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Fig. 3.

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Binned mixing matrices as band-pass filters and the physical scales mixed for each redshift tomographic bin edge. Top: redshift as a function of multipole for different wave-numbers. The coloured horizontal dashed-lines are the centre of the redshift tomographic bins used in the analysis and shown in Fig. 1; the black lines are curves of constant wavenumber, k = /χ(z), in units of h Mpc−1 for a given and z, where χ(z) is the co-moving distance. Bottom: the KiDS-1000 pseudo-Cs binned mixing matrices (see Fig. 2, for example). These are convolved with the theory Cs (see Eq. (23)) to model the effect of multipole mixing introduced by the survey mask. The filters are calculated using all the multipoles inside the eight log-spaced bandwidths from 76 ≤  ≤ 1500.

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