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Second-order nonlinear susceptibility origin

Induced Polarization and Origin of the Second Order Nonlinear Susceptibility... [Pg.383]

The subindices f, j, k indicate base directions (x,y,z) in Cartesian coordinates. Xfj i2co co,co) represents a second order nonlinear susceptibility tensor, a tensor or third rank, responsible for SHG process while Ej(a)) and Ej (co) are the laser field amplitudes in j and k directions. Pf 2coi) is the induced SHG nonlinear polarization in i direction at twice the fundamental frequency, which couples to and generates light field radiation Ei(2co) in twice the original angular frequency 2 CO. Summation over j and k is implied in Eq. (1) by the Einstein summation convention. Please notice that xfk(2(o cOy(o) vanishes for a medium with centro-sym-metry. For a non-centro-symmetry medium, not all the tensor elements exist. [Pg.21]

Lalama, S.J., Garito, A.F. Origin of the nonlinear second-order optical susceptibility of organic systems. Phys. Rev. A 20, 1179-1194 (1979)... [Pg.147]

X and x are the second and third-order nonlinear optical susceptibilities. Two important manifestations of optical nonlinearities are harmonic generation and refractive fndex modulation by electric and optical fields. Their origin can conveniently be explained by considering a plane wave propagation through the nonlinear medium. The polarization is then given by... [Pg.564]

In isotropic media the reflection of all vectors at the origin should not change the nonlinear susceptibility. This yields Xijk = —Xijk which could be only fulfilled by Xijk = 0. In all media with an inversion center the second-order susceptibility tensor vanishes This means, for instance, that optical frequency doubling in gases is not possible. [Pg.332]

Barnik et al. observed the same effect but deduced a much smaller nonlinear susceptibility from the measurements than Arakelyan et al. They provided a different interpretation as well in their opinion SHG was due to electric- quadrupole effects. (Quadrupole effects originate from the coupling between the polarization P and the spatial derivatives of the electric field.) As second-order quadrupole effects are not forbidden by the existence of an inversion centre the interpretation of Barnik et ai is compatible with the generally accepted symmetry properties of nematics. A detailed theoretical analysis of the problem was given by Ou-Yang et Their results indicate also that the quadrupole mechanism is responsible for SHG in MBBA rather than the existence of noncentrosymmetric blocks. [Pg.13]


See other pages where Second-order nonlinear susceptibility origin is mentioned: [Pg.110]    [Pg.288]    [Pg.920]    [Pg.143]    [Pg.356]    [Pg.109]    [Pg.82]    [Pg.471]    [Pg.495]    [Pg.130]    [Pg.356]    [Pg.87]    [Pg.700]    [Pg.238]    [Pg.20]    [Pg.402]    [Pg.383]    [Pg.36]    [Pg.339]    [Pg.146]    [Pg.285]    [Pg.282]   
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