References
- Barkovskii , L. M. and Fedorov , F. I. 1974 . Dokl. An SSSR , 218 : 1313
- Barkovskii , L. M. and Borzdov , G. N. 1975 . Optika i Spek. , 39 : 150
- Alshits , V. I. , Antipov , V. V. , Sorokin , N. G. , Chizhikov , S. I. and Shuvalov , A. L. 1987 . Izv. AN SSSR, Ser. Fiz. , 51 : 1733
- In order not to encumber the expressions we here and subsequently take N as odd, which is clearly unimportant for N ≫ 1 for approximate purposes
- Lyamov , V. E. 1983 . Polarization Effects and Interaction Anisotropy for Acoustic Waves in Crystals [in Russian] . Izd. MGU Moscow ,
- Zaitseva , M. P. , Kokorin , Yu. I. , Sandler , Yu. M. , Zrazhevskii , V. M. , Sorokin , B. P. and Sysoev , A. M. 1986 . Nonlinear Electromechanical Parameters for Acentric Crystals [in Russian] , Edited by: Aleksandrov , K. S. Novosibirsk : Nauka .
- It can be shown that the correlation of values lj (0) related with the condition σ = L practically does not tell on the results of calculation at N ≫ 1
- Antipov , V. V. , Blistanov , A. A. , Sorokin , N. G. and Chizhikov , S. I. 1985 . Kristallografiya , 30 : 743
- The height of the maximum on the curve calculated at ρG/l (0) ≈ 0.045 is normalized on the experiment because the full data on the measurements of the nonlinear coefficients for LiNbO3 which are necessary to calculate the electroacoustic parameter ζ, are absent in literature (see also3)