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The differential conductance below Tc (dI/dV)S, divided by the normal state conductance (dI/dV)N is given by the half sphere integration over solid angle38 :where E is the quasiparticle energy and N is the incidence angle (relative to the interface normal) in the normal material, N is the conductance from normal to normal material with the same geometry, andwhere electron like and hole like quasiparticle effective pair potentials with the corresponding phases i.In case of c axis tunnelling, the hole like and the electron like quasiparticles transmitted into the superconductor experience the same effective pair potentials, which have similar dependence on the azimuthal angle in the ab plane . The total Andreev reflection spectrum is obtained by calculating the reflection and the transmission in the proximity region, followed by reflection at the interface between the two materials. The calculated spectra in this two stage scattering model with the modified gaps as fit parameters show good agreement with the experimental conductance measurements (Fig.