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an exponential operator eK. Using the properties of M as developed in Section 3.1.3, show that the trace of K is zero.
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Tables 4.5. and 4.6. summarizethe results. Table 4.5. shows that the optimal design reduces the criterion and the Cram&-Rao variance for target parameter u significantly. Table 4.6. shows that the optimal design is concentrated in three points only: -2.21,0, and 2.21. At each of the points -2.21 and 2.21, three observations are made.
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Table 11.12 Average Heat of Combustion and Yields of Products for Polymers from the Data Measured in the ASTM E2058 Fire Propagation Apparatusa
Fitting a CPU is easy because of the ZIF socket that it fits into on the motherboard. ZIF stands for Zero Insertion Force, and that s exactly what you need when fitting a CPU. The hundreds of pins on the base of the CPU are designed to slip effortlessly into the ZIF socket (see Figure 14-11).
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where Fsat is the saturation uence (J/cm2), Iout is the desired output irradiance (W/cm2), A is the beam area in the ampli er (cm2), Pout is the desired output power (W), and n is the number of ampli er passes. It is intuitively reasonable that to generate a constant output power from the ampli er system, an exponentially rising seed laser input power is required. As energy is extracted from the laser ampli er at a constant rate, the gain decreases exponentially. An exponentially rising input pulse pro le can therefore be used to compensate this loss in gain, maintaining nearconstant output power during the pulse. In the case of the laser system described here, our output energy goal was 40 J in a 500-ns pulse (80 MW) after the last of the eight gain passes. This would then ensure an energy of .30 J (60 MW) in the beam after it is reformatted in the anamorphic telescope and coupled out through the Faraday optical isolation stage to the harmonic converter. With an Fsat 5 J/cm2 for the Schott APG-1 laser glass used for the zigzag slab and a beam area of 0.7 12 cm2, a simple application of the above formula yields an optimal exponential time constant t 65 ns for the injected seed pulse. This very simple derivation does not take into account optical losses for the components of the beam train and linear absorption in the ampli er glass. However, it provides a very effective tool for con guring the pulse shape of the injected pulse. We experimentally veri ed that a time constant of 60ns provides the desired 60 MW over 500 ns (30 J/pulse) to the second harmonic converter. 5.4.3 Long-pulse SBS phase conjugation
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