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and the intrinsic aberration is just Wfocus . It is important to point out that this method works for Twyman Green well as for Fizeau interferometers.

Watched folders can be individual folders, hard drive partitions, or dedicated hard drives. When you choose Settings Watched Folders, a dialog box appears enabling you to establish preferences for the watched folders and distillation attributes. The options available in the Watched Folders dialog box include the following: Watched folders list: The list window displays all folders you have identified to be watched. The name of the watched folder appears in the list as well as the directory path. In Figure 5-23, notice the directory is D:\ and the folder name is Acro5 Bible as might be viewed in Windows. On the Macintosh, the name of your drive (for example, Macintosh HD) appears first in the list followed by the folder name(s).

Address ------10.10.0.5 100.100.100.100

Add smooth arc to end of active path Add cusp to end of active path Add point to end of active magnetic selection Delete last point added with standard or Magnetic Pen tool Draw freehand path segment

Table 16.11 Compressive and Flexural Tests for FRC [86] Comp. Strength (MP a) 52.6 52.2 51.5 61.8 40.7 Flex. Strength (MP a) 4.65 4.58 4.99 4.09 4.35

Conjugate Lasers with the objective of showing the impact of these innovative concepts on the architectures and performances of a new class of solid-state lasers Phase conjugate lasers exhibit adaptive correction of their own aberrations whatever their operating conditions, and they provide maximum brightness to the user for a large diversity of scienti c or industrial applications The critical issue of this very attractive approach is to identify the most ef cient media and nonlinear mechanisms that operate at the required wavelengths In this perspective, the book presents the basic physical phenomena and materials involved for ef cient generation of the conjugate waves for speci c examples of laser sources The book also develops in detail an analysis of the laser architectures and nonlinear mirrors that are best suited to operate in continuous-wave or pulsed regimes, respectively.

The ability of phase conjugate lasers to deliver beams with a high spatial and spectral quality is clearly outlined in the different chapters After a brief overview of the basic principles of nonlinear optical phase conjugation in 1, a large part of the book is devoted to lasers, including a Brillouin phase conjugating mirror In 2 the principles, the basic properties, the materials (bulk and ber geometry), and performances of stimulated Brillouin scattering (SBS) mirrors are presented Such nonlinear mirrors can be implemented inside a laser resonator as shown in 3 Besides the demonstration of high brightness operation, the authors analyze in detail the stability and the mode structures of these unconventional nonlinear resonators To achieve high power with a near-diffraction-limited beam, master-oscillator power-ampli er (MOPA) con gurations are demonstrated in 4 in which both liquid and glass ber Brillouin conjugators are used.

The ber presents the advantages of compactness and lower energy threshold due to the long interaction length of the ber medium However, to achieve very high energy the use of SBS liquid cells is required as presented in 5 Using the capability of phase conjugation to phase-lock several beams issued from different ampli ers, the authors demonstrate up to 100 J of output energy while keeping the beam quality close the diffraction limit Some applications may require solid-state SBS mirrors instead of liquid cells For that purpose, the authors of 6 investigate and characterize SBS properties of bulk solid-state materials like organic crystals and glasses The previous chapters have concerned the ability of SBS mirrors to compensate for phase aberrations of gain media It is also important to highlight (as done in 7) that an SBS nonlinear mirror can perform pulse compression in the time domain.

The a posteriori probability < ( k )of the detected symbol can be obtained without the knowledge of the term P ( v k ) , if the a posteriori probability has unity support (i.e. the sum of the a posteriori probabilities of all symbols is unity): (9.9)