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2 steps that are particularly pronounced for laser pulse durations longer than 10 times the Brillouin acoustic decay constant. The source of these instabilities was attributed to the noise that initiates and sustains the stimulated scattering process. At face value, this result would prevent the generation of transform-limited temporal coherence from an SBS phase conjugated ampli er system. However, our understanding of the four-wave mixing process in the SBS loop and its independence of noise at focus to sustain it [47] lead us to believe that we should not observe these phase drifts with the loop. Measurements of the high-energy pulses from the laser system con rmed this prediction. Similar conclusions have been reached by other researchers [50]. In order to measure the coherence length of the 500-ns output pulses, a stabilized single-frequency diode-pumped Nd:YLF laser operating with CW output was used as a reference source. Full-aperture attenuated samples of 25-J pulses at 1053 nm from the phase-conjugated ampli er system were heterodyned with the reference laser on a 1-GHz PIN photodiode and recorded using a digital oscilloscope. The reference laser was tuned to an offset of 100 200 MHz from the frequency of the high-energy laser, and the resulting heterodyne beat was measured. As seen in Fig. 5.25a, the waveforms exhibited good temporal contrast and a smooth temporal envelope, consistent with the laser pulse shape. Analysis of the beat frequency, c# upc-a reader C# UPC-A Barcode Scanner Library - Read & Scan UPC-A Using ...
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