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effect The thermal focal lens depends on the operating conditions of the ampli er, and especially on the absorbed average pump power [51, 56] For a pulsed pumping, the higher the repetition rate, the shorter the thermal focal lens [56] With typical values, the focal lens is about 50 cm for a ashlamp-pumped Nd:YAG ampli er at a repetition rate of 100 Hz It has also been observed and explained that thermal lensing effects differ for intracavity and extracavity operations [57] The thermal lens is hardly corrected by a compensative diverging lens having the same optical power as the laser rod, because transient effects occur in the rod for instance, during the warm-up of the laser Moreover, for a strong pumping, the thermal lens is not spherical but rather highly aberrated [58] As an example, an experimental study was performed on a 1.

064-mm longitudinally diode-pumped Nd:YVO4 laser probed by a 1074-mm Nd:YAP laser to avoid chromatic dispersion errors It revealed that spherical aberration and astigmatism had a Zernike coef cient half as high as defocusing [59] Consequently, adaptative devices are required Optical phase conjugation is one of them Section 842 is devoted to the use of photorefractive BaTiO3:Rh crystals for the realization of MOPA with phase conjugate mirror Section 843 compares this technique to other ways of performing dynamic wavefront correction: Photorefractive beam clean-up, intracavity active wavefront compensation, or, as widely discussed in other chapters of this book, stimulated Brillouin scattering, gain gratings, or thermal nonlinearity 842 MOPA laser sources including a photorefractive self-pumped phase conjugate mirror The rst compensation of a passive aberration by double pass after re ection on a phase conjugate mirror (using stimulated Brillouin scattering) was performed in 1972 [60].

The production, use, and control of x-rays are important aspects of radiation protection. When used in medicine, the medical goal as well as the protection goal is to optimize the parameters of purposeful exposures to obtain the greatest benefit (i.e., diagnostic information or treatment) while avoiding unnecessary radiation exposure of patients and workers. Fortunately, these are compatible goals: the sharpest and clearest x-ray images are obtained when those features that optimize exposure are also used. It is, unfortunately, also possible to obtain acceptable x-ray images with unnecessary exposures of patients and, even worse, to obtain x-ray images that do not contain the requisite information. Both circumstances impose unnecessary radiation, and can be especially harmful when a patient does not receive essential medical information. As shown in Figure 15-1, there are four major interconnected categories of physical principles in an x-ray system designed to optimize image quality and patient exposure:

Less than one year later, a master-oscillator power-ampli er (MOPA) structure using a Ruby ampli er was demonstrated [61] Many laser geometries have been tested with various nonlinear media in which phase conjugation was performed The MOPA structures, depicted in Fig 823 and demonstrated at 106 mm with either internal loop or ring BaTiO3:Rh phase conjugate mirrors, have been evaluated in a collaborative work between Thales Research and Technology (France) and the Laboratoire Charles Fabry de l Institut d Optique (France) [62] The laser beam experiences two (Fig 823a) or four passes (Fig 823b) in an Nd:YAG ampli er pumped by ashlamps at a repetition rate of 10 Hz No care was taken to compensate for depolarization that is negligible at a repetition rate of 10 Hz The oscillator is an intracavity- ltered Q-switched Nd:YAG laser delivering 20-ns pulses at a repetition rate of 10 Hz.

Note To add a folder to AutoCAD s support file search path, choose Tools Options and click the plus sign (+) next to Support File Search Path on the Files tab. Choose Add. Type in a folder path or choose Browse to locate one.

Table 13.17 lists the parent-child relationships. The xsl:attribute should be placed immediately after its parent. If it isn t parented by xsl:element, xsl:attribute-set, or xsl:copy, a new attribute will be created on the context node.

The beam diameter at 1/e 2 at the output of the oscillator is 25 mm A rst half-wave plate/Glan polarizer GP1 device is used to vary the incident energy in the ampli er rod The device formed by GP1, the Faraday rotator FR1, the half-wave plate, and the Glan polarizer GP2 suppresses beams propagating back to the oscillator and performs the extraction of the output beam after a double pass in the ampli er rod (Fig 823a) In the four-pass con guration, a Faraday rotator FR2 is inserted after the ampli er rod, so that the beam is directed to the phase conjugate mirror only after a double pass in the.