CALCULATION OF THE RISE TRANSIENT AND RELAXATION-TIME OF THE INDUCED DIPOLE KERR-EFFECT

The exact calculation of the rise transient oil the birefringence and the corresponding relaxation times by different theoretical methods is described, in particular the Kerr-effect response of an assembly of n onpolar but anisotropically polarizable molecules following the imposi tion of a constant electric field is studied by solving the Smoluchows ki equation. This equation is transformed into a set of differential r ecurrence relations containing Legendre polynomials of even order only . By taking the Laplace transform of the birefringence function, it is shown that tile singularity at s = 0 (zero-frequency limit) may be re moved so that the relaxation lime for the rise process may br exactly expressed as a sum of products of summer functions and its first deriv atives. The second approach is based on a matrix method where the spec trum of eigenvalues lambda(2j) and their associated amplitudes A(2j) ( extracted from the first components of eigenvectors) are calculated al lowing one to express the relaxation time as Sigma A(2j)(lambda(2j)(-1 )). Numerical values of this time are tabulated for a large range of g values (0 < g < 40), g being the parameter measuring the ratio of the orientational energy arising from the electrical polarizabilities s t o tile thermal energy. II is thus demonstrated that the lowest eigenva lue (lambda(2)) dominates almost completely the rise process. The effe ctive relaxation time is also calculated exactly and expressed very si mply as the ratio of two Kummer functions. Its evolution as a function of g leads to behavior similar to that of the relaxation timi obtaine d either from the kummer functions or from the eigenvalue method. It i s characterized by a maximum situated around g =?, which is interestin g in view of experimental applications.