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the overlapping rst and third foci in the SBS cell generate a four-wave mixing interaction that serves to strongly stabilize the Stokes return from the phase conjugate mirror. The effect of this interaction is to feed a portion of the generated Stokes signal back through the loop and into the phase conjugated wave. The stimulated scattering system then does not rely on input light scattered from acoustic noise at focus to sustain the Stokes return after the SBS threshold is reached. This increased stability is readily apparent upon comparing the input/output power plots for the single focus cell and the loop in Fig. 5.17. The power uctuations observed in the single-focus SBS mirror were not reproducible from shot to shot but were always of comparable magnitude to the curve shown. This data were collected by simply placing a block in the beam after the rst pass through the SBS cell, reducing the phase conjugator to a simple single focus. Besides the signi cant decrease in the power threshold, the Stokes power uctuations are dramatically reduced when the loop is unblocked. The four-wave mixing interaction also plays a crucial role in maintaining temporal phase stability in the laser ampli er output, as will be described in the upcoming discussion on coherence length. Bi-exponential oscillator buildup As can be seen in the hysteresis of the data curves in Fig. 5.17, even when using the SBS loop geometry, the lowest possible threshold is not achieved with the 60-ns input pulse rise times required for 500- to 1000-ns pulse ampli cation. One way of lowering the transient SBS
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Certain save options that once were available only via the Save a Copy command now appear in the Save dialog box all the time. You also get access to these options when you choose Save As or press its keyboard shortcut, Ctrl+Shift+S. Figure 3-7 shows the dialog box.
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Figure 10-33: A mechanical drawing showing a small section of a porcupine mixer. 3. Choose Fillet from the Modify toolbar. At the Select first object or [Undo/ Polyline/Radius/Trim/Multiple]: prompt, right-click and choose Radius. At the Specify fillet radius <1/2>: prompt, type 5/8 .
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where m is the dielectric constant of the metal lm and ns is the refractive index of the dielectric medium, in this case liquid. The evanescent wave can couple by resonance (hence surface plasmon resonance) with plasmons in the metal when K ev = K sp . This happens only at speci c values of . Some energy is lost from the incident light as a result
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Figure 4-23: Here I use the Channel Mixer command to repair the blue channel by mixing in 10 percent of the red channel and 30 percent of the green channel. The red and green channels remain unaffected.
NO-dependent vasorelaxation (Lembo et al., 2000). These endothelium-dependent vasodilators are distinct from the endotheliumindependent vasodilators such as sodium nitroprusside, which breaks down to yield NO directly. NO can be inactivated or quenched by various compounds, including reactive oxygen species (ROS) generated, for example, by the advanced glycation end-products (AGE), which accumulate in diabetes and are taken up into cells via speci c receptors (RAGE) (Figure 12.13). Endothelium-dependent vasodilatation (usually in response to acetylcholine) can be measured using forearm blood- ow techniques. Impairment of this response that is, endothelial motor dysfunction is a striking feature of type 2 diabetes, insulin resistance, dyslipidaemia (especially hypertriglyceridaemia) and obesity (Steinberg et al., 1996; Watts et al., 1996; Shimokawa, 1999). Impaired vasorelaxation will raise peripheral resistance and therefore blood pressure. Moreover, this abnormality is particularly important because prospective studies have shown it to be a powerful predictor of atherogenesis, CAD and myocardial infarction (Sch chinger, Britten and Zeiher, 2000). Loss of insulin action in inducing eNOS a potential manifestation of insulin insensitivity was previously held responsible for endothelial dysfunction in insulin-resistant states, but
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