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The area of the self-starting generation was calculated also in the plane of the frequency detuning and the logarithmic gain in ampli er 1 at a constant noise intensity (j1j2/IS 1027) (Fig 1015b) This computation showed that there is an optimal frequency shift of the interacting waves at which the generation threshold in the self-starting laser is minimal Such frequency shift can occur because of noise mechanical vibrations of the mirror in the cavity Note that the calculated minimal threshold gain (a1l1 1) is in accordance with experimental results (all parameters of the calculated equations were chosen similar to those in the experiment with NLC cell with thermal nonlinearity) The threshold logarithmic gain essentially decreased with an increase in the NLC nonlinearity beff (Fig 1015b, region 2).

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This result also agrees with experiment: Near the nematic isotropic transition point the nonlinearity of NLC increases and the self-starting generation threshold decreases Thus, our numerical computation showed the presence of self-starting oscillations in the cavity completed by RIG induced in NLC by generating beams themselves 1033 Experimental investigation of the self-starting lasers An experimental scheme of the laser oscillator with a dynamic holographic mirror written in the NLC cell by generation waves is shown in Fig 1016 The scheme consists of three ash lamp-pumped Nd:YAG ampli ers, a polarizer, ordinary mirrors, and a NLC cell The pump pulse duration is 03 ms The origin of the gratings in the NLC completing the cavity was investigated by incorporating a quartz rotator (QR) and a Faraday rotator (FR) at different locations in the scheme.

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This arrangement allowed for four-wave interactions of a selfintersecting generated beam that started from spontaneous emission The laser system was investigated at a variable repetition rate of pumping, ranging from 1 Hz to 30 Hz This variation allowed us to de ne the role of the RIGs in FWM due to the slow-response orientation nonlinearity or thermal nonlinearity of the NLC In our experiments, NLC cells with different thicknesses of nematic materials were used: a 75-mm layer of pure 5CB (nematic isotropic transition temperature is 368C) with the planar orientation of the NLC director, a 05-mm layer of pure 5CB.

Figure 9-8

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The birefringent, double-focus lens L1 is a symmetrical triplet, consisting of a central bio-concave calcite lens and two biconvex glass lenses The optic axis of calcite lies in the plane of the lens The triplet is so designed as to have zero power for the ordinary ray and a focal length of a few centimeters for the extraordinary ray As in the case of Burch s interferometer (Section 32), this arrangement gives explicit information about wavefront deformations since a part of the incident light is focused on a small region in the aperture of the system under test and acts as the reference beam The system under test in Figure 317 is the concave mirror The center of the triplet lens is located at the center of curvature of the mirror.

A lens L2 with its focus F1 on the mirror surface is placed just to the right of the triplet A quarter-wave plate with its principal axes at 45 to the optic axis of the calcite lens is also placed to the right of L1 A collimated beam of linearly polarized light is incident from the left The lens L1 splits it up into an ordinary beam and an extraordinary beam The O beam, undeviated by L1, is brought to focus at F1 by the lens L2 An image of the source is thus formed at F1 On its return journey, the O beam is collimated by the lens L2 , and since its vibration direction has been rotated through 90 because of the double passage through the quarter-wave plate, it is refracted to F01 by the lens L1 .

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