next up previous contents
Next: 5.2 The Long-Wavelength Problem Up: 5. Anomalous Diameter Dependence of Thermal Conductivity in Ultra-Thin Silicon Nanowires Previous: 5. Anomalous Diameter Dependence of Thermal Conductivity in Ultra-Thin Silicon Nanowires   Contents

5.1 Phonon Transmission Function

Figure 5.1: The normalized transmission function for silicon nanowires of diameters $ D=1~\mathrm{nm}$ (blue), $ 2~\mathrm{nm}$ (red) and $ 12~\mathrm{nm}$ (green). Inset: The density of phonon states per unit volume for the same diameters.
Image TransmissionDOS

Figure. 5.1 depicts the transmission function per unit area as a function of frequency for $ \textless 100\textgreater$ nanowires of diameters $ D=12~\mathrm{nm}$ , $ 2~\mathrm{nm}$ , and $ 1~\mathrm{nm}$ . The inset of Fig. 5.1 shows the density of states per unit volume of these nanowires versus frequency. Note that we use the $ \textless 100\textgreater$ transport orientation throughout this chapter. The basic features we describe, however, are valid for different orientations as well. The transmission of the $ 12~\mathrm{nm}$ nanowire as well as the DOS follow the $ \omega^2$ relation of bulk at low frequencies. For thinner diameters, however, the transmission and DOS are constant at low frequencies, and increase as the diameter is reduced. The fact that there is a constant transmission at $ \omega=0$ for the acoustic branches leads to a strong manifestation of the long-wavelength problem in the thermal conductivity as we will see below.


next up previous contents
Next: 5.2 The Long-Wavelength Problem Up: 5. Anomalous Diameter Dependence of Thermal Conductivity in Ultra-Thin Silicon Nanowires Previous: 5. Anomalous Diameter Dependence of Thermal Conductivity in Ultra-Thin Silicon Nanowires   Contents
H. Karamitaheri: Thermal and Thermoelectric Properties of Nanostructures