Abstract
The important quantitiy in any nonlinear light scattering phenomenon is the nonlinear molecular susceptibility where N indicates Nth order dependence on the inducing electric field and the subscripts i, j , k , l, … denote directions in a Cartesian coordinate system indicating polarization directions of the generated and incident radiation. In general, ∼ denotes a vector, ≈ denotes a tensor of rank two and ≈ will identify tensors of rank greater than two. The susceptibility X(N) is a tensor of rank N+1. Third order effects include Coherent Stokes and Anti-Stokes Raman Scattering, the a.c. and d.c. Kerr effects, third harmonic generation, self-focussing, self-phase modulation, stimulated Brillouin scattering, stimulated Raman scattering, Raman induced Kerr effect and inverse Raman.
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© 1982 D. Reidel Publishing Company
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Fleming, J.W., Harvey, A.B. (1982). Classical Approach to Third-Order Non-Linear Susceptibilities. In: Kiefer, W., Long, D.A. (eds) Non-Linear Raman Spectroscopy and Its Chemical Aplications. NATO Advanced Study Institutes Series, vol 93. Springer, Dordrecht. https://doi.org/10.1007/978-94-009-7912-3_6
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DOI: https://doi.org/10.1007/978-94-009-7912-3_6
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