REVIEW 3 major objections 5 minor 69 references
Nearest-neighbour distance maps turn halo catalogues into continuous images that, combined with kNN-CDF statistics in a hybrid neural network, recover Omega_m and sigma_8 from the Quijote suite with R^2 of 0.80 and 0.93 respectively.
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
T0 review · deepseek-v4-flash
2026-08-03 21:47 UTC pith:S3M6OSOL
load-bearing objection Useful new field-level representation and a sensible hybrid architecture, but the headline accuracy claims hinge on an unspecified train/test split and an overstatement of 'state-of-the-art'. the 3 major comments →
Learning Cosmology from Nearest Neighbour Statistics
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
A discrete catalogue of halo positions can be converted into a continuous field by assigning to every spatial point the distance to its k-th nearest halo, producing a set of 2D 'NN distance maps'. These maps preserve spatial information that the kNN-CDF summary statistics throw away, yet the maps alone are insufficient: a ResNet trained on them fails to constrain sigma_8. The central result is that a hybrid network combining the maps (via a ResNet-18 backbone) with the kNN-CDFs (via a fully connected network) performs best, achieving R^2 = 0.80 and 0.93 for Omega_m and sigma_8, respectively. This is the paper's main claim: that the joint use of nearest-neighbour distance maps and kNN-CDFs yi
What carries the argument
The key object is the nearest-neighbour distance map: for each pixel of a 2D slice through the simulation box, compute the distance to the 1st, 2nd, 3rd, or 4th nearest halo, producing a smooth image that encodes local clustering geometry (the 1NN map's critical points correspond to faces, edges, and nodes of the Voronoi tessellation of the halos). The second piece is the hybrid neural network architecture: a ResNet-18 processes the distance maps, its 512-dimensional feature vector is concatenated with the 200-bin (4 x 50) kNN-CDF vector, and an MLP regresses the posterior means and standard deviations of Omega_m and sigma_8. The maps carry spatial information; the CDFs carry global clusteri
Load-bearing premise
The reported accuracy figures assume the training, validation, and test sets are split simulation-by-simulation, so no map from a simulation used in training appears in the test set—but the paper only says 'We split the available input data into training (80%), validation (10%), and testing (10%)' and never states that the split is at the simulation level.
What would settle it
Retrain the hybrid Map+CDF model on the Quijote halo catalogues with a strict per-simulation split (e.g., leave out entire simulations for testing) and compare the test R^2 and relative errors to the paper's reported values. If the test R^2 for sigma_8 drops substantially below 0.93 or the relative error rises above 3%, the quoted metrics are inflated by data leakage. Alternatively, inspect the original split indices to check whether any test map shares a simulation ID with a training map.
If this is right
- If the reported accuracy holds, upcoming surveys like Euclid, DESI, and LSST can extract Omega_m and sigma_8 from dense halo catalogues using standard CNNs on distance maps, avoiding the memory and compute costs of point-cloud networks.
- The hybrid approach recovers sigma_8 (R^2 = 0.93) far better than either the maps alone (R^2 = 0.00) or the CDFs alone (R^2 = 0.59), indicating that the combination of local spatial fields and global statistics is a promising general recipe for likelihood-free inference.
- A proof-of-concept with dark matter particles instead of halos yields even tighter constraints (R^2 = 0.98 for sigma_8), suggesting the method benefits from more complete tracer samples and may be applicable to galaxy catalogs with higher number densities.
- The framework's 5–24x speedup over point-cloud/GNN baselines (about 2 hours on a single A100 GPU versus 2 days) could make field-level simulation-based inference tractable at survey scale.
Where Pith is reading between the lines
- The paper leaves implicit that the NN distance maps and kNN-CDFs are complementary views of the same underlying field—one local differential, the other global cumulative—and that this complementarity, rather than the specific architecture, is what drives the gain. A testable extension would be to feed the same two inputs into a simple concatenated MLP and check whether the improvement persists wit
- An editorial concern: the reported numbers are only trustworthy if the 80/10/10 train/validation/test split is done per simulation, so no halo field from a training simulation appears in the test set. The paper does not state this explicitly; a map-level split would leak correlated data and inflate all metrics, especially for sigma_8.
- The authors mention future work on including halo velocities and masses. A natural extension would be to concatenate scalar halo features (mass, velocity dispersion) as extra map channels, which could break the bias–sigma_8 degeneracy they suspect limits the maps-only model.
- The method's reliance on a fixed number of query points (10^4 per slice) and 10 random slices per simulation suggests a sensitivity to map resolution and slice selection; an ablation varying these would clarify how robust the constraints are.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper introduces "nearest-neighbour (NN) distance maps," a field-level representation of discrete halo catalogues in which each pixel stores the distance to the k-th nearest halo, and combines these maps with kNN-CDF summary statistics as inputs to a neural network. Using 2,000 Quijote Latin Hypercube simulations and 10^5 most massive halos per simulation, the authors train three models: a CDF-only fully connected network, a ResNet-18 map-only model, and a hybrid map+CDF model, to predict Omega_m and sigma_8. The hybrid model is reported as best: R^2 = 0.80 and 0.93 and relative errors 15.3% and 3.2% for Omega_m and sigma_8, respectively (Table 1, Fig. 4). The paper also compares against the two-point correlation function and several recent Quijote-based machine-learning methods, claiming state-of-the-art accuracy and 5-10x computational efficiency.
Significance. The NN distance map idea is a natural and potentially useful extension of kNN-CDFs: it converts sparse halo catalogues into dense, CNN-friendly fields while preserving spatial information, and it avoids the memory and compute costs of point-cloud/graph methods. The paper uses the public Quijote suite and makes direct comparisons to several existing methods, which is helpful for the community. The specific claims, however, rest on the integrity of the train/test split and on the stability of the reported metrics. If the split is indeed simulation-level and the results are reproducible across seeds, the hybrid framework is a valuable, computationally cheap alternative for parameter inference from halo catalogues. As written, the central quantitative claims are not yet fully supported.
major comments (3)
- [Section 3.3 and Section 2.1] The train/validation/test split is not specified as being performed at the simulation level. Section 2.1 generates 20,000 maps from 2,000 simulations, with 10 maps per simulation. If the split described in Section 3.3 is a random map-level split, maps from the same simulation and the same cosmology will appear in both training and test sets. Because the 10 slices of a simulation share the same halo field and large-scale modes, the network can memorize realization-specific features rather than learning the Omega_m-sigma_8 dependence, which would inflate every metric in Table 1 and Fig. 4. The authors must state explicitly whether the split is by simulation, and if not, re-run with a simulation-level split. Even with a simulation-level split, the 10 maps per simulation are highly correlated; the validation metrics should either be computed per simulation or the effective number of independ
- [Section 4, Table 1] The reported metrics are based on a single training run with no repeated-seed or bootstrap error bars. For Omega_m, the difference between CDF-only and Map+CDF is small (R^2 = 0.79 vs 0.80; MSE = 2.9e-3 vs 2.6e-3). Without multiple training runs, it is not possible to assess whether the hybrid improvement is significant. Similarly, the Map-only sigma_8 result (R^2 = 0.00) could be a seed-dependent pathology. Please provide mean and standard deviation over at least 5 random seeds, or otherwise demonstrate that the rankings in Table 1 are stable.
- [Section 5 and Abstract] The abstract's claim of 'state-of-the-art, if not the best, accuracy' is not supported by the paper's own comparison. In Section 5, Cuesta-Lazaro & Mishra-Sharma (2023) is quoted as achieving ~5% relative error on Omega_m, while the present hybrid model reports 15.3%. The comparisons also use different halo selections (10^5 halos here versus 5,000 or 8,192 in the cited works), which is not an apples-to-apples comparison. Either temper the claim to 'competitive accuracy' or provide a matched comparison under identical halo selections and training setups.
minor comments (5)
- [Section 2.1, step 4] The wording 'we randomly select 10 maps corresponding to each NN distance' is ambiguous. If each map is a 4-channel stack of 1NN-4NN distances from the same slice, the total of 20,000 maps is consistent with 2,000 simulations x 10 slices. Please clarify this in the text.
- [Figure 1 caption] The caption says the actual maps are 'produced with 10^2 random query points' in a 100x100 grid, but a 100x100 grid has 10^4 query points. Please correct this typo.
- [Section 3.4 and Table 1] The chi^2 values are interpreted as 'close to 1 indicates calibrated errors,' but some entries are far from 1 (e.g., CDF-only Omega_m chi^2 = 0.65; Appendix A Map-only Omega_m chi^2 = 2.89). The statement in Section 5 that 'our study does not suffer from any such issues' needs more support than a single chi^2 value; a calibration plot or coverage test would be appropriate.
- [Section 5] The paper says the method is '5-10 times more computationally efficient than some of the existing point-cloud-based ML methods,' but later quotes a 24x speedup relative to Chatterjee & Villaescusa-Navarro (2025). Please make the efficiency comparison consistent and specify which methods the 5-10x factor refers to.
- [Reproducibility] Please report the random seed(s) used for the slice selection, the train/validation/test split, and the neural network initialization. No code or data products are provided, so these details are important for reproducibility.
Circularity Check
No significant circularity: the reported constraints are empirical supervised-learning results on held-out Quijote data, not derivations that reduce to their inputs.
full rationale
The paper's central quantitative claims (hybrid Map+CDF gives R^2 = 0.80 and 0.93 and relative errors ~15% and ~3% for Omega_m and sigma_8) are obtained by training neural networks on Quijote halo catalogues and evaluating on a held-out split (Sec. 3.3, Table 1, Fig. 4). This is a direct empirical measurement of generalization performance, not a quantity that is equal to its inputs by construction. The new NN distance maps are introduced as input features, and no equation in the paper defines the inferred parameters in terms of the training labels or vice versa. The kNN-CDF formalism is cited from prior work by the same group (Banerjee & Abel 2021a,b), but the present results do not depend on those cited theorems being true: the CDFs are used as network inputs and the accuracy is measured, not derived from the citations. Self-citations appear as background motivation and method context, not as load-bearing justifications for the headline accuracy. One non-circularity concern is that Sec. 3.3 states only 'We split the available input data into training (80%), validation (10%), and testing (10%)' without specifying whether the split is per simulation; since Sec. 2.1 generates 20,000 maps from 2,000 simulations, a map-level split could cause leakage and inflate the metrics. This is a statistical validity issue rather than a circular step, and without evidence it cannot support a circularity finding. The comparison with prior work is also explicit and admits where other methods perform better (e.g., Cuesta-Lazaro & Mishra-Sharma's ~5% Omega_m error vs the present 15.3%). Overall, no derivation in the paper is equivalent to its own input by definition, so the circularity score is 0.
Axiom & Free-Parameter Ledger
free parameters (3)
- Neural network weights and hyperparameters (ResNet-18 backbone + inference MLP) =
Optimized via OPTUNA over >100 trials; final layer sizes/learning rates/weight decay not tabulated
- Map-generation choices (10 random 2D slices per simulation, 100x100 query grid, 10 Mpc/h slice spacing, k=1..4, 50 CDF b
- Halo sample selection (10^5 most massive halos per simulation)
axioms (6)
- standard math kNN-CDFs capture combinations of all N-point functions of the underlying clustering (Banerjee & Abel 2021b).
- domain assumption Quijote Latin Hypercube halo catalogs accurately encode the cosmological parameter dependence of halo clustering at z=0 within the quoted parameter ranges.
- domain assumption Ten 2D NN-distance slices per simulation retain sufficient 3D clustering information for inference.
- domain assumption The 10^5 most massive halos form a sufficient tracer sample; discarding lower-mass halos does not bias the learned Ωm-σ8 mapping.
- standard math The moment-matching loss (Eq. 4) yields calibrated posterior mean and standard deviation estimates (Jeffrey & Wandelt 2020).
- ad hoc to paper Random selection of 10 slices per simulation yields representative, non-redundant training samples.
read the original abstract
Extracting cosmological parameters from galaxy/halo catalogues with sub-percent level accuracy is an important aspect of modern cosmology, especially in view of ongoing and upcoming surveys such as Euclid, DESI, and LSST. While traditional two-point statistics have been known to be suboptimal for this task, recently proposed k-Nearest Neighbour (kNN) based summary statistics have demonstrated tighter constraining power. Building on the kNN statistics, we introduce a new field-level representation of discrete halo catalogues - NN distance maps. We employ this technique on the halo catalogues obtained from Quijote N-body simulation suites. By combining these maps with kNN-based summary statistics, we train a hybrid neural network to infer cosmological parameters, showing that the resulting constraints achieve state-of-the-art, if not the best, accuracy. In addition, our hybrid framework is 5-10 times more computationally efficient than some of the existing point-cloud-based ML methods.
Figures
Reference graph
Works this paper leans on
-
[1]
Abazajian, K., Abdulghafour, A., Addison, G. E., et al. 2022, arXiv e-prints, arXiv:2203.08024
Pith/arXiv arXiv 2022
-
[2]
2020, Phys
Ajani, V ., Peel, A., Pettorino, V ., et al. 2020, Phys. Rev. D, 102, 103531
2020
-
[3]
2019, in The 25th ACM SIGKDD International Conference on Knowledge Discovery & Data Mining, 2623–2631
Akiba, T., Sano, S., Yanase, T., Ohta, T., & Koyama, M. 2019, in The 25th ACM SIGKDD International Conference on Knowledge Discovery & Data Mining, 2623–2631
2019
-
[4]
2022, arXiv e-prints, arXiv:2211.12346
Anagnostidis, S., Thomsen, A., Kacprzak, T., et al. 2022, arXiv e-prints, arXiv:2211.12346
Pith/arXiv arXiv 2022
-
[5]
Anbajagane, D. et al. 2023, Mon. Not. Roy. Astron. Soc., 526, 5530
2023
-
[6]
F., Rocha, A
Azevedo, B. F., Rocha, A. M. A., & Pereira, A. I. 2024, Machine Learning, 113, 4055
2024
- [7]
-
[8]
& Abel, T
Banerjee, A. & Abel, T. 2022, Monthly Notices of the Royal Astronomical So- ciety, 519, 4856
2022
-
[9]
2022, Mon
Banerjee, A., Kokron, N., & Abel, T. 2022, Mon. Not. Roy. Astron. Soc., 511, 2765
2022
-
[10]
E., Villaescusa-Navarro, F., Massara, E., et al
Bayer, A. E., Villaescusa-Navarro, F., Massara, E., et al. 2021, Detecting neutrino mass by combining matter clustering, halos, and voids
2021
-
[11]
2014, arXiv e-prints, arXiv:1403.5237
Benitez, N., Dupke, R., Moles, M., et al. 2014, arXiv e-prints, arXiv:1403.5237
Pith/arXiv arXiv 2014
-
[12]
2025, Monthly Notices of the Royal Astronomical Society, 538, 2204
Chand, E., Banerjee, A., Foreman, S., & Villaescusa-Navarro, F. 2025, Monthly Notices of the Royal Astronomical Society, 538, 2204
2025
-
[13]
& Villaescusa-Navarro, F
Chatterjee, A. & Villaescusa-Navarro, F. 2025, ApJ, 985, 132
2025
-
[14]
Chen, X., Yang, Q., Wu, J., Li, H., & Tan, K. C. 2023, arXiv e-prints, arXiv:2305.16594
Pith/arXiv arXiv 2023
-
[15]
Colas, T., d’Amico, G., Senatore, L., Zhang, P., & Beutler, F. 2020, J. Cosmology Astropart. Phys., 2020, 001
2020
-
[16]
R., Abel, T., & Banerjee, A
Coulton, W. R., Abel, T., & Banerjee, A. 2024, Mon. Not. Roy. Astron. Soc., 534, 1621
2024
-
[17]
Cuesta-Lazaro, C. & Mishra-Sharma, S. 2023, arXiv e-prints, arXiv:2311.17141 d’Amico, G., Gleyzes, J., Kokron, N., et al. 2020, J. Cosmology Astropart. Phys., 2020, 005
Pith/arXiv arXiv 2023
-
[18]
J., et al
Dattilo, A., Vanderburg, A., Shallue, C. J., et al. 2019, AJ, 157, 169 de Santi, N. S. M., Shao, H., Villaescusa-Navarro, F., et al. 2023, ApJ, 952, 69
2019
-
[19]
Demiss, B. A. & Elsaigh, W. A. 2024, Engineering Research Express, 6, 032102 DESI Collaboration, Aghamousa, A., Aguilar, J., et al. 2016, arXiv e-prints, arXiv:1611.00036
Pith/arXiv arXiv 2024
-
[20]
2022, arXiv e-prints, arXiv:2204.07646 Euclid Collaboration: Castro, T., Fumagalli, A., Angulo, R
Eickenberg, M., Allys, E., Moradinezhad Dizgah, A., et al. 2022, arXiv e-prints, arXiv:2204.07646 Euclid Collaboration: Castro, T., Fumagalli, A., Angulo, R. E., et al. 2022, arXiv e-prints, arXiv:2208.02174
Pith/arXiv arXiv 2022
-
[21]
2019, Phys
Fluri, J., Kacprzak, T., Lucchi, A., et al. 2019, Phys. Rev. D, 100, 063514
2019
-
[22]
2020, MNRAS, 498, 464
Friedrich, O., Uhlemann, C., Villaescusa-Navarro, F., et al. 2020, MNRAS, 498, 464
2020
-
[23]
2025, arXiv e-prints, arXiv:2502.07713
Gangopadhyay, K., Banerjee, A., & Abel, T. 2025, arXiv e-prints, arXiv:2502.07713
arXiv 2025
-
[24]
2019, MNRAS, 484, 282
Gillet, N., Mesinger, A., Greig, B., Liu, A., & Ucci, G. 2019, MNRAS, 484, 282
2019
- [25]
-
[26]
2021, arXiv e-prints, arXiv:2104.03976
Gualdi, D., Gil-Marin, H., & Verde, L. 2021, arXiv e-prints, arXiv:2104.03976
Pith/arXiv arXiv 2021
-
[27]
2020, arXiv e-prints, arXiv:2009.02290
Gualdi, D., Novell, S., Gil-Marín, H., & Verde, L. 2020, arXiv e-prints, arXiv:2009.02290
Pith/arXiv arXiv 2020
-
[28]
Gupta, K. R. & Banerjee, A. 2024, Mon. Not. Roy. Astron. Soc., 531, 4619
2024
-
[29]
2020, Jour- nal of Cosmology and Astroparticle Physics, 2020, 040–040
Hahn, C., Villaescusa-Navarro, F., Castorina, E., & Scoccimarro, R. 2020, Jour- nal of Cosmology and Astroparticle Physics, 2020, 040–040
2020
-
[30]
S., Habaebi, M
Halbouni, A., Gunawan, T. S., Habaebi, M. H., et al. 2022, IEEE Access, 10, 99837 Harnois-Déraps, J., Martinet, N., Castro, T., et al. 2021, MNRAS, 506, 1623
2022
-
[31]
2022, ApJ, 937, 83
Hassan, S., Villaescusa-Navarro, F., Wandelt, B., et al. 2022, ApJ, 937, 83
2022
-
[32]
2016, in 2016 IEEE Conference on Com- puter Vision and Pattern Recognition (CVPR, 1
He, K., Zhang, X., Ren, S., & Sun, J. 2016, in 2016 IEEE Conference on Com- puter Vision and Pattern Recognition (CVPR, 1
2016
-
[33]
Ho, M., Bartlett, D. J., Chartier, N., et al. 2024, arXiv e-prints, arXiv:2402.05137
Pith/arXiv arXiv 2024
-
[34]
Hortua, H. J. 2021, arXiv e-prints, arXiv:2112.11865
Pith/arXiv arXiv 2021
-
[35]
2025, arXiv e-prints, arXiv:2507.03707 Ivezi´c, Ž., Kahn, S
Huang, N., Stiskalek, R., Lee, J.-Y ., et al. 2025, arXiv e-prints, arXiv:2507.03707 Ivezi´c, Ž., Kahn, S. M., Tyson, J. A., et al. 2019, ApJ, 873, 111
arXiv 2025
-
[36]
2020, arXiv e-prints, arXiv:2009.08459
Jeffrey, N., Alsing, J., & Lanusse, F. 2020, arXiv e-prints, arXiv:2009.08459
Pith/arXiv arXiv 2020
-
[37]
Jeffrey, N. & Wandelt, B. D. 2020, arXiv e-prints, arXiv:2011.05991
Pith/arXiv arXiv 2020
-
[38]
2006, IEEE Transactions on Visualiza- tion and Computer Graphics, 12, 581 Article number, page 7 A&A proofs:manuscript no
Jones, M., Baerentzen, J., & Sramek, M. 2006, IEEE Transactions on Visualiza- tion and Computer Graphics, 12, 581 Article number, page 7 A&A proofs:manuscript no. main
2006
-
[39]
Kingma, D. P. & Ba, J. 2014, CoRR, abs/1412.6980
Pith/arXiv arXiv 2014
-
[40]
Krause, E. et al. 2025, Astrophys. J., 990, 99
2025
-
[41]
Y ., Abrams, N., Andrews, J., et al
Lam, C. Y ., Abrams, N., Andrews, J., et al. 2023, arXiv e-prints, arXiv:2306.12514
Pith/arXiv arXiv 2023
-
[42]
2011, arXiv e-prints, arXiv:1110.3193
Laureijs, R., Amiaux, J., Arduini, S., et al. 2011, arXiv e-prints, arXiv:1110.3193
Pith/arXiv arXiv 2011
-
[43]
Lee, J.-Y . & Villaescusa-Navarro, F. 2025, arXiv e-prints, arXiv:2505.23904
Pith/arXiv arXiv 2025
-
[44]
2022, arXiv e-prints, arXiv:2204.02945 Lucas Makinen, T., Heavens, A., Porqueres, N., et al
Liu, W., Jiang, A., & Fang, W. 2022, arXiv e-prints, arXiv:2204.02945 Lucas Makinen, T., Heavens, A., Porqueres, N., et al. 2025, J. Cosmology As- tropart. Phys., 2025, 095
Pith/arXiv arXiv 2022
-
[45]
L., Charnock, T., Lemos, P., et al
Makinen, T. L., Charnock, T., Lemos, P., et al. 2022, The Open Journal of Astro- physics, 5, 18
2022
-
[46]
A., Liu, J., Zorrilla Matilla, J
Marques, G. A., Liu, J., Zorrilla Matilla, J. M., et al. 2019, J. Cosmology As- tropart. Phys., 2019, 019 Mobina Hosseini, S. & Soleimanpour Salmasi, B. 2025, arXiv e-prints, arXiv:2508.05842
Pith/arXiv arXiv 2019
-
[47]
2021, arXiv e-prints, arXiv:2111.12088
Naidoo, K., Massara, E., & Lahav, O. 2021, arXiv e-prints, arXiv:2111.12088
Pith/arXiv arXiv 2021
-
[48]
J., Yuan, S., & Garrison, L
Ntampaka, M., Eisenstein, D. J., Yuan, S., & Garrison, L. H. 2020, ApJ, 889, 151
2020
-
[49]
2019, PyTorch: An Imperative Style, High- Performance Deep Learning Library
Paszke, A., Gross, S., Massa, F., et al. 2019, PyTorch: An Imperative Style, High- Performance Deep Learning Library
2019
-
[50]
D., Laureijs, R., Stagnaro, L., et al
Racca, G. D., Laureijs, R., Stagnaro, L., et al. 2016, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, V ol. 9904, Space Tele- scopes and Instrumentation 2016: Optical, Infrared, and Millimeter Wave, ed. H. A. MacEwen, G. G. Fazio, M. Lystrup, N. Batalha, N. Siegler, & E. C. Tong, 99040O
2016
-
[51]
2017, arXiv e-prints, arXiv:1711.02033
Ravanbakhsh, S., Oliva, J., Fromenteau, S., et al. 2017, arXiv e-prints, arXiv:1711.02033
Pith/arXiv arXiv 2017
-
[52]
2023, arXiv e-prints, arXiv:2311.01588
Roncoli, A., ´Ciprijanovi´c, A., V oetberg, M., Villaescusa-Navarro, F., & Nord, B. 2023, arXiv e-prints, arXiv:2311.01588
Pith/arXiv arXiv 2023
-
[53]
2021, arXiv e-prints, arXiv:2102.01696
Samushia, L., Slepian, Z., & Villaescusa-Navarro, F. 2021, arXiv e-prints, arXiv:2102.01696
Pith/arXiv arXiv 2021
-
[54]
1996, Proc
Schmalzing, J., Kerscher, M., & Buchert, T. 1996, Proc. Int. Sch. Phys. Fermi, 132, 281
1996
-
[55]
2022, arXiv e-prints, arXiv:2209.06843
Shao, H., Villaescusa-Navarro, F., Villanueva-Domingo, P., et al. 2022, arXiv e-prints, arXiv:2209.06843
Pith/arXiv arXiv 2022
-
[56]
2019, in 2019 Asia-Pacific signal and information processing association annual summit and conference (AP- SIPA ASC), IEEE, 939–944
Shi, X., Wang, T., Wang, L., Liu, H., & Yan, N. 2019, in 2019 Asia-Pacific signal and information processing association annual summit and conference (AP- SIPA ASC), IEEE, 939–944
2019
-
[57]
Siraj, M. S. & Ahad, M. 2020, in 2020 Joint 9th International Conference on
2020
-
[58]
Informatics, Electronics & Vision (ICIEV) and 2020 4th International Con- ference on Imaging, Vision & Pattern Recognition (icIVPR), IEEE, 1–7
2020
-
[59]
2020, MNRAS, 495, 4006
Uhlemann, C., Friedrich, O., Villaescusa-Navarro, F., Banerjee, A., & Codis, S. 2020, MNRAS, 495, 4006
2020
-
[60]
Valogiannis, G. & Dvorkin, C. 2021, arXiv e-prints, arXiv:2108.07821
Pith/arXiv arXiv 2021
-
[61]
2022, ApJS, 259, 61
Villaescusa-Navarro, F., Genel, S., Anglés-Alcázar, D., et al. 2022, ApJS, 259, 61
2022
-
[62]
2020, The Astrophysical Journal Supplement Series, 250, 2
Villaescusa-Navarro, F., Hahn, C., Massara, E., et al. 2020, The Astrophysical Journal Supplement Series, 250, 2
2020
-
[63]
Villaescusa-Navarro, F. et al. 2022, Astrophys. J., 929, 132
2022
-
[64]
& Villaescusa-Navarro, F
Villanueva-Domingo, P. & Villaescusa-Navarro, F. 2022, ApJ, 937, 115
2022
-
[65]
2021, arXiv e-prints, arXiv:2111.14874
Villanueva-Domingo, P., Villaescusa-Navarro, F., Genel, S., et al. 2021, arXiv e-prints, arXiv:2111.14874
Pith/arXiv arXiv 2021
-
[66]
2022, Mon
Wang, Y ., Banerjee, A., & Abel, T. 2022, Mon. Not. Roy. Astron. Soc., 514, 3828
2022
-
[67]
2023, Monthly Notices of the Royal Astronom- ical Society, 522, 3935
Yuan, S., Zamora, A., & Abel, T. 2023, Monthly Notices of the Royal Astronom- ical Society, 522, 3935
2023
-
[68]
2022, Ieee Access, 10, 47361
Zeng, C., Ma, C., Wang, K., & Cui, Z. 2022, Ieee Access, 10, 47361
2022
-
[69]
2025, Astrophys
Zhou, Z., Cisewski-Kehe, J., Fang, K., & Banerjee, A. 2025, Astrophys. J., 979, 194 Article number, page 8 Atrideb Chatterjee et al.: Learning Cosmology from Nearest Neighbour Statistics 0.1 0.2 0.3 0.4 0.5 Truth 0.1 0.2 0.3 0.4 0.5Prediction CDF-Only m R2=0.79 =17.3% 2 = 0.65 MSE = 2.90e-03 0.6 0.7 0.8 0.9 1.0 Truth 0.6 0.7 0.8 0.9 1.0Prediction CDF-Only...
2025
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.