96
P. K. Das et al.
Fig. 68 The curves of C 2 versus (electric quantum limit) at terahertz frequency in n-channel
accumulation layers of n-Indium Arsenide where (E/E g ) 1 for (a) the band structure containing
3 energy band constants and (b) the band structure containing 2 energy band constants
Fig. 69 The curves of C 2 versus E 0 (electric quantum limit) at terahertz frequency in n-channel
accumulation layers of n-Indium Arsenide where (E/E g ) 1 for the band structure containing 3
energy band constants
4 Conclusion
We investigate the influence of terahertz frequency on the elastic constants in
extremely degenerate (ED) 2D systems taking quantized films (QFs) and accumulation layers (ALs) of nonlinear optical, tetragonal, ternary, quaternary, III–V, II–VI,
IV–VI and strained compounds, respectively. It has been found taking ED QFs and
P. K. Das et al.
Fig. 68 The curves of C 2 versus (electric quantum limit) at terahertz frequency in n-channel
accumulation layers of n-Indium Arsenide where (E/E g ) 1 for (a) the band structure containing
3 energy band constants and (b) the band structure containing 2 energy band constants
Fig. 69 The curves of C 2 versus E 0 (electric quantum limit) at terahertz frequency in n-channel
accumulation layers of n-Indium Arsenide where (E/E g ) 1 for the band structure containing 3
energy band constants
4 Conclusion
We investigate the influence of terahertz frequency on the elastic constants in
extremely degenerate (ED) 2D systems taking quantized films (QFs) and accumulation layers (ALs) of nonlinear optical, tetragonal, ternary, quaternary, III–V, II–VI,
IV–VI and strained compounds, respectively. It has been found taking ED QFs and