For numerical results, consider a plate of ZnO with 2h ¼ 2 μm, p 0 ¼ 2 Â 10
24 m
À3
and n 0 ¼ 1.2 Â 10
23 m
À3 . Typical dispersion curves found numerically are shown in
Fig. 2.12. The dispersion curves are complex because conduction is dissipative.
References
1. Y.X. Luo, C.L. Zhang, W.Q. Chen, J.S. Yang, An analysis of PN junctions in piezoelectric
semiconductors. J. Appl. Phys. 122, 204502 (2017)
2. R.F. Pierret, Semiconductor Device Fundamentals (Pearson, Uttar Pradesh, 1996)
3. Y.X. Luo, R.R. Cheng, C.L. Zhang, W.Q. Chen, J.S. Yang, Electromechanical fields near a
circular PN junction between two piezoelectric semiconductors. Acta Mech. Solida Sin. 31,
127–140 (2018)
4. J.S. Yang, A semi-infinite anti-plane crack in a piezoelectric semiconductor. Int. J. Fract. 130,
L169–L174 (2004)
5. J.S. Yang, An anti-plane crack in a piezoelectric semiconductor. Int. J. Fract. 136, L27–L32
(2005)
6. F. Zhu, S.H. Ji, J.Q. Zhu, Z.H. Qian, J.S. Yang, Study on the influence of semiconductive
property for the improvement of nanogenerator by wave mode approach. Nano Energy 52,
474–484 (2018)
0
1
Im( )( m
-1 )
2
3
4
5
5
4
Re( )( m
-1 )
3
2
1
0
15
5
0
20
10
(10 9
rad/s)
B
C
A
D
E
F
Fig. 2.12 Dispersion
curves of antiplane waves
References
29
Précédent

- 36/233

Suivant