Non-commutative system-bath couplings in the NESB model enhance heat current, optimize rectification, and alter scaling laws at weak coupling and adiabatic limits.
Here we have ˙QX 2 (t) = dQX 2 (t)/dt and the Bose-Einstein distribution function nν(ω) = 1 /(exp(βνω)− 1)
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Unusual Transport Properties with Non-Commutative System-Bath Coupling Operators
Non-commutative system-bath couplings in the NESB model enhance heat current, optimize rectification, and alter scaling laws at weak coupling and adiabatic limits.