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Relation between nonlinear refractive index and third-order susceptibility in absorbing media

机译:吸收介质中非线性折射率与三阶磁化率的关系

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Expressions relating complex third-order optical susceptibility (chi((3)) = chi(R)((3)) + ichi(t)((3))) index (n(2)) and nonlinear absorption coefficient (,8) have been formulated that eliminate the commonly used approximation of a negligible linear absorption coefficient. The resulting equations do not show the conventional linear dependence of chi(R)((3)) with n(2) and chi(t)((3)) with beta. Nonlinear refraction and absorption result instead from the interplay between the real and imaginary parts of the first- and third-order susceptibilities of the material. This effect is illustrated in the case of a metal-dielectric nanocomposite for which n(2) and beta values were experimentally obtained by Z-scan measurements and for which the use of the new formulas for chi(R)((3)) and chi(t)((3)) yield a large correction and a sign reversal for chi(t)((3)) . (C) 2004 Optical Society of America.
机译:复杂的三阶光学磁化率(chi((3))= chi(R)((3))+ ichi(t)((3)))指数(n(2))和非线性吸收系数(,8的公式已消除了可忽略的线性吸收系数的常用近似值。所得方程式未显示n(2)为chi(R)((3))和beta为chi(t)((3))的常规线性关系。相反,非线性折射和吸收是由材料的一阶和三阶磁化率的实部和虚部之间的相互作用引起的。在金属介电纳米复合材料的情况下,可以说明这种效果,其中通过Z扫描测量通过实验获得了n(2)和β值,并且使用了chi(R)((3))和chi(t)((3))对chi(t)((3))产生较大的校正和符号反转。 (C)2004年美国眼镜学会。

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