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Effect of the energy dependence of the carrier scattering time on the thermoelectric power factor of quantum wells and nanowires
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10.1063/1.4729381
/content/aip/journal/apl/100/24/10.1063/1.4729381
http://aip.metastore.ingenta.com/content/aip/journal/apl/100/24/10.1063/1.4729381
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(a) as a function of film thickness for the range of p values investigated. The black arrow indicates the trend of increasing p. Starting with the bottom curve, the values of p are −0.8, −0.5, −0.2, 0 (CRTA), 0.2, 0.4, 0.5, 0.8, 1, and 1.5. (b) Bulk values as a function of p.

Image of FIG. 2.
FIG. 2.

(a) Bulk normalized as a function of p and film thickness a. The contour line of value 1, where equals the bulk value, is highlighted by the dashed black line. The solid black line traces the valley, and the inset shows this minimum value as a function of p. (b) Bulk normalized as a function of p and nanowire radius r. Dashed black line marks where equals the bulk value. The solid black line traces the valley and the inset shows this minimum value as a function of p. Note that in both (a) and (b) the vertical axis of the color scale bar is not scaled linearly.

Image of FIG. 3.
FIG. 3.

(a) Scattering times , , and the total as a function of carrier energy. (b) as a function of film thickness for p 1= −0.5, p 2= 0.4, and various ratios of coefficients C 1 and C 2. The black arrow indicates the trend of increasing C 1 /C 2.

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/content/aip/journal/apl/100/24/10.1063/1.4729381
2012-06-13
2014-04-20
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Effect of the energy dependence of the carrier scattering time on the thermoelectric power factor of quantum wells and nanowires
http://aip.metastore.ingenta.com/content/aip/journal/apl/100/24/10.1063/1.4729381
10.1063/1.4729381
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