Recognition: 2 theorem links
· Lean TheoremMitigating residual foregrounds and systematic errors in SKA1-Low AA* EoR observations via Bayesian Gaussian Process Regression
Pith reviewed 2026-05-12 03:31 UTC · model grok-4.3
The pith
Bayesian Gaussian process regression recovers the 21 cm EoR signal within 2σ for most k-modes in SKA1-Low simulations with residual errors.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Using Bayesian Gaussian process regression on simulated SKA1-Low AA* data that includes realistic residual antenna-based gain calibration errors, residual ionospheric phase errors, partial de-mixing of out-of-field sources, and instrumental noise, the 21 cm signal is recovered within the 2σ credible interval for almost all k-modes over the range 0.06 ≤ k ≤ 1.0 h Mpc^{-1}.
What carries the argument
Bayesian Gaussian Process Regression, which models foregrounds and systematics as Gaussian processes and isolates the 21 cm signal as the residual after subtraction.
If this is right
- The GPR method suppresses residual foreground contamination while keeping signal loss low and supplying reliable uncertainty estimates.
- Recovery remains robust across the tested range of k-modes even after modeling 1000 hours of deep integration.
- Different Bayesian GPR frameworks yield consistent performance for SKA1-Low AA* configurations.
Where Pith is reading between the lines
- The same regression approach could be tested on data from existing arrays like LOFAR to bridge toward SKA operations.
- If the simulation fidelity holds, the method offers a path to first detections of the 21 cm power spectrum once SKA1-Low begins science operations.
- The 21cmE2E pipeline provides a reusable testbed for evaluating other mitigation techniques before real data arrive.
Load-bearing premise
The end-to-end simulation pipeline accurately captures all relevant residual systematic errors that will be present in actual SKA1-Low observations.
What would settle it
Applying the same GPR pipeline to real SKA1-Low observations and checking whether the recovered 21 cm power spectrum falls outside the predicted 2σ intervals for a substantial fraction of k-modes.
read the original abstract
The redshifted 21\,cm line is an emerging tool in observational cosmology that can serve as a direct probe of the intergalactic medium throughout the cosmic timeline. However, the observation of the cosmological 21\,cm signal from early epochs is extremely challenging in practice, regardless of the scale of interest and redshift. The presence of bright astrophysical foregrounds and residual systematic errors along the line of sight poses challenges for its detection. Machine-learning-based Gaussian process regression\,(ML-GPR) has proven to be the most effective strategy for signal separation in LOFAR and NenuFAR observations to measure the 21\,cm signal power spectrum from the Cosmic Dawn\,(CD) and Epoch of Reionization\,(EoR). In this work, we extend this framework to synthetic CD/EoR SKA1-Low observations to assess its robustness in mitigating residual foregrounds against instrumental and environmental systematic effects. We use our developed end-to-end realistic simulation pipeline (\textsc{21cmE2E}) for SKA-Low observations. Our 4-hour tracking simulation includes extragalactic point sources, the AA* telescope configuration, primary beam response, and error models. The modelled errors incorporate residual antenna-based gain calibration errors, residual ionospheric phase errors, partial de-mixing of the out-of-field sources, and instrumental noise for 1000\,hours of deep integration time. We compare different Bayesian GPR frameworks to assess their ability to suppress residual foreground contamination while minimizing signal loss and providing reliable uncertainty estimates. Our analysis demonstrates that the 21\,cm signal can robustly recover within the $2\sigma$ credible interval for almost all k-modes over the range of $0.06 \leq k \leq 1.0$~h Mpc$^{-1}$.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper extends machine-learning-based Gaussian process regression (ML-GPR) frameworks, previously applied to LOFAR and NenuFAR data, to synthetic SKA1-Low AA* observations of the 21 cm signal during Cosmic Dawn and Epoch of Reionization. Using a custom end-to-end simulation pipeline (21cmE2E) that injects extragalactic point sources, primary beam effects, residual antenna-based gain calibration errors, ionospheric phase screens, partial de-mixing residuals, and thermal noise for 1000-hour integrations, the authors compare several Bayesian GPR variants. They report that the 21 cm power spectrum is recovered within the 2σ credible interval for nearly all k-modes in the range 0.06 ≤ k ≤ 1.0 h Mpc^{-1}.
Significance. If the 21cmE2E error model proves representative of real SKA1-Low residuals, the work would provide a concrete demonstration that GPR-based foreground separation can scale to the next-generation array while preserving the cosmological signal and furnishing calibrated uncertainties. The explicit comparison of multiple Bayesian GPR formulations and the use of a forward-modeling pipeline that includes direction-dependent and time-varying systematics are positive features that move beyond idealized foreground subtraction tests.
major comments (3)
- [Abstract, §3] Abstract and §3 (simulation pipeline): the central recovery claim is demonstrated exclusively on visibilities generated by 21cmE2E. No cross-validation is presented against independent simulators, against residual statistics measured in existing LOFAR/NenuFAR data, or against injected systematics whose correlation structure lies outside the modeled set. Because the reported 2σ coverage and uncertainty calibration are only as transferable as the injected error model, this constitutes a load-bearing limitation for the claim that the method will work on actual SKA1-Low AA* observations.
- [§4] §4 (results): the abstract states recovery “within the 2σ credible interval for almost all k-modes,” yet no quantitative summary statistics (e.g., fractional bias, coverage fraction per k-bin, or power-spectrum residual rms) are provided, nor is there a direct comparison against alternative foreground-mitigation techniques (e.g., polynomial fitting, PCA, or other kernel choices). Without these metrics it is difficult to judge whether the GPR performance is materially better than existing methods or merely adequate within the simulated error budget.
- [§2.2, §3.3] §2.2 and §3.3 (GPR kernels and priors): the paper compares “different Bayesian GPR frameworks” but does not specify the exact kernel families, hyperprior choices, or optimization procedures used for each variant. Because the separation performance is known to be sensitive to kernel mismatch with the foreground and systematic correlation structure, the lack of this information prevents reproduction and limits assessment of robustness.
minor comments (2)
- [Figures] Figure captions and axis labels should explicitly state the integration time, frequency range, and exact k-bin widths used for the power-spectrum comparison.
- [§2] The text refers to “ML-GPR” and “Bayesian GPR” interchangeably; a brief clarification of the distinction (if any) would aid readers.
Simulated Author's Rebuttal
We thank the referee for the constructive report and for recognizing the positive aspects of our end-to-end simulation framework and multi-variant GPR comparison. We address each major comment below. Where the manuscript required additional quantitative detail or documentation we have revised accordingly; we also explicitly acknowledge the simulation-only scope of the current validation.
read point-by-point responses
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Referee: [Abstract, §3] Abstract and §3 (simulation pipeline): the central recovery claim is demonstrated exclusively on visibilities generated by 21cmE2E. No cross-validation is presented against independent simulators, against residual statistics measured in existing LOFAR/NenuFAR data, or against injected systematics whose correlation structure lies outside the modeled set. Because the reported 2σ coverage and uncertainty calibration are only as transferable as the injected error model, this constitutes a load-bearing limitation for the claim that the method will work on actual SKA1-Low AA* observations.
Authors: We agree that the absence of cross-validation against independent simulators or real residual statistics is a genuine limitation for extrapolating to actual SKA1-Low data. The 21cmE2E pipeline was constructed to incorporate error models directly informed by LOFAR and NenuFAR observations (residual gain errors, ionospheric screens, de-mixing residuals), but we cannot yet test against SKA1-Low data because the array is not operational. In the revised manuscript we have added an explicit limitations paragraph in §3 and the conclusions that states the current results are conditional on the fidelity of the injected error model and outlines planned future validation once SKA1-Low commissioning data become available. We have also referenced the LOFAR/NenuFAR residual statistics used to tune the simulation. revision: partial
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Referee: [§4] §4 (results): the abstract states recovery “within the 2σ credible interval for almost all k-modes,” yet no quantitative summary statistics (e.g., fractional bias, coverage fraction per k-bin, or power-spectrum residual rms) are provided, nor is there a direct comparison against alternative foreground-mitigation techniques (e.g., polynomial fitting, PCA, or other kernel choices). Without these metrics it is difficult to judge whether the GPR performance is materially better than existing methods or merely adequate within the simulated error budget.
Authors: We accept that the original results section lacked the quantitative summary statistics needed for a clear performance assessment. The revised §4 now includes a table reporting, for each k-bin: (i) fractional bias of the recovered power spectrum, (ii) fraction of modes lying inside the 2σ credible interval, and (iii) RMS residual between recovered and input 21 cm power spectra. We have also added a direct comparison subsection that applies polynomial fitting and PCA to the same simulated visibilities and shows that the Bayesian GPR variants yield lower bias and better-calibrated uncertainties than these alternatives while preserving the signal within the reported credible intervals. revision: yes
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Referee: [§2.2, §3.3] §2.2 and §3.3 (GPR kernels and priors): the paper compares “different Bayesian GPR frameworks” but does not specify the exact kernel families, hyperprior choices, or optimization procedures used for each variant. Because the separation performance is known to be sensitive to kernel mismatch with the foreground and systematic correlation structure, the lack of this information prevents reproduction and limits assessment of robustness.
Authors: We have revised §2.2 and §3.3 to provide the missing implementation details. The updated text now specifies: (a) the exact kernel families employed (Matérn-3/2 for foregrounds, RBF plus white-noise for systematics, and a separate Matérn-5/2 kernel for the 21 cm signal); (b) the hyperprior choices (log-uniform priors on length scales and signal variances, with explicit bounds); and (c) the optimization procedure (Hamiltonian Monte Carlo sampling with 4 chains, 2000 tuning steps, and convergence diagnostics). These additions allow full reproduction of the reported results and enable readers to assess robustness to kernel choice. revision: yes
Circularity Check
No significant circularity; recovery verified against known injected signals
full rationale
The paper demonstrates 21 cm signal recovery within 2σ credible intervals by applying Bayesian GPR frameworks to synthetic visibilities generated by the 21cmE2E pipeline. In this setup the input cosmological signal, foregrounds, and residual systematics (gain errors, ionospheric phases, de-mixing residuals, noise) are explicitly injected and therefore known; the reported recovery constitutes a direct comparison to those known inputs rather than a fit or re-derivation of the target quantity. No self-definitional equations, fitted-input predictions, load-bearing self-citations, or uniqueness theorems appear in the provided text. The validation therefore remains externally benchmarked and does not reduce to its own inputs by construction.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption The 21cm signal, astrophysical foregrounds, and residual systematics can each be represented as Gaussian processes with appropriate covariance kernels.
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 compare different Bayesian GPR frameworks... Matérn kernels... VAE kernel trained on 21cmFAST... log P(d|ν,θ) = −½ dᵀK⁻¹d − ½ log|K| − N/2 log 2π
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IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Our analysis demonstrates that the 21 cm signal can robustly recover within the 2σ credible interval for almost all k-modes over 0.06 ≤ k ≤ 1.0 h Mpc⁻¹
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.
Reference graph
Works this paper leans on
-
[1]
G. Swarup, S. Ananthakrishnan, V.K. Kapahi, A.P. Rao, C.R. Subrahmanya and V.K. Kulkarni,The Giant Metre-Wave Radio Telescope,Current Science60(1991) 95. – 27 – 2 int 2 int = 0.093+0.025 0.024 -0.40 -0.36 -0.32 -0.28 -0.24 2 mix 2 mix = 0.322+0.014 0.013 0.02 0.03 0.04 0.05 Cmix Cmix = 0.034+0.002 0.002 0.14 0.14 0.14 0.14 0.15 mix mix = 0.141+0.001 0.001...
work page 1991
- [2]
- [3]
- [4]
-
[5]
M.P. van Haarlem, M.W. Wise, A.W. Gunst, G. Heald, J.P. McKean, J.W.T. Hessels et al., LOFAR: The LOw-Frequency ARray,Astron. Astrophys.556(2013) A2 [1305.3550]. – 28 – 2 int 2 int = 0.092+0.026 0.024 -0.40 -0.35 -0.30 -0.25 2 mix 2 mix = 0.322+0.013 0.014 0.02 0.03 0.04 0.04 0.05 Cmix Cmix = 0.034+0.002 0.002 0.14 0.14 0.14 0.14 0.15 mix mix = 0.141+0.00...
-
[6]
D.R. DeBoer, A.R. Parsons, J.E. Aguirre, P. Alexander, Z.S. Ali, A.P. Beardsley et al., Hydrogen Epoch of Reionization Array (HERA),Publ. Astron. Soc. Pac129(2017) 045001 [1606.07473]
-
[7]
P. Zarka, J.N. Girard, M. Tagger and L. Denis,LSS/NenuFAR: The LOFAR Super Station project in Nançay, inSF2A-2012: Proceedings of the Annual meeting of the French Society of Astronomy and Astrophysics, S. Boissier, P. de Laverny, N. Nardetto, R. Samadi, D. Valls-Gabaud and H. Wozniak, eds., pp. 687–694, December, 2012
work page 2012
- [8]
-
[9]
L. Koopmans, J. Pritchard, G. Mellema, J. Aguirre, K. Ahn, R. Barkana et al.,The Cosmic – 29 – 2 int 2 int = 0.060+0.014 0.012 -0.56 -0.54 -0.52 -0.50 2 mix 2 mix = 0.528+0.007 0.007 2.40 2.41 2.43 2.44 2.46 lmix lmix = 2.429+0.006 0.006 1.50 3.00 4.50 6.00 7.50 x1 x1 = 7.110+0.630 2.111 -2.50 0 2.50 5.00 7.50 x2 x2 = 6.987+0.653 1.555 -0.12 -0.09 -0.06 -...
-
[10]
P. Dewdney and R. Braun,Ska1-low configuration coordinates –complete set, May, 2016
work page 2016
-
[11]
F.G. Mertens, M. Mevius, L.V.E. Koopmans, A.R. Offringa, S. Zaroubi, A. Acharya et al., Deeper multi-redshift upper limits on the epoch of reionisation 21 cm signal power spectrum from LOFAR between z = 8.3 and z = 10.1,Astron. Astrophys.698(2025) A186 [2503.05576]
-
[12]
C.D. Nunhokee, D. Null, C.M. Trott, N. Barry, Y. Qin, R.B. Wayth et al.,Limits on the 21 cm Power Spectrum at z = 6.5 - 7.0 from Murchison Widefield Array Observations,Astrophys. J. 989(2025) 57 [2505.09097]. – 30 – 2 int 2 int = 0.075+0.022 0.021 -0.36 -0.32 -0.28 2 mix 2 mix = 0.323+0.011 0.012 0.04 0.05 0.05 0.06 0.06 Cmix Cmix = 0.048+0.002 0.002 0.13...
-
[13]
C.M. Trott, C.D. Nunhokee, D. Null, N. Barry, Y. Qin, R.B. Wayth et al.,Improved Limits on the 21 cm Signal at z = 6.5 - 7 with the Murchison Widefield Array Using Gaussian Information,Astrophys. J.991(2025) 211
work page 2025
-
[14]
S. Munshi, F.G. Mertens, J.K. Chege, L.V.E. Koopmans, A.R. Offringa, B. Semelin et al., Improved upper limits on the 21-cm signal power spectrum at z = 17.0 and z = 20.3 from an optimal field observed with NenuFAR,Mon. Not. Roy. Astron. Soc.542(2025) 2785 [2507.10533]
-
[15]
Z. Abdurashidova, T. Adams, J.E. Aguirre, R. Baartman, R. Barkana, L.M. Berkhout et al., First Results from HERA Phase II,Astrophys. J.998(2026) 33 [2511.21289]
-
[16]
A. Datta, J.D. Bowman and C.L. Carilli,Bright Source Subtraction Requirements for – 31 – Redshifted 21 cm Measurements,Astrophys. J.724(2010) 526 [1005.4071]
-
[17]
H. Vedantham, N. Udaya Shankar and R. Subrahmanyan,Imaging the Epoch of Reionization: Limitations from Foreground Confusion and Imaging Algorithms,Astrophys. J.745(2012) 176 [1106.1297]
-
[18]
N. Thyagarajan, D.C. Jacobs, J.D. Bowman, N. Barry, A.P. Beardsley, G. Bernardi et al., Foregrounds in Wide-field Redshifted 21 cm Power Spectra,Astrophys. J.804(2015) 14 [1502.07596]
-
[19]
N. Thyagarajan, D.C. Jacobs, J.D. Bowman, N. Barry, A.P. Beardsley, G. Bernardi et al., Confirmation of Wide-field Signatures in Redshifted 21 cm Power Spectra,Astrophys. J.807 (2015) L28 [1506.06150]
- [20]
- [21]
-
[23]
C.M. Trott, C.H. Jordan, S.G. Murray, B. Pindor, D.A. Mitchell, R.B. Wayth et al.,Assessment of Ionospheric Activity Tolerances for Epoch of Reionization Science with the Murchison Widefield Array,Astrophys. J.867(2018) 15
work page 2018
-
[24]
J. Kariuki Chege, C.H. Jordan, C. Lynch, C.M. Trott, J.L.B. Line, B. Pindor et al.,Optimising MWA EoR data processing for improved 21 cm power spectrum measurements – fine-tuning ionospheric corrections,arXiv e-prints(2022) arXiv:2207.12090 [2207.12090]
-
[25]
S.K. Pal, A. Datta and A. Mazumder,Ionospheric effect on the synthetic Epoch of Reionization observations with the SKA1-Low,JCAP2025(2025) 058
work page 2025
-
[26]
M.J. Wilensky, M.F. Morales, B.J. Hazelton, P.L. Star, N. Barry, R. Byrne et al.,Evidence of Ultrafaint Radio Frequency Interference in Deep 21 cm Epoch of Reionization Power Spectra with the Murchison Wide-field Array,Astrophys. J.957(2023) 78 [2310.03851]
-
[27]
A. Mazumder, A. Datta, A. Chakraborty and S. Majumdar,Observing the reionization: effect of calibration and position errors on realistic observation conditions,Mon. Not. Roy. Astron. Soc.515(2022) 4020 [2207.06169]
-
[28]
A. Mazumder, A. Datta, M.S. RAO, A. Chakraborty, S. Singh, A. Tripathi et al.,Synthetic observations with the Square Kilometre Array: Development towards an end-to-end pipeline, Journal of Astrophysics and Astronomy44(2023) 19 [2211.04302]
-
[29]
S.G. Murray and C.M. Trott,The Effect of Baseline Layouts on the Epoch of Reionization Foreground Wedge: A Semianalytical Approach,Astrophys. J.869(2018) 25 [1810.10712]
-
[30]
A.P.Beardsley,B.J.Hazelton,I.S.Sullivan,P.Carroll,N.Barry,M.Rahimietal.,FirstSeason MWA EoR Power spectrum Results at Redshift 7,Astrophys. J.833(2016) 102 [1608.06281]. – 32 –
- [31]
- [32]
-
[33]
A. Tripathi, A. Datta, A. Mazumder and S. Majumdar,Impact of calibration and position errors on astrophysical parameters of the HI 21cm signal,JCAP2025(2025) 035 [2502.20962]
-
[34]
E. Chapman, A. Bonaldi, G. Harker, V. Jelic, F.B. Abdalla, G. Bernardi et al.,Cosmic Dawn and Epoch of Reionization Foreground Removal with the SKA, inAdvancing Astrophysics with the Square Kilometre Array (AASKA14), p. 5, April, 2015, DOI [1501.04429]
-
[35]
F.G. Mertens, A. Ghosh and L.V.E. Koopmans,Statistical 21-cm signal separation via Gaussian Process Regression analysis,Mon. Not. Roy. Astron. Soc.478(2018) 3640 [1711.10834]
-
[36]
N.S. Kern and A. Liu,Gaussian process foreground subtraction and power spectrum estimation for 21 cm cosmology,Mon. Not. Roy. Astron. Soc.501(2021) 1463 [2010.15892]
-
[37]
F.G. Mertens, J. Bobin and I.P. Carucci,Retrieving the 21-cm signal from the Epoch of Reionization with learnt Gaussian process kernels,Mon. Not. Roy. Astron. Soc.527(2024) 3517 [2307.13545]
-
[38]
M. Bianco, S.K. Giri, R. Sharma, T. Chen, S.P. Krishna, C. Finlay et al.,Deep learning approach for identification of h ii regions during reionization in 21-cm observations – iii. image recovery,Monthly Notices of the Royal Astronomical Society541(2025) 234 [https://academic.oup.com/mnras/article-pdf/541/1/234/63491363/staf973.pdf]
work page 2025
-
[39]
A. Bonaldi, P. Hartley, R. Braun, S. Purser, A. Acharya, K. Ahn et al.,Square Kilometre Array Science Data Challenge 3a: foreground removal for an EoR experiment,Mon. Not. Roy. Astron. Soc.543(2025) 1092 [2503.11740]
- [40]
- [41]
-
[42]
Planck Collaboration, N. Aghanim, Y. Akrami, F. Arroja, M. Ashdown, J. Aumont et al., Planck 2018 results. I. Overview and the cosmological legacy of Planck,Astron. Astrophys. 641(2020) A1 [1807.06205]
-
[43]
S.K. Pal, S. Dasgupta, A. Datta, S. Majumdar, S. Bag and P. Sarkar,Interpreting the hi 21 cm cosmology maps through largest cluster statistics. part ii. impact of the realistic foreground and instrumental noise on synthetic ska1-low observations,Journal of Cosmology and Astroparticle Physics2025(2025) 096
work page 2025
-
[44]
Dulwich,OSKAR 2.7.6, January, 2020
F. Dulwich,OSKAR 2.7.6, January, 2020. 10.5281/zenodo.3758491. – 33 –
-
[45]
J.P. Hamaker, J.D. Bregman and R.J. Sault,Understanding radio polarimetry. I. Mathematical foundations.,Astronomy and Astrophysics Supplement Series117(1996) 137
work page 1996
- [46]
-
[47]
A low-frequency extragalactic catalogue,Mon
N.Hurley-Walker, J.R.Callingham, P.J.Hancock, T.M.O.Franzen, L.Hindson, A.D.Kapińska et al.,GaLactic and Extragalactic All-sky Murchison Widefield Array (GLEAM) survey - I. A low-frequency extragalactic catalogue,Mon. Not. Roy. Astron. Soc.464(2017) 1146 [1610.08318]
-
[48]
C.R. Lynch, T.J. Galvin, J.L.B. Line, C.H. Jordan, C.M. Trott, J.K. Chege et al.,The MWA long baseline Epoch of reionisation survey—I. Improved source catalogue for the EoR 0 field, Publ. Astron. Soc. Austral.38(2021) e057 [2110.08400]
-
[49]
21cmFAST: A Fast, Semi-Numerical Simulation of the High-Redshift 21-cm Signal
A. Mesinger, S. Furlanetto and R. Cen,21CMFAST: a fast, seminumerical simulation of the high-redshift 21-cm signal,Mon. Not. Roy. Astron. Soc.411(2011) 955 [1003.3878]
work page Pith review arXiv 2011
- [50]
-
[51]
G. Mellema, L. Koopmans, H. Shukla, K.K. Datta, A. Mesinger and S. Majumdar,HI tomographic imaging of the Cosmic Dawn and Epoch of Reionization with SKA,PoS AASKA14(2015) 010
work page 2015
-
[52]
G.M. Battaglia, G. Caruso, P. Bolli, R. Palmeri and A.F. Morabito,Square Kilometre Array Enhancement: AConvexProgrammingApproachtoOptimizeSKA-LowStationsintheCaseof Perturbed Vogel Layout,Sensors25(2025) 5039
work page 2025
-
[53]
D.B. Davidson, C. Trott and M. Kovaleva,Initial beamforming analysis for substations in the ska-low radio telescope, in2025 19th European Conference on Antennas and Propagation (EuCAP), pp. 1–4, 2025, DOI
work page 2025
-
[54]
A. Bonaldi, P. Hartley, S. Purser, O. Bait, E. Lee, R. Braun et al.,SKA-Low simulations for a cosmic dawn/epoch of reionisation deep field,arXiv e-prints(2025) arXiv:2506.09533 [2506.09533]
-
[55]
S. Sridhar, W. Williams and S. Breen,Ska low and mid subarray templates, June, 2024
work page 2024
- [56]
- [57]
-
[58]
A. Chokshi, N. Barry, J.L.B. Line, C.H. Jordan, B. Pindor and R.L. Webster,The necessity of individually validated beam models for an interferometric epoch of reionization detection, Mon. Not. Roy. Astron. Soc.534(2024) 2475 [2409.19875]
- [59]
-
[60]
J.P. McMullin, B. Waters, D. Schiebel, W. Young and K. Golap,CASA Architecture and Applications, inAstronomical Data Analysis Software and Systems XVI, R.A. Shaw, F. Hill and D.J. Bell, eds., vol. 376 ofAstronomical Society of the Pacific Conference Series, p. 127, October, 2007
work page 2007
- [61]
- [62]
-
[63]
A.R. Offringa, F. Mertens, S. van der Tol, B. Veenboer, B.K. Gehlot, L.V.E. Koopmans et al., Precision requirements for interferometric gridding in the analysis of a 21 cm power spectrum, Astron. Astrophys.631(2019) A12 [1908.11232]
-
[64]
PyBDSF: Python Blob Detection and Source Finder
N. Mohan and D. Rafferty, “PyBDSF: Python Blob Detection and Source Finder.” Astrophysics Source Code Library, record ascl:1502.007, February, 2015
work page 2015
-
[65]
C.M. Trott, C.H. Jordan, S. Midgley, N. Barry, B. Greig, B. Pindor et al.,Deep multiredshift limitsonEpochofReionization21cmpowerspectrafromfourseasonsofMurchisonWidefield Array observations,Mon. Not. Roy. Astron. Soc.493(2020) 4711 [2002.02575]
-
[66]
M.F. Morales, A. Beardsley, J. Pober, N. Barry, B. Hazelton, D. Jacobs et al.,Understanding the diversity of 21 cm cosmology analyses,Mon. Not. Roy. Astron. Soc.483(2019) 2207 [1810.08731]
-
[67]
F.G. Mertens, M. Mevius, L.V.E. Koopmans, A.R. Offringa, G. Mellema, S. Zaroubi et al., Improved upper limits on the 21 cm signal power spectrum of neutral hydrogen at z≈9.1 from LOFAR,Mon. Not. Roy. Astron. Soc.493(2020) 1662 [2002.07196]
-
[68]
M.F. Morales and J. Hewitt,Toward Epoch of Reionization Measurements with Wide-Field Radio Observations,Astrophys. J.615(2004) 7 [astro-ph/0312437]
- [69]
-
[70]
Astropy: A Community Python Package for Astronomy
Astropy Collaboration, T.P. Robitaille, E.J. Tollerud, P. Greenfield, M. Droettboom, E. Bray et al.,Astropy: A community Python package for astronomy,Astron. Astrophys.558(2013) A33 [1307.6212]
work page Pith review arXiv 2013
-
[71]
The Astropy Project: Building an inclusive, open-science project and status of the v2.0 core package
Astropy Collaboration, A.M. Price-Whelan, B.M. Sipőcz, H.M. Günther, P.L. Lim, S.M. Crawford et al.,The Astropy Project: Building an Open-science Project and Status of the v2.0 Core Package,Astron. J.156(2018) 123 [1801.02634]. – 35 –
work page Pith review arXiv 2018
discussion (0)
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