Constraining Spatial Curvature with Priors from Swampland Conjectures
Pith reviewed 2026-05-22 04:10 UTC · model grok-4.3
The pith
Swampland-motivated priors on the slope and field range of an exponential quintessence potential in a curved universe produce a mild shift in the best-fit value of spatial curvature Ω_k from Planck, DESI BAO, and supernova observations.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Our analysis indicates that the swampland-motivated prior mildly shifts the values of Ω_k.
Load-bearing premise
The de Sitter swampland conjecture can be directly translated into a prior on λ that excludes the curved ΛCDM limit, and the distance conjecture correctly restricts field excursion, with no additional model-dependent uncertainties affecting the parameter inference.
read the original abstract
We study a string-motivated theoretical prior on the quintessential dark energy model with exponential potential, \( V(\phi) = V_0 e^{-\lambda \phi} \), allowing for non-zero spatial curvature. First, we formulate the corresponding dynamical system and investigate its cosmological evolution numerically, illustrating the phase-space behaviour and the influence of curvature on the background dynamics. In open universes (\( \Omega_k > 0 \)), it has been suggested that a curvature-related fixed point may support accelerated expansion even for relatively steep potentials compatible with swampland considerations. Next, we explicitly impose swampland-motivated priors on the slope parameter $\lambda$, restricting it to values consistent with the de Sitter conjecture that excludes the (curved) $\Lambda$CDM limit. Furthermore, we restrict our considerations to the range of field excursion that is consistent with the swampland distance conjecture. Our primary interest is the possibility that such theoretically-motivated priors may shift values of cosmological parameters inferred by observational data, compared with the standard analysis based on theory-agnostic priors such as a sufficiently wide flat prior. We examine this possibility using a combination of Planck CMB data, DESI BAO measurements, and recent Type Ia supernova samples, performing a Bayesian inference of the model parameters. Our analysis indicates that the swampland-motivated prior mildly shifts the values of $\Omega_k$.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript studies a quintessence model with exponential potential V(φ)=V0 exp(−λφ) in the presence of spatial curvature. It formulates the corresponding dynamical system, performs numerical evolution to illustrate phase-space behavior and the role of curvature fixed points in supporting acceleration, imposes swampland-motivated priors on λ (lower bound from the de Sitter conjecture excluding the λ→0 limit and upper bound on field excursion from the distance conjecture), and performs Bayesian inference on Planck CMB + DESI BAO + Type Ia supernova data. The central result is that these priors produce a mild shift in the posterior for Ωk relative to a wide flat prior.
Significance. If the mapping from swampland conjectures to the λ prior is robust and free of unaccounted model dependence introduced by curvature, the work provides a concrete example of how string-theory-motivated theoretical constraints can be folded into cosmological parameter estimation and potentially influence inferences about spatial curvature. The dynamical-system analysis and use of current data sets are positive features, but the reported mildness of the shift limits the immediate observational impact.
major comments (2)
- [§3 and §4.1] §3 (phase-space analysis) and §4.1 (prior construction): the de Sitter conjecture is mapped to a hard lower cutoff on λ that explicitly excludes the λ→0 (curved ΛCDM) limit, yet the text notes that a curvature-related fixed point can support accelerated expansion even for relatively steep potentials. It is not shown whether this fixed point remains accessible under the adopted λ cutoff or whether the cutoff introduces an artificial tension that drives the reported Ωk shift.
- [§4.2 and results] §4.2 and results section: the claim that the swampland prior produces a data-driven mild shift in Ωk requires that the prior itself does not already force the shift by construction. No explicit comparison of the full posterior chains (or at least the marginal Ωk posteriors) with and without the λ cutoff is provided, making it impossible to separate prior volume effects from genuine data constraints.
minor comments (2)
- Notation for the curvature density parameter is occasionally written as Ωk and occasionally as Ω_K; consistent use throughout would improve readability.
- The numerical evolution plots in the phase-space figures would benefit from explicit annotation of the curvature fixed point and the location of the swampland cutoff in λ.
Simulated Author's Rebuttal
We thank the referee for the careful and constructive report. We address the two major comments point by point below. We agree that additional material will strengthen the manuscript and will incorporate revisions accordingly.
read point-by-point responses
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Referee: [§3 and §4.1] §3 (phase-space analysis) and §4.1 (prior construction): the de Sitter conjecture is mapped to a hard lower cutoff on λ that explicitly excludes the λ→0 (curved ΛCDM) limit, yet the text notes that a curvature-related fixed point can support accelerated expansion even for relatively steep potentials compatible with swampland considerations. It is not shown whether this fixed point remains accessible under the adopted λ cutoff or whether the cutoff introduces an artificial tension that drives the reported Ωk shift.
Authors: The de Sitter conjecture supplies a lower bound λ ≳ O(1), which excludes the λ → 0 limit while retaining the steeper potentials for which the curvature fixed point in open universes is known to permit acceleration. Because the fixed point is precisely relevant for the larger-λ regime allowed by the prior, it remains accessible; the prior does not remove the dynamical channel that supports acceleration. The reported mild shift in Ωk occurs because the prior removes the near-flat potentials that would otherwise permit Ωk closer to zero while still fitting the data. We will add a short discussion and an illustrative phase-space trajectory for λ values inside the adopted prior range to make this accessibility explicit. revision: yes
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Referee: [§4.2 and results] §4.2 and results section: the claim that the swampland prior produces a data-driven mild shift in Ωk requires that the prior itself does not already force the shift by construction. No explicit comparison of the full posterior chains (or at least the marginal Ωk posteriors) with and without the λ cutoff is provided, making it impossible to separate prior volume effects from genuine data constraints.
Authors: We agree that an explicit side-by-side comparison of the Ωk marginal posteriors (and ideally the full chains) obtained with the swampland-motivated prior versus a broad flat prior on λ is the clearest way to separate prior-volume effects from data-driven shifts. In the revised manuscript we will include these marginal posteriors together with a brief quantitative discussion of the difference. revision: yes
Circularity Check
No significant circularity; derivation relies on external conjectures and data.
full rationale
The paper's chain begins with an independent formulation of the dynamical system for the exponential quintessence model including curvature, followed by numerical phase-space analysis. It then adopts swampland conjectures (de Sitter and distance) as external theoretical priors on λ and field range, explicitly chosen to exclude the λ→0 limit. These priors are imposed before performing Bayesian inference on Planck CMB, DESI BAO, and supernova data. The reported mild shift in Ω_k is a direct, non-circular consequence of the prior choice combined with the likelihood; no step reduces by construction to a fitted input, self-citation, or renamed ansatz. The derivation remains self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
free parameters (1)
- λ prior bounds
axioms (2)
- domain assumption de Sitter swampland conjecture: |∇V|/V ≥ c with c of order unity, excluding flat potentials such as the curved ΛCDM limit
- domain assumption swampland distance conjecture: field excursion Δφ remains O(1)
Lean theorems connected to this paper
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
we explicitly impose swampland-motivated priors on the slope parameter λ, restricting it to values consistent with the de Sitter conjecture that excludes the (curved) ΛCDM limit
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IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
a curvature-related fixed point may support accelerated expansion even for relatively steep potentials
What do these tags mean?
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- supports
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- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
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- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
Tensions between the Early and the Late Universe
L. Verde, T. Treu, and A. G. Riess. Tensions between the Early and the Late Universe.Nature Astron., 3: 891, 2019. doi: 10.1038/s41550-019-0902-0
work page internal anchor Pith review doi:10.1038/s41550-019-0902-0 2019
-
[2]
Eleonora Di Valentino, Olga Mena, Supriya Pan, Luca Visinelli, Weiqiang Yang, Alessandro Melchiorri, David F. Mota, Adam G. Riess, and Joseph Silk. In the realm of the Hubble tension—a review of solutions.Class. Quant. Grav., 38(15):153001, 2021. doi: 10.1088/1361-6382/ac086d
-
[3]
2022, NewAR, 95, 101659, doi: 10.1016/j.newar.2022.101659
Leandros Perivolaropoulos and Foteini Skara. Challenges forΛCDM: An update.New Astron. Rev., 95: 101659, 2022. doi: 10.1016/j.newar.2022.101659
-
[4]
Elcio Abdalla et al. Cosmology intertwined: A review of the particle physics, astrophysics, and cosmology associated with the cosmological tensions and anomalies.JHEAp, 34:49–211, 2022. doi: 10.1016/j.jheap.2022.04.002
work page internal anchor Pith review doi:10.1016/j.jheap.2022.04.002 2022
-
[5]
A Step in understanding the Hubble tension.Phys
Daniel Aloni, Asher Berlin, Melissa Joseph, Martin Schmaltz, and Neal Weiner. A Step in understanding the Hubble tension.Phys. Rev. D, 105(12):123516, 2022. doi: 10.1103/PhysRevD.105.123516
-
[6]
Vivian Poulin, Tristan L. Smith, and Tanvi Karwal. The Ups and Downs of Early Dark Energy solutions to the Hubble tension: A review of models, hints and constraints circa 2023.Phys. Dark Univ., 42:101348,
work page 2023
-
[7]
doi: 10.1016/j.dark.2023.101348
-
[8]
Sunny Vagnozzi. Seven Hints That Early-Time New Physics Alone Is Not Sufficient to Solve the Hubble Tension.Universe, 9(9):393, 2023. doi: 10.3390/universe9090393
-
[9]
Marc Kamionkowski and Adam G. Riess. The Hubble Tension and Early Dark Energy.Ann. Rev. Nucl. Part. Sci., 73:153–180, 2023. doi: 10.1146/annurev-nucl-111422-024107
-
[10]
G., et al., 2022, @doi [The Astrophysical Journal Letters] 10.3847/2041-8213/ac5c5b , 934, L7
Adam G. Riess, Wenlong Yuan, Lucas M. Macri, Dillon Brout, Dan Scolnic, Stefano Casertano, et al. A Comprehensive Measurement of the Local Value of the Hubble Constant with 1 km s−1 Mpc−1 Uncertainty from the Hubble Space Telescope and the SH0ES Team.Astrophys. J. Lett., 934:L7, 2022. doi: 10.3847/2041-8213/ac5c5b
-
[11]
2020, , 641, A6, 10.1051/0004-6361/201833910
N. Aghanim et al. Planck 2018 results. VI. Cosmological parameters.Astron. Astrophys., 641:A6, 2020. doi: 10.1051/0004-6361/201833910. [Erratum: Astron. Astrophys. 652, C4 (2021)]
-
[14]
L. F. Secco, S. Samuroff, E. Krause, B. Jain, J. Blazek, M. Raveri, et al. Dark Energy Survey Year 3 Results: Cosmology from Cosmic Shear and Robustness to Modeling Uncertainty.Phys. Rev. D, 105(2):023515,
-
[15]
doi: 10.1103/PhysRevD.105.023515
-
[16]
KiDS-1000 Cosmology: Cosmic shear constraints and comparison between two point statistics.Astron
Marika Asgari, Chieh-An Lin, Benjamin Joachimi, Benjamin Giblin, Catherine Heymans, Hendrik Hildebrandt, et al. KiDS-1000 Cosmology: Cosmic shear constraints and comparison between two point statistics.Astron. Astrophys., 645:A104, 2021. doi: 10.1051/0004-6361/202039070
-
[17]
A. G. Adame et al. DESI 2024 VI: cosmological constraints from the measurements of baryon acoustic oscillations.JCAP, 02:021, 2025. doi: 10.1088/1475-7516/2025/02/021
-
[18]
M. Abdul Karim et al. DESI DR2 Results II: Measurements of Baryon Acoustic Oscillations and Cosmological Constraints.Phys. Rev. D, 112(8):083515, 2025. doi: 10.1103/tr6y-kpc6
-
[19]
M. Chevallier and D. Polarski. Accelerating Universes with Scaling Dark Matter.Int. J. Mod. Phys. D, 10: 213–224, 2001. doi: 10.1142/S0218271801000822
-
[20]
Eric V . Linder. Exploring the expansion history of the universe.Phys. Rev. Lett., 90:091301, 2003. doi: 10.1103/PhysRevLett.90.091301. – 20 –
-
[21]
T. M. C. Abbott et al. Dark Energy Survey: Implications for cosmological expansion models from the final DES baryon acoustic oscillation and supernova data.Phys. Rev. D, 113(6):063530, 2026. doi: 10.1103/z2q4-qcdq
-
[22]
Probing the dynamics of Gaussian dark energy equation of state using DESI BAO.Mon
Saddam Hussain, Simran Arora, Anzhong Wang, and Benjamin Rose. Probing the dynamics of Gaussian dark energy equation of state using DESI BAO.Mon. Not. Roy. Astron. Soc., 545(2):staf1924, 2025. doi: 10.1093/mnras/staf1924
-
[23]
William Giar `e, Mahdi Najafi, Supriya Pan, Eleonora Di Valentino, and Javad T. Firouzjaee. Robust preference for Dynamical Dark Energy in DESI BAO and SN measurements.JCAP, 10:035, 2024. doi: 10.1088/1475-7516/2024/10/035
-
[24]
Dynamical dark energy parametrizations in VCDM.Phys
Simran Arora, Antonio De Felice, and Shinji Mukohyama. Dynamical dark energy parametrizations in VCDM.Phys. Rev. D, 112(12):123518, 2025. doi: 10.1103/l5bx-snl3
-
[25]
Aleksandr Chatrchyan, Florian Niedermann, Vivian Poulin, and Martin S. Sloth. Confronting cold new early dark energy and its equation of state with updated CMB, supernovae, and BAO data.Phys. Rev. D, 111(4):043536, 2025. doi: 10.1103/PhysRevD.111.043536
-
[26]
Changyu You, Dan Wang, and Tao Yang. Dynamical dark energy implies a coupled dark sector: Insights from DESI DR2 via a data-driven approach.Phys. Rev. D, 112(4):043503, 2025. doi: 10.1103/f6v7-n9fr
-
[27]
Mateus Scherer, Miguel A. Sabogal, Rafael C. Nunes, and Antonio De Felice. Challenging theΛCDM model: 5σevidence for a dynamical dark energy late-time transition.Phys. Rev. D, 112(4):043513, 2025. doi: 10.1103/n86r-sjgm
-
[28]
2022, ApJ, 938, 113, doi: 10.3847/1538-4357/ac8b7a
Dan Scolnic, Dillon Brout, Anthony Carr, Adam G. Riess, Tamara M. Davis, Arianna Dwomoh, David O. Jones, Noor Ali, Pranav Charvu, Rebecca Chen, et al. The pantheon+ analysis: The full dataset and light-curve release.The Astrophysical Journal, 938(2):113, 2022. doi: 10.3847/1538-4357/ac8b7a
-
[29]
2022, title The Pantheon+ Analysis: Cosmological Constraints , , 938, 110, 10.3847/1538-4357/ac8e04
Dillon Brout, Dan Scolnic, Brodie Popovic, Adam G. Riess, Joe Zuntz, Rick Kessler, Anthony Carr, Tamara M. Davis, Samuel Hinton, David O. Jones, et al. The pantheon+ analysis: Cosmological constraints.The Astrophysical Journal, 938(2):110, 2022. doi: 10.3847/1538-4357/ac8e04
-
[31]
Marina Cort ˆes and Andrew R. Liddle. Interpreting DESI’s evidence for evolving dark energy.JCAP, 12: 007, 2024. doi: 10.1088/1475-7516/2024/12/007
-
[32]
G. Efstathiou. Evolving dark energy or supernovae systematics?Mon. Not. Roy. Astron. Soc., 538(2):875, 2025
work page 2025
-
[34]
Escamilla, William Giar `e, Eleonora Di Valentino, Rafael C
Luis A. Escamilla, William Giar `e, Eleonora Di Valentino, Rafael C. Nunes, and Sunny Vagnozzi. The state of the dark energy equation of state circa 2023.JCAP, 05:091, 2024. doi: 10.1088/1475-7516/2024/05/091
-
[35]
Measuring cosmic curvature with non-CMB observations.Phys
Peng-Ju Wu and Xin Zhang. Measuring cosmic curvature with non-CMB observations.Phys. Rev. D, 112 (6):063514, 2025. doi: 10.1103/sn3q-q589
-
[36]
K. Lehnert. Hitchhiker’s guide to the swampland: The cosmologist’s handbook to the string-theoretical swampland programme. 2025
work page 2025
-
[37]
N. B. Agmon, A. Bedroya, M. J. Kang, and C. Vafa. Lectures on the string landscape and the swampland. 2022
work page 2022
- [38]
-
[39]
Hyperbolic field space and swampland conjecture for DBI scalar.JCAP, 09:072, 2019
Shuntaro Mizuno, Shinji Mukohyama, Shi Pi, and Yun-Long Zhang. Hyperbolic field space and swampland conjecture for DBI scalar.JCAP, 09:072, 2019. doi: 10.1088/1475-7516/2019/09/072
-
[40]
de Sitter swampland conjecture and the Higgs potential.Phys
Frederik Denef, Arthur Hebecker, and Timm Wrase. de Sitter swampland conjecture and the Higgs potential.Phys. Rev. D, 98(8):086004, 2018. doi: 10.1103/PhysRevD.98.086004
-
[41]
Hitoshi Murayama, Masahito Yamazaki, and Tsutomu T. Yanagida. Do We Live in the Swampland? JHEP, 12:032, 2018. doi: 10.1007/JHEP12(2018)032
-
[42]
D. Andriot and C. Roupec. Further refining the de sitter swampland conjecture.Fortsch. Phys., 67(1-2): 1800105, 2019
work page 2019
- [43]
-
[44]
G. F. Casas and I. Ruiz. Cosmology of light towers and swampland constraints.JHEP, 12:193, 2024
work page 2024
-
[45]
S. Laliberte and R. Brandenberger. String gases and the swampland.JCAP, 07:046, 2020
work page 2020
-
[46]
Supersymmetric hybrid inflation in light of CMB experiments and swampland conjectures.Chin
Waqas Ahmed and Shabbar Raza. Supersymmetric hybrid inflation in light of CMB experiments and swampland conjectures.Chin. Phys. C, 49(1):013106, 2025. doi: 10.1088/1674-1137/ad7c27
-
[47]
Shuntaro Mizuno, Shinji Mukohyama, Shi Pi, and Yun-Long Zhang. Universal Upper Bound on the Inflationary Energy Scale from the Trans-Planckian Censorship Conjecture.Phys. Rev. D, 102(2):021301,
-
[48]
doi: 10.1103/PhysRevD.102.021301
-
[49]
Exponential quintessence: curved, steep and stringy?JHEP, 08:117, 2024
David Andriot, Susha Parameswaran, Dimitrios Tsimpis, Timm Wrase, and Ivonne Zavala. Exponential quintessence: curved, steep and stringy?JHEP, 08:117, 2024. doi: 10.1007/JHEP08(2024)117
-
[50]
Dynamical Analysis of Scalar Field Cosmologies with Spatial Curvature
Mateja Gosenca and Peter Coles. Dynamical Analysis of Scalar Field Cosmologies with Spatial Curvature.Open J. Astrophys., 1(1):1, 2016. doi: 10.21105/astro.1502.04020
work page internal anchor Pith review Pith/arXiv arXiv doi:10.21105/astro.1502.04020 2016
-
[51]
R. J. van den Hoogen, Alan A. Coley, and David Wands. Scaling solutions in Robertson-Walker space-times.Class. Quant. Grav., 16:1843–1851, 1999. doi: 10.1088/0264-9381/16/6/317
-
[52]
Accelerated expansion of an open universe and string theory realizations.Phys
David Andriot, Dimitrios Tsimpis, and Timm Wrase. Accelerated expansion of an open universe and string theory realizations.Phys. Rev. D, 108(12):123515, 2023. doi: 10.1103/PhysRevD.108.123515
-
[53]
Is curvature-assisted quintessence observationally viable?Phys
George Alestas, Matilda Delgado, Ignacio Ruiz, Yashar Akrami, Miguel Montero, and Savvas Nesseris. Is curvature-assisted quintessence observationally viable?Phys. Rev. D, 110(10):106010, 2024. doi: 10.1103/PhysRevD.110.106010
-
[54]
Prateek Agrawal, Georges Obied, Paul J. Steinhardt, and Cumrun Vafa. On the Cosmological Implications of the String Swampland.Phys. Lett. B, 784:271–276, 2018. doi: 10.1016/j.physletb.2018.07.040
-
[55]
The Landscape, the Swampland and the Era of Precision Cosmology.Fortsch
Yashar Akrami, Renata Kallosh, Andrei Linde, and Valeri Vardanyan. The Landscape, the Swampland and the Era of Precision Cosmology.Fortsch. Phys., 67(1-2):1800075, 2019. doi: 10.1002/prop.201800075
-
[56]
Swampland Conjectures and Late-Time Cosmology.Phys
Marco Raveri, Wayne Hu, and Savdeep Sethi. Swampland Conjectures and Late-Time Cosmology.Phys. Rev. D, 99(8):083518, 2019. doi: 10.1103/PhysRevD.99.083518
-
[57]
James M. Cline. Quintessence, cosmological horizons, and self-tuning.JHEP, 08:035, 2001. doi: 10.1088/1126-6708/2001/08/035
-
[58]
On the geometry of the string landscape and the swampland.Nuclear Physics B, 766:21–33, 2007
Hirosi Ooguri and Cumrun Vafa. On the geometry of the string landscape and the swampland.Nuclear Physics B, 766:21–33, 2007. doi: 10.1016/j.nuclphysb.2006.10.033
-
[59]
The swampland: Introduction and review.Fortschritte der Physik, 67(6):1900037, 2019
Eran Palti. The swampland: Introduction and review.Fortschritte der Physik, 67(6):1900037, 2019. doi: 10.1002/prop.201900037
-
[60]
Distance and de sitter conjectures on the swampland.Physics Letters B, 788:180–184, 2019
Hirosi Ooguri, Eran Palti, Gary Shiu, and Cumrun Vafa. Distance and de sitter conjectures on the swampland.Physics Letters B, 788:180–184, 2019. doi: 10.1016/j.physletb.2018.11.018. – 22 –
-
[61]
N. Aghanim et al. Planck 2018 results. V . CMB power spectra and likelihoods.Astron. Astrophys., 641:A5,
work page 2018
-
[62]
doi: 10.1051/0004-6361/201936386
-
[63]
K. Lodha et al. Extended Dark Energy analysis using DESI DR2 BAO measurements.Phys. Rev. D, 112(8): 083511, 2025. doi: 10.1103/w4c6-1r5j
-
[64]
U. Andrade et al. Validation of the DESI DR2 Measurements of Baryon Acoustic Oscillations from Galaxies and Quasars.Phys. Rev. D, 112(8):083512, 2025. doi: 10.1103/kdys-w8vl
-
[65]
DES Collaboration, T. M. C. Abbott, et al. The dark energy survey: Cosmology results with ˜1500 new high-redshift type ia supernovae using the full 5-year dataset.Astrophys. J. Lett., 973(1):L14, 2024. doi: 10.3847/2041-8213/ad6f9f
-
[66]
B. O. S ´anchez, D. Brout, M. Vincenzi, M. Sako, K. Herner, R. Kessler, et al. The dark energy survey supernova program: Light curves and 5 yr data release.Astrophys. J., 975(1):5, 2024. doi: 10.3847/1538-4357/ad739a
-
[67]
Union Through UNITY: Cosmology with 2,000 SNe Using a Unified Bayesian Framework.Astrophys
David Rubin et al. Union Through UNITY: Cosmology with 2,000 SNe Using a Unified Bayesian Framework.Astrophys. J., 986(2):231, 2025. doi: 10.3847/1538-4357/adc0a5
-
[68]
GetDist: a Python package for analysing Monte Carlo samples.JCAP, 08:025, 2025
Antony Lewis. GetDist: a Python package for analysing Monte Carlo samples.JCAP, 08:025, 2025. doi: 10.1088/1475-7516/2025/08/025
-
[69]
H. Akaike. A new look at the statistical model identification.IEEE T rans. Automatic Control, 19(6):716–723,
-
[70]
doi: 10.1109/TAC.1974.1100705
-
[71]
Estimating the Dimension of a Model.Annals Statist., 6:461–464, 1978
Gideon Schwarz. Estimating the Dimension of a Model.Annals Statist., 6:461–464, 1978. – 23 –
work page 1978
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