Symmetry group analysis partitions 2^n current configurations on an n-terminal ring into orbits labeled by winding number W; for n=3, non-reciprocal responses appear only after simultaneous T and I breaking, with geometry selecting allowed patterns, as shown in a three-quantum-dot superconducting to
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Symmetry Classification of Non-Reciprocal Responses in Multiterminal Ring Devices
Symmetry group analysis partitions 2^n current configurations on an n-terminal ring into orbits labeled by winding number W; for n=3, non-reciprocal responses appear only after simultaneous T and I breaking, with geometry selecting allowed patterns, as shown in a three-quantum-dot superconducting to