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Optimization of nanotube thermal interconnects for near-field radiative heat transport
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10.1063/1.4745202
/content/aip/journal/apl/101/6/10.1063/1.4745202
http://aip.metastore.ingenta.com/content/aip/journal/apl/101/6/10.1063/1.4745202

Figures

Image of FIG. 1.
FIG. 1.

(a) and (b) Schematic representation of the vertical forest of identical metallic SWNTs of length L and radius R placed at a distance d above the substrate. (c) and (d) G, Kapitza conductance as a function of ωr and ωp , electron relaxation and plasma frequencies, and polariton frequency, ωpol , for a vertical forest of identical metallic (15,0) SWNTs of length L = 500 nm, and different metallic (c) and polar dielectric (d) substrates at , and distance d = 3.4 Å.

Image of FIG. 2.
FIG. 2.

(a) Spectral Kapitza conductance, , for the same system as in Fig. 1, and (b) dielectric contrast of the interface as a function of frequency.

Image of FIG. 3.
FIG. 3.

Spectral Kapitza conductance, , for the same system as in Fig. 1 as a function of frequency.

Image of FIG. 4.
FIG. 4.

Kapitza conductance, G, between the vertical forest of identical metallic SWNTs and different substrates as a function of (a) SWNT length L (for R = 0.59 nm) and (b) SWNT radius R (for L = 500 nm). d = 3.4 Å, . .

Image of FIG. 5.
FIG. 5.

Temperature dependence of the Kapitza conductance, G, between vertical forest of identical (15,0) metallic SWNTs and (a) dielectric or (b) metal interfaces. d = 3.4 Å, , L = 500 nm.

Tables

Generic image for table
Table I.

Kapitza conductance, G, between the vertical forest of identical metallic (15,0) SWNTs of length L = 500 nm and different substrates. , d = 3.4 Å, .

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/content/aip/journal/apl/101/6/10.1063/1.4745202
2012-08-08
2014-04-17
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Optimization of nanotube thermal interconnects for near-field radiative heat transport
http://aip.metastore.ingenta.com/content/aip/journal/apl/101/6/10.1063/1.4745202
10.1063/1.4745202
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