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Third harmonic generation susceptibility

Third-order susceptibilities of the PAV cast films were evaluated with the third-harmonic generation (THG) measurement [31,32]. The THG measurement was carried out at fundamental wavelength of 1064 nm and between 1500 nm and 2100 nm using difference-frequency generation combined with a Q-switched Nd YAG laser and a tunable dye laser. From the ratio of third-harmonic intensities I3m from the PAV films and a fused quartz plate ( 1 thick) as a standard, the value of x(3) was estimated according to the following equation derived by Kajzar et al. [33] ... [Pg.322]

Shcheslavskiy, V., Petrov, G. I., and Yakovlev, V. V. 2003. Nonlinear optical susceptibility measurements in solutions using third-harmonic generation at interfaces. Appl. Phys. Lett. 82 3982-84. [Pg.165]

Characterization of Molecular Hyperpolarizabilities Using Third Harmonic Generation. Third harmonic generation (THG) is the generation of light at frequency 3co by the nonlinear interaction of a material and a fundamental laser field at frequency co. The process involves the third-order susceptibility x 3K-3 , , ) where —3 represents an output photon at 3 and the three s stand for the three input photons at . Since x(3) is a fourth (even) rank tensor property it can be nonzero for all material symmetry classes including isotropic media. This is easy to see since the components of x(3) transform like products of four spatial coordinates, e.g. x4 or x2y2. There are 21 components that are even under an inversion operation and thus can be nonzero in an isotropic medium. Since some of the terms are interrelated there are only four independent terms for the isotropic case. [Pg.79]

In the third-harmonic generation, the third-order susceptibility leads to a nonlinear polarization component which oscillates at the third-harmonic frequency of the incident laser beam. This leads to a light wave at the third-harmonic frequency of the fundamental wave. As optical frequencies are involved and since the output frequency is different from the input frequency only the electronic nonlinearities can participate without any contributions from thermal or orientational effects. Because one needs fast nonlinearities for all-optical signal processing, the main interest is directed towards the fast electronic nonlinearities. Therefore and also due to its simplicity, third-harmonic generation is a very attractive method to characterize newly developed materials. [Pg.142]

Fig. 5. Concentration series of a third-harmonic generation experiment. The third-order nonlinear optical susceptibilities of the solutions are analyzed with the solvent nonlinearity -Tchci f°r c = 0 and the slope dx ldc proportional to the second-order hyperpolarizability yof the molecule under investigation... Fig. 5. Concentration series of a third-harmonic generation experiment. The third-order nonlinear optical susceptibilities of the solutions are analyzed with the solvent nonlinearity -Tchci f°r c = 0 and the slope dx ldc proportional to the second-order hyperpolarizability yof the molecule under investigation...
While the above discussion clearly highlights the importance of including solvent effects in the calculations, the calculated properties cannot be compared directly with experimental results. This is mainly caused by the many different conventions used for representing hyperpolarizabilities and susceptibilities. However, the calculated properties can be combined with appropriate, calculated Lorentz/Onsager local field factors to obtain macroscopic susceptibilities that can be compared with experimental results. For water, we used this to calculate the refractive index and the third harmonic generation (THG) and the electric field-induced second harmonic (EFISH) non-linear susceptibilities. The results are collected in Table 3-11. [Pg.86]

II. MEASUREMENT OF THE THIRD ORDER SUSCEPTIBILITY OF TRANS-(CH)x BY THIRD HARMONIC GENERATION (14)... [Pg.375]

Another potential application of fully converted polydiacetylenes is based upon their unusual non-linear optical properties. Sauteret et al. found that the third order susceptibilities of TCDU and TS increases by about a factor of 600 upon polymerization and become comparable to those of inorganic semiconductors like GaAs or germanium. This is a consequence of the increase of n-electron delocalization upon polymerization. Polymeric diacetylenes can therefore be used as efficient elements for third harmonic generation. In Ref. this effect has been employed for tripling the frequencies of 1.89 pm and 2.62 pm radiation. [Pg.43]

Meredith, G.R., Buchalter, B., Hanzlik, C. Third-order susceptibility determination by third harmonic generation. II, J. Chem. Phys. 78, 1543—1551 (1983)... [Pg.459]

Table 4. Third order NLO susceptibilities and molecular second hyperpolarizabilities of simple catenane and rotaxane molecules as determined by the optical third harmonic generation technique... Table 4. Third order NLO susceptibilities and molecular second hyperpolarizabilities of simple catenane and rotaxane molecules as determined by the optical third harmonic generation technique...
Laser lights with short wavelengths are important in optical data processing, and conjugated polymers are expected to be useful materials for their generation. Optical third-harmonic generation measurements have been performed for poly(phenylacetylenes) " The magnitudes of the third-order susceptibility were 7 x 10 esu for poly(phenylacetylene) and in the order of 10 -10" esu for its derivatives . ... [Pg.983]

Third Harmonic Generation (THG) is achieved when (Oi = (O2 = (Oj = (0. In this case the constant 4 = 1/4. The third order nonlinear coefficient C is related to the third order susceptibility as follows... [Pg.2114]

Abstract The anisotropic third-order nonlinear optical susceptibility of monodomain samples of nematic solutions of poly[l,4-phenylene-2,6-benzobisthiazole], PBT, a rodlike polymer, have been studied by third harmonic generation. Corresponding measurements have also been made for isotropic solutions of PBT. A substantial off-diagonal component of X( H-3co o),co,co) is measured, resulting in the generation of an elliptically polarized third harmonic signal for a fundamental linearly polarized along the director. [Pg.189]


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