2011
DOI: 10.1103/physrevb.83.153417
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Enhanced thermopower under a time-dependent gate voltage

Abstract: We derive formal expressions of time-dependent energy and heat currents through a nanoscopic device using the Keldysh nonequilibrium Green function technique. Numerical results are reported for a metal/dot/metal junction where the dot level energy is abruptly changed by a step-shaped voltage pulse. Analytical linear responses are obtained for the time-dependent thermoelectric coefficients. We show that the Seebeck coefficient can be enhanced in the transient regime up to an amount (here rising 40%) controlled … Show more

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Cited by 58 publications
(45 citation statements)
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“…Here, the nanoscale system itself provides the strong energy dependence required for thermoelectric effects, both through strong size-quantization and Coulomb interaction. Models of this kind are relevant in many thermoelectric studies [38,[42][43][44][45] and the duality applies to their description, even when the energy-independent coupling is strong and the temperature is low [29], cf. [36,37].…”
Section: Overview Of Main Ideas and Resultsmentioning
confidence: 99%
“…Here, the nanoscale system itself provides the strong energy dependence required for thermoelectric effects, both through strong size-quantization and Coulomb interaction. Models of this kind are relevant in many thermoelectric studies [38,[42][43][44][45] and the duality applies to their description, even when the energy-independent coupling is strong and the temperature is low [29], cf. [36,37].…”
Section: Overview Of Main Ideas and Resultsmentioning
confidence: 99%
“…For the time-dependent heat current due to electrons, the transient heat current has been investigated for a quantum dot under an upward pulse of gate voltage within the WBL where the enhanced thermal power was observed [31]. It is desirable to study the transient heat current when the external bias is switched on.…”
Section: Introductionmentioning
confidence: 99%
“…In the case of P ac , since it is a second-order quantity, it has a contribution not only of the frozen solutions but also of the corrections ∆λ V,ω (t) and ∆B 2 V,ω (t). Explicit expressions of the Onsager coefficients L 21 and L 22 in terms of the frozen solutions and the corrections can be found in Appendix C, where we also show the validity of the Onsager reciprocal relation (30), and that the dissi-pative coefficient reads…”
Section: Transport Coefficientsmentioning
confidence: 58%