Andreev Reflection and Pair Breaking Effects at the Superconductor/Magnetic Semiconductor Interface
R.P. Panguluri, K.C. Ku, T. Wojtowicz, X. Liu, J.K. Furdyna, Y.B., Lyanda-Geller, N. Samarth, B. Nadgorny

TL;DR
This study examines Andreev reflection at superconductor/magnetic semiconductor interfaces, revealing pair-breaking effects in ferromagnetic (Ga,Mn)As that influence conductance spectra and enable spin polarization measurement.
Contribution
It demonstrates that pair-breaking effects in (Ga,Mn)As affect Andreev reflection spectra and introduces a method to evaluate spin polarization in magnetic semiconductors.
Findings
Conventional Andreev reflection observed in non-magnetic (Ga,Be)As.
Conductance spectra in ferromagnetic (Ga,Mn)As show broadened density of states.
Estimated spin polarization in (Ga,Mn)As is 83+/-17%.
Abstract
We investigate the applicability of spin polarization measurements using Andreev reflection in a point contact geometry in heavily doped dilute magnetic semiconductors, such as (Ga,Mn)As. While we observe conventional Andreev reflection in non-magnetic (Ga,Be)As epilayers, our measurements indicate that in ferromagnetic (Ga,Mn)As epilayers with comparable hole concentration the conductance spectra can only be adequately described by a broadened density of states and a reduced superconducting gap. We suggest that these pair-breaking effects stem from inelastic scattering in the metallic impurity band of (Ga,Mn)As and can be explained by introducing a finite quasiparticle lifetime or a higher effective temperature. For (Ga,Mn)As with 8% Mn concentration and 140 K Curie temperature we evaluate the spin polarization to be 83+/-17%. PACS numbers: 72.25.Dc,72.25.Mk,74.45.+c
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