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0, and 0 s (corresponding to the previous cases), (2) 30, 10, and 10 s, and (3) 60, 20, and 20 s, respectively. The results are plotted in Figure 14.10. As seen from the plots, as the data generation rate reduces from case (1) to (2) to (3), the cost of the put operation and the throughput per processor improves, since the network is less congested. The jump is more signi cant from case (1) to (2) and less signi cant from case (2) to (3).

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Keystroke Ctrl-A Ctrl-B Ctrl-D Ctrl-E Ctrl-F Action Go to left edge of window Cursor left, wrapping to previous line if appropriate Delete character under cursor Go to right edge (stripspaces off) or end of line (stripspaces on) Cursor right, wrapping to next line when appropriate

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A key interest in such adaptive laser systems arises in high average power solid-state lasers where maintenance of high beam quality is problematic due to thermally induced phase and polarization distortions A schematic of a self-starting adaptive laser oscillator is shown in Fig 1112 The system shows the gain SPPC loop scheme in combination with a partial re ector as an output coupler In this type of system, initiation of laser action is due to ampli ed spontaneous emission from the laser ampli ers The spontaneous emission has low spatial and spectral coherence but has been shown to be suf cient to form a weak gain diffraction grating that can lead to the growth of the intracavity ux and the selection of increasing coherence of the radiation Operation on a TEM00 spatial and single-longitudinal mode has been demonstrated [14, 27].

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where the current in the nonlinear element is computed through the time domain ig (t) = imax tgh g V cos( 0 t + v ) imax Ig cos( 0 t + g ) = (1.121)

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In one system based on ashlamp-pumped Nd:YAG laser rods [14], the transient onset and spectral selectivity of the gain gratings produced an output with energy of 600 mJ in a 10-ns single-longitudinal mode pulse Self-adaptation of the spatial quality was demonstrated by correction of an intracavity phase plate distorter The diagram in Fig 1112 shows the self-adaptive laser with additional polarization elements (quarter-wave retardation plates QW1, QW2) that allow the system to correct polarization distortions in the loop section of the resonator [15] The use of two quarterwave plates to achieve counterpropagating orthogonally circular polarized beams in laser resonators is a common technique to prevent spatial hole burning due to the counterpropagating beams and is associated with mode hopping of the laser frequency In the FWM beam con guration, shown by the shaded interaction region of Fig 11.

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where a is the rate of change of the reference phase. Since we are controlling the reference phase, a is well known, and the sinusoidal and cosinusoidal signals with this same frequency can be generated. This cosinusoidal signal is correlated with the interferogram intensity at each point: hI1 x; y i lim which reduces to hI1 x; y i I 00 x; y cos f x; y 14:169 1 T!1 T Z

Note A module name (as well as the names of other forms and controls) must start with a letter and can be up to 31 characters. Only letters, numbers, and the underscore character are allowed.

12, it also provides the necessary conditions to achieve vector phase conjugation (VPC) [29] and thereby correct for depolarization distortions as well as phase distortions in the laser ampli ers The action of VPC by FWM in a laser ampli er has been investigated experimentally in an Nd:YAG ampli er [30] and analyzed theoretically [31]..

Table B-1 (continued)

20 25 30 35 40

Do not start variable names with numbers. End all your statements with a semicolon ( ; ). Most JavaScript parsers are very forgiving regarding the syntax structure of your scripts, but this is implementation dependent, and in case of ambiguity the script fails.

java code 128 reader

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java code 128 reader

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java code 128 reader