2008
DOI: 10.1140/epjb/e2008-00195-8
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Quantum thermal transport in nanostructures

Abstract: In this colloquia review we discuss methods for thermal transport calculations for nanojunctions connected to two semi-infinite leads served as heat-baths. Our emphases are on fundamental quantum theory and atomistic models. We begin with an introduction of the Landauer formula for ballistic thermal transport and give its derivation from scattering wave point of view. Several methods (scattering boundary condition, mode-matching, Piccard and Caroli formulas) of calculating the phonon transmission coefficients … Show more

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Cited by 564 publications
(547 citation statements)
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References 222 publications
(342 reference statements)
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“…For diffusive systems, the answer is given by Fourier's law [11][12][13] which is true only in the linear response regime, i.e., when the temperature difference between the baths is small. However for harmonic or ballistic systems, the heat current is given by a Landauer-like formula [3,7,10] which was first derived for electronic transport. Landauer formula on the contrary to the Fourier's law is true for arbitrary temperature differences between the leads.…”
Section: Introductionmentioning
confidence: 99%
“…For diffusive systems, the answer is given by Fourier's law [11][12][13] which is true only in the linear response regime, i.e., when the temperature difference between the baths is small. However for harmonic or ballistic systems, the heat current is given by a Landauer-like formula [3,7,10] which was first derived for electronic transport. Landauer formula on the contrary to the Fourier's law is true for arbitrary temperature differences between the leads.…”
Section: Introductionmentioning
confidence: 99%
“…1), and finally thermal conductance σ is obtained by Landauer formula. 15 Since GNRs with larger width (W) will have more phonon transport channels and thus larger thermal conductance, the scaled thermal conductance, defined as thermal conductance per unit area (σ/S ), is introduced to describe thermal transport properties for materials with different widths. Herein, the cross sectional area S is defined to be S = Wδ, where δ = 0.335 nm is chosen as the layer separation in graphite.…”
mentioning
confidence: 99%
“…Finally, to self-consistently compute the I-V characteristics of the models after CASTEP geometry optimization in Fig. 6, the I-V characteristics of these systems were calculated using DFT with the non-equilibrium Green's function (NEGF) 35 approach in density functional tight binding and much more (DFTB+) 36 code. The case in which the left (right) electrode was the positive (negative) was defined as the application of a positive bias along the z axis.…”
Section: A Methodologymentioning
confidence: 99%