Fig. 4.
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Marginalised 1σ errors on cosmological parameters relative to their corresponding fiducial value for the pessimistic baseline case, which equals to |fR0| = 5 × 10−6. We show results for GCsp (purple); WL (blue); GCsp + WL (orange); the combination of all photometric probes, including cross correlations, WL + GCph + XCph (red); and the combination of all spectroscopic and photometric probes, GCsp + WL + GCph + XCph, (yellow). One can see that the constraints on log10|fR0| and σ8 are similar among GCsp and WL, but for other parameters such as the Hubble parameter, h, or the fraction of baryons, Ωb, 0, the constraints coming from GCsp alone are even more stringent than the constraints of all photometric probes combined on their own.
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