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Noether Symmetry in a Non-Metricity Theory with a Boundary Term: Exact Solutions and Bayesian Cosmological Constraints

General Relativity and Quantum Cosmology · Submitted 24 Sep 2026 · 104 references

Pith's verdict: Competent, honestly-scoped Noether-symmetry paper with genuinely new DESI DR2 constraints, but the central exact-solution derivation rests on a false branch-elimination claim that a referee should force them to fix.

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arXiv ID2609.29303 (version 1)
Pith IDQJLIR6X7, Pith's permanent record of this paper and its review
CitationL K Duchaniya, Pooja Vishwakarma, Yu Shi. "Noether Symmetry in a Non-Metricity Theory with a Boundary Term: Exact Solutions and Bayesian Cosmological Constraints." arXiv:2609.29303 (2026). https://pith.science/paper/QJLIR6X7
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Referee report
The paper

The paper claims

A power-law $f(Q,B)$ modified-gravity model, fixed by a Noether symmetry, reproduces the standard model's background expansion and yields $H_0=67.5$ km/s/Mpc on CC+DESI DR2 data, matching the Planck 2018 value.

The reading

This paper claims that a modified theory of gravity built from the non-metricity scalar $Q$ and its boundary term $B$, taken in the multiplicative power-law form $f(Q,B)=f_0(-Q)^\alpha B^\beta$, admits exact power-law cosmological solutions whose functional form is selected by a Noether symmetry of the point-like Lagrangian. Because the symmetry forces $a(t)=a_0(t-t_0)^{2(\alpha+\beta)/3}$, the model accelerates whenever $\alpha+\beta>3/2$, while recovering the standard radiation, matter, and stiff eras at particular parameter values. Constrained with combined cosmic-chronometer and DESI DR2 BAO data, the model returns $H_0=67.5^{+1.4}_{-1.6}$ km/s/Mpc, consistent with Planck 2018, with fit statistics nearly matching $\Lambda$CDM. The authors read this as evidence that the $f(Q,B)$ model is a viable geometric alternative description of late-time cosmology that brackets, rather than resolves, the Hubble tension.

What carries the argument

The central object is the point-like Lagrangian (3.5) on configuration space $(a,Q,B)$, from which Noether's theorem yields the conserved charge (4.16). Applying the Rund-Trautman identity to this Lagrangian forces the infinitesimal generator to be the simultaneous scaling (4.37) of $t$, $a$, $Q$, and $B$, which in turn selects the multiplicative power-law form $f(Q,B)=f_0(-Q)^\alpha B^\beta$. Substituting that form into the scale-factor Euler-Lagrange equation gives the factorisation (4.42), whose first factor vanishing fixes $s=2(\alpha+\beta)/3$ and hence the scale factor (4.44); the deceleration parameter $q=3/(2(\alpha+\beta))-1$ then makes the acceleration condition $\alpha+\beta>3/2$ explicit.

Extended reading notes

Core claim

The central claim is that the Noether symmetry of the point-like Lagrangian (3.5) selects the multiplicative power-law $f(Q,B)=f_0(-Q)^\alpha B^\beta$ together with a conserved Noether charge, and that the resulting exact solution $a(t)=a_0(t-t_0)^{2(\alpha+\beta)/3}$ produces late-time acceleration when $\alpha+\beta>3/2$. Integrated numerically and fit to CC, Pantheon+, SH0ES, and DESI DR2 data, the reconstructed Hubble evolution tracks the $\Lambda$CDM background, with the CC+DESI DR2 combination giving $\Delta\mathrm{AIC}=1.41$, $\Delta\mathrm{BIC}=4.93$, and $H_0=67.5^{+1.4}_{-1.6}$ km/s/Mpc, while the SN-inclusive combinations yield higher values reaching $74.4^{+3.8}_{-4.1}$ km/s/Mpc. The paper reads the dataset-dependent span of $H_0$ and the near-parity of the fit statistics as demonstrating that the power-law $f(Q,B)$ model is a viable alternative to the standard cosmological paradigm.

Load-bearing premise

The load-bearing premise is that the power-law solution and the acceleration bound $\alpha+\beta>3/2$ follow unavoidably from the theory, but the second factor of equation (4.42), which is $2(\alpha+\beta-1)(3s-1+\beta)$, vanishes at $s=(1-\beta)/3$ without violating the non-degeneracy conditions, so the expanding branch $s=2(\alpha+\beta)/3$ is selected by assertion rather than derived, and the numerical fit further seeds the modified Hubble evolution with $\Lambda$CDM boundary conditions at $z=0$.

Editorial extensions

If this is right

  • If correct, the power-law $f(Q,B)$ model provides a geometry-only alternative to $\Lambda$CDM whose background expansion fits the combined CC+DESI DR2 data nearly as well as the standard model ($\Delta\mathrm{AIC}=1.41$, $\Delta\mathrm{BIC}=4.93$).
  • The exact solution reproduces the conventional radiation, matter, and stiff eras for $\alpha+\beta=3/4$, $1$, and $1/2$, connecting the modified theory to standard cosmological epochs.
  • The inferred $H_0$ spans the range between early-Universe and locally calibrated determinations (from $67.5$ to $74.4$ km/s/Mpc), so the model brackets the Hubble tension without resolving it.
  • The reconstructed deceleration parameter turns negative at $z_{\mathrm{trans}}\approx0.44$-$0.50$ across dataset combinations, with present-day $q_0\approx-0.58$ to $-0.62$, consistent with observed late-time acceleration.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • Because the numerical integration seeds the $f(Q,B)$ Hubble evolution with $\Lambda$CDM initial conditions at $z=0$, the reported parity with $\Lambda$CDM may partly inherit that seeding; a fully self-consistent test would draw initial conditions from the $f(Q,B)$ solution itself, and the $H_0$ and $\Delta\mathrm{AIC}$ values could shift as a result.
  • The stiff-like high-redshift behavior $\omega(z)>1/3$ in the reconstructed EoS is flagged by the authors as integration-sensitive; extending their reading, I would test it by forward-integrating from high redshift with matching conditions rather than trusting the backward reconstruction.
  • The matter-dominated solution $\alpha+\beta=1$ lies precisely on the degenerate branch that the non-degeneracy condition excludes, so the claimed recovery of the standard epochs from the exact solution is not continuously connected to the non-degenerate branch analysed for cosmology.
  • The background-only fit says nothing about structure growth; if the model is a genuine alternative, its perturbation-level behavior (for instance the growth rate $f\sigma_8$) should be checked against redshift-space distortion data before the 'viable alternative' claim is taken as settled.
Original abstract

We investigate the cosmological implications of a power-law $f(Q, B)$ gravity model, where $Q$ denotes the non-metricity scalar and $B$ is the associated boundary term. We employ the Noether symmetry approach to identify the admissible functional form of the gravitational Lagrangian and to obtain the corresponding conserved quantities and exact cosmological solutions. Using the exact solution, we find that for this model parameter condition $\alpha+\beta>\frac{3}{2}$, the model exhibits the accelerating phase of the Universe. Furthermore, we have also discussed the model with recent observational data using a Bayesian Markov Chain Monte Carlo analysis. We consider different combinations of Cosmic Chronometers (CC), Pantheon+ \& SH0ES, and DESI DR2 observations to constrain the model parameters and the Hubble constant $H_0$. The inferred value of $H_0$ depends on the adopted dataset combination, ranging from a higher value for the CC+Pantheon+ combination to a lower value for CC+DESI DR2, with the latter yielding $H_0=67.5^{+1.4}_{-1.6}\,\mathrm{km\,s^{-1}\, Mpc^{-1}}$, consistent with the Planck 2018 CMB-preferred value within the standard $\Lambda$CDM framework. The inferred \(H_0\) is strongly dataset dependent, spanning the range between the early-Universe and locally calibrated determinations. We further examine the posterior covariance and correlation matrices to identify parameter degeneracies and assess the robustness of the MCMC constraints. The background evolution also exhibits late-time accelerated expansion and remains compatible with the observational constraints. These results demonstrate that the $f(Q, B)$ model provides a viable alternative description of late-time cosmology.

The compiled record

The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-25: 1 request, 7,811 input tokens.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.68 · human participants 0.01 · controlled comparison 0.08 · randomized assignment 0.01 · states quantitative result 0.99 · compares with prior results 0.74 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

We investigate the cosmological implications of a power-law $f(Q, B)$ gravity model, where $Q$ denotes the non-metricity scalar and $B$ is the associated boundary term. We employ the Noether symmetry approach to identify the admissible functional form of the gravitational Lagrangian and to obtain the corresponding conserved quantities and exact cosmological solutions. Using the exact solution, we find that for this model parameter condition $\alpha+\beta>\frac{3}{2}$, the model exhibits the accelerating phase of the Universe. Furthermore, we have also discussed the model with recent observational data using a Bayesian Markov Chain Monte Carlo analysis. We consider different combinations of Cosmic Chronometers (CC), Pantheon+ \& SH0ES, and DESI DR2 observations to constrain the model parameters and the Hubble constant $H_0$. The inferred value of $H_0$ depends on the adopted dataset combination, ranging from a higher value for the CC+Pantheon+ combination to a lower value for CC+DESI DR2, with the latter yielding $H_0=67.5^{+1.4}_{-1.6}\,\mathrm{km\,s^{-1}\, Mpc^{-1}}$, consistent with the Planck 2018 CMB-preferred value within the standard $\Lambda$CDM framework. The inferred \(H_0\) is strongly dataset dependent, spanning the range between the early-Universe and locally calibrated determinations. We further examine the posterior covariance and correlation matrices to identify parameter degeneracies and assess the robustness of the MCMC constraints. The background evolution also exhibits late-time accelerated expansion and remains compatible with the observational constraints. These results demonstrate that the $f(Q, B)$ model provides a viable alternative description of late-time cosmology.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 We investigate the cosmological implications of a power-law $f(Q, B)$ gravity model, where $Q$ denotes the non-metricity scalar and $B$ is the associated boundary term. contribution 0.84 0.78 0.03 asserted 0.71
s1 We employ the Noether symmetry approach to identify the admissible functional form of the gravitational Lagrangian and to obtain the corresponding conserved quantities and exact cosmological solutions. method 0.95 0.96 0.04 asserted 0.97
s2 Using the exact solution, we find that for this model parameter condition $\alpha+\beta>\frac{3}{2}$, the model exhibits the accelerating phase of the Universe. result 1.00 0.96 0.15 asserted 1.00
s3 Furthermore, we have also discussed the model with recent observational data using a Bayesian Markov Chain Monte Carlo analysis. method 0.80 0.96 0.04 asserted 0.98
s4 We consider different combinations of Cosmic Chronometers (CC), Pantheon+ \& SH0ES, and DESI DR2 observations to constrain the model parameters and the Hubble constant $H_0$. method 0.96 0.94 0.03 asserted 0.97
s5 The inferred value of $H_0$ depends on the adopted dataset combination, ranging from a higher value for the CC+Pantheon+ combination to a lower value for CC+DESI DR2, with the latter yielding $H_0=67.5^{+1.4}_{-1.6}\,\mathrm{km\,s^{-1}\, Mpc^{-1}}$, consistent with the Planck 2018 CMB-preferred value within the standard $\Lambda$CDM framework. result 1.00 0.94 0.13 asserted 0.93
s6 The inferred \(H_0\) is strongly dataset dependent, spanning the range between the early-Universe and locally calibrated determinations. result 0.75 0.89 0.07 asserted 1.00
s7 We further examine the posterior covariance and correlation matrices to identify parameter degeneracies and assess the robustness of the MCMC constraints. method 0.85 0.95 0.03 asserted 0.73
s8 The background evolution also exhibits late-time accelerated expansion and remains compatible with the observational constraints. result 0.97 0.88 0.08 asserted 0.99
s9 These results demonstrate that the $f(Q, B)$ model provides a viable alternative description of late-time cosmology. interpretation 1.00 0.83 0.89 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 0.99 · evidence from analysis of existing data 0.93.

What was examined, and what was not

sources read
  • arXiv listing abstract v1
not examined
  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
levels run
  • P abstract
not run
  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

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

Figures
Figure 1. The marginalized posterior distributions and the corresponding 68% and 95% confidence contours for the f(Q, B) model parameters, derived from the different dataset combinations
Figure 2. Posterior covariance matrices obtained from the converged MCMC chains for the differ￾ent combinations of observational datasets. The diagonal elements represent the posterior variances of the parameters, while the off-diagonal elements quantify their joint covariance. H0 m0 M H0 m0 M 1.00 -0.12 -0.11 0.04 0.96 -0.12 1.00 0.86 0.21 0.09 -0.11 0.86 1.00 -0.19 0.02 0.04 0.21 -0.19 1.00 0.08 0.96 0.09 0.02 0.08 1.00 CC + PN + & SH0ES Dataset 1.00 0.75 0.50 0.25 0.00 0.25 0.50 0.75 1.00 H0 m0 M H0 m0 M 1.00 -0.04 -0.04 0.05 1.00 -0.04 1.00 0.99 -0.76 0.01 -0.04 0.99 1.00 -0.74 0.00 0.05…
Figure 3. Posterior correlation matrices obtained from the converged MCMC chains for the different combinations of observational datasets. The matrix elements quantify the strength and direction of the posterior correlations between the model parameters, with Rij = 1 indicating perfect positive correlation, Rij = −1 indicating perfect negative correlation, Rij = 0 no correlation, Rij > 0 positive correlation and Rij < 0 negative correlation. 5.0.3 Late-Time Cosmology In this section, we will analyze the fundamental cosmological parameters to explore the late￾time dynamics of the f(Q, B)…
Figure 4. Evolutionary behavior of the Hubble parameters and ΛCDM model in redshift for the data sets combination. 0.0 0.5 1.0 1.5 2.0 2.5 z 1.0 0.5 0.0 0.5 1.0 1.5 q(z) Evolution for CC + PN + & SH0ES Dataset f(Q, B) 95% C.L. f(Q, B) 68% C.L. f(Q, B) model CDM model q = 1 q = 0 0.0 0.5 1.0 1.5 2.0 2.5 z 1.0 0.5 0.0 0.5 1.0 1.5 q(z) Evolution for CC + PN + Dataset f(Q, B) 95% C.L. f(Q, B) 68% C.L. f(Q, B) model CDM model q = 1 q = 0 0.0 0.5 1.0 1.5 2.0 2.5 z 1.0 0.5 0.0 0.5 1.0 1.5 q(z) Evolution for CC + DESI DR2 Dataset f(Q, B) 95% C.L. f(Q, B) 68% C.L. f(Q, B) model CDM model q = 1 q = 0
Figure 5. Evolutionary behavior of the deceleration parameters and ΛCDM model in redshift for the data sets combination. In
Figure 6. Evolutionary behavior of the Equation-of-state parameter and ΛCDM model in redshift for the data sets combination. local measurements in the late Universe. Notably, incorporating the SH0ES prior results in an upward shift of the estimated H0, enhancing its alignment with local measurements, whereas the CC+DESI DR2 analysis stays closer to the CMB-preferred values. The inferred H0 is strongly dataset dependent, spanning the range between the early-Universe and locally calibrated determinations. 64 66 68 70 72 74 76 78 H0 [km s 1 Mpc 1 ] Planck Collab. 2020 A&A 641 A6 [CMB (Planck)]…
Figure 7. Whisker plot illustrating a comparison between the observational determinations of the Hubble constant H0 and the constraints obtained from the f(Q, B) gravity model. The black markers represent measurements reported in the literature, whereas the red markers correspond to the results obtained in this work for the CC+PN+, CC+PN+& SH0ES, and CC+DESI DR2 dataset combina￾tions. Horizontal error bars denote the 1σ confidence intervals. – 25 –
Figure 8. The marginalized posterior distributions and the corresponding 68% and 95% confidence contours for the ΛCDM model parameters, derived from the different dataset combinations. Acknowledgments Y.S. and L.K.D. acknowledge the support of the National Natural Science Foundation of China under Grant Nos. T2241005 and 12075059, as well as the startup fund of USTC. References [1] P.J.E. Peebles, B. Ratra, Rev. Mod. Phys. 75, 559 (2003). DOI 10.1103/RevModPhys.75.559 [2] E.J. Copeland, M. Sami, S. Tsujikawa, Int. J. Mod. Phys. D 15, 1753 (2006). DOI 10.1142/S021827180600942X [3] A.G. Riess, e

Figures reproduced from arXiv:2609.29303 by the authors.

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