Raman Scattering by Optical Modes of Metals

Author(s):  
James H. Parker ◽  
D. W. Feldman ◽  
M. Ashkin
2009 ◽  
Vol 1221 ◽  
Author(s):  
Brian K Ridley ◽  
Angela Dyson

AbstractAn enduring problem in the engineering of high-power semiconductor devices is how to mitigate the effect of heating. Heating means the proliferation of phonons, and phonons, interacting with electrons directly affect the electronic performance of the device. Nowhere is this more evident than the role of hot polar-optical phonons in reducing the drift velocity in the channel of an HFET and hence reducing its performance at high frequencies. The task of describing hot-phonon effects is complicated by the coupling to plasma modes. We present a theory of coupled plasmon-phonon modes in GaN, how they interact with electrons and how their lifetime becomes density-dependent. Raman scattering in bulk material shows a reduction of lifetime with increasing density and we offer an explanation for this in terms of the frequency dependence of the anharmonic decay mechanism. Hot-phonon effects, however, involve modes with wave-vectors beyond those probed by Raman scattering. By adopting a single-pole approximation for these modes we have obtained the lifetime dependence on wave vector, electron temperature and density.


1968 ◽  
Vol 21 (9) ◽  
pp. 607-608 ◽  
Author(s):  
D. W. Feldman ◽  
James H. Parker ◽  
M. Ashkin

2006 ◽  
Vol 85 (3) ◽  
pp. 287-297 ◽  
Author(s):  
K.W. Adu ◽  
Q. Xiong ◽  
H.R. Gutierrez ◽  
G. Chen ◽  
P.C. Eklund

2013 ◽  
Vol 27 (05) ◽  
pp. 1350035 ◽  
Author(s):  
RU HAN ◽  
XIAOYA FAN

The Raman spectra of 4H- SiC with hexagonal defect have been investigated as a function of the excitation wavelength. As the excitation wavelength increases, the excitation wavelength dependence of Raman spectrum of hexagonal defect is very different from that of the free defect zone in 4H- SiC . Four electronic Raman scattering peaks are seen to be significantly enhanced with longer wavelength excitation. In hexagonal defect, the optical modes ( E 2( TO ), E 1( TO ) and A 1( LO )) and the second-order Raman spectrum are broadened and redshifted as the excitation wavelength increased. But the positions of these bands obtained from the free defect zone do not change within our experimental error. Structure defects are regarded as the origin of those abnormal phenomena in hexagonal defect, and the structure ordering of hexagonal defect may have some similarity with SiC monofilaments.


1983 ◽  
Vol 44 (11) ◽  
pp. 313-318 ◽  
Author(s):  
Masaaki Takashige ◽  
Terutaro Nakamura ◽  
Yutaka Aikawa

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