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The expression forI (B) Q (ω) = n ˆΣa,α ˆG2,2 α,a o+,− is deduced fromI (A) Q (ω)in Eq

Taking into account the other component of the spectral supercurrent In this subsubsection of the SM, we present the final step in the evaluation of the quartet current susceptibil

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Floquet-Multiple Andreev Reflections

cond-mat.mes-hall · 2026-05-04 · unverdicted · novelty 6.0

Quartet and higher-order processes in three-terminal ballistic Josephson junctions produce Floquet-MAR conductance and noise resonances parameterized by bias voltage and electrochemical potential.

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  • Floquet-Multiple Andreev Reflections cond-mat.mes-hall · 2026-05-04 · unverdicted · none · ref 61

    Quartet and higher-order processes in three-terminal ballistic Josephson junctions produce Floquet-MAR conductance and noise resonances parameterized by bias voltage and electrochemical potential.