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capability of aberration compensation was also shown in the earliest research works on Fourier optics and holography. Kogelnik [2] had already demonstrated that static aberrations can be compensated by using conventional holographic recording. After processing of the photographic media and proper readout of the hologram, it generated the backward conjugate wave for a clear image restoration through a distorting media. The analogy of phase conjugation with dynamic holography was then outlined by Yariv [3] and in early experiments with photorefractive crystals [4], and it contributed to extend the eld of applications, thus including parallel image processing, optical correlation for pattern recognition, holographic interferometry for non destructive testing, incoherent to coherent image conversion, novelty lters for moving object detection [3]. It was then recognized that when doing simultaneous recording and readout of a volume hologram with beams having the same or nearly the same wavelength, the incident or conjugate waves can be ampli ed [5 8]. This is due to the energy transfer from the pump beams which interfere with the probe beam in the volume of the nonlinear media. These phenomena of mutual coupling of waves interfering in the nonlinear media are of great importance in view of applications and have led to remarkable uni ed treatments of the elds of nonlinear optics and dynamic holography. These interactions have led to outstanding applications to coherent beam ampli cation and to ampli ed phase conjugation. The possibility of amplifying the amplitude of a complex wavefront through a third-order nonlinearity

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Instead of calling a conversion function, you can use parentheses in your format string and PyArg_ParseTuple unpacks sequence arguments on the fly:

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Some drawings are too large to fit on a floppy disk, and the number of disks that you need to store all of your drawings may make easy storage impossible. You ll probably want to invest in one of the many types of removable backup systems. These come in four main types: Tape drives (internal or external) are cheap and good for entire hard-drive backups. Disk cartridge drives offer the convenience of a floppy disk but with more capacity. Read/write DVD-ROM or CD-ROM drives enable you to write to a DVD or CD-ROM. Optical drives have the longest life (at least 30 years) and resist accidental erasure. If your drawings are really important to you, back them up twice and store one backup set off-site. This way, if your office burns down, you haven t lost everything. Remote backup services provide this type of archiving for you, and you can access your files through modem or the Internet. The secret to backing up is to create a schedule and then stick to it. For example, you may do a complete hard-drive backup once a week, and do drawing backups at the end of each day. Each situation is different, but take the time to think about your needs, create a system, and let everybody know about it. Then do it.

f 1 , BW (MHz, %) 1530, 3.1 1498, 3.7 1484, 3.8 1568, 3.1 1524, 4.1 1496, 3.5 1560, 3.3 1538, 3.8 1498, 2.8

Username is user account name that will be used to launch the program or shortcut file specified. After this command is entered, you re prompted to supply the user s password, as shown in Figure 1-23. For a complete breakdown of switches and settings associated with the runas command, enter runas / at the Command Prompt.

Best Practices for SAN Deployment Key Points 23 Using SANs for High Availability Configuring an HA SAN

Figure 11.4 shows an alternative way of presenting the Airy pattern; the vertical height of the gure represents the relative intensity. Such a gure is sometimes called a diffraction solid. Figure 11.5 represents the same solid with increased vertical scale to show the details of the outer rings. 11.2.2. The Defocused Airy Pattern One of the earliest ndings of practical experience in star testing is that it is very useful to examine the defocused point spread function on both sides of the best focal plane. This may seem paradoxical, but it is found to be much easier to diagnose the aberrations from the defocused image than from the image at best focus. We therefore show in Figure 11.6 the contours of constant intensity (isophots) in a plane containing the optical axis. The axes correspond to a radial coordinate in the image plane (vertical axis) and to the defocus distance along the principal way. The image plane coordinate is the same dimensionless coordinate as was used in Figures 11.1 and 11.2 and the defocus coordinate, explained in the caption, is also dimensionless. The scales are such that the geometrical cone of rays would have a semiangle of 45 , but by using appropriate values of the convergence angle x and the wavelength A, the diagram can represent any coney Several features of this distribution are worth noting. It is symmetrical about the true focal plane. There are zeros ( dark spots ) along the axis, equally spaced (apart from one missing at the focal plane) and alternating with maxima. The intensity along the axis is shown in Figure 11.7. In Figure 11.6, the out-of-focus patterns consist of bright

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