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In BaTiO3, for pulse duration larger than 10 ns, the recombination time of free holes is shorter than the pulse duration. Consequently, the photorefractive effect builds up during the pulses. Nothing happens between the pulses, as long as thermal excitation can be neglected during the pulse interval. Let us summarize the observed effects when BaTiO3 is illuminated with nanosecond visible light. Under pulsed illumination, the saturation of the free carrier density was theoretically revealed [24]. This effect causes a nonconstant intensity photorefractive rise-time product, contrary to the CW illumination at suf ciently high illumination (SI @ b). It was also shown that the density of free

To illustrate some of the points discussed above, this section outlines the quantitative risk analysis that was used in the selection of a preferred option for a strategic river crossing.

#you wish to get a high BYTES hit ratio, you should probably If you wish to increase speed more than your want to

Some directive values can be constructed using the bitwise operators OR (|), AND (&), and NOT (~ or !). Flags can be turned on using any of the values 1, On, True, or Yes (and turned off with 0, Off, False, or No). Comment lines begin with a semicolon (;).

Figure 8.11. Schematic representation of the ring self-pumped phase conjugate mirror. Phase conjugate beams are observed in plane (P). Ai are the complex amplitudes of interacting beams in a plane wave model. PZT, piezo mirror used to wash out the re ection gratings.

So to retrieve a list of members that list travel as one of their interests, you could use:

The POLYGON command creates a polyline, meaning that the entire polygon is one object, rather than a series of line segments. In the exercise that follows, I indicate inches with a double prime (") and feet with a single prime ('). You may find this notation clearer when a measurement has both feet and inches, but you do not actually need to type the double prime for inches. When you have a measurement that is only in inches, it saves time to leave out the double prime.

where both 0 and are small compared to 1 . Expanding in Taylor series F (s + j ) around s = j 1 we get (see Appendix A.10) F (s + j ) F (j 1 ) = F (j ) ( j 0 ) + = 0 (5.52)

f 1 , BW (MHz, %) 1660, 2.0 1601, 1.6 1549, 1.5 1503, 1.5

public void setPictureName(String pictureName) { this.pictureName = pictureName; } public String getRequestId() { return requestId; } public void setRequestId(String requestId) { this.requestId = requestId; } public String getUserName() { return userName; } public void setUserName(String userName) { this.userName = userName; } }

The importance of ePR is that data travels with the patient and contains all pertinent medical information about the patient. The traditional ePR system very seldomly contains images or multimedia data. The multimedia ePR systems presented in this chapter, and in s 23 and 24, include all forms of media data in the ePR database. So the multimedia ePR constitutes a complete information system.

Things we believe might exist: Particle physics theories (particularly those aiming at unification of fundamental forces) have a habit of throwing up all manner of new and as-yet-undiscovered particles, several of which are plausible dark matter candidates. Particle physicists regard supersymmetry as the most solidly-founded extension to standard particle theory, and it has the nice property of associating a new companion particle to each of the particles we already know about. In the simplest scenarios, the lightest supersymmetric particle (LSP) is stable and is an excellent cold dark matter candidate. Depending on the model the particle in question might be called the photino, or gravitino, or neutralino. They are also sometimes known as WIMPs - Weakly Interacting Massive Particles.