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23 O L Antipov and A S Kuzhelev, Self-pumped phase conjugation of laser beams in a nematic liquid-crystal layer with nonreciprocal feedback, Quantum Electron 25(1), 49 52 (1995) 24 OL Antipov, S I Belyaev, and A S Kuzhelev, Orientational self-pumped phase conjugation in a layer of the nematic liquid crystal with a nonrecoprocal feedback, Izv Vuzov: Radiophysics, XXXVIII(3 4), 304 311 (1995) (in Russian) 25 O L Antipov, A S Kuzhelev, and V V Turygin, Optimization of phase-conjugate mirrors made of nematic liquid crystals in a two-pass ampli er, Quantum Electron 24(5), 411 415 (1994) 26 Yu A Arutyunov, and A I Khizhniak, Generation conditions of phase conjugated waves in ring laser with local nonstationary nonlinearity, Sov Quantum Electron 16(4), 789 792 (1989) 27 A P Mazur, A D Novikov, S G Odulov, and M S Soskin, Parametric generation in media with local response in incompleted resonator, JETP Lett.



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If you accidentally click a handle that isn t the last one placed, you ll create the effect of dragging the wrong handle and disrupt the shape of the region. If this happens, undo the last point by choosing Edit Undo or by removing the last Action in





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51(10), 503 506 (1990) 28 A V Mamaev and V V Shkunov, Instability of near-contrunning waves in medium with local nonlinearity, Sov Quantum Electron 19(3), 560 566 (1991) 29 O L Antipov, Parametric oscillation by joint stimulated scattering of near-counterruning laser beams, PhD Thesis, Nizhny Novgorod State University (1992) 30 O L Antipov, N A Dvorjaninov, and V Sheshkauskas, Parametric generation and selfpumped phase conjugation of intersecting laser beams in NLC layer doped by dye, JETP Lett 53, 610 612 (1991) 31 Iam-Choon Khoo, Hong Li, and Yu Liang, Self-starting optical phase conjugation in dyed nematic liquid crystals with stimulated thermal-scattering effect, Opt Lett 18, 1490 1492 (1993) 32 P Meindl, R Macdonald, H J Eichler, and O L Antipov, Low threshold self-pumped phase conjugation of an Ar -laser beam in dye-doped nematic liquid crystals, Mol Cryst Liq Cryst 282, 429 435 (1996) 33 M A.

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This approximate relation is valid for 1 GHz < f < 6 GHz and -90" < 8 < 90'. The frequency f and the angle 8 are measured in GHz and degrees, respectively. Note that equation (3.54) is a normalised equation and has a gain of unity f = 2 GHz and 8 = 0'. The bandpass behaviour of equation (3.54) in both frequency and angle makes it an appropriate measure of non-ideal properties of each antenna element. The antenna spacing is assumed to be dl = d2 = 0.025 m. With substitution of c = 3 x 10' m/s for the velocity of wave propagation, into equations (3.24) and (3.25) yields

m=1

Anisimov, Critical Phenomena in Liquids and Liquid Crystals, Nauka, Moscow (1987) (in Russian) 34 S T Wu, U Efron, and L D Hess, Appl Phys Lett 44, 1033 (1984) 35 O L Antipov, S I Belyaev, H A Pasmanik, Four-pass laser ampli er with PC-NLC mirror, Laser Phys 4(6), 1185 1189 (1994) 36 G J Linford, E R Peressini, W R Sooy, and M L Spaer, Very long lasers, Appl Opt 13, 379 390 (1974) 37 O L Antipov, D V Chausov, A S Kuzhelev, and A P Zinoviev, Self-starting laser oscillator with a nonlinear nematic liquid crystal mirror, J Opt Soc Am B 18(1), 13 20, (2001)..

+ Aa: - P:)2 + 4(P,

(x xi ).

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