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Figure 17-17: The Form View tab of the Plot Style Table Editor. Now go through each of the properties and make any changes that you want. In Table view, you need to click the property in the Plot Styles column for a drop-down list to appear. The properties are as follows: Color: You can specify a color other than the default, which is Object Color. For example, you might want to create a plot style that plots everything in black or red. For more options, choose Select Color and define a color in the Select Color dialog box. (See 11 for an explanation of how to use the Select Color dialog box.) Dither: Dithering is a method of using dot patterns to approximate a greater range of colors. Not all plotters support dithering. Dithering gives the impression of more colors but can make thin lines and dim colors look unclear. Grayscale: Converts objects to grayscale, if supported by the plotter. You could use grayscale to deemphasize certain layers. Pen # and Virtual Pen #: These settings apply to pen plotters only (the Virtual Pen # setting applies to non-pen plotters that can simulate pen plotters) and specify which pen to use for the object that is assigned the plot style.

conduction band. In general, so-called metals are good conductors because the partly lled conduction band overlaps with a lled valence band, and vacant energy states in the conduction band are thus readily available to electrons. In insulators, the conduction band and valence band are separated by a wide forbidden band, and electrons do not have enough energy to jump from one band to another. In intrinsic semiconductors, the forbidden gap is narrow, and at normal temperatures some electrons at the top of the valence band can move by thermal agitation into the conduction band. In a so-called doped semiconductor, the doping impurities essentially create one or more thin separate conduction bands in the forbidden band. In this context, the gap refers to the gap between energy bands, that is, from the upper boundary of the valence band to the lower boundary of the conduction band [31].

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Physical (Electrical, Thermal, Elastic) Properties (n, m); n m is divisible by 3 (n, m); n m is not divisible by 3 n (12.9 k ) 1 10 4 -cm 1013 A/m2 2000 W/m/K 100 nm 10 11 s 1 TPa 1.28 TPa 30 GPa

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chosen that was 05 mm in diameter, corresponding approximately to the distance between the rst minima in the horizontal dimension of the measured far eld pro le The expected transmission of this bucket for a 125 diffraction-limited beam is calculated to be 96% As illustrated in Fig 511b, a transmission of *92% was measured across the range of output energies up to 25 J This 5% reduction in the expected transmission is reasonable based on the fact that the t between the super-Gaussian and measured near- eld pro les shown in Figs 510b and 510c is not perfect The small-scale irradiance modulation on the beam pro le is expected to contribute to a small reduction in Strehl, as was observed in the measurements 534.

These are N - K linear equations in the K unknown coefficients XI, . . . , XK. Therefore, for solving (2.8) for the X k , the number of observations N should be at least 2 K . However, in many applications N will be larger than 2K. Then, the system of equations (2.8) is verd:termiped and is solved in the least squares sense. This means that the solution e = (el . . [ K ) for the vector of coefficients X = (XI . . . X K ) ~ taken as that value of ~ is e = (e, . . .t K ) T that minimizes the least squares criterion

3 Average power operation In the present con guration of this ashlamp-pumped Nd:glass ampli er system, the lamps can be pulsed at repetition rates of up to 6 Hz with 25 kJ of deposited electrical energy per pulse without reaching the stress fracture limit of the ampli er glass When the laser ampli er system is operated in the SBS phase conjugated con guration, the near- eld irradiance distribution and far- eld divergence described in the previous section is maintained up to this full pulse repetition frequency In fact, in an experiment in which the ampli er slab was intentionally thermally loaded above 6 Hz, near-diffraction-limited output divergence was preserved up to the last laser pulses before the slab fractured The ampli er system has been operated for periods exceeding 1 hr with average output power above 150 W Figure 5.

12 illustrates continuous records of laser pulse energies between 25 J and 27 J for 4-, 5-, and 6-Hz operation The temporal pro le of the ampli ed output pulses is characterized by a smooth, unmodulated envelope without a steep leading edge that would be.

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