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The parameter H can be expressed as H NQ Qd (l/zch) NQ (l/zd) (where NQ (Q/Qd)2, Q is the real divergence of the pumping beam, zd (kQQd)21 is the diffraction length of the speckled beam) Analysis of the dependence Gth(NQ) for xed (but different) values of the parameter (l/zd) showed that the condition (24) (for predominance of the phase conjugated beam over angular displacement scattering waves) is ful lled when the diffraction length of the speckled beam is comparable with the thickness of the nonlinear layer: (l/zd) ! 1 [29] This means that for the nonlinear layer with a mirror at the boundary, the mechanism for selection of the phase conjugate wave is caused both by the diffraction in the nonlinear layer and by the nonlinear ampli cation (similar to the ordinal backward SBS of a focused beam [5]).

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The admittance matrix Y is a function of the values of the elements of the circuit, both linear (passive elements and parasitic elements of the active device) and linearised (intrinsic elements of the active device); it is also a function of the (angular) frequency The condition for the existence of an oscillation at a generic frequency 0 therefore is the scalar equation: det(Y ) = 0 (52) The left-hand side of the equation can be seen as a function of the frequency, which is the unknown of eq (52), for xed values of the elements of the circuit: this is the case in which an existing circuit is analysed for determination of its stability: det(Y ) = F ( 0 ) = 0.

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Strictly speaking, the analysis of the phase conjugate conditions is valid for plane envelope of the speckle-inhomogeneous beam Another approach to investigation of generation of scattering beams by the joint SRS of speckle-heterogeneous laser beams with Gaussian envelope showed that the phase conjugation condition in the nonlinear layer with mirror boundary can be realized under similar condition, when (l/zd) ! 1 [15] The SPPC condition obtained concerns only the nonlinear layer with a mirrorre ecting wall In case of the feedback loop with a long pass, the phase conjugation can be achieved even in a layer with thickness less than the diffraction length of the pumping beam 1023 Experimental investigations of self-pumped phase conjugation of laser beams in nematic liquid-crystal layers 1023.

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1 Self-pumped phase conjugation by thermal scattering Phase conjugation of laser beams by joint SRS was investigated in NLC layers both with thermal and orientational nonlinearity The SPPC of laser beam with pulse duration ranging from several microseconds to several milliseconds at different wavelengths (5145 nm, 1064 nm, 106 mm) was realized in the NLC layer with a feedback loop [15, 23 25, 29 32] A simple phase conjugate mirror was made using the NLC layer at the mirror surface (Fig 106) The NLC layer with different thickness was used The planar orientation of molecules in the NLC layer with thickness of 100 200 mm was achieved by creating a relief on the window surface coating The homeotropic orientation of nematic molecules in the layer 05 2.

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0 mm in thickness was achieved by applying the ac electric eld of 1 2 kV/cm at 50 Hz across the cell The voltage was applied both to a thin electroconducting coating on the glass window and to a metallic mirror Several mixtures of cyanobiphenyls (with intrinsic absorption of a % 01 05 cm21 at 1064 nm) or dye-doped cyanobiphenyls (with absorption of 40 100 cm21) were used as the NLC The laser beams were focused in the NLC layer The focal waist length inside the NLC layer was chosen comparable with the layer thickness The joint near-forward thermal scattering of the intersecting incident and mirror-re ected beams resulted in generation of a phase-conjugated beam (Figs 107a and 107b) Both threshold of.

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