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1 shows the con guration of the FSPCF The phase conjugator provides feedback to every laser diode element in the array Between the diode array and the phase conjugator, a frequency lter and a spatial lter select, respectively, a narrow frequency range and a single spatial mode from the output of the array The phase conjugator is mounted off-axis, with an angle u between the axis of the laser diode array and the phase conjugator This asymmetric arrangement combines high output coupling ef ciency with signi cant enhancement of both the spatial and temporal coherence of the laser output The phase conjugate wave from the phase conjugator retraces the output wave from the laser diode array, such that at all points the wavefronts of the phase conjugate wave coincide with those from the laser diode array.

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[8] B Sch ppert, A fast and reliable method for computer analysis of microwave mixers , IEEE u Trans Microwave Theory Tech, 34(19), 110 119, 1986 [9] MJ Rosario, J Costa Freire, Design techniques for MESFET mixers for maximum conversion gain , IEEE Trans Microwave Theory Tech, 38(12), 1972 1979, 1990 [10] YH Liew, J Joe, RF and IF ports matching circuit synthesis for a simultaneous conjugatematched mixer using quasi-linear analysis , IEEE Trans Microwave Theory Tech, 50(9), 2056 2062, 2002 [11] F Giannini, G Leuzzi, E Limiti, F Morgia, Optimum nonlinear design of active microwave mixers , Proc GAAS 2000 , Paris (France), Oct 2000 [12] P Harrop, TACM Clasem, Modelling of a FET mixer , Electron Lett, 14(12), 369 370, 1978 [13] C Camacho-Pe alosa, CS Aitchison, Analysis and design of MESFET gate mixers , IEEE n Trans.

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This autoretracing property is key to the use of phase conjugate feedback to improve the spatial and temporal coherence of laser diode arrays Since the same principle may also be applied to broad area lasers, laser bars, and stacked arrays, phase conjugate feedback can be used with diode laser systems at.

effects These effects include self-focusing, optical breakdown, and Raman scattering However, this is not the case when the ampli cation regime corresponding to two-cell con guration is applied to SBS compression The latter allows for ef cient compression of powerful laser pulses Numerical simulation of SBS pulse compression using quasi-1D approximation was reported in Ref 49 In the work described, carbon tetrachloride was used as the SBS-active medium The pump was focused using a 50-cm focal length lens placed at the front window of the cell It was found that with an increase in the convergence angle, b % D=F, at which a pump was focused into the cell, the Stokes pulse leading edge became increasingly steeper and less time was required for the pulse to reach maximum instantaneous power.

Microwave Theory Tech, MTT-35, 643 652, 1987 [14] YK Kwoon, D Pavlidis, Phasor diagram analysis of millimetre-wave HEMT mixers , IEEE Trans Microwave Theory Tech, MTT-43(9), 2165 2167, 1995 [15] JCH Cayrou, M Gayral, J Graffeuil, JF Sautereau, Simple expression for conversion gain of MESFET drain mixers , Electron Lett, 29(17), 1514 1516, 1993..

Biochemical Sciences, 23, 138 43. A review of structure function relationship in GroEL. Shtilerman, M., Lorimer, G.H. and Englander, S.W. (1999). Chaperonin function: folding by forced unfolding. Science, 284, 822 5. Xu, Z.H., Horwich, A.L. and Sigler, P.B. (1997). The crystal structure of the asymmetric GroEL-GroES-(ADP)(7) chaperonin complex. Nature, 388, 741 50. The crystal structure of the GroEL/GroES system.

Although SBS re ectivity also increases monotonically with the converging angle, a minimum Stokes pulse duration in the simulation could be obtained at an optimum beam diameter Dopt 2:25 mm (bopt % 4:5 mrad) For b bopt , the Stokes pulse leading edge does not change, but for larger angles the trailing edge elongates The trailing edge tends to have the same shape as that found in the case of the tight focusing normally used in experiments on phase conjugation In the quasi-1D model the value of compression, K, strongly depends on the nonlinear medium s relaxation time, t For an 8-mJ pump with optimum converging angle, reduction of t from 1 ns to 05 ns increases the compression K from 176 to 228 and increases the SBS re ectivity R from 072 to 082 [37].

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In that work it was also shown that, given factors such as pulse width and energy, the compression, K, is more ef cient for pumping pulses with leading edges having a steeper-than2 Gaussian pro le In particular, for P * t exp( t2 =1:5tP ) we obtain K 24:8 at t 0:5 ns and EL 6 mJ.

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