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Expanding the logarithm to first-order leads to a term S(1) eff = 2gnR Z dt Xq(t), (17) where nR = −i R dω 2π G< RR(ω)

The photon perspective The effective action for the photons takes the form iSeff[X] = iS0[X] + tr ln −i(1 − ˇG0 ◦ ˇV ) , (16) where ◦ denotes a temporal convolution

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Simulating electron-vibron energy transfer with quantum dots and resonators

cond-mat.mes-hall · 2024-07-03 · unverdicted · novelty 4.0

The work shows a gate-tunable interference effect in a voltage-biased triple quantum dot system that produces a minimum in charge current coinciding with a maximum in energy transfer to a capacitively coupled damped resonator representing a vibrational mode.

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  • Simulating electron-vibron energy transfer with quantum dots and resonators cond-mat.mes-hall · 2024-07-03 · unverdicted · none · ref 1

    The work shows a gate-tunable interference effect in a voltage-biased triple quantum dot system that produces a minimum in charge current coinciding with a maximum in energy transfer to a capacitively coupled damped resonator representing a vibrational mode.