2009
DOI: 10.1007/s10955-009-9697-1
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ThermoElectric Transport Properties of a Chain of Quantum Dots with Self-Consistent Reservoirs

Abstract: We introduce a model for charge and heat transport based on the Landauer-Büttiker scattering approach. The system consists of a chain of N quantum dots, each of them being coupled to a particle reservoir. Additionally, the left and right ends of the chain are coupled to two particle reservoirs. All these reservoirs are independent and can be described by any of the standard physical distributions: Maxwell-Boltzmann, FermiDirac and Bose-Einstein. In the linear response regime, and under some assumptions, we fir… Show more

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Cited by 37 publications
(49 citation statements)
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References 59 publications
(112 reference statements)
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“…57 . To simulate a thermal gradient and compute the thermopower, however, we have also to selfconsistently set the temperature of the thermal environment, which we compute via the voltage-temperature probe method 61,64 . We begin with a general presentation of the VTP technique.…”
Section: Method: Voltage-temperature Probementioning
confidence: 99%
“…57 . To simulate a thermal gradient and compute the thermopower, however, we have also to selfconsistently set the temperature of the thermal environment, which we compute via the voltage-temperature probe method 61,64 . We begin with a general presentation of the VTP technique.…”
Section: Method: Voltage-temperature Probementioning
confidence: 99%
“…The advantage of such ap-proach lies in its simplicity and independence from microscopic details of inelastic processes. Probe terminals have been widely used in the literature and proved to be useful to unveil nontrivial aspects of phase-breaking processes [49], heat transport and rectification [22,23,118,52,24,112,13,120], and thermoelectric transport [73,57,56,75,76,124,126,135,136,122,67,15,11,27,25]. The approach can be generalized to any number n p of probe reservoirs.…”
Section: Inelastic Scattering and Probe Terminalsmentioning
confidence: 99%
“…We have previously [40] studied the asymmetric forces in this system neglecting the coupling to electrode phonons. Figure 1 shows the average excess kinetic energy [ΔE n ¼ E n ðeVÞ − E n ð0Þ] [41][42][43][44][45][46] of atoms along the chain for three different Fermi levels E F . The structure is almost mirror symmetric.…”
Section: H Y S I C a L R E V I E W L E T T E R S Week Ending 6 March mentioning
confidence: 99%