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As a conclusion, in the nanosecond illumination regime for pulsed average intensities up to 20 MW . cm22 at 1.06 mm, the gain is intensity-independent, while the intensity rise-time product keeps constant. The maximum gain is marginaly smaller than the one measured in the CW illumination regime. So, contrary to the results obtained in the visible range, nanosecond and CW illumination regimes are nearly equivalent for BaTiO3:Rh at 1.06 mm for intensities up to 20 MW . cm22, which is favorable for applications. BaTiO3:Rh is a photorefractive material with high gain and low absorption at 1.06 mm. It is accurately described by a three-charge state model, which agrees with spectroscopic and photorefractive studies. Oxidation of these crystals reduces signi cantly the rise time of the photorefractive effect, but, because it also increases the permanent absorption, it is not suited for dynamic wavefront correction of powerful lasers. Nevertheless, oxidation might be very useful for low-power applications at laser diode wavelengths. For as-grown BaTiO3:Rh at 1.06 mm, nanosecond and CW illuminations are nearly equivalent in terms of photorefractive gain and time constant for pulsed intensites up to 20 MW . cm22. This latter result, which differs from these obtained in the visible range, is a key point for applications to Qswitched Nd:YAG lasers. Such a high photorefractive gain and low absorption material is attractive for high re ectivity phase conjugation, as will be discussed in the next section. 8.3 SELF-PUMPED PHASE CONJUGATION

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6. (Optional) Choose a secondary sort order using the next pop-up menu and Triangle Sort Order button. 7. (Optional) Choose a third subsort order using the next pop-up menu and Triangle Sort Order button. 8. Click Sort to perform the sort. If you re not happy with the results, you can undo the sort by choosing Edit Undo, or by removing the sort from the History palette.

As in Section 10.2, we will begin with Euler methods. Therefore, following (10.21) we may Taylor-expand x(t) and y(t) about the sampling time t = tn . As (k) (k) before, for convenience we may de ne xn = x (k) (tn ), yn = y (k) (tn ). The relevant expansions are given by

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In the standard window mode, you have access to scroll bars, just as you do in just about every other major application. But as you become more proficient with Photoshop, you ll use the scroll bars less and less. One way to bypass the scroll bars is to use the keyboard equivalents listed in Table 2-1.

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Technical graphics in three dimensions are notoriously difficult to draw by hand. Luckily a number of mathematics programs are available to do the calculations and produce convincing illustrations. The Maple program has been used extensively to produce the diagrams in [1] and this book and this appendix shows some of the expressions used. Other mathematics programs also have graphics outputs and there are a number of computer programs that can translate from one language to another.

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5. 6.

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of biomacromolecules (20 40 A2 ) In protein crystallography the variation of the temperature factor as a function of primary structure is frequently presented as a plot which can be useful in distinguishing exible regions from more rigid parts of the structure A measure of the progress of the re nement process is provided by the R factor which was de ned in Section 651 (Equation (617)) This represents a summation of the difference between observed structure factors and those calculated from the model However, the R factor is not an indication of the precision of the structure in that two models with the same R factor may have bond angles and lengths determined with quite different precision In situations where the preliminary model is close to the true structure, the comparison may be made using a least squares procedure.

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