below. Revisions have been made to improve the theoretical motivation, clarify the analysis procedure, and expand the BBN section. We believe these changes enhance the clarity and robustness of our conclusions regarding the viability of the f(Q, L_m) gravity model as an alternative to ΛCDM.
read point-by-point responses
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Referee: [§2] §2 (model definition, around Eq. (7)–(9)): the specific functional form adopted for f(Q, L_m) is introduced without an independent theoretical derivation or stability analysis; the successful MCMC fit to the deceleration-to-acceleration transition and BBN consistency appear to rely on this choice, which is therefore load-bearing for the central viability claim.
Authors: The specific functional form for f(Q, L_m) is a phenomenological choice designed to introduce non-minimal coupling between non-metricity and the matter Lagrangian in a simple, analytically manageable way. It builds upon existing models in the modified gravity literature. We will revise the manuscript to include additional theoretical motivation for this choice and a discussion of the stability of the Friedmann equations derived from it. A full linear perturbation analysis is left for future work, as the current focus is on background cosmology and observational constraints. revision: partial
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Referee: [§4] §4 (MCMC analysis and results): parameters are constrained using the same DESI DR2 BAO, CC, and GW datasets that are subsequently invoked to claim agreement with the observed transition and quintessence-like EoS; this circularity reduces the independence of the empirical support and requires explicit discussion of potential post-hoc selection effects.
Authors: We disagree that this constitutes problematic circularity. The MCMC analysis constrains the model parameters using the observational datasets, after which we analyze the implications for the expansion history and effective EoS using those best-fit values. This is the standard approach for testing modified gravity models. The deceleration-to-acceleration transition emerges from the dynamics of the constrained model. In the revision, we will add a paragraph explicitly discussing the independence of the model selection from the data fitting and addressing potential selection effects. revision: partial
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Referee: [§5] §5 (BBN incorporation): while the BBN freeze-out constraint is applied to tighten parameter bounds, the manuscript provides insufficient detail on the precise implementation, propagation of nuclear-rate systematics, or sensitivity of the late-time fit to variations in the early-universe assumptions.
Authors: We thank the referee for pointing this out. The revised manuscript will include a more detailed description of the BBN freeze-out implementation, including the specific formulas employed, how nuclear rate uncertainties are considered (by adopting conservative bounds from the literature), and a sensitivity test demonstrating that the late-time constraints remain robust under reasonable variations in early-universe parameters. revision: yes
Circularity Check
MCMC fit to BAO/CC/GW/BBN data presented as successful description of transition and viability as ΛCDM alternative
specific steps
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fitted input called prediction
[Abstract]
"The model is further tested against a combined set of observational data, including DESI DR2 BAO, previous BAO measurements, cosmic chronometers (CC), and gravitational-wave (GW) standard sirens, using a Markov Chain Monte Carlo (MCMC) approach. Further by incorporating the Big Bang Nucleosynthesis (BBN) freeze-out constraint, we place stringent limits on the model parameters... The resulting constraints exhibit strong agreement with observations, with the model successfully describing the transition from decelerated to accelerated expansion. ... Overall, the f(Q,L_m) framework emerges as a vi"
Model parameters are obtained by MCMC fitting to the identical observational datasets (DESI DR2 BAO, CC, GW sirens, BBN) against which agreement and viability are then claimed. The 'strong agreement', 'successful description' of the transition, and emergence as 'viable alternative' are therefore direct consequences of the fit converging within the chosen functional form, not independent theoretical predictions.
full rationale
The paper derives modified Friedmann equations from a chosen f(Q, L_m) ansatz, then constrains its free parameters via MCMC on the same late-time and BBN datasets used to assert agreement and physical viability. The resulting 'strong agreement', 'successful description' of deceleration-to-acceleration transition, quintessence-like EoS, and status as viable alternative are outputs of the fit rather than independent predictions. BBN supplies an external early-universe anchor but does not alter the fact that late-time success is statistically forced by construction of the fit. This is a clear instance of fitted input called prediction; the theoretical framework itself is not circular.
Axiom & Free-Parameter Ledger
free parameters (1)
- f(Q, L_m) model parameters
axioms (2)
- domain assumption The universe follows the FLRW metric with homogeneous isotropic expansion
- domain assumption Non-metricity Q is non-minimally coupled to the matter Lagrangian L_m
Reference graph
Works this paper leans on
-
[1]
Observational Evidence from Supernovae for an Accelerating Universe and a Cosmological Constant
A. G. Riess et al., “Observational evidence from supernovae for an accelerating universe and a cosmological constant,” Astron. J.116, 1009 (1998), arXiv:astro-ph/9805201
work page internal anchor Pith review arXiv 1998
-
[2]
Measurements of Omega and Lambda from 42 High-Redshift Supernovae
S. Perlmutter et al., “Measurements of Omega and Lambda from 42 high-redshift supernovae,”Astrophys. J.517, 565 (1999), arXiv:astro-ph/9812133
work page internal anchor Pith review arXiv 1999
-
[3]
The Supernova Legacy Survey: Measurement of Omega_M, Omega_Lambda and w from the First Year Data Set
P. Astier et al., “The Supernova Legacy Survey: Measurement ofΩM,Ω Lambdaandωfrom the first year data set,” Astron. Astrophys.447, 31 (2006), arXiv:astro-ph/0510447
work page Pith review arXiv 2006
-
[4]
D. N. Spergel et al., “First-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Determination of Cosmological Parameters,”Astrophys. J. Suppl. Ser.148, 175 (2003), arXiv:astro-ph/0302209
work page Pith review arXiv 2003
-
[5]
Cosmological parameters from SDSS and WMAP,
M. Tegmark et al., “Cosmological parameters from SDSS and WMAP,”Phys. Rev. D69, 103501 (2004), arXiv:astro- ph/0310723
- [6]
-
[7]
D. J. Eisenstein et al., “Detection of the Baryon Acoustic Peak in the Large-Scale Correlation Function of SDSS Luminous Red Galaxies,”Astrophys. J.633, 560 (2005), arXiv:astro-ph/0501171
work page Pith review arXiv 2005
-
[8]
The cosmological constant problem,
S. Weinberg, “The cosmological constant problem,”Rev. Mod. Phys.61, 1 (1989)
1989
-
[9]
J. Martin, “Everything You Always Wanted To Know About The Cosmological Constant Problem (But Were Afraid To Ask),”Comptes Rendus Physique13, 566 (2012), arXiv:1205.3365 [astro-ph.CO]
work page Pith review arXiv 2012
-
[10]
Yang, Y., Ren, X., Wang, Q., Lu, Z., Zhang, D., Cai, Y.-F., & Saridakis, E. N. (2024). Quintom cosmology and modified gravity after DESI 2024.Science Bulletin, 69(17), 2698–2704. https://doi.org/10.1016/j.scib.2024.07.029
-
[11]
Yang, Y., Ren, X., Wang, B., Cai, Y.-F., & Saridakis, E. N. (2024). Data reconstruction of the dynamical connection function inf(Q)cosmology.Monthly Notices of the Royal Astronomical Society, 533(2), 2232–2241. https://doi.org/10.1093/mnras/stae1905
- [12]
- [13]
-
[14]
Dimakis, N., Roumeliotis, M., Paliathanasis, A., Apostolopoulos, P. S., & Christodoulakis, T. (2022). Self- similar cosmological solutions in symmetric teleparallel theory: FLRW spacetimes.Phys. Rev. D,106(12), 123516. doi:10.1103/PhysRevD.106.123516
-
[15]
Basilakos, S., Paliathanasis, A., & Saridakis, E. N. (2025). Equivalence off(Q)cosmology with quintom-like scenario: The phantom field as effective realization of the non-trivial connection.Phys. Lett. B,868, 139658. doi:10.1016/j.physletb.2025.139658
-
[16]
Khyllep, W., Paliathanasis, A., & Dutta, J. (2021). Cosmological solutions and growth index of matter perturbations in f(Q)gravity.Phys. Rev. D,103(10), 103521. doi:10.1103/PhysRevD.103.103521
-
[17]
Unified cosmic history in modified gravity: From F(R) theory to Lorentz non-invariant models.Phys
Nojiri, S., &Odintsov, S.D.(2011).Unifiedcosmichistoryinmodifiedgravity: FromF(R)theorytoLorentznon-invariant models.Phys. Rept.,505, 59–144. doi:10.1016/j.physrep.2011.04.001
-
[18]
Nojiri, S., & Odintsov, S. D. (2024). Well-definedf(Q)gravity, reconstruction of FLRW spacetime and unification of inflation with dark energy epoch.Phys. Dark Univ.,45, 101538. doi:10.1016/j.dark.2024.101538
-
[19]
Nojiri, S., & Odintsov, S. D. (2024).f(Q)Gravity with Gauss–Bonnet Corrections: From Early-Time Inflation to Late- Time Acceleration.Fortschritte der Physik,72(9-10), 2400113. doi:10.1002/prop.202400113
-
[20]
Odintsov, S. D., Oikonomou, V. K., & Sharov, G. S. (2025). Einstein-Gauss-Bonnet cosmology confronted with observa- tions. Journal of High Energy Astrophysics, 47, 100398. doi:10.1016/j.jheap.2025.100398
-
[21]
Odintsov, S. D., Oikonomou, V. K., & Sharov, G. S. (2026). Dynamical dark energy from F(R) gravity models unifying inflation with dark energy: Confronting the latest observational data. Journal of High Energy Astrophysics, 50, 100471. doi:10.1016/j.jheap.2025.100471
-
[22]
Odintsov, S. D., Oikonomou, V. K., & Sharov, G. S. (2026). Viable F(R) scenarios unifying inflation with realistic dynamical dark energy. Journal of High Energy Astrophysics, 52, 100579. doi: 10.1016/j.jheap.2026.100579
-
[23]
Clifton, T., Ferreira, P. G., Padilla, A., & Constantinos Skordis. (2012). Modified gravity and cosmology. Physics Reports, 513(1-3), 1–189. doi:10.1016/j.physrep.2012.01.001
-
[24]
Buchdahl, H. A. (1970). Non-Linear Lagrangians and Cosmological Theory. Monthly Notices of the Royal Astronomical Society, 150(1), 1–8. https://doi.org/10.1093/mnras/150.1.1 16
-
[25]
Jose Beltrán Jiménez, Heisenberg, L., Koivisto, T. S., & Pekar, S. (2020). Cosmology in f(Q) geometry. 101(10). doi:10.1103/physrevd.101.103507
-
[26]
Hayashi, K., & Shirafuji, T. (1979). New general relativity. Physical Review D, 19(12), 3524–3553. https://doi.org/10.1103/physrevd.19.3524
-
[28]
Beltrán Jiménez, J., Heisenberg, L., & Koivisto, T. (2019). The Geometrical Trinity of Gravity. Universe, 5(7), 173. doi:10.3390/universe5070173
-
[29]
Amit Samaddar, & Surendra Sanasam. (2024). Dynamical system method of viscous fluid in f(T) gravity theory. Physica Scripta, 99(3), 035219–035219. doi:10.1088/1402-4896/ad232a
-
[30]
Amit Samaddar, Singh, S. S., & Alam, M. K. (2023). Dynamical system approach of interacting dark energy models with minimally coupled scalar field. International Journal of Modern Physics D, 32(09). doi:10.1142/s0218271823500621
-
[31]
Frusciante, N. (2021). Signatures of f(Q) gravity in cosmology. Physical Review, 103(4). doi:10.1103/physrevd.103.044021
-
[32]
Tiberiu Harko, Francisco, Nojiri, S., & Odintsov, S. D. (2011). f(R,T)gravity. Physical Review, 84(2). doi:10.1103/physrevd.84.024020
-
[33]
Harko, T. (2008). Modified gravity with arbitrary coupling between matter and geometry. Physics Letters B, 669(5), 376–379. doi:10.1016/j.physletb.2008.10.007
-
[34]
Harko, T. and Lobo, F.S.N. (2010) f (R, Lm) Gravity. The European Physical Journal C, 70, 373-379. doi:10.1140/epjc/s10052-010-1467-3
-
[35]
Harko, T., Lobo, F. S. N., Otalora, G., & Saridakis, E. N. (2014).f(T, τ)gravity and cosmology. Journal of Cosmology and Astroparticle Physics, 2014(12), 021–021. doi:10.1088/1475-7516/2014/12/021
-
[36]
Amit Samaddar, & Singh, S. S. (2023). Qualitative stability analysis of cosmological models inf(T, ϕ)gravity. General Relativity and Gravitation, 55(10). doi:10.1007/s10714-023-03163-y
-
[37]
Amit Samaddar, & Singh, S. S. (2023). Qualitative stability analysis of cosmological parameters in f(T, B) gravity. The European Physical Journal C, 83(4). doi:10.1140/epjc/s10052-023-11458-2
-
[38]
S.A. Narawade, M. Koussour, & Mishra, B. (2023). Constrained f(Q,T) gravity accelerating cosmological model and its dynamical system analysis. Nuclear Physics B, 992, 116233–116233. doi:10.1016/j.nuclphysb.2023.116233
-
[39]
Ayush Hazarika, Arora, S., Sahoo, P. K., & Tiberiu Harko. (2025).f(Q, Lm)gravity, and its cosmological implications. Physics of the Dark Universe, 50, 102092–102092. doi:10.1016/j.dark.2025.102092
- [40]
-
[41]
Heisenberg, L. (2019). A systematic approach to generalisations of General Relativity and their cosmological implications. Physics Reports, 796, 1–113. doi:10.1016/j.physrep.2018.11.006
-
[42]
Journal of High Energy Astrophysics, 44, 164–171
KairatMyrzakulov, M.Koussour, O.Donmez, Cilli, A., E.Güdekli, &J.Rayimbaev.(2024).Observationalanalysisoflate- time acceleration inf(Q, L)gravity. Journal of High Energy Astrophysics, 44, 164–171. doi:10.1016/j.jheap.2024.09.014
-
[43]
Myrzakulov, Y., Donmez, O., Koussour, M., Alizhanov, D., Bekchanov, S., & Rayimbaev, J. (2024). Late-time cos- mology inf(Q, L m)gravity: Analytical solutions and observational fits. Physics of the Dark Universe, 46, 101614. doi:10.1016/j.dark.2024.101614
-
[44]
Physics of the Dark Universe, 48, 101829
Myrzakulov, Y., Donmez, O., Koussour, M., Muminov, S., Davletov, I.Y., &Rayimbaev, J.(2025).Constrainingf(Q, Lm) gravity with bulk viscosity. Physics of the Dark Universe, 48, 101829. doi:10.1016/j.dark.2025.101829
- [45]
-
[46]
(2003) Introduction to Cosmology
Ryden, B. (2003) Introduction to Cosmology. Addison Wesley, San Francisco, CA. - References - Scientific Research Publishing. (2021). https://www.scirp.org/reference/referencespapers?referenceid=3024559
2003
-
[47]
Y. Myrzakulov, Alnadhief H.A. Alfedeel, M. Koussour, S. Muminov, Hassan, E. I., & J. Rayimbaev. (2025). Modified cosmology in f(Q,L) gravity. Physics Letters B, 866, 139506–139506. doi:10.1016/j.physletb.2025.139506
-
[48]
Nuclear Physics B, 1012, 116834
Samaddar, A., &Singh, S.S.(2025).Anovelapproachtobaryogenesisinf(Q, L)gravityanditscosmologicalimplications. Nuclear Physics B, 1012, 116834. doi:10.1016/j.nuclphysb.2025.116834
-
[49]
Swagat Mishra, S., Patel, S., & Sahoo, P. K. (2026). BBN to late-time acceleration inf(T, Lm)gravity. Physics Letters B, 872, 140098. doi:10.1016/j.physletb.2025.140098
-
[50]
Mishra, S. S., Kolhatkar, A., & Sahoo, P. K. (2024). Big Bang Nucleosynthesis constraints onf(T, τ)gravity. Physics Letters B, 848, 138391. doi:10.1016/j.physletb.2023.138391
-
[51]
Bhattacharjee, S., & Sahoo, P. K. (2020). Big bang nucleosynthesis and entropy evolution in f(R, T) gravity. The European Physical Journal Plus, 135(4). doi:10.1140/epjp/s13360-020-00361-4 17
-
[52]
Jose Beltran Jimenez, Heisenberg, L., & Koivisto, T. S. (2018). Coincident general relativity. Physical Review, 98(4). doi:10.1103/physrevd.98.044048
-
[53]
Sahni, V., Shafieloo, A., & Starobinsky, A. A. (2008). Two new diagnostics of dark energy.Physical Review D,78(10), 103502. https://doi.org/10.1103/PhysRevD.78.103502
-
[54]
D., Basilakos, S., & Saridakis, E
Barrow, J. D., Basilakos, S., & Saridakis, E. N. (2021). Big Bang Nucleosynthesis constraints on Barrow entropy. Physics Letters B, 815, 136134. doi:10.1016/j.physletb.2021.136134
-
[55]
K. A. Olive, G. Steigman, T. P. Walker, Primordial nucleosynthesis: theory and observations,Phys. Rep.333, 389 (2000)
2000
-
[56]
R. H. Cyburt et al., Big bang nucleosynthesis: present status,Phys. Rev. Mod. Phys.88, 015004 (2016). https://doi.org/10.1103/PhysRevModPhys.88.015004
-
[57]
D. F. Torres, H. Vucetich, A. Plastino, Early universe test of non-extensive statistics,Phys. Rev. Lett.79, 1588 (1997). https://doi.org/10.1103/PhysRevLett.79.1588
-
[58]
Lambiase, Dark matter relic abundance and big bang nucleosynthesis in Hořava’s gravity,Phys
G. Lambiase, Dark matter relic abundance and big bang nucleosynthesis in Hořava’s gravity,Phys. Rev. D83, 107501 (2011). https://doi.org/10.1103/PhysRevD.83.107501
-
[59]
K. A. Olive et al., Review of particle physics,Chin. Phys. C38, 0900001 (2014). https://doi.org/10.1088/1674- 1137/38/9/090001
-
[60]
Lambiase, Lorentz invariance breakdown and constraints from big-bang nucleosynthesis,Phys
G. Lambiase, Lorentz invariance breakdown and constraints from big-bang nucleosynthesis,Phys. Rev. D72, 087702 (2005). https://doi.org/10.1103/PhysRevD.72.087702
-
[61]
K. A. Olive, E. Skillman, G. Steigman, The primordial abundance of4He: an update,Astrophys. J.483, 788 (1997). https://doi.org/10.1086/304265
-
[62]
Abdul Karim, M., Aguilar, J., Ahlen, S., Alam, S., Allen, L., Prieto, C. A., Brieden, S. (2025). DESI DR2 re- sults. II. Measurements of baryon acoustic oscillations and cosmological constraints. Physical Review D, 112(8). https://doi.org/10.1103/tr6y-kpc6
- [63]
-
[64]
E. Chaussidonet al.. (2025).Early Time Solution as an Alternative to the Late Time Evolving Dark Energy with DESI DR2 BAO. [arXiv:2503.24343]
-
[65]
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]
-
[66]
A. Paliathanasis. (2025).Dark Energy within the Generalized Uncertainty Principle in Light of DESI DR2. [arXiv:2503.20896]
-
[67]
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
-
[68]
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.
- [69]
-
[70]
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
- [71]
-
[72]
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
-
[73]
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
work page Pith review arXiv 2014
-
[74]
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. Monthly Notices of the Royal Astronomical Society,482(3), 3497–3513. arXiv:1801.03043
-
[75]
Baryon acoustic oscillations in the Ly α forest of BOSS quasars
Busca, N. G., et al. (2013). Baryon Acoustic Oscillations in the Ly-αforest of BOSS quasars.Astronomy & Astrophysics, 552, A96. arXiv:1211.2616
- [76]
- [77]
-
[78]
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
work page Pith review arXiv 2017
-
[79]
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
- [80]
-
[81]
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
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