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1980
DOI: 10.1177/107769908005700318
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Cited by 4 publications
(2 citation statements)
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“…b The power-law model for the primordial spectrum is P(k) = ∆ 2 R k k 0 ns−1 ther varies significantly as the cosmological parameters are varied within their errors in the flat cosmology we consider in this work. The P (k) constraints from the CMB alone overlap well with the power spectrum measurements from the SDSS DR7 LRG sample (Reid et al 2010), which have been deconvolved from their window functions. The ACT data allow us to probe the power spectrum today at scales 0.001 < k < 0.19 Mpc −1 using only the CMB, improving on previous constraints using microwave data.…”
Section: Reconstructed P (K)mentioning
confidence: 53%
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“…b The power-law model for the primordial spectrum is P(k) = ∆ 2 R k k 0 ns−1 ther varies significantly as the cosmological parameters are varied within their errors in the flat cosmology we consider in this work. The P (k) constraints from the CMB alone overlap well with the power spectrum measurements from the SDSS DR7 LRG sample (Reid et al 2010), which have been deconvolved from their window functions. The ACT data allow us to probe the power spectrum today at scales 0.001 < k < 0.19 Mpc −1 using only the CMB, improving on previous constraints using microwave data.…”
Section: Reconstructed P (K)mentioning
confidence: 53%
“…The data points between 0.02 < k < 0.19 Mpc −1 show the SDSS DR7 LRG sample, and have been deconvolved from their window functions, with a bias factor of 1.18 applied to the data. This has been rescaled from the Reid et al (2010) 2011). The bottom panel shows the same data plotted on axes where we relate the power spectrum to a mass variance, ∆ M /M, and illustrates how the range in wavenumber k (measured in Mpc −1 ) corresponds to range in mass scale of over 10 orders of magnitude.…”
Section: Discussionmentioning
confidence: 99%