2016
DOI: 10.1016/j.crhy.2016.08.005
|View full text |Cite
|
Sign up to set email alerts
|

Nonlinear phenomena in quantum thermoelectrics and heat

Abstract: We review recent developments in nonlinear quantum transport through nanostructures and mesoscopic systems driven by thermal gradients or in combination with voltage biases. Low-dimensional conductors are excellent platforms to analyze both the thermoelectric and heat dynamics beyond linear response because due to their small size a small temperature difference applied across regions gives rise to large thermal biases. We offer a theoretical discussion based on the scattering approach to highlight the differen… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3

Citation Types

0
54
0
1

Year Published

2017
2017
2024
2024

Publication Types

Select...
9

Relationship

3
6

Authors

Journals

citations
Cited by 67 publications
(55 citation statements)
references
References 107 publications
0
54
0
1
Order By: Relevance
“…In these examples the charge carriers are electrons and the sign change of the thermopower means that they travel from the cold side to the hot side, which may appear counterintuitive. Other nonlinear effects can occur if the characteristic relaxation length of electrons and or phonons exceeds the sample size [10], because the energy of electrons and/or phonons is no longer controlled by the temperature of the bath, but by the generated electric bias, including Coulomb interactions [11,12].Observing such negative thermopower at the nanoscale is difficult for at least two reasons: the currents tend to be small and it is hard to maintain a constant temperature difference across such short distances. Here we argue that a generic class of tubular nanowires, to be defined in more detail below, are ideal systems for both realizing and observing negative thermopower.…”
mentioning
confidence: 99%
See 1 more Smart Citation
“…In these examples the charge carriers are electrons and the sign change of the thermopower means that they travel from the cold side to the hot side, which may appear counterintuitive. Other nonlinear effects can occur if the characteristic relaxation length of electrons and or phonons exceeds the sample size [10], because the energy of electrons and/or phonons is no longer controlled by the temperature of the bath, but by the generated electric bias, including Coulomb interactions [11,12].Observing such negative thermopower at the nanoscale is difficult for at least two reasons: the currents tend to be small and it is hard to maintain a constant temperature difference across such short distances. Here we argue that a generic class of tubular nanowires, to be defined in more detail below, are ideal systems for both realizing and observing negative thermopower.…”
mentioning
confidence: 99%
“…In these examples the charge carriers are electrons and the sign change of the thermopower means that they travel from the cold side to the hot side, which may appear counterintuitive. Other nonlinear effects can occur if the characteristic relaxation length of electrons and or phonons exceeds the sample size [10], because the energy of electrons and/or phonons is no longer controlled by the temperature of the bath, but by the generated electric bias, including Coulomb interactions [11,12].…”
mentioning
confidence: 99%
“…In contrast, we are here interested in the regime where a normal current is transformed into a supercurrent as in the Andreev reflection. The issue is interesting in view of recent developments in the field of nonlinear quantum thermoelectrics [33] and its connection to spin caloritronics (i.e., the production of spin currents with thermal means) in superconductors [34].…”
Section: Introductionmentioning
confidence: 99%
“…Despite the fact that nonlinear thermoelectrics [20] in Kondo-correlated systems is quite a new topic, there is already a number of interesting results in the last years. Most of them are focused on the study of the Seebeck coefficient S = V th θ employing a large variety of methods: nonperturbative resonant tunneling approximation [21], second-order perturbation theory for the onsite Coulomb interaction [22], slave-boson noncrossing approximation (NCA) [23], generalized Keldyshbased NCA [24], nonequilibrium Green's functions beyond Hartree-Fock [25], quantum [26] and auxiliary [27] master equation approaches and dual fermions renormalized perturbation theory [28].…”
Section: Introductionmentioning
confidence: 99%