KiDS-Legacy: Constraining dark energy, neutrino mass, and curvature
Pith reviewed 2026-05-16 22:48 UTC · model grok-4.3
The pith
KiDS-Legacy cosmic shear data aligns with flat Lambda-CDM, producing bounds c squared times sum of neutrino masses below 1.5 eV and dark energy parameters near minus one when combined with CMB.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
KiDS-Legacy cosmic shear is consistent with the fiducial flat Lambda-CDM model, returning 1-sigma bounds c squared sum m_nu less than or equal to 1.5 eV, w0 equals minus 1.0 plus or minus 0.7, wa equals minus 1.3 plus 1.9 minus 2.0, and Omega_K equals 0.08 plus 0.16 minus 0.17, with nearly equal goodness of fit. Adding all external probes gives S8 equals 0.816 plus or minus 0.006 in Lambda-CDM and 0.837 plus or minus 0.008 in w0waCDM. The w0waCDM model shows no significant improvement over Lambda-CDM when shear and CMB lensing are combined (Bayes factor 0.07) but reaches 2.6 sigma suspiciousness tension once all probes are included.
What carries the argument
KiDS-Legacy cosmic shear power spectrum combined with CMB temperature and polarization, CMB lensing, galaxy redshift-space distortions, and baryon acoustic oscillations to constrain extended parameter spaces.
If this is right
- Cosmic shear and CMB lensing together yield no strong evidence favoring w0waCDM over Lambda-CDM.
- Full multi-probe combination produces a 2.6 sigma suspiciousness tension only in the w0waCDM extension.
- The S8 constraint remains robust when the model space is opened beyond flat Lambda-CDM.
- Neutrino mass sum is limited to c squared times sum m_nu less than or equal to 1.5 eV at one sigma.
Where Pith is reading between the lines
- The stability of S8 across models suggests KiDS data are unlikely to be the sole driver of any existing S8 discrepancy with other probes.
- Continued consistency would imply that next-generation surveys can tighten neutrino and dark-energy bounds without encountering new tensions.
- The multi-probe combination approach can be used to test whether mild tensions in extended models grow or disappear with larger datasets.
Load-bearing premise
KiDS-Legacy cosmic shear measurements contain no significant unmodeled systematics that would bias their direct combination with CMB data.
What would settle it
A tension exceeding 3 sigma or a Bayes factor much larger than 1 between KiDS-Legacy shear and Planck CMB specifically in the w0waCDM parameter space would falsify the reported consistency.
Figures
read the original abstract
We constrained minimally extended cosmological models with the cosmic shear analysis of the final data release from the Kilo-Degree Survey (KiDS-Legacy) in combination with external probes. Due to the consistency of the KiDS-Legacy analysis with the cosmic microwave background (CMB), we could combine these datasets reliably for the first time. Additionally, we used CMB lensing, galaxy redshift-space distortions, and baryon acoustic oscillations. We assessed, in turn, the effects of spatial curvature, varying neutrino masses, and an evolving dark energy component on cosmological constraints from KiDS-Legacy alone and from KiDS-Legacy combined with external probes. We find KiDS-Legacy to be consistent with the fiducial flat $\Lambda$-cold dark matter ($\Lambda$CDM) analysis with $c^2 \sum m_\nu\leq 1.5\,$eV, $w_0 = -1.0\pm 0.7$, and $w_a = -1.3^{+1.9}_{-2.0}$ while $\Omega_K = 0.08^{+0.16}_{-0.17}$ (1$\sigma$ bounds) with an almost equal goodness of fit. The $w_0w_a$CDM model is not a significant improvement over $\Lambda$CDM when cosmic shear and CMB lensing are combined, yielding a Bayes factor $B = 0.07$. If all probes are combined, however, $B$ increases to 2.73, corresponding to a $2.6\sigma$ suspiciousness tension. The constraint on $S_8 = \sigma_8\sqrt{\Omega_\mathrm{m}/0.3}$ is robust to opening up the parameter space for cosmic shear. Adding all external datasets to KiDS-Legacy, we find $S_8 = 0.816 \pm 0.006$ in $\Lambda$CDM and $S_8 = 0.837 \pm 0.008$ in $w_0 w_a$CDM for all probes combined.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript presents cosmological parameter constraints from the final KiDS-Legacy cosmic shear dataset combined with CMB, CMB lensing, BAO, and RSD probes. It reports consistency with flat ΛCDM in minimally extended models (spatial curvature, massive neutrinos, w0-wa dark energy), with 1σ bounds Ω_K = 0.08^{+0.16}_{-0.17}, c²∑m_ν ≤ 1.5 eV, w0 = -1.0 ± 0.7, wa = -1.3^{+1.9}_{-2.0}, robust S8 values (0.816 ± 0.006 in ΛCDM; 0.837 ± 0.008 in w0waCDM), and Bayes factors showing no strong preference for w0waCDM (B=0.07 for shear+lensing) but B=2.73 (2.6σ suspiciousness) for the full combination.
Significance. If the central consistency claim holds, the work supplies updated, multi-probe constraints on curvature, neutrino mass, and dynamical dark energy from the completed KiDS survey, with explicit Bayes-factor model comparison and demonstration that S8 remains stable when the parameter space is opened. The reported near-equal goodness-of-fit in the base model and the tension metric in extensions provide concrete, falsifiable outputs for the community.
major comments (1)
- [Abstract] Abstract: The assertion that KiDS-Legacy is 'consistent with the fiducial flat ΛCDM analysis' and can therefore be 'combined reliably for the first time' is load-bearing for all joint constraints, yet the same data combination yields B=2.73 and 2.6σ suspiciousness once w0 and wa are freed. The manuscript must demonstrate that this tension is not produced by residual shear-calibration, photo-z, or IA systematics that are absorbed into the extra parameters; without such a test the reliability of the extended-model posteriors cannot be assessed.
minor comments (2)
- [Abstract] Abstract: The neutrino-mass bound is written 'c² ∑ m_ν ≤ 1.5 eV'; the manuscript should state explicitly whether this is the 95 % upper limit, the precise prior range, and whether c² is included for dimensional consistency or is a notational convention.
- [Abstract] Abstract: The S8 values are quoted to three decimal places (0.816 ± 0.006); the text should indicate whether this precision is limited by statistical or systematic uncertainty and whether the error bars include the full covariance with external probes.
Simulated Author's Rebuttal
We thank the referee for their careful and constructive review. The major comment raises an important point about the robustness of our consistency claims and the reliability of the extended-model constraints. We address it directly below and will revise the manuscript accordingly.
read point-by-point responses
-
Referee: [Abstract] Abstract: The assertion that KiDS-Legacy is 'consistent with the fiducial flat ΛCDM analysis' and can therefore be 'combined reliably for the first time' is load-bearing for all joint constraints, yet the same data combination yields B=2.73 and 2.6σ suspiciousness once w0 and wa are freed. The manuscript must demonstrate that this tension is not produced by residual shear-calibration, photo-z, or IA systematics that are absorbed into the extra parameters; without such a test the reliability of the extended-model posteriors cannot be assessed.
Authors: We agree that the mild tension (B=2.73, 2.6σ suspiciousness) in the w0waCDM extension requires explicit checks that it is not an artifact of unaccounted systematics being absorbed by the extra parameters. The base-model consistency (equal goodness-of-fit and stable S8) underpins our claim that the datasets can be combined, but we acknowledge the referee's request for a targeted test in the extended space. In the revised manuscript we will add a new subsection (in Section 5 or 6) that (i) re-runs the full combination with shear-calibration and photo-z nuisance parameters fixed to their fiducial values and shows that the suspiciousness remains at ~2.5σ, (ii) reports the posterior on the IA amplitude in both ΛCDM and w0waCDM (demonstrating it does not shift to compensate for the tension), and (iii) quantifies the contribution of each external probe to the Bayes factor. These tests will be presented alongside the existing robustness checks already performed for the base model. We maintain that the 2.6σ level does not invalidate the combination but agree that the additional verification strengthens the paper. revision: yes
Circularity Check
No circularity: constraints from direct fits to independent datasets
full rationale
The paper reports standard Bayesian parameter inference on KiDS-Legacy cosmic shear combined with CMB, BAO, and RSD data. Reported bounds on Omega_K, sum m_nu, w0, and wa, along with Bayes factors and S8 values, are direct outputs of the likelihood evaluation on external observations. No equation or claim reduces a derived quantity to a fitted input by construction, no self-citation is invoked as a uniqueness theorem to force the modeling choice, and the consistency statement rests on explicit goodness-of-fit comparisons rather than any self-referential step. The analysis is therefore self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
free parameters (4)
- w0
- wa
- sum m_nu
- Omega_K
axioms (2)
- domain assumption General relativity and the standard model of particle physics describe the background cosmology
- domain assumption Cosmic shear measurements are free of significant unaccounted systematics when combined with CMB
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
We find KiDS-Legacy to be consistent with the fiducial flat ΛCDM analysis with c² Σmν ≤ 1.5 eV, w0 = −1.0±0.7, wa = −1.3+1.9−2.0 while ΩK = 0.08+0.16−0.17 (1σ bounds) with an almost equal goodness of fit.
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
The constraint on S8 = σ8 √(Ωm/0.3) is robust to opening up the parameter space for cosmic shear.
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- 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
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Forward citations
Cited by 2 Pith papers
-
Measuring neutrino mass and asymmetry through galaxy pairwise peculiar velocity
Galaxy pairwise peculiar velocities from Cosmicflows-4 yield M_ν = 0.24^{+0.34}_{-0.18} eV and η² = 2.14^{+0.30}_{-0.32} (7σ non-zero asymmetry) in the CMB framework, consistent with prior Planck results.
-
Evidence for deviation in gravitational light deflection from general relativity at cosmological scales with KiDS-Legacy and CMB lensing
KiDS-Legacy weak lensing plus CMB data yields a 3 sigma deviation in light deflection from GR in a Lambda CDM background, with the signal driven by large-scale CMB lensing amplitudes.
Reference graph
Works this paper leans on
-
[1]
, " * write output.state after.block = add.period write newline
ENTRY address archiveprefix author booktitle chapter edition editor howpublished institution eprint doi url journal key month note number organization pages publisher school series title type volume year adsurl label extra.label sort.label short.list INTEGERS output.state before.all mid.sentence after.sentence after.block FUNCTION init.state.consts #0 'be...
-
[2]
" write newline "" before.all 'output.state := FUNCTION n.dashify 't := "" t empty not t #1 #1 substring "-" = t #1 #2 substring "--" = not "--" * t #2 global.max substring 't := t #1 #1 substring "-" = "-" * t #2 global.max substring 't := while if t #1 #1 substring * t #2 global.max substring 't := if while FUNCTION word.in bbl.in " " * FUNCTION format....
-
[3]
N., Arnold , K., Austermann , J., et al
Abazajian , K. N., Arnold , K., Austermann , J., et al. 2015, http://dx.doi.org/10.1016/j.astropartphys.2014.05.014 black Astropart. Phys. , 63, 66 https://ui.adsabs.harvard.edu/abs/2015APh....63...66A
-
[4]
2025, Journal of Cosmology and Astroparticle Physics, 2025, 021, doi: 10.1088/1475-7516/2025/02/021
Adame , A. G., Aguilar , J., Ahlen , S., et al. 2025, http://dx.doi.org/10.1088/1475-7516/2025/02/021 black , 2025, 021 https://ui.adsabs.harvard.edu/abs/2025JCAP...02..021A
-
[6]
2021, PhRvD, 103, 083533, doi: 10.1103/PhysRevD.103.083533
Alam , S., Aubert , M., Avila , S., et al. 2021 b , http://dx.doi.org/10.1103/PhysRevD.103.083533 black , 103, 083533 https://ui.adsabs.harvard.edu/abs/2021PhRvD.103h3533A
-
[7]
Amon , A., Gruen , D., Troxel , M. A., et al. 2022, http://dx.doi.org/10.1103/PhysRevD.105.023514 black , 105, 023514 https://ui.adsabs.harvard.edu/abs/2022PhRvD.105b3514A
-
[8]
KiDS-1000 Cosmology: Cosmic shear constraints and comparison between two point statistics.Astron
Asgari , M., Lin , C.-A., Joachimi , B., et al. 2021, http://dx.doi.org/10.1051/0004-6361/202039070 black , 645, A104 https://ui.adsabs.harvard.edu/abs/2021A&A...645A.104A
-
[9]
Asgari , M., Schneider , P., & Simon , P. 2012, http://dx.doi.org/10.1051/0004-6361/201218828 black , 542, A122 https://ui.adsabs.harvard.edu/abs/2012A&A...542A.122A
-
[10]
Bacon , D. J., Refregier , A. R., & Ellis , R. S. 2000, http://dx.doi.org/10.1046/j.1365-8711.2000.03851.x black , 318, 625 https://ui.adsabs.harvard.edu/abs/2000MNRAS.318..625B
-
[11]
candl: cosmic microwave background analysis with a differentiable likelihood
Balkenhol , L., Trendafilova , C., Benabed , K., & Galli , S. 2024, http://dx.doi.org/10.1051/0004-6361/202449432 black , 686, A10 https://ui.adsabs.harvard.edu/abs/2024A&A...686A..10B
-
[12]
E., Paviot , R., Vargas Maga \ n a , M., et al
Bautista , J. E., Paviot , R., Vargas Maga \ n a , M., et al. 2021, http://dx.doi.org/10.1093/mnras/staa2800 black , 500, 736 https://ui.adsabs.harvard.edu/abs/2021MNRAS.500..736B
-
[13]
Bayat , Z. & Hertzberg , M. P. 2025, http://dx.doi.org/10.1088/1475-7516/2025/08/065 black , 2025, 065 https://ui.adsabs.harvard.edu/abs/2025JCAP...08..065B
-
[14]
Ben \' tez , N. 2000, http://dx.doi.org/10.1086/308947 black , 536, 571 http://adsabs.harvard.edu/abs/2000ApJ...536..571B
-
[15]
Bigwood , L., Amon , A., Schneider , A., et al. 2024, http://dx.doi.org/10.1093/mnras/stae2100 black , 534, 655 https://ui.adsabs.harvard.edu/abs/2024MNRAS.534..655B
-
[16]
2022, title The Pantheon+ Analysis: Cosmological Constraints , , 938, 110, 10.3847/1538-4357/ac8e04
Brout , D., Scolnic , D., Popovic , B., et al. 2022, http://dx.doi.org/10.3847/1538-4357/ac8e04 black , 938, 110 https://ui.adsabs.harvard.edu/abs/2022ApJ...938..110B
-
[17]
C., Simon , P., Porth , L., et al
Broxterman , J. C., Simon , P., Porth , L., et al. 2025, https://ui.adsabs.harvard.edu/abs/2025arXiv250908365B http://dx.doi.org/10.48550/arXiv.2509.08365 black arXiv e-prints , arXiv:2509.08365
-
[18]
The Atacama Cosmology Telescope: DR6 Constraints on Extended Cosmological Models
Calabrese , E., Hill , J. C., Jense , H. T., et al. 2025, https://ui.adsabs.harvard.edu/abs/2025arXiv250314454C http://dx.doi.org/10.48550/arXiv.2503.14454 black arXiv e-prints , arXiv:2503.14454
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.2503.14454 2025
-
[19]
Caldwell , R. R. & Linder , E. V. 2025, https://ui.adsabs.harvard.edu/abs/2025arXiv251107526C http://dx.doi.org/10.48550/arXiv.2511.07526 black arXiv e-prints , arXiv:2511.07526
-
[20]
Camphuis , E., Quan , W., Balkenhol , L., et al. 2025, https://ui.adsabs.harvard.edu/abs/2025arXiv250620707C http://dx.doi.org/10.48550/arXiv.2506.20707 black arXiv e-prints , arXiv:2506.20707
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.2506.20707 2025
-
[21]
Carron , J., Mirmelstein , M., & Lewis , A. 2022, http://dx.doi.org/10.1088/1475-7516/2022/09/039 black , 2022, 039 https://ui.adsabs.harvard.edu/abs/2022JCAP...09..039C
-
[22]
2022, Target Selection and Validation of DESI Quasars, doi: 10.3847/1538-4357/acb3c2
Chaussidon , E., Y \`e che , C., Palanque-Delabrouille , N., et al. 2023, http://dx.doi.org/10.3847/1538-4357/acb3c2 black , 944, 107 https://ui.adsabs.harvard.edu/abs/2023ApJ...944..107C
-
[23]
Chevallier , M. & Polarski , D. 2001, http://dx.doi.org/10.1142/S0218271801000822 black Int. J. Mod. Phys. D , 10, 213 https://ui.adsabs.harvard.edu/abs/2001IJMPD..10..213C
-
[24]
Choudhury , S. R. & Hannestad , S. 2020, http://dx.doi.org/10.1088/1475-7516/2020/07/037 black , 2020, 037 https://ui.adsabs.harvard.edu/abs/2020JCAP...07..037C
-
[25]
Cort \^e s , M. & Liddle , A. R. 2024, http://dx.doi.org/10.1088/1475-7516/2024/12/007 black , 2024, 007 https://ui.adsabs.harvard.edu/abs/2024JCAP...12..007C
-
[26]
Dalal , R., Li , X., Nicola , A., et al. 2023, http://dx.doi.org/10.1103/PhysRevD.108.123519 black , 108, 123519 https://ui.adsabs.harvard.edu/abs/2023PhRvD.108l3519D
-
[27]
Dark Energy Survey and Kilo-Degree Survey Collaboration , Abbott , T. M. C., Aguena , M., et al. 2023, http://dx.doi.org/10.21105/astro.2305.17173 black OJA , 6, 36 https://ui.adsabs.harvard.edu/abs/2023OJAp....6E..36D
-
[28]
de Jong , J. T. A., Verdoes Kleijn , G. A., Kuijken , K. H., & Valentijn , E. A. 2013, http://dx.doi.org/10.1007/s10686-012-9306-1 black Experimental Astronomy , 35, 25 https://ui.adsabs.harvard.edu/abs/2013ExA....35...25D
-
[29]
de Mattia , A., Ruhlmann-Kleider , V., Raichoor , A., et al. 2021, http://dx.doi.org/10.1093/mnras/staa3891 black , 501, 5616 https://ui.adsabs.harvard.edu/abs/2021MNRAS.501.5616D
-
[30]
de Salas , P. F., Forero , D. V., Gariazzo , S., et al. 2021, http://dx.doi.org/10.1007/JHEP02(2021)071 black JHEP , 2021, 71 https://ui.adsabs.harvard.edu/abs/2021JHEP...02..071D
-
[31]
DESI Collaboration , Abdul-Karim , M., Aguilar , J., et al. 2025, http://dx.doi.org/10.1103/tr6y-kpc6 black , 112, 083515 https://ui.adsabs.harvard.edu/abs/2025PhRvD.112h3515A
-
[32]
Di Valentino , E., Said , J. L., Riess , A., et al. 2025, http://dx.doi.org/10.1016/j.dark.2025.101965 black Physics of the Dark Universe , 49, 101965 https://ui.adsabs.harvard.edu/abs/2025PDU....4901965D
-
[33]
du Mas des Bourboux , H., Rich , J., Font-Ribera , A., et al. 2020, http://dx.doi.org/10.3847/1538-4357/abb085 black , 901, 153 https://ui.adsabs.harvard.edu/abs/2020ApJ...901..153D
-
[34]
2013, The Messenger, 154, 32 https://ui.adsabs.harvard.edu/abs/2013Msngr.154...32E
Edge , A., Sutherland , W., Kuijken , K., et al. 2013, The Messenger, 154, 32 https://ui.adsabs.harvard.edu/abs/2013Msngr.154...32E
work page 2013
-
[35]
Efstathiou , G. 2025, http://dx.doi.org/10.1093/mnras/staf906 black , 540, 2844 https://ui.adsabs.harvard.edu/abs/2025MNRAS.540.2844E
-
[36]
NuFit-6.0: updated global analysis of three- flavor neutrino oscillations
Esteban , I., Gonzalez-Garcia , M. C., Maltoni , M., et al. 2024, http://dx.doi.org/10.1007/JHEP12(2024)216 black Journal of High Energy Physics , 2024, 216 https://ui.adsabs.harvard.edu/abs/2024JHEP...12..216E
-
[37]
The fate of hints: updated global analysis of three-flavor neutrino oscillations,
Esteban , I., Gonzalez-Garcia , M. C., Maltoni , M., Schwetz , T., & Zhou , A. 2020, http://dx.doi.org/10.1007/JHEP09(2020)178 black JHEP , 2020, 178 https://ui.adsabs.harvard.edu/abs/2020JHEP...09..178E
-
[38]
Euclid Collaboration , Archidiacono , M., Lesgourgues , J., et al. 2025, http://dx.doi.org/10.1051/0004-6361/202450859 black , 693, A58 https://ui.adsabs.harvard.edu/abs/2025A&A...693A..58E
-
[39]
Euclid Collaboration , Blanchard , A., Camera , S., et al. 2020, http://dx.doi.org/10.1051/0004-6361/202038071 black , 642, A191 https://ui.adsabs.harvard.edu/abs/2020A&A...642A.191E
-
[40]
Fenech Conti , I., Herbonnet , R., Hoekstra , H., et al. 2017, http://dx.doi.org/10.1093/mnras/stx200 black , 467, 1627 https://ui.adsabs.harvard.edu/abs/2017MNRAS.467.1627F
-
[41]
C., Dvornik , A., Hoekstra , H., et al
Fortuna , M. C., Dvornik , A., Hoekstra , H., et al. 2025, http://dx.doi.org/10.1051/0004-6361/202452347 black , 694, A322 https://ui.adsabs.harvard.edu/abs/2025A&A...694A.322C
-
[42]
Freedman , W. L., Madore , B. F., Hoyt , T. J., et al. 2025, http://dx.doi.org/10.3847/1538-4357/adce78 black , 985, 203 https://ui.adsabs.harvard.edu/abs/2025ApJ...985..203F
-
[43]
Ge , F., Millea , M., Camphuis , E., et al. 2025, http://dx.doi.org/10.1103/PhysRevD.111.083534 black , 111, 083534 https://ui.adsabs.harvard.edu/abs/2025PhRvD.111h3534G
-
[44]
Gerbino , M. & Lattanzi , M. 2017, http://dx.doi.org/10.3389/fphy.2017.00070 black Front. Phys. , 5, 70 https://ui.adsabs.harvard.edu/abs/2017FrP.....5...70G
-
[45]
Gil-Mar \' n , H., Bautista , J. E., Paviot , R., et al. 2020, http://dx.doi.org/10.1093/mnras/staa2455 black , 498, 2492 https://ui.adsabs.harvard.edu/abs/2020MNRAS.498.2492G
-
[46]
Hahn , C., Wilson , M. J., Ruiz-Macias , O., et al. 2023, http://dx.doi.org/10.3847/1538-3881/accff8 black , 165, 253 https://ui.adsabs.harvard.edu/abs/2023AJ....165..253H
-
[47]
Handley , W. & Lemos , P. 2019, http://dx.doi.org/10.1103/PhysRevD.100.023512 black , 100, 023512 https://ui.adsabs.harvard.edu/abs/2019PhRvD.100b3512H
-
[48]
Harris , C. R., Millman , K. J., van der Walt , S. J., et al. 2020, http://dx.doi.org/10.1038/s41586-020-2649-2 black , 585, 357 https://ui.adsabs.harvard.edu/abs/2020Natur.585..357H
-
[49]
Herold , L. & Karwal , T. 2025, https://ui.adsabs.harvard.edu/abs/2025arXiv250612004H http://dx.doi.org/10.48550/arXiv.2506.12004 black arXiv e-prints , arXiv:2506.12004
-
[51]
Hou , J., S \'a nchez , A. G., Ross , A. J., et al. 2021 b , http://dx.doi.org/10.1093/mnras/staa3234 black , 500, 1201 https://ui.adsabs.harvard.edu/abs/2021MNRAS.500.1201H
-
[52]
2015, MNRAS, 449, 848, doi: 10.1093/mnras/stu2693
Howlett , C., Ross , A. J., Samushia , L., Percival , W. J., & Manera , M. 2015, http://dx.doi.org/10.1093/mnras/stu2693 black , 449, 848 https://ui.adsabs.harvard.edu/abs/2015MNRAS.449..848H
-
[53]
Hunter, J. D. 2007, http://dx.doi.org/10.1109/MCSE.2007.55 black Computing in Science & Engineering , 9, 90
-
[54]
M., Simonovi \'c , M., & Zaldarriaga , M
Ivanov , M. M., Simonovi \'c , M., & Zaldarriaga , M. 2020, http://dx.doi.org/10.1103/PhysRevD.101.083504 black , 101, 083504 https://ui.adsabs.harvard.edu/abs/2020PhRvD.101h3504I
-
[55]
Kaiser , N., Wilson , G., & Luppino , G. A. 2000, arXiv e-prints, astro https://ui.adsabs.harvard.edu/abs/2000astro.ph..3338K
work page 2000
-
[56]
Kamionkowski , M. & Riess , A. G. 2023, http://dx.doi.org/10.1146/annurev-nucl-111422-024107 black Ann. Rev. Nucl. Part. Sci. , 73, 153 https://ui.adsabs.harvard.edu/abs/2023ARNPS..73..153K
-
[57]
KATRIN Collaboration , Aker , M., Batzler , D., et al. 2025, http://dx.doi.org/10.1126/science.adq9592 black Science , 388, 180 https://ui.adsabs.harvard.edu/abs/2025Sci...388..180K
-
[58]
2025, arXiv e-prints, arXiv:2507.07991 https://ui.adsabs.harvard.edu/abs/2025arXiv250707991K
Kova c , M., Nicola , A., Bucko , J., et al. 2025, arXiv e-prints, arXiv:2507.07991 https://ui.adsabs.harvard.edu/abs/2025arXiv250707991K
-
[59]
Lange , J. U. 2023, http://dx.doi.org/10.1093/mnras/stad2441 black , 525, 3181 https://ui.adsabs.harvard.edu/abs/2023MNRAS.525.3181L
-
[60]
doi:10.1016/j.physrep.2006.04.001 , eprint =
Lesgourgues , J. & Pastor , S. 2006, http://dx.doi.org/10.1016/j.physrep.2006.04.001 black , 429, 307 https://ui.adsabs.harvard.edu/abs/2006PhR...429..307L
-
[61]
GetDist: a Python package for analysing Monte Carlo samples.JCAP, 08:025, 2025
Lewis , A. 2025, http://dx.doi.org/10.1088/1475-7516/2025/08/025 black , 2025, 025 https://ui.adsabs.harvard.edu/abs/2025JCAP...08..025L
-
[62]
The Astrophysical Journal , year = 2000, month = aug, volume = 538, number = 2, pages =
Lewis , A., Challinor , A., & Lasenby , A. 2000, http://dx.doi.org/10.1086/309179 black , 538, 473 https://ui.adsabs.harvard.edu/abs/2000ApJ...538..473L
-
[63]
Lewis , A. & Chamberlain , E. 2025, http://dx.doi.org/10.1088/1475-7516/2025/05/065 black , 2025, 065 https://ui.adsabs.harvard.edu/abs/2025JCAP...05..065L
-
[64]
Li , S.-S., Hoekstra , H., Kuijken , K., et al. 2023 a , http://dx.doi.org/10.1051/0004-6361/202347236 black , 679, A133 https://ui.adsabs.harvard.edu/abs/2023A&A...679A.133L
-
[65]
Li , S.-S., Kuijken , K., Hoekstra , H., et al. 2023 b , http://dx.doi.org/10.1051/0004-6361/202245210 black , 670, A100 https://ui.adsabs.harvard.edu/abs/2023A&A...670A.100L
-
[66]
Li , X., Zhang , T., Sugiyama , S., et al. 2023 c , http://dx.doi.org/10.1103/PhysRevD.108.123518 black , 108, 123518 https://ui.adsabs.harvard.edu/abs/2023PhRvD.108l3518L
-
[67]
Linder , E. V. 2003, http://dx.doi.org/10.1103/PhysRevLett.90.091301 black , 90, 091301 https://ui.adsabs.harvard.edu/abs/2003PhRvL..90i1301L
-
[68]
Louis , T., La Posta , A., Atkins , Z., et al. 2025, http://dx.doi.org/10.1088/1475-7516/2025/11/062 black , 2025, 062 https://ui.adsabs.harvard.edu/abs/2025JCAP...11..062L
-
[69]
Loureiro , A., Cuceu , A., Abdalla , F. B., et al. 2019, http://dx.doi.org/10.1103/PhysRevLett.123.081301 black , 123, 081301 https://ui.adsabs.harvard.edu/abs/2019PhRvL.123h1301L
-
[70]
Madhavacheril , M. S., Qu , F. J., Sherwin , B. D., et al. 2024, http://dx.doi.org/10.3847/1538-4357/acff5f black , 962, 113 https://ui.adsabs.harvard.edu/abs/2024ApJ...962..113M
-
[71]
Mead , A. J., Brieden , S., Tr \"o ster , T., & Heymans , C. 2021, http://dx.doi.org/10.1093/mnras/stab082 black , 502, 1401 https://ui.adsabs.harvard.edu/abs/2021MNRAS.502.1401M
-
[72]
Miller , L., Heymans , C., Kitching , T. D., et al. 2013, http://dx.doi.org/10.1093/mnras/sts454 black , 429, 2858 https://ui.adsabs.harvard.edu/abs/2013MNRAS.429.2858M
-
[73]
TheAtacamaCosmologyTelescope: DR6 Maps
Naess , S., Guan , Y., Duivenvoorden , A. J., et al. 2025, https://ui.adsabs.harvard.edu/abs/2025arXiv250314451N http://dx.doi.org/10.48550/arXiv.2503.14451 black arXiv e-prints , arXiv:2503.14451
-
[74]
Neveux , R., Burtin , E., de Mattia , A., et al. 2020, http://dx.doi.org/10.1093/mnras/staa2780 black , 499, 210 https://ui.adsabs.harvard.edu/abs/2020MNRAS.499..210N
-
[75]
Omori , Y., Baxter , E. J., Chang , C., et al. 2023, http://dx.doi.org/10.1103/PhysRevD.107.023529 black , 107, 023529 https://ui.adsabs.harvard.edu/abs/2023PhRvD.107b3529O
-
[76]
Pan , Z., Bianchini , F., Wu , W. L. K., et al. 2023, http://dx.doi.org/10.1103/PhysRevD.108.122005 black , 108, 122005 https://ui.adsabs.harvard.edu/abs/2023PhRvD.108l2005P
-
[77]
Measurements of Omega and Lambda from 42 High-Redshift Supernovae
Perlmutter , S., Aldering , G., Goldhaber , G., et al. 1999, http://dx.doi.org/10.1086/307221 black , 517, 565 https://ui.adsabs.harvard.edu/abs/1999ApJ...517..565P
work page internal anchor Pith review doi:10.1086/307221 1999
-
[78]
2020, , 641, A6, 10.1051/0004-6361/201833910
Planck Collaboration , Aghanim , N., Akrami , Y., et al. 2020 a , http://dx.doi.org/10.1051/0004-6361/201833910 black , 641, A6 https://ui.adsabs.harvard.edu/abs/2020A&A...641A...6P
-
[79]
Planck Collaboration , Aghanim , N., Akrami , Y., et al. 2020 b , http://dx.doi.org/10.1051/0004-6361/201936386 black , 641, A5 https://ui.adsabs.harvard.edu/abs/2020A&A...641A...5P
-
[80]
Prince , H. & Dunkley , J. 2019, http://dx.doi.org/10.1103/PhysRevD.100.083502 black , 100, 083502 https://ui.adsabs.harvard.edu/abs/2019PhRvD.100h3502P
-
[81]
Qu , F. J., Ge , F., Kimmy Wu , W. L., et al. 2025, https://ui.adsabs.harvard.edu/abs/2025arXiv250420038Q http://dx.doi.org/10.48550/arXiv.2504.20038 black arXiv e-prints , arXiv:2504.20038
-
[82]
Qu , F. J., Sherwin , B. D., Madhavacheril , M. S., et al. 2024, http://dx.doi.org/10.3847/1538-4357/acfe06 black , 962, 112 https://ui.adsabs.harvard.edu/abs/2024ApJ...962..112Q
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.