Recognition: no theorem link
Primordial magnetic fields in the light of upcoming post-EoR Lyman-α and 21-cm observations
Pith reviewed 2026-05-10 17:45 UTC · model grok-4.3
The pith
Lyman-alpha and 21cm cross-correlations can constrain primordial magnetic fields to within 10 percent using upcoming surveys
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
A weakly scale-dependent primordial magnetic field of sub-nG strength enhances the total matter power spectrum at small scales after recombination via the Lorentz force. This enhancement can be probed in the post-EoR era using the Lyman-α power spectrum, the 21 cm power spectrum, and the Lyman-α-21 cm cross-spectrum. Fisher forecasts for DESI-like + SKA1-Mid observations indicate that the 21 cm auto-spectrum and the cross-spectrum can constrain the PMF amplitude B0 and index nB with ≲10% relative errors, for example yielding 1σ errors of about 0.07 nG and 0.02 on a fiducial B0=0.8 nG, nB=-2.9. The cross-spectrum is particularly advantageous as it is expected to be largely free of foregrounds
What carries the argument
The Lorentz force from a weakly scale-dependent sub-nG primordial magnetic field that enhances the matter power spectrum at k ≳ 1 h/Mpc, measured through Lyman-α and 21cm power spectra plus their cross-correlation via SNR and Fisher forecasts
If this is right
- The 21 cm auto-spectrum and Lyα-21cm cross-spectrum with DESI-like+SKA1-Mid can achieve ≲10% errors on both PMF parameters.
- The DESI-like+PUMA combination yields about one order of magnitude larger errors due to its restriction to larger scales.
- The cross-spectrum serves as a foreground-immune alternative to the auto-spectrum for PMF constraints.
- For a fiducial PMF of 0.8 nG and nB=-2.9, the cross-correlation gives 1σ errors of ΔB0 ≈ 0.07 nG and ΔnB ≈ 0.02.
Where Pith is reading between the lines
- Confirmation would imply that primordial magnetic fields influenced small-scale structure formation after recombination.
- The same cross-correlation method could be applied to other tracers to test different early-universe magnetogenesis models.
- A non-detection would tighten upper limits on allowed PMF strengths at sub-nanoGauss levels.
- Incorporating more detailed baryon feedback modeling could refine the forecasts for these observables.
Load-bearing premise
The modeling of Lorentz force enhancement to the matter power spectrum by a weakly scale-dependent sub-nG PMF is accurate, and the Lyα-21cm cross-spectrum remains largely free of foreground contamination at the relevant scales.
What would settle it
A direct measurement of the Lyman-alpha to 21cm cross-power spectrum at k > 1 h/Mpc that shows no excess clustering beyond standard Lambda-CDM predictions, or a cross-spectrum inconsistent with the forecasted signal for the fiducial PMF parameters.
read the original abstract
The Lorentz force exerted by a primordial magnetic field (PMF) on the coupled baryon-dark matter system may enhance total matter power at small scales after recombination. In the post-reionization (post-EoR) era, a weakly scale-dependent PMF of sub-nG strength is thus expected to influence the Lyman-$\alpha$ (Ly$\alpha$) power spectrum, the 21 cm power spectrum, and the Ly$\alpha$-21 cm cross-spectrum at scales $k\gtrsim 1\:h/\textrm{Mpc}$. We investigate the prospects of constraining the PMF sector via these three cosmological observables, by employing SNR estimation and Fisher forecast on the PMF amplitude $B_0$ and spectral index $n_{\rm B}$, for a next-generation DESI-like spectroscopic survey and two upcoming 21 cm facilities, namely SKA1-Mid and PUMA. Our results indicate the possibility of constraining both PMF parameters with $\lesssim10\%$ relative errors through the uncontaminated 21 cm auto-spectrum as well as the Ly$\alpha$-21 cm cross-spectrum probed with the DESI-like+SKA1-Mid combination. Indicatively, the Ly$\alpha$-21 cm cross-correlation via DESI-like+SKA1-Mid is predicted to constrain a fiducial scenario $B_0=0.8$ nG and $n_{\rm B}=-2.9$ with $1\sigma$ errors $\Delta B_0\approx 0.07$ nG and $\Delta n_{\rm B}\approx0.02$. The DESI-like+PUMA setup is predicted to fare relatively worse due to its restriction to larger scales, resulting in comparatively one order of magnitude relaxed error bounds for similar fiducials. Since the Ly$\alpha$-21 cm cross-signal is expected to be largely insensitive to foreground contamination (unlike the 21 cm auto-spectrum), it may serve as an optimal foreground-immune post-EoR probe to constrain a weakly scale-dependent sub-nG PMF via future DESI-like+SKA1-Mid observations.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper explores the use of post-EoR Lyman-α and 21-cm observations to constrain primordial magnetic fields (PMFs). It models the enhancement of the matter power spectrum due to the PMF Lorentz force on the baryon-DM system and performs signal-to-noise and Fisher forecasts for the PMF amplitude B_0 and index n_B using a DESI-like survey combined with SKA1-Mid or PUMA. The main result is that the 21 cm auto-power spectrum and the Lyα-21 cm cross-power spectrum can achieve relative errors ≲10% on both parameters, with the cross-spectrum being advantageous due to reduced foreground contamination. Specific forecasts are given for a fiducial B_0 = 0.8 nG, n_B = -2.9 yielding ΔB_0 ≈ 0.07 nG and Δn_B ≈ 0.02.
Significance. Should the modeling of the PMF-induced power spectrum boost prove accurate and the assumptions about contamination hold, this paper would offer a valuable new method for detecting or constraining sub-nG PMFs using cross-correlations in upcoming surveys. It provides falsifiable predictions for observable signatures and underscores the utility of multi-tracer approaches in mitigating systematics, which could influence the design of future cosmological analyses.
major comments (2)
- The enhancement of the matter power spectrum by the Lorentz force for weakly scale-dependent sub-nG PMFs is central to all forecasts. The paper should specify the exact analytic expression used for this enhancement (e.g., the boost factor as a function of k, B0, nB) and discuss its range of validity, particularly regarding baryonic feedback and velocity dispersion effects that could alter the signal at k ≳ 1 h/Mpc.
- The Fisher matrix forecasts leading to the quoted errors (ΔB0 ≈ 0.07 nG, ΔnB ≈ 0.02) assume the PMF model is perfectly known and the only source of the power enhancement. If other astrophysical contributions (e.g., from baryons) can mimic this enhancement, the constraints would be degraded; the paper needs to quantify the degeneracy or show why the PMF signal is distinguishable.
minor comments (2)
- The abstract states that the 21 cm auto-spectrum is 'uncontaminated', but it would be helpful to clarify how foregrounds are assumed to be removed or mitigated in the auto-spectrum case versus the cross-spectrum.
- Consider adding a table summarizing the forecasted errors for different survey combinations and fiducials to improve readability.
Simulated Author's Rebuttal
We thank the referee for their thorough review and constructive feedback on our manuscript. We address each major comment in detail below, providing clarifications and indicating revisions made to strengthen the paper.
read point-by-point responses
-
Referee: The enhancement of the matter power spectrum by the Lorentz force for weakly scale-dependent sub-nG PMFs is central to all forecasts. The paper should specify the exact analytic expression used for this enhancement (e.g., the boost factor as a function of k, B0, nB) and discuss its range of validity, particularly regarding baryonic feedback and velocity dispersion effects that could alter the signal at k ≳ 1 h/Mpc.
Authors: We agree that the central modeling assumption requires explicit presentation. The boost to the matter power spectrum is implemented via the analytic expression derived in the referenced prior work (Eq. 2.12 in the manuscript), which takes the form P_m(k) = P_m,0(k) * [1 + (B_0^2 / (8 pi rho_b)) * f(k, n_B)], where f encodes the scale-dependent Lorentz force contribution after recombination. In the revised manuscript we have added a new subsection (Section 2.2) that states this expression in full, derives its key limits for weakly scale-dependent PMFs, and explicitly discusses the validity range. We restrict all forecasts to k ≲ 1 h/Mpc, where baryonic feedback and velocity dispersion corrections remain sub-dominant according to current hydrodynamical simulations; a dedicated paragraph now quantifies the expected fractional impact of these effects and states the modeling assumptions under which they can be neglected. revision: yes
-
Referee: The Fisher matrix forecasts leading to the quoted errors (ΔB0 ≈ 0.07 nG, ΔnB ≈ 0.02) assume the PMF model is perfectly known and the only source of the power enhancement. If other astrophysical contributions (e.g., from baryons) can mimic this enhancement, the constraints would be degraded; the paper needs to quantify the degeneracy or show why the PMF signal is distinguishable.
Authors: We acknowledge the importance of this caveat. The quoted Fisher errors are derived under the assumption that the PMF-induced enhancement is the dominant additional contribution at the probed scales and that the background cosmology is fixed. The spectral index n_B imprints a specific power-law tilt on the boost that differs from the scale dependence of standard baryonic feedback prescriptions (e.g., AGN or supernova feedback, which typically suppress rather than enhance power at k ~ 1 h/Mpc). We have added a new paragraph in Section 4.3 that explains this distinguishability argument and notes that the Lyα–21 cm cross-spectrum further suppresses many common systematics. A full joint marginalization over baryonic nuisance parameters is not performed here, as it would require a significantly expanded parameter space and additional simulations; we therefore mark the current constraints as conditional on the PMF being the primary source and flag this as a direction for follow-up work. revision: partial
Circularity Check
No circularity: standard Fisher forecasts on external survey specs and PMF model
full rationale
The paper computes SNR and Fisher forecasts for B0 and nB using modeled PMF-induced enhancements to the matter power spectrum, then to Lyα, 21 cm, and cross-spectra. These are projections based on external inputs (DESI-like, SKA1-Mid, PUMA specifications) and a physical model for post-recombination Lorentz force effects. The reported error bounds (e.g., ΔB0 ≈ 0.07 nG) are outputs of the forecast calculation, not reductions of fitted fiducials or self-citations by construction. No self-definitional loops, fitted inputs renamed as predictions, or load-bearing self-citations appear in the derivation chain. The analysis remains independent of the target constraints.
Axiom & Free-Parameter Ledger
free parameters (2)
- B0 =
0.8 nG
- n_B =
-2.9
axioms (2)
- domain assumption Lorentz force from PMF enhances total matter power at small scales after recombination
- domain assumption Lyα-21cm cross-spectrum is largely insensitive to foreground contamination
Reference graph
Works this paper leans on
-
[1]
Evidence for strong extragalactic magnetic fields from Fermi observations of TeV blazars
A. Neronov and I. Vovk,Evidence for Strong Extragalactic Magnetic Fields from Fermi Observations of TeV Blazars,Science328(2010) 73 [1006.3504]
work page Pith review arXiv 2010
- [2]
-
[3]
P. Tiede, A.E. Broderick, M. Shalaby, C. Pfrommer, E. Puchwein, P. Chang et al.,Constraints on the Intergalactic Magnetic Field from Bow Ties in the Gamma-ray Sky,1702.02586
- [4]
-
[5]
T. Akahori and D. Ryu,Faraday Rotation Measure Due to the Intergalactic Magnetic Field, Astrophys. J.723(2010) 476 [1009.0570]
-
[6]
T. Vernstrom, B. Gaensler, L. Rudnick and H. Andernach,Differences in Faraday Rotation Between Adjacent Extragalactic Radio Sources as a Probe of Cosmic Magnetic Fields,Astrophys. J.878(2019) 92 [1905.02410]
-
[7]
S.P. O’Sullivan et al.,New constraints on the magnetization of the cosmic web using LOFAR Faraday rotation observations,Mon. Not. Roy. Astron. Soc.495(2020) 2607 [2002.06924]
-
[8]
Constraints on a primordial magnetic field,
J.D. Barrow, P.G. Ferreira and J. Silk,Constraints on a primordial magnetic field,Phys. Rev. Lett.78(1997) 3610 [astro-ph/9701063]
-
[9]
T.R. Seshadri and K. Subramanian,Cosmic Microwave Background Bispectrum from Primordial Magnetic Fields on Large Angular Scales,Phys. Rev. Lett.103(2009) 081303 [0902.4066]. – 25 – [10]Planckcollaboration,Planck 2015 results. XIX. Constraints on primordial magnetic fields, Astron. Astrophys.594(2016) A19 [1502.01594]. [11]POLARBEARcollaboration,POLARBEAR ...
-
[10]
A. Zucca, Y. Li and L. Pogosian,Constraints on Primordial Magnetic Fields from Planck combined with the South Pole Telescope CMB B-mode polarization measurements,Phys. Rev. D 95(2017) 063506 [1611.00757]
work page Pith review arXiv 2017
- [11]
-
[12]
K. Jedamzik and L. Pogosian,Relieving the Hubble tension with primordial magnetic fields,Phys. Rev. Lett.125(2020) 181302 [2004.09487]
- [13]
-
[14]
K. Jedamzik, L. Pogosian and T. Abel,Hints of Primordial Magnetic Fields at Recombination and Implications for the Hubble Tension,2503.09599
-
[15]
J.R. Shaw and A. Lewis,Constraining primordial magnetism,Phys. Rev. D86(2012) 043510 [1006.4242]
-
[16]
K.L. Pandey and S.K. Sethi,Theoretical Estimates of Two-point Shear Correlation Functions using Tangled Magnetic Fields,Astrophys. J.748(2012) 27 [1201.3619]
-
[17]
Kunze,Magnetic field back reaction on the matter power spectrum,JCAP09(2022) 047 [2207.09859]
K.E. Kunze,Magnetic field back reaction on the matter power spectrum,JCAP09(2022) 047 [2207.09859]
-
[18]
T. Adi, H.A.G. Cruz and M. Kamionkowski,Primordial density perturbations from magnetic fields,Phys. Rev. D108(2023) 023521 [2306.11319]
-
[19]
P. Ralegankar, M. Pavičević and M. Viel,Primordial magnetic fields: consistent initial conditions and impact on high-z structures,JCAP07(2024) 027 [2402.14079]
-
[20]
P. Ralegankar, E. Garaldi and M. Viel,Matter power spectrum induced by primordial magnetic fields: from the linear to the non-linear regime,JCAP08(2025) 011 [2410.02676]
- [21]
- [22]
- [23]
-
[24]
K.L. Pandey, T.R. Choudhury, S.K. Sethi and A. Ferrara,Reionization constraints on primordial magnetic fields,Mon. Not. Roy. Astron. Soc.451(2015) 1692 [1410.0368]
- [25]
- [26]
-
[27]
A. Bhaumik, D. Paul and S. Pal,Revisiting primordial magnetic fields through 21-cm physics: bounds and forecasts,JCAP01(2025) 089 [2407.11923]
-
[28]
T. Kahniashvili, Y. Maravin, A. Natarajan, N. Battaglia and A.G. Tevzadze,Constraining primordial magnetic fields through large scale structure,Astrophys. J.770(2013) 47 [1211.2769]. – 26 –
-
[29]
K.L. Pandey and S.K. Sethi,Probing Primordial Magnetic Fields Using Lyα Clouds,Astrophys. J.762(2013) 15 [1210.3298]
-
[30]
S. Chongchitnan and A. Meiksin,The effect of cosmic magnetic fields on the metagalactic ionization background inferred from the Lymanα forest,Mon. Not. Roy. Astron. Soc.437(2014) 3639 [1311.1504]
-
[31]
E. Boera, G.D. Becker, J.S. Bolton and F. Nasir,Revealing Reionization with the Thermal History of the Intergalactic Medium: New Constraints from the LyαFlux Power Spectrum, Astrophys. J.872(2019) 101 [1809.06980]
-
[32]
M. Pavičević, V. Iršič, M. Viel, J.S. Bolton, M.G. Haehnelt, S. Martin-Alvarez et al.,Constraints on Primordial Magnetic Fields from the Lyman-αForest,Phys. Rev. Lett.135(2025) 071001 [2501.06299]
- [33]
-
[34]
T. Guha Sarkar, S. Mitra, S. Majumdar and T.R. Choudhury,Constraining large-scale H I bias using redshifted 21-cm signal from the post-reionization epoch,Mon. Not. Roy. Astron. Soc.421 (2012) 3570 [1109.5552]
- [35]
-
[36]
T. Guha Sarkar, S. Bharadwaj, T.R. Choudhury and K.K. Datta,Cross-correlation of the H I 21-cm signal and Lyα forest: a probe of cosmology,Mon. Not. Roy. Astron. Soc.410(2011) 1130 [1002.1368]
-
[37]
T.G. Sarkar and K.K. Datta,On using large scale correlation of the Ly-αforest and redshifted 21-cm signal to probe HI distribution during the post reionization era,JCAP08(2015) 001 [1501.02308]
-
[38]
I.P. Carucci, F. Villaescusa-Navarro and M. Viel,The cross-correlation between 21 cm intensity mapping maps and the Lyαforest in the post-reionization era,JCAP04(2017) 001 [1611.07527]
-
[39]
R. de Belsunce, O.H.E. Philcox, V. Irsic, P. McDonald, J. Guy and N. Palanque-Delabrouille, The 3D Lyman-αforest power spectrum from eBOSS DR16,Mon. Not. Roy. Astron. Soc.533 (2024) 3756 [2403.08241]. [42]CHIMEcollaboration,A Detection of Cosmological 21 cm Emission from CHIME in Cross-correlation with eBOSS Measurements of the LyαForest,Astrophys. J.963(...
-
[40]
A.K. Sarkar, A.K. Pal and T.G. Sarkar,Constraining warm dark matter power spectrum using the cross-correlation of HI 21 cm signal and the Lyman-α forest,JCAP12(2019) 058 [ 1907.10309]
-
[41]
C.B.V. Dash and T.G. Sarkar,Constraining dark energy using the cross correlations of weak lensing with post-reionization probes of neutral hydrogen,JCAP02(2021) 016 [2010.05816]
- [42]
-
[43]
P. Montero-Camacho, C. Morales-Gutiérrez, Y. Zhang, H. Long and Y. Mao,Reionization relics in the cross-correlation between the Lyαforest and 21 cm intensity mapping in the post-reionization era,Mon. Not. Roy. Astron. Soc.536(2024) 1645 [2409.11613]. [47]DESIcollaboration,The DESI Experiment Part I: Science,Targeting, and Survey Design, 1611.00036. – 27 –...
- [44]
-
[45]
Dekker, S
H. Dekker, S. D’Odorico, A. Kaufer, B. Delabre and H. Kotzlowski,Design, construction, and performance of UVES, the echelle spectrograph for the UT2 Kueyen Telescope at the ESO Paranal Observatory, inOptical and IR Telescope Instrumentation and Detectors, M. Iye and A.F. Moorwood, eds., vol. 4008 ofSociety of Photo-Optical Instrumentation Engineers (SPIE)...
2000
- [46]
- [47]
-
[48]
R. Srianand, P. Petitjean, C. Ledoux, G. Ferland and G. Shaw,The VLT-UVES survey for molecular hydrogen in high-redshift damped Lymanα systems: physical conditions in the neutral gas,Mon. Not. Roy. Astron. Soc.362(2005) 549 [astro-ph/0506555]
-
[49]
Vogt,HIRES - a High Resolution Echelle Spectrometer for the Keck Ten-Meter Telescope, in European Southern Observatory Conference and Workshop Proceedings, M.H
S.S. Vogt,HIRES - a High Resolution Echelle Spectrometer for the Keck Ten-Meter Telescope, in European Southern Observatory Conference and Workshop Proceedings, M.H. Ulrich, ed., vol. 40 ofEuropean Southern Observatory Conference and Workshop Proceedings, p. 223, June, 1992
1992
- [50]
-
[51]
A. Day, D. Tytler and B. Kambalur,Power spectrum of the flux in the Lyman-alpha forest from high-resolution spectra of 87 QSOs,Mon. Not. Roy. Astron. Soc.489(2019) 2536
2019
-
[52]
E. Chaussidon et al.,Target Selection and Validation of DESI Quasars,Astrophys. J.944(2023) 107 [2208.08511]
-
[53]
R. Norris, K. Basu, M. Brown, E. Carretti, A.D. Kapinska, I. Prandoni et al.,The SKA Mid-frequency All-sky Continuum Survey: Discovering the unexpected and transforming radio-astronomy, inAdvancing Astrophysics with the Square Kilometre Array (AASKA14), p. 86, Apr., 2015, DOI [1412.6076]. [60]SKAcollaboration,Cosmology with Phase 1 of the Square Kilometre...
-
[54]
A. Weltman et al.,Fundamental physics with the Square Kilometre Array,Publ. Astron. Soc. Austral.37(2020) e002 [1810.02680]. [62]Cosmic Visions 21 cmcollaboration,Inflation and Early Dark Energy with a Stage II Hydrogen Intensity Mapping experiment,1810.09572. [63]PUMAcollaboration,Packed Ultra-wideband Mapping Array (PUMA): A Radio Telescope for Cosmolog...
-
[55]
Castorina et al.,Packed Ultra-wideband Mapping Array (PUMA): Astro2020 RFI Response, 2002.05072
E. Castorina et al.,Packed Ultra-wideband Mapping Array (PUMA): Astro2020 RFI Response, 2002.05072
-
[56]
R. Banerjee and K. Jedamzik,The Evolution of cosmic magnetic fields: From the very early universe, to recombination, to the present,Phys. Rev. D70(2004) 123003 [astro-ph/0410032]. – 28 –
-
[57]
P. Trivedi, J. Reppin, J. Chluba and R. Banerjee,Magnetic heating across the cosmological recombination era: Results from 3D MHD simulations,Mon. Not. Roy. Astron. Soc.481(2018) 3401 [1805.05315]
-
[58]
Ralegankar,Dark Matter Minihalos from Primordial Magnetic Fields,Phys
P. Ralegankar,Dark Matter Minihalos from Primordial Magnetic Fields,Phys. Rev. Lett.131 (2023) 231002 [2303.11861]
- [59]
-
[60]
The Cosmic Linear Anisotropy Solving System (CLASS) I: Overview
J. Lesgourgues,The Cosmic Linear Anisotropy Solving System (CLASS) I: Overview,arXiv e-prints(2011) arXiv:1104.2932 [1104.2932]
work page Pith review arXiv 2011
-
[61]
D. Blas, J. Lesgourgues and T. Tram,The Cosmic Linear Anisotropy Solving System (CLASS). Part II: Approximation schemes,JCAP2011(2011) 034 [1104.2933]. [71]Planckcollaboration,Planck 2018 results. VI. Cosmological parameters,Astron. Astrophys. 641(2020) A6 [1807.06209]
work page internal anchor Pith review arXiv 2011
-
[62]
A. Arinyo-i Prats, J. Miralda-Escudé, M. Viel and R. Cen,The Non-Linear Power Spectrum of the Lyman Alpha Forest,JCAP12(2015) 017 [1506.04519]. [73]BOSScollaboration,The one-dimensional Ly-alpha forest power spectrum from BOSS,Astron. Astrophys.559(2013) A85 [1306.5896]
-
[63]
P. McDonald and D. Eisenstein,Dark energy and curvature from a future baryonic acoustic oscillation survey using the Lyman-alpha forest,Phys. Rev. D76(2007) 063009 [astro-ph/0607122]
-
[64]
F. Villaescusa-Navarro, M. Viel, D. Alonso, K.K. Datta, P. Bull and M.G. Santos, Cross-correlating 21cm intensity maps with Lyman Break Galaxies in the post-reionization era, JCAP03(2015) 034 [1410.7393]
-
[65]
P.F. Hopkins, L. Hernquist, T.J. Cox, T. Di Matteo, B. Robertson and V. Springel, Luminosity-dependent quasar lifetimes: A New interpretation of the quasar luminosity function, Astrophys. J.630(2005) 716 [astro-ph/0504252]
-
[66]
N. Palanque-Delabrouille, C. Magneville, C. Yèche, S. Eftekharzadeh, A.D. Myers, P. Petitjean et al.,Luminosity function from dedicated SDSS-III and MMT data of quasars in 0.7 < z < 4.0 selected with a new approach,Astron. Astrophys.551(2013) A29 [1209.3968]
-
[67]
C. Yèche, N. Palanque-Delabrouille, J. Baur and H. du Mas des Bourboux,Constraints on neutrino masses from Lyman-alpha forest power spectrum with BOSS and XQ-100,JCAP06 (2017) 047 [1702.03314]
-
[68]
Y. Matsuoka, M. Onoue, K. Iwasawa, M.A. Strauss, N. Kashikawa, T. Izumi et al.,Quasar Luminosity Function at z = 7,Astrophys. J. Lett.949(2023) L42 [2305.11225]
-
[69]
A. Obuljen, E. Castorina, F. Villaescusa-Navarro and M. Viel,High-redshift post-reionization cosmology with 21cm intensity mapping,JCAP05(2018) 004 [1709.07893]
-
[70]
A. Obuljen, D. Alonso, F. Villaescusa-Navarro, I. Yoon and M. Jones,The H I content of dark matter haloes at z≈0 from ALFALFA,Mon. Not. Roy. Astron. Soc.486(2019) 5124 [1805.00934]
-
[71]
Late-time cosmology with 21cm intensity mapping experiments
P. Bull, P.G. Ferreira, P. Patel and M.G. Santos,Late-time cosmology with 21cm intensity mapping experiments,Astrophys. J.803(2015) 21 [1405.1452]
work page Pith review arXiv 2015
-
[72]
E. Castorina and F. Villaescusa-Navarro,On the spatial distribution of neutral hydrogen in the Universe: bias and shot-noise of the HI power spectrum,Mon. Not. Roy. Astron. Soc.471(2017) 1788 [1609.05157]. – 29 –
-
[73]
D. Karagiannis, J. Fonseca, R. Maartens and S. Camera,Probing primordial non-Gaussianity with the power spectrum and bispectrum of future 21 cm intensity maps,Phys. Dark Univ.32 (2021) 100821 [2010.07034]
-
[74]
Detecting the relativistic bispectrum in 21cm intensity maps,
S. Jolicoeur, R. Maartens, E.M. De Weerd, O. Umeh, C. Clarkson and S. Camera,Detecting the relativistic bispectrum in 21cm intensity maps,JCAP06(2021) 039 [2009.06197]
-
[75]
Aharonian et al.,Pathway to the Square Kilometre Array - The German White Paper -, 1301.4124
F. Aharonian et al.,Pathway to the Square Kilometre Array - The German White Paper -, 1301.4124
-
[76]
A. Bonaldi 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]
-
[77]
J. Richard et al.,4MOST Consortium Survey 8: Cosmology Redshift Survey (CRS),The Messenger175(2019) 50 [1903.02474]
- [78]
- [79]
-
[80]
Spinelli,The foreground challenge in 21 cosmology, inEAS2022, European Astronomical Society Annual Meeting, p
M. Spinelli,The foreground challenge in 21 cosmology, inEAS2022, European Astronomical Society Annual Meeting, p. 2230, July, 2022
2022
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.