In multivalley SNS junctions, constant-voltage I-V curves show two peaks at voltages set by inelastic and inter-valley relaxation times that can exceed Ic(T), while constant-current bias yields nonlinear resistance orders of magnitude below the normal-state value.
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Altermagnets enable planar Josephson junctions that host Majorana end modes controlled by crystallographic orientation, extending naturally to high-Tc platforms.
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I-V characteristics of SNS junctions with a multivalley normal region
In multivalley SNS junctions, constant-voltage I-V curves show two peaks at voltages set by inelastic and inter-valley relaxation times that can exceed Ic(T), while constant-current bias yields nonlinear resistance orders of magnitude below the normal-state value.
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Topological altermagnetic Josephson junctions
Altermagnets enable planar Josephson junctions that host Majorana end modes controlled by crystallographic orientation, extending naturally to high-Tc platforms.