1972
DOI: 10.1016/0022-3093(72)90146-9
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Investigation of thermal conductivity of semiconducting melts

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1974
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Cited by 14 publications
(4 citation statements)
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“…10 However, at high temperatures (>700 °C), the increase in κ in bulk RTG SiGe alloys is attributed to the bipolar effect. 10,66 On the other hand in nanostructured samples, the carriers are dominantly scattered by nanoscale defects whereas at higher temperatures these charge carriers are dominantly scattered by acoustic phonons. 17 The κ comprises of contributions from both lattice (κ L ) and electronic (κ e ) parts with κ e being related to σ by the Wiedemann-Franz law, 67 κ e = LσT.…”
Section: Thermal Transportmentioning
confidence: 99%
“…10 However, at high temperatures (>700 °C), the increase in κ in bulk RTG SiGe alloys is attributed to the bipolar effect. 10,66 On the other hand in nanostructured samples, the carriers are dominantly scattered by nanoscale defects whereas at higher temperatures these charge carriers are dominantly scattered by acoustic phonons. 17 The κ comprises of contributions from both lattice (κ L ) and electronic (κ e ) parts with κ e being related to σ by the Wiedemann-Franz law, 67 κ e = LσT.…”
Section: Thermal Transportmentioning
confidence: 99%
“…The σ of Bi 2 Te 3 is consistently positively correlated with pressure, as shown in figures 6(a) and (d), which is related to the increased carrier mobility at high pressure [51]. The carrier scattering mechanism of semiconductors is generally dominated by acoustic wave scattering from lattice vibrations [52], in which case their carrier mobility (µ) generally versus temperature by µ ∝ T −α ,where α is a positive constant, demonstrates the negative correlation between mobility and temperature. Therefore, according to σ = neµ [53], the flat or slightly increasing trend of σ with temperature in figure 6(a) is due to the increase in carrier concentration (n).…”
Section: Resultsmentioning
confidence: 93%
“…The Wiedemann-Franz law is applied to estimate k e ¼ sLT, where L ¼ 2.44 Â 10 À8 W U K À2 denotes the Lorenz number and s the measured electrical conductivity at a given temperature T. The upturn behavior of k can be attributed to bipolar contribution to the electronic thermal conductivity. Hence, we consider the bipolar contribution of the thermal conductivity k bp , which can be expressed using the following equation 44,45 k bp ¼ 3LsT…”
Section: Resultsmentioning
confidence: 99%
“…The upturn behavior of κ can be attributed to bipolar contribution to the electronic thermal conductivity. Hence, we consider the bipolar contribution of the thermal conductivity κ bp , which can be expressed using the following equation 44,45 where E g is calculated using the Arrhenius relationship. The combined results ( κ e + κ bp ) for electronic contribution to the thermal conductivity are illustrated in Fig.…”
Section: Resultsmentioning
confidence: 99%