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The point-contact spectroscopy technique actually measures, in the limit of ballistic transport, a spin polarization at (Formula presented) given by (Formula presented) which is weighted by the relative Fermi velocities (Formula presented) for spin-up and spin-down electrons as opposed to the unweighted P relevant to the present analysis. The level of the pseudogap in (Formula presented) [dashed line in inset to Fig. 33(a)] is set to give simply (Formula presented) at (Formula presented) neglecting the Fermi velocity weighting for now.
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The point-contact spectroscopy technique actually measures, in the limit of ballistic transport, a spin polarization at (Formula presented) given by (Formula presented) which is weighted by the relative Fermi velocities (Formula presented) for spin-up and spin-down electrons as opposed to the unweighted P relevant to the present analysis. The level of the pseudogap in (Formula presented) [dashed line in inset to Fig. 33(a)] is set to give simply (Formula presented) at (Formula presented) neglecting the Fermi velocity weighting for now.
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