Titlebook: High-Peak-Power Nd: Glass Laser Systems; David C. Brown Book 1981 Springer-Verlag Berlin Heidelberg 1981 laser

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the invasion of exotic species. The genus . for instance is currently invading Belgian watercourses in increasing numbers. Since no Belgian Biotic Index (BBI) tolerance class is defined for ., this may cause inconsistencies in index calculations as well. In order to eliminate these, a semi-fixed ta

MIR

aspersion

Optical and Physical Properties of Laser Glasses, in the consideration of laser glasses for practical applications. We refer particularly to impurity problems, thermal-shock resistance, durability, and intrinsic stress, all of which have been found to be important for consideration, in addition to the more fundamental properties previously discuss

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Damage Effects in High-Peak-Power Nd : Glass Laser Systems,amage threshold to minimize the diameter. Although the general subject of optically induced damage has matured considerably in recent years, progress has been slow owing to the experimental and theoretical complexities. At the present time, workers in the field cannot even agree on the basic physica

NIL

Nonlinear Effects in High-Peak Power Nd: Glass Laser Systems,ll known to the experimentalist in this area. Although the basics of self-focusing theory (Sect.7.2–4) were known for some time previous to the advent of the construction of large Nd:glass laser systems, the major contribution here is the development of semi-phenomenological theories that enable the

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The Design of High-Peak-Power Nd : Glass Laser Systems,r) and the long-pulse (high-energy) regimes. Although we will treat here only the design of the high-peak-power systems, the optimization procedure for high-energy systems is straightforward and, in fact, much simpler.

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Glass Laser Physics,damental physics of the trivalent rare-earth Nd ion in various glass and crystalline hosts. It is worthwhile pausing here to understand the reasons for Nd:glass becoming the predominant optical material to be used today.

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Amplifiers for High-Peak Power Nd : Glass Laser Systems,t level. Optimization of the performance of such amplifiers leads to maximum system performance at minimum cost. In this chapter we investigate the general characteristics and present operating conditions for disk, active-mirror and rod amplifiers. It will be shown how it is possible to design an op