Future Parameter Constraints from Weak Lensing CMB and Galaxy Lensing Power- and Bispectra
Pith reviewed 2026-05-19 02:33 UTC · model grok-4.3
The pith
The bispectrum from future CMB and galaxy weak lensing can rival the power spectrum in tightening cosmological parameter constraints.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In the absence of systematics both the CMB and galaxy lensing bispectra are detectable at high signal-to-noise. With a weak prior the bispectrum significantly improves parameter constraints by breaking degeneracies. On small scales where non-linear effects dominate the bispectrum's constraining power can rival that of the power spectrum. Combining CMB and galaxy lensing yields tighter bounds, particularly on neutrino mass. These results hold after post-Born corrections are applied.
What carries the argument
Joint power- and bispectrum analysis of CMB weak lensing and galaxy weak lensing, including their cross-correlations, applied to an eight-parameter model (ΛCDM plus neutrino mass sum plus dark energy equation of state).
If this is right
- With weak priors the bispectrum breaks degeneracies and improves constraints on neutrino mass and dark energy parameters.
- On small scales the bispectrum becomes as constraining as the power spectrum.
- Combining CMB and galaxy lensing power and bispectra produces tighter limits than either probe alone, especially for neutrino mass.
- Post-Born corrections leave the main conclusions about the value of the bispectrum unchanged.
Where Pith is reading between the lines
- Analyses of real data will need accurate modeling of non-Gaussian covariance before the forecasted bispectrum gains can be realized.
- Joint CMB-galaxy lensing pipelines that routinely include higher-order statistics could become standard for stage 4 surveys.
- Similar gains may appear in other higher-order lensing statistics if their covariance and modeling challenges are solved.
Load-bearing premise
The forecasts assume the absence of systematics in the lensing measurements and that non-Gaussian covariance and baryonic feedback can be neglected or perfectly modeled.
What would settle it
Actual stage 4 survey data in which the measured bispectrum signal-to-noise falls well below the forecasted high values, or in which parameter improvements fail to appear once non-Gaussian covariance and baryonic effects are included, would falsify the predicted gains.
read the original abstract
Upcoming stage 4 surveys, such as the Simons Observatory, LSST, and Euclid, are poised to measure weak gravitational lensing of the Cosmic Microwave Background (CMB) and galaxies with unprecedented precision. While the power spectrum is the standard statistic used to analyze weak lensing data, non-Gaussianity from non-linear structure growth encodes additional cosmological information in higher-order statistics. We forecast the ability of future surveys to constrain cosmological parameters using the weak lensing power spectrum and bispectrum from both CMB and galaxy surveys, including their cross-correlations. We consider an eight-parameter model ($\Lambda$CDM + $\sum m_\nu$ + $w_0$) and assess constraints for stage 4 survey specifications. In the absence of systematics, both the CMB and galaxy lensing bispectra are found to be detectable at high signal-to-noise. We test two priors: a ''strong'' one based on constraints from CMB temperature and $E$-mode polarization anisotropies, and a ''weak'' one with minimal assumptions. With the weak prior, the bispectrum significantly improves parameter constraints by breaking degeneracies. For strong priors, improvements are more limited, especially for the CMB bispectrum. On small scales, where non-linear effects dominate, the bispectrum's constraining power can rival that of the power spectrum. We also find strong synergy between CMB and galaxy lensing; combining both probes leads to tighter constraints, particularly on neutrino mass. It was recently found that the CMB lensing bispectrum is strongly affected by the Born approximation, so we also consider post-Born corrections but find that our main conclusions remain the same. These results highlight the potential of higher-order lensing statistics and motivate further work on neglected effects such as non-Gaussian covariance, instrumental systematics, and baryonic feedback.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript forecasts cosmological parameter constraints from the weak lensing power spectrum and bispectrum of CMB and galaxy lensing, including their cross-correlations, for upcoming Stage-4 surveys such as Simons Observatory, LSST, and Euclid. Using an eight-parameter model (ΛCDM + ∑mν + w0), the authors compare constraints under strong (CMB temperature and E-mode polarization) and weak priors. They report that with the weak prior the bispectrum significantly improves constraints by breaking degeneracies, that on small scales the bispectrum's constraining power can rival the power spectrum, and that strong synergy exists between CMB and galaxy lensing (especially for neutrino mass). Post-Born corrections are tested but do not alter the main conclusions. All results assume the absence of systematics.
Significance. If the stated assumptions hold, the work demonstrates the value of including bispectra alongside power spectra for future weak-lensing analyses, particularly when priors are weak, and quantifies the synergy between CMB and galaxy lensing probes. The forward modeling under explicit Stage-4 survey specifications and the explicit check that post-Born corrections leave conclusions unchanged are strengths that support the forecasts.
major comments (2)
- The headline claim that the bispectrum rivals the power spectrum on small scales (Abstract) is load-bearing for the central result yet rests on the assumption that non-Gaussian covariance and baryonic feedback can be neglected or perfectly modeled. The manuscript itself flags these effects as neglected and to be addressed later; because baryonic feedback modifies the matter bispectrum at the 10-30% level on the relevant scales, a quantitative sensitivity test or error budget for these terms would be required to substantiate the small-scale rivalry statement.
- The numerical forecasts are presented without detailed error budgets, full specification of the covariance matrix construction, or validation against mock catalogs (as noted in the reader's assessment of soundness). This omission affects the ability to assess the robustness of the reported high signal-to-noise detections and the claimed degeneracy-breaking improvements.
minor comments (1)
- The abstract states that main conclusions survive post-Born corrections; a short quantitative summary of the size of these corrections in the results section would improve clarity for readers.
Simulated Author's Rebuttal
We thank the referee for their careful and constructive review of our manuscript. We address each of the major comments in detail below and indicate the revisions we plan to make.
read point-by-point responses
-
Referee: The headline claim that the bispectrum rivals the power spectrum on small scales (Abstract) is load-bearing for the central result yet rests on the assumption that non-Gaussian covariance and baryonic feedback can be neglected or perfectly modeled. The manuscript itself flags these effects as neglected and to be addressed later; because baryonic feedback modifies the matter bispectrum at the 10-30% level on the relevant scales, a quantitative sensitivity test or error budget for these terms would be required to substantiate the small-scale rivalry statement.
Authors: We agree with the referee that our headline claim in the abstract is presented under the modeling assumptions detailed in the paper, specifically the neglect of non-Gaussian covariance, baryonic feedback, and other systematics, which are explicitly noted as topics for future investigation. The statement is intended to highlight the potential information content within this simplified framework. To better substantiate the claim and address the concern, we will revise the abstract and discussion sections to more prominently qualify the result as holding in the absence of these effects. We will also add a short paragraph discussing the expected magnitude of baryonic feedback effects on the bispectrum, drawing from existing studies, to provide a basic error budget perspective. A full quantitative sensitivity test would require a separate, more computationally intensive analysis that we plan to pursue in follow-up work. revision: partial
-
Referee: The numerical forecasts are presented without detailed error budgets, full specification of the covariance matrix construction, or validation against mock catalogs (as noted in the reader's assessment of soundness). This omission affects the ability to assess the robustness of the reported high signal-to-noise detections and the claimed degeneracy-breaking improvements.
Authors: We thank the referee for highlighting this aspect of the presentation. In the revised manuscript, we will include an expanded methods section with a more complete specification of how the covariance matrix is constructed, including the Gaussian approximation used and any assumptions regarding the survey specifications. We will also add a dedicated subsection on the error budget, summarizing the primary sources of uncertainty in our forecasts. Regarding validation against mock catalogs, while this would be ideal for full robustness checks, it is not feasible within the current scope due to the high computational cost for bispectrum calculations at stage-4 precision. Our forecasts follow established methodologies in the literature for such predictions, and we will cite relevant works to support this approach. These changes should enhance the reader's ability to evaluate the results. revision: yes
Circularity Check
Forecasts use forward modeling under explicit priors and survey specs with no recycled fits or self-referential reductions
full rationale
The paper performs forward modeling of survey observables under stated priors and survey specifications; no fitted parameters from existing data are recycled into the reported forecasts. The derivation chain consists of standard cosmological modeling, computation of power spectra and bispectra, and Fisher forecasts for parameter constraints. Explicit caveats on neglected effects (non-Gaussian covariance, baryonic feedback, systematics) are stated as limitations rather than hidden assumptions that close a loop. No self-definitional steps, fitted inputs renamed as predictions, or load-bearing self-citations appear in the provided text. The central claims about degeneracy breaking and rival constraining power on small scales follow directly from the modeled signals under the stated idealizations.
Axiom & Free-Parameter Ledger
free parameters (1)
- Stage-4 survey specifications
axioms (2)
- domain assumption Absence of systematics in weak-lensing measurements
- standard math Standard eight-parameter cosmological model
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
We forecast the ability of future surveys to constrain cosmological parameters using the weak lensing power spectrum and bispectrum from both CMB and galaxy surveys, including their cross-correlations. We consider an eight-parameter model (ΛCDM + ∑mν + w0) and assess constraints for stage 4 survey specifications.
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
-
[2]
A unified model for the evolution of galaxies and quasars , volume =
David J. Bacon, Alexandre R. Refregier, and Richard S. Ellis. “Detection of weak gravitational lensing by large-scale structure”. In: Monthly Notices of the Royal Astronomical Society 318.2 (Oct. 2000), pp. 625–640. issn: 1365-2966. doi: 10.1046/j.1365-8711.2000.03851.x. url: http://dx.doi.org/10.1046/j.1365-8711.2000.03851.x
-
[3]
Large-Scale Cosmic Shear Measurements
N. Kaiser, G. Wilson, and G. Luppino. “Large-Scale Cosmic Shear Measurements”. In: arXiv preprint astro-ph/0003338 (2000)
work page internal anchor Pith review Pith/arXiv arXiv 2000
-
[4]
David M. Wittman et al. “Detection of weak gravitational lensing distortions of distant galaxies by cosmic dark matter at large scales”. In: Nature 405.6783 (May 2000), pp. 143–148. issn: 1476-4687. doi: 10.1038/35012001. url: http://dx.doi.org/10.1038/35012001
-
[5]
L. Van Waerbeke et al. Detection of correlated galaxy ellipticities on CFHT data: first ev- idence for gravitational lensing by large-scale structures . 2000. arXiv: astro - ph / 0002500 [astro-ph]. url: https://arxiv.org/abs/astro-ph/0002500
work page internal anchor Pith review Pith/arXiv arXiv 2000
-
[6]
Cosmology with cosmic shear observations: a review
Martin Kilbinger. “Cosmology with cosmic shear observations: a review”. In: Reports on Progress in Physics 78.8 (2015), p. 086901. doi: 10.1088/0034- 4885/78/8/086901 . url: https://arxiv.org/abs/1411.0115
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1088/0034- 2015
-
[7]
L. Van Waerbeke, Y. Mellier, T. Erben, et al. “Detection of correlated galaxy ellipticities from CFH12k VLT data: first evidence for gravitational lensing by large-scale structures”. In: Astronomy & Astrophysics 358 (2000), pp. 30–44
work page 2000
-
[8]
Matthias Bartelmann and Peter Schneider. “Weak gravitational lensing”. In: Physics Reports 340 (2001), pp. 291–472
work page 2001
-
[9]
Planck Collaboration. “Planck 2018 results. VIII. Gravitational lensing”. In: arXiv e-prints (July 2018). arXiv: 1807.06210 [astro-ph.CO]
-
[10]
The Simons Observatory: science goals and forecasts
PAR Ade, J Aguirre, Z Ahmed, et al. “The Simons Observatory: science goals and forecasts”. In: Journal of Cosmology and Astroparticle Physics 2019.02 (2019), p. 056
work page 2019
-
[11]
LSST: From Science Drivers to Reference Design and Anticipated Data Products
ˇZ. Ivezi´ c, S. M. Kahn, J. A. Tyson, et al. “LSST: From Science Drivers to Reference Design and Anticipated Data Products”. In: The Astrophysical Journal 873.2 (2019), p. 111
work page 2019
-
[12]
Laureijs and others (Euclid Collaboration)
R. Laureijs and others (Euclid Collaboration). Euclid Definition Study Report. ESA/SRE(2011)12
work page 2011
-
[13]
arXiv: 1110.3193. – 17 –
work page internal anchor Pith review Pith/arXiv arXiv
-
[14]
Mass Reconstruction with Cosmic Microwave Background Polarization
Wayne Hu and Takemi Okamoto. “Mass Reconstruction with Cosmic Microwave Background Polarization”. In: The Astrophysical Journal 574.2 (Aug. 2002), pp. 566–574. issn: 1538-4357. doi: 10.1086/341110. url: http://dx.doi.org/10.1086/341110
-
[15]
Weak Gravitational Lensing and Its Cosmological Ap- plications
Henk Hoekstra and Bhuvnesh Jain. “Weak Gravitational Lensing and Its Cosmological Ap- plications”. In: Annual Review of Nuclear and Particle Science 58.1 (2008), pp. 99–123
work page 2008
-
[16]
Weak lensing statistics as a probe of non-Gaussian initial conditions
F. Bernardeau, L. Van Waerbeke, and Y. Mellier. “Weak lensing statistics as a probe of non-Gaussian initial conditions”. In: Astronomy & Astrophysics 322 (1997), pp. 1–18
work page 1997
-
[17]
Cosmological parameters from lensing power spectrum and bis- pectrum tomography
M. Takada and B. Jain. “Cosmological parameters from lensing power spectrum and bis- pectrum tomography”. In: Monthly Notices of the Royal Astronomical Society 340 (2003), pp. 580–608
work page 2003
-
[18]
Detection of the CMB lensing – galaxy bispectrum
Gerrit S. Farren et al. “Detection of the CMB lensing – galaxy bispectrum”. In: (Nov. 2023). arXiv: 2311.04213 [astro-ph.CO]
-
[19]
Constraints from CMB lensing tomography with projected bispectra
Lea Harscouet et al. “Constraints from CMB lensing tomography with projected bispectra”. In: (July 2025). arXiv: 2507.07968 [astro-ph.CO]
-
[20]
Sudeep Das et al. “Detection of the Power Spectrum of Cosmic Microwave Background Lens- ing by the Atacama Cosmology Telescope”. In: Phys. Rev. Lett. 107 (2011), p. 021301. doi: 10.1103/PhysRevLett.107.021301. arXiv: 1103.2124 [astro-ph.CO]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevlett.107.021301 2011
-
[21]
Planck 2013 results. XVII. Gravitational lensing by large-scale structure
Planck Collaboration. “Planck 2013 results. XVII. Gravitational lensing by large-scale struc- ture”. In: Astron. Astrophys. 571 (2014), A17. doi: 10.1051/0004-6361/201321543. arXiv: 1303.5077 [astro-ph.CO]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1051/0004-6361/201321543 2013
-
[22]
Planck 2015 results. XV. Gravitational lensing
Planck Collaboration. “Planck 2015 results. XV. Gravitational lensing”. In: Astron. Astro- phys. 594 (2016), A15. doi: 10.1051/0004-6361/201525941. arXiv: 1502.01591 [astro-ph.CO]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1051/0004-6361/201525941 2015
-
[23]
CFHTLenS: higher order galaxy–mass correlations probed by galaxy–galaxy–galaxy lensing
P. Simon et al. “CFHTLenS: higher order galaxy–mass correlations probed by galaxy–galaxy–galaxy lensing”. In: Monthly Notices of the Royal Astronomical Society 430.3 (Feb. 2013), pp. 2476–
work page 2013
-
[24]
issn: 0035-8711. doi: 10.1093/mnras/stt069 . url: http://dx.doi.org/10.1093/ mnras/stt069
-
[27]
Impact of Next-to-Leading Order Contributions to Cosmic Mi- crowave Background Lensing
Giovanni Marozzi et al. “Impact of Next-to-Leading Order Contributions to Cosmic Mi- crowave Background Lensing”. In: Physical Review Letters 118.21 (May 2017). issn: 1079-
work page 2017
-
[28]
doi: 10 . 1103 / physrevlett . 118 . 211301. url: http : / / dx . doi . org / 10 . 1103 / PhysRevLett.118.211301
-
[29]
Impact of post-Born lensing on the CMB
Geraint Pratten and Antony Lewis. “Impact of post-Born lensing on the CMB”. In: Journal of Cosmology and Astroparticle Physics 2016.08 (Aug. 2016), pp. 047–047. issn: 1475-7516. doi: 10 . 1088 / 1475 - 7516 / 2016 / 08 / 047. url: http : / / dx . doi . org / 10 . 1088 / 1475 - 7516/2016/08/047
work page 2016
-
[30]
The Born and lens–lens corrections to weak gravi- tational lensing angular power spectra
Charles Shapiro and Asantha Cooray. “The Born and lens–lens corrections to weak gravi- tational lensing angular power spectra”. In: Journal of Cosmology and Astroparticle Physics 2006.03 (Mar. 2006), pp. 007–007. issn: 1475-7516. doi: 10.1088/1475-7516/2006/03/007. url: http://dx.doi.org/10.1088/1475-7516/2006/03/007. – 18 –
-
[31]
CMB-lensing beyond the Born approximation
Giovanni Marozzi et al. “CMB-lensing beyond the Born approximation”. In: Journal of Cos- mology and Astroparticle Physics 2016.09 (Sept. 2016), pp. 028–028. issn: 1475-7516. doi: 10.1088/1475-7516/2016/09/028 . url: http://dx.doi.org/10.1088/1475-7516/2016/ 09/028
-
[32]
CMB lensing beyond the leading order: Temperature and polariza- tion anisotropies
Giovanni Marozzi et al. “CMB lensing beyond the leading order: Temperature and polariza- tion anisotropies”. In: Physical Review D 98.2 (July 2018). issn: 2470-0029. doi: 10.1103/ physrevd.98.023535. url: http://dx.doi.org/10.1103/PhysRevD.98.023535
-
[33]
Alexandre Barthelemy, Sandrine Codis, and Francis Bernardeau. “Post-Born corrections to the one-point statistics of (CMB) lensing convergence obtained via large deviation theory”. In: Monthly Notices of the Royal Astronomical Society 494.3 (Apr. 2020), pp. 3368–3382. issn: 1365-2966. doi: 10.1093/mnras/staa931. url: http://dx.doi.org/10.1093/mnras/ staa931
-
[34]
Quadratic estimators for CMB weak lensing
Abhishek S. Maniyar et al. “Quadratic estimators for CMB weak lensing”. In: Phys. Rev. D 103.8 (2021), p. 083524. doi: 10 . 1103 / PhysRevD . 103 . 083524. arXiv: 2101 . 12193 [astro-ph.CO]
work page 2021
-
[35]
Reconstruction of lensing from the cosmic microwave background polarization
Christopher M. Hirata and Uroˇ s Seljak. “Reconstruction of lensing from the cosmic microwave background polarization”. In: Physical Review D 68.8 (Oct. 2003). issn: 1089-4918. doi: 10.1103/physrevd.68.083002. url: http://dx.doi.org/10.1103/PhysRevD.68.083002
-
[36]
Efficient computation of cosmic microwave background anisotropies in closed FRW models
Antony Lewis, Anthony Challinor, and Anthony Lasenby. “Efficient computation of cosmic microwave background anisotropies in closed FRW models”. In: The Astrophysical Journal 538 (2000), pp. 473–476
work page 2000
-
[37]
An improved fitting formula for the dark matter bispectrum
Hector Gil-Marin et al. “An improved fitting formula for the dark matter bispectrum”. In: Journal of Cosmology and Astroparticle Physics 2012.02 (2012), p. 047. doi: 10.1088/1475- 7516/2012/02/047. arXiv: 1111.4477 [astro-ph.CO]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1088/1475- 2012
-
[38]
Scott Dodelson and Fabian Schmidt. Modern Cosmology. 2nd. Elsevier, 2020. isbn: 978-0-12- 815948-4
work page 2020
-
[39]
Determination of inflationary observables by cosmic microwave background anisotropy experiments
Lloyd Knox. “Determination of inflationary observables by cosmic microwave background anisotropy experiments”. In: Physical Review D 52.8 (1995), pp. 4307–4318. doi: 10.1103/ PhysRevD.52.4307
work page 1995
-
[40]
Karhunen–Lo` eve eigenvalue prob- lems in cosmology: how should we tackle large data sets?
Max Tegmark, Andrew N. Taylor, and Alan F. Heavens. “Karhunen–Lo` eve eigenvalue prob- lems in cosmology: how should we tackle large data sets?” In: The Astrophysical Journal 480.1 (1997), pp. 22–35. doi: 10.1086/303939
-
[41]
Astronomy & Astrophysics , month =
N. Aghanim et al. “Planck2018 results: VI. Cosmological parameters”. In: Astronomy and Astrophysics 641 (Sept. 2020), A6. issn: 1432-0746. doi: 10.1051/0004-6361/201833910 . url: http://dx.doi.org/10.1051/0004-6361/201833910
-
[42]
Roy, Dynamical dark energy in the light of DESI 2024 data, Phys
Nandan Roy et al. “Dynamical dark energy in the light of DESI 2024 data”. In: arXiv preprint (2024). arXiv: 2406.00634 [astro-ph.CO]. url: https://arxiv.org/abs/2406.00634
-
[43]
CMB-S4 Science Book, First Edition
Kevork N. Abazajian et al. CMB-S4 Science Book, First Edition . 2016. arXiv: 1610.02743 [astro-ph.CO]. url: https://arxiv.org/abs/1610.02743
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[44]
Euclid Assessment Study Report for the ESA Cosmic Visions
R. Laureijs et al. Euclid Assessment Study Report . Tech. rep. ESA, 2009. arXiv: 0912.0914
work page internal anchor Pith review Pith/arXiv arXiv 2009
-
[45]
KiDS-1000 catalogue: Weak gravitational lensing shear measure- ments
Benjamin Kuijken and et al. “KiDS-1000 catalogue: Weak gravitational lensing shear measure- ments”. In: A&A 652 (2021), A30. doi: 10.1051/0004-6361/202040857. arXiv: 2007.01845. – 19 –
-
[46]
Euclid Preparation - X. The Euclid Photometric-Redshift Challenge
Euclid Collaboration: G. Desprez, S. Paltani, J. Coupon, et al. “Euclid Preparation - X. The Euclid Photometric-Redshift Challenge”. In: Astronomy and Astrophysics 644 (2020), A31. doi: 10.1051/0004-6361/202039403 . url: https://www.aanda.org/articles/aa/pdf/ 2020/12/aa39403-20.pdf
-
[47]
Steven M. Kahn, Justin R. Bankert, Srinivasan Chandrasekharan, et al. “LSST System Per- formance”. In: LSST Science Book, Version 2.0 . Accessed: 2025-02-11. 2009. url: https: //www.lsst.org/sites/default/files/docs/sciencebook/SB_3.pdf
work page 2025
-
[48]
Constraints on neutrino mass from cosmic microwave background and large-scale structure
Z. Pan and L. Knox. “Constraints on neutrino mass from cosmic microwave background and large-scale structure”. In: Monthly Notices of the Royal Astronomical Society 454.3 (Oct. 2015), pp. 3200–3206. issn: 1365-2966. doi: 10.1093/mnras/stv2164. url: http://dx.doi. org/10.1093/mnras/stv2164
-
[49]
The skewness of the distance-redshift relation in LambdaCDM
T. Schiavone, E. Di Dio, and G. Fanizza. “The skewness of the distance-redshift relation in LambdaCDM”. In: Journal of Cosmology and Astroparticle Physics 2024.02 (Feb. 2024), p. 050. issn: 1475-7516. doi: 10.1088/1475-7516/2024/02/050. url: http://dx.doi.org/ 10.1088/1475-7516/2024/02/050
-
[50]
Precise and accurate cosmology with CMB× LSS power spectra and bispectra
Shu-Fan Chen, Hayden Lee, and Cora Dvorkin. “Precise and accurate cosmology with CMB× LSS power spectra and bispectra”. In: JCAP 05 (2021), p. 030. doi: 10.1088/1475-7516/2021/ 05/030. arXiv: 2103.01229 [astro-ph.CO]
-
[51]
CMB multipole measurements in the presence of foregrounds
Ang´ elica de Oliveira-Costa and Max Tegmark. “CMB multipole measurements in the presence of foregrounds”. In: Physical Review D 74.2 (July 2006). issn: 1550-2368. doi: 10 . 1103 / physrevd.74.023005. url: http://dx.doi.org/10.1103/PhysRevD.74.023005
-
[52]
Parameter constraints from cross-correlation of CMB lensing with galaxy clustering
Marcel Schmittfull and Uroˇ s Seljak. “Parameter constraints from cross-correlation of CMB lensing with galaxy clustering”. In: Physical Review D 97.12 (2018), p. 123540. doi: 10.1103/ PhysRevD.97.123540. arXiv: 1710.09465
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[53]
Bias to CMB lensing measure- ments from the bispectrum of large-scale structure
Vanessa B¨ ohm, Marcel Schmittfull, and Blake D. Sherwin. “Bias to CMB lensing measure- ments from the bispectrum of large-scale structure”. In: Physical Review D 94.4 (Aug. 2016). issn: 2470-0029. doi: 10.1103/physrevd.94.043519 . url: http://dx.doi.org/10.1103/ PhysRevD.94.043519
-
[54]
Physical Review D111(1), 016020 (2025) https://doi.org/10.1103/PhysRevD
Vanessa B¨ ohm et al. “Effect of non-Gaussian lensing deflections on CMB lensing measure- ments”. In: Physical Review D 98.12 (Dec. 2018). issn: 2470-0029. doi: 10.1103/physrevd. 98.123510. url: http://dx.doi.org/10.1103/PhysRevD.98.123510
-
[55]
Jia Liu et al. “CMB lensing beyond the power spectrum: Cosmological constraints from the one-point probability distribution function and peak counts”. In: Physical Review D 94.10 (Nov. 2016). issn: 2470-0029. doi: 10.1103/physrevd.94.103501 . url: http://dx.doi. org/10.1103/PhysRevD.94.103501
-
[56]
Delensing CMB polarization with external datasets
Kendrick M Smith et al. “Delensing CMB polarization with external datasets”. In: Journal of Cosmology and Astroparticle Physics 2012.06 (June 2012), pp. 014–014. issn: 1475-7516. doi: 10 . 1088 / 1475 - 7516 / 2012 / 06 / 014. url: http : / / dx . doi . org / 10 . 1088 / 1475 - 7516/2012/06/014
work page 2012
-
[57]
Baryonic feedback biases on fundamental physics from lensed CMB power spectra
Fiona McCarthy, J. Colin Hill, and Mathew S. Madhavacheril. “Baryonic feedback biases on fundamental physics from lensed CMB power spectra”. In: Physical Review D 105.2 (Jan. 2022). issn: 2470-0029. doi: 10.1103/physrevd.105.023517 . url: http://dx.doi.org/ 10.1103/PhysRevD.105.023517. – 20 –
-
[58]
Baryonic effects on CMB lens- ing and neutrino mass constraints
Eegene Chung, Simon Foreman, and Alexander van Engelen. “Baryonic effects on CMB lens- ing and neutrino mass constraints”. In: Phys. Rev. D 101 (6 Mar. 2020), p. 063534. doi: 10.1103/PhysRevD.101.063534 . url: https://link.aps.org/doi/10.1103/PhysRevD. 101.063534
-
[59]
Pranjal R. S. et al. Impact of cosmology dependence of baryonic feedback in weak lensing
-
[60]
url: https://arxiv.org/abs/2410.21980
arXiv: 2410.21980 [astro-ph.CO]. url: https://arxiv.org/abs/2410.21980
-
[61]
Avoiding baryonic feedback effects on neutrino mass measurements from CMB lensing
Fiona McCarthy, Simon Foreman, and Alexander van Engelen. “Avoiding baryonic feedback effects on neutrino mass measurements from CMB lensing”. In: Physical Review D 103.10 (May 2021). issn: 2470-0029. doi: 10.1103/physrevd.103.103538 . url: http://dx.doi. org/10.1103/PhysRevD.103.103538
-
[62]
Weak Gravitational Lensing Bispectrum
Asantha Cooray and Wayne Hu. “Weak Gravitational Lensing Bispectrum”. In: The Astro- physical Journal 548.1 (Feb. 2001), pp. 7–18. issn: 1538-4357. doi: 10.1086/318660 . url: http://dx.doi.org/10.1086/318660
-
[63]
George Casella and Roger L. Berger. Statistical Inference. 2nd. Duxbury Pacific Grove, CA,
-
[64]
Max Tegmark. “Cosmic Confusion: Degeneracies among Cosmological Parameters Derived from Measurements of Microwave Background Anisotropies”. In:Monthly Notices of the Royal Astronomical Society 294.2 (1997), pp. 337–348. doi: 10.1093/mnras/294.2.337
-
[65]
Fun- damental limits on constraining primordial non-Gaussianity
Alba Kalaja, P. Daniel Meerburg, and William R. Pimentel Guilherme L.and Coulton. “Fun- damental limits on constraining primordial non-Gaussianity”. In: Journal of Cosmology and Astroparticle Physics 2021.04 (Apr. 2021), p. 050. issn: 1475-7516. doi: 10 . 1088 / 1475 - 7516/2021/04/050. url: http://dx.doi.org/10.1088/1475-7516/2021/04/050. A Weak Lensing ...
-
[66]
Xℓ(−ℓ), Xℓ(−ℓ+1), · · ·, Xℓ(ℓ−1), Xℓℓ
By definition ⟨XℓmX ′ ℓ′m′⟩ = (2π)3δℓℓ′δmm′CXX ′ ℓ , so you can average over the measurements done for different values ofm, i.e. Xℓ(−ℓ), Xℓ(−ℓ+1), · · ·, Xℓ(ℓ−1), Xℓℓ. This results in the (2 ℓ + 1)−1 factor in the power spectrum covariance. – 28 –
-
[67]
This is where experimental noise is incorporated into the calculation
The tilde is used to denote the power spectrum as calculated earlier, plus the noise power spectrum, N XX ′ ℓ , which is the power spectrum of the noise associated with the estimator of the field. This is where experimental noise is incorporated into the calculation. Under the Gaussian approximation, the covariance matrix vanishes except for 3 × 3 block m...
-
[68]
d.p.” stands for “distinct permutations
vanishes. It can then be shown that the entries of each block matrix are given as (Covℓ1ℓ2ℓ3)XY Z,X ′Y ′Z′ = ˜CXX ′ ℓ1 ˜CY Y ′ ℓ2 ˜CZZ ′ ℓ3 + δℓ1ℓ2 ˜CXY ′ ℓ1 ˜CY X ′ ℓ2 ˜CZZ ′ ℓ3 + δℓ2ℓ3 ˜CXX ′ ℓ1 ˜CY Z ′ ℓ2 ˜CZX ′ ℓ3 +δℓ3ℓ1 ˜CXZ ′ ℓ1 ˜CY Y ′ ℓ2 ˜CZX ′ ℓ3 + δℓ1ℓ2δℓ2ℓ3 ˜CXY ′ ℓ1 ˜CY Z ′ ℓ2 ˜CZX ′ ℓ3 + ˜CXZ ′ ℓ1 ˜CY X ′ ℓ2 ˜CZY ′ ℓ3 . With our ordering, thi...
-
[69]
All survey parameters are the same as in section 4. weak priors CMB lensing Gal. lensing CMB × Gal. lensing Par prior Cℓ Bℓ1 ℓ2 ℓ3 Cℓ + Bℓ1 ℓ2 ℓ2 Cℓ Bℓ1 ℓ2 ℓ3 Cℓ + Bℓ1 ℓ2 ℓ3 Cℓ Bℓ1 ℓ2 ℓ3 Cℓ + Bℓ1 ℓ2 ℓ3 H0 17 17 16 6.5 13 4.2 1.8 1.6 1.5 1.0 103Ωbh2 0.50 0.50 0.50 0.50 0.50 0.48 0.48 0.50 0.48 0.46 Ωch2 0.29 0.0070 0.012 0.0063 0.0095 0.0049 0.0041 0.0050 ...
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.