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Fig. 1.

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Angular power spectrum (blue dots) estimated with the NLIC method, with 1σ Fisher errors. These error bars include cosmic variance, approximated as Gaussian (see Fig. 1 in Planck Collaboration VI 2020). The ΛCDM best fit model (), with a power-law fluctuation distribution and kmin = 0, is shown in black. The red curve (for kmin = 2.82/rdec) is the best fit to the whole range of ’s with an optimized kmin ≠ 0. The two curves are indistinguishable at  ≳ 6, but deviate significantly from each other for the low multipole moments, corresponding to large angles (≳60°). The Sachs-Wolfe contribution to dominates at  ≲ 30, while local physical effects, such as acoustic oscillations, dominate at  ≳ 30.

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