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The Power Spectrum of the Sunyaev-Zel'dovich Effect
Astrophysics · Submitted 9 Dec 1999
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim For cluster- normalized CDM models, the SZ power spectrum is comparable to the primordial power spectrum around l=2000.
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The abstract, sentence by sentence
(Abridged) The hot gas in the IGM produces anisotropies in the Cosmic Microwave Background (CMB) through the thermal Sunyaev-Zel'dovich (SZ) effect. The SZ effect is a powerful probe of large-scale structure in the universe and must be carefully subtracted from measurements of the primary CMB anisotropies. We use moving-mesh hydrodynamical simulations to study the 3-dimensional statistics of the gas, and compute the mean comptonization parameter and the angular power spectrum of the SZ fluctuations, for different cosmologies. We compare these results with predictions using the Press-Schechter formalism. We find that the two methods agree approximately, but differ in details. We discuss this discrepancy, and show that resolution limits the reliability of our results to the 200<l<2000 range. For cluster- normalized CDM models, the SZ power spectrum is comparable to the primordial power spectrum around l=2000. We show that groups and filaments (kT<5 keV) contribute about 50% of the SZ power spectrum at l=500. About half of the SZ power spectrum on these scales is produced at redshifts z<0.1, and can thus be detected and removed using existing catalogs of galaxies and X-ray clusters. We discuss the implications of these results for the future MAP and Planck Surveyor missions.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | (Abridged) The hot gas in the IGM produces anisotropies in the Cosmic Microwave Background (CMB) through the thermal Sunyaev-Zel'dovich (SZ) effect. | background 1.00 | 0.05 | 0.04 | asserted 1.00 |
| s1 | The SZ effect is a powerful probe of large-scale structure in the universe and must be carefully subtracted from measurements of the primary CMB anisotropies. | background 1.00 | 0.06 | 0.05 | asserted 1.00 |
| s2 | We use moving-mesh hydrodynamical simulations to study the 3-dimensional statistics of the gas, and compute the mean comptonization parameter and the angular power spectrum of the SZ fluctuations, for different cosmologies. | method 0.72 | 0.97 | 0.06 | asserted 0.98 |
| s3 | We compare these results with predictions using the Press-Schechter formalism. | method 0.90 | 0.87 | 0.03 | asserted 0.74 |
| s4 | We find that the two methods agree approximately, but differ in details. | result 1.00 | 0.94 | 0.11 | asserted 0.99 |
| s5 | We discuss this discrepancy, and show that resolution limits the reliability of our results to the 200<l<2000 range. | limitation 1.00 | 0.91 | 0.07 | asserted 1.00 |
| s6 | For cluster- normalized CDM models, the SZ power spectrum is comparable to the primordial power spectrum around l=2000. | result 1.00 | 0.88 | 0.29 | asserted 1.00 |
| s7 | We show that groups and filaments (kT<5 keV) contribute about 50% of the SZ power spectrum at l=500. | result 1.00 | 0.94 | 0.13 | asserted 1.00 |
| s8 | About half of the SZ power spectrum on these scales is produced at redshifts z<0.1, and can thus be detected and removed using existing catalogs of galaxies and X-ray clusters. | result 0.78 | 0.88 | 0.15 | asserted 0.99 |
| s9 | We discuss the implications of these results for the future MAP and Planck Surveyor missions. | interpretation 0.90 | 0.42 | 0.05 | unclear 0.90 |
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Original abstract
(Abridged) The hot gas in the IGM produces anisotropies in the Cosmic Microwave Background (CMB) through the thermal Sunyaev-Zel'dovich (SZ) effect. The SZ effect is a powerful probe of large-scale structure in the universe and must be carefully subtracted from measurements of the primary CMB anisotropies. We use moving-mesh hydrodynamical simulations to study the 3-dimensional statistics of the gas, and compute the mean comptonization parameter and the angular power spectrum of the SZ fluctuations, for different cosmologies. We compare these results with predictions using the Press-Schechter formalism. We find that the two methods agree approximately, but differ in details. We discuss this discrepancy, and show that resolution limits the reliability of our results to the 200<l<2000 range. For cluster- normalized CDM models, the SZ power spectrum is comparable to the primordial power spectrum around l=2000. We show that groups and filaments (kT<5 keV) contribute about 50% of the SZ power spectrum at l=500. About half of the SZ power spectrum on these scales is produced at redshifts z<0.1, and can thus be detected and removed using existing catalogs of galaxies and X-ray clusters. We discuss the implications of these results for the future MAP and Planck Surveyor missions.
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References
How the literature uses it
16 arXiv papers cite this in 21 sentences
Papers citing it · 13 sentences without a confident label
Uses its data or values 2 papers
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The amplitude of these signals is more uncertain, but even within our standard cosmological paradigm, one expects an average $y$-parameter of $y≃10^-7-10^-6$ due to the large-scale structure and the reionization epoch [ref] , with the most recent computations giving $y≃2-6$ [ref] .
Spectral distortions of the CMB dipole · Introduction · 0.91
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Several estimates for this contribution were obtained, yielding values for the total $y$-parameter at the level $y≃few-6$ [ref] .
The Cosmic Microwave Background: Spectral Distortions · Reionization and structure formation · 0.88
Cites it as background 5 papers
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The mean electron pressure $⟨P_e⟩$ is related to the density-weighted mean temperature of electrons in the universe, defined as $T̅_e ≡⟨n_eT_e⟩/⟨n_e⟩$ [ref] .
Testing the SZ-based tomographic approach to the thermal history of the universe with pressure-density cross-correlations: Insights from the Magneticum simulation · The density-weighted mean electron temperature Te · 0.96
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The contribution from the peaks in the large scale structure and the effect of baryonic physics to the $y$-type distortion fluctuations has been studied by many groups using numerical simulations as well as analytically [ref] .
Limits on the fluctuating part of $y$-type distortion monopole from Planck and SPT results · Introduction · 0.87
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However, we have many astrophyscial/cosmological sources inducing spectral distortions: decaying or annihilating particles [ref] , reionization and structure formation [ref] , primordial black holes [ref] , cosmic strings [ref] , small-scale magnetic fields [ref] , the adiabatic cooling of matter [ref] , cosmological recombination [ref] , gravitino decay [ref] , and the dissipation of primordial density perturbations [ref] which is the main concern of this paper.
CMB Spectral $\mu$-Distortion of Multiple Inflation Scenario · Introduction · 0.94
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