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Q-switched lasers with an SBS cell can reach even slightly higher ef ciencies than comparable free running lasers as will be shown in Section 37 Inside a laser resonator the SBS threshold can be reduced by a resonant generation of the sound wave [19, 20] from the longitudinal laser modes It will be shown in Section 35 that the resonance condition for the so-called start resonator is a key precondition for reliable operation of a laser oscillator with phase conjugating SBS mirror The re ection at the moving sound wave in the SBS mirror leads to a Doppler shift (Brillouin shift) of the backscattered light This causes a transient longitudinal mode spectrum of the SBS laser as will be shown in Section 36 There are other possibilities than SBS to realize a phase conjugating cavity mirror.

In the 1970s and 1980s, four-wave mixing and BEFWM were more in the focus to realize phase conjugating laser mirrors (see, eg, Refs 21 23) These techniques lead to PCMs without a threshold behavior But high-quality pump beams are required to realize such a PCM Photorefractive cavity mirrors are discussed in 9 of this book, gain gratings in 10 and other techniques in s 10 and 11 32 SURVEY OF DIFFERENT RESONATOR CONCEPTS WITH BRILLOUIN MIRRORS The rst laser resonator with an SBS mirror was realized in 1967 by Pohl [24] This was even before experimental and theoretical evidence was found that SBS can be.

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The embedded style sheet is called internal in GoLive terminology because it is embedded internally in the top of your page. Because it is internal, it can apply only to that page. The external style sheet is a freestanding document and is therefore available to any page within your site. In both cases, the code for the styles and their effect is the same. And either way, you create the style sheet using the CSS Selector Inspector.

Understanding Images on the Web . . . . . Graphic formats A quick overview Collecting Images in the Site Window . . . Collecting images . . . . . . . . . . . . Organizing your images . . . . . . . . Previewing Images . . . . . . . . . . . . . . File Preview . . . . . . . . . . . . . . . Page Preview . . . . . . . . . . . . . . Previewing an image file . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 251 252 255 255 256 257 257 257 258

so a change in the noise gure can be related to a change in the noise factor by dFcas = dFcas 4.343 dB dfcas = dfcas = 4.343 dB 10 Fcas /10 dfcas fcas

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Thus the Gibbs sampling process recovers the marginal of interest: ( ) The two-step nature of the process ensures that the stationary process remains ( ) since the detailed balance equation is maintained: (u | ) ( )P [ |u)] =.

*All the companies whose names are asterisked were kind enough to furnish keyboard and mouse kits for this book.

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