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Fig. 1

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Large-scale structure observables for the different MG models evaluated at the fiducial values of the model parameters used for the Fisher matrix analysis. Top left: linear (dashed) and non-linear (solid lines) matter power spectrum Pδδ(z, k) entering Eqs. (36) and (30), respectively, evaluated at redshift ζ = 0, for KM1 (ϵ2,0 = –0.04, blue), JBD1 (ωBD = 800, red) and nDGPl (Ωrc = 0.25, green). Top right: ratio of the matter power spectra for the above mentioned models with respect to their ΛCDM counterpart with the same value of σ8 today, for the linear (dashed) and non-linear (solid) cases. Bottom left: cosmic shear (WL) angular power spectra for the auto-correlation of the first photometric bin C1,1WL()$C_{1,1}^{{\rm{WL}}}(\ell )$ (solid line) and the cross-correlation of the first and last bin C1,10WL()$C_{1,10}^{{\rm{WL}}}(\ell )$ (dotted line), defined in Eq. (30) for the three models considered above, with the same colour labelling. Bottom right: ratio of the cosmic shear Ci,j() to their ΛCDM counterpart, for the bin combination i = j = 1 and i = 1; j = 10.

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