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Mirror system

To make an oscillator from an amplifier requires, in the language of electronics, positive feedback. In lasers this is provided by the active medium being between two mirrors, both of them highly reflecting but one rather less so in order to allow some of the stimulated radiation to leak out and form the laser beam. The region bounded by the mirrors is called the laser cavity. Various mirror systems are used but that shown in Figure 9.1, consisting of... [Pg.337]

Optical devices or optical systems have provided most of the available strong shock data and were the primary tools used in the early shock-compression investigations. They are still the most widely used systems in fundamental studies of high explosives. The earliest systems, the flash gap and mirror systems on samples, provided discrete or continuous measurements of displacement versus time. [Pg.65]

We present the basics of optical design as it applies to two mirrored telescope systems. We discuss Zemike decomposition of wave-front error and the description of Strehl in terms of small Zemike errors. We also discuss the balancing of aberrations for a two mirror system and present the Ritchey-Chrdtien design as an example of a zero coma system. [Pg.37]

For any two-mirror system we can use geometric optics to derive equations that describe some important parameters. (For derivations see Schroeder, 2000). The effective system focal length can be determined in terms of the individual focal lengths and mirror separation ... [Pg.45]

In special applications people have built telescopes with very sparse arrays of mirrors in order to sample the resolution space with minimum number of mirrors. Systems like this may give greater angular resolution (longer baseline) but have less sensitivity due to the smaller collecting area. [Pg.66]

Figure 3.29 The intensity of the second harmonic wave generated in an autocorrelator as a function of the displacement of the moving mirrors system. The insets show the intensity versus time curves for pulses A and B of Figure 3.28 (solid and dashed lines, respectively). Figure 3.29 The intensity of the second harmonic wave generated in an autocorrelator as a function of the displacement of the moving mirrors system. The insets show the intensity versus time curves for pulses A and B of Figure 3.28 (solid and dashed lines, respectively).
The sample was placed in a quartz cell in a thermostated holder (25 + 0.5 °C). The laser line was focused by a lens and mirror system and the scattored light... [Pg.33]

In addition to an intense source and a well matched monochromator/mirror system, detectors require optimisation. For protein XAS, it is now well established that fluorescence detection is the preferred mode of detection Multi-detector... [Pg.79]

A mirror system for directing or focusing light energy... [Pg.164]

The software sends location information to the laser/mirror system, which then directs light energy to specific regions of a thin layer of photoreactive chemical (UV curable formulation) present on a movable platform in the reservoir. Simultaneously, the information package directs the system to lower the platform slowly with the cured slice of the object into the reservoir. ... [Pg.164]

The state-of-the-art mirror system now in use is a glass second-surface silver mirror backed with copper and paint, as shown in Fig. 2. For this system, the characterization and study of the glass/silver, silver/copper, and copper/paint interfaces before and after various stages of use are clearly required to understand the multilayer mirror stack. The methods of characterization outlined in Sec. 2.4 of Ref. 3, especially those of ISS, XPS, AES, and SIMS, are clearly applicable to this problem. In ter facial degradation reactions may begin at the silver/glass interface... [Pg.338]

Figure 2. Potential modes of degradation at interfaces in a typical mirror system. Figure 2. Potential modes of degradation at interfaces in a typical mirror system.
Dew point temperature Chilled mirror system with platinum resistance thermometer 0.3°C... [Pg.517]

For DRIFT studies, a wood wafer, paper sheet, or milled wood sample dispersed in KBr (or KC1) is placed in a cup at the focal point of the concave, ellipsoidal mirror so that the incident light is focused on the sample. The scattered light coming from the sample is collected from the concave mirror and directed by a suitable mirror system to the detector of the FTIR instrument. The pressure used for smoothing the sample has to be adjusted so that reproducible results can be obtained (Yeboah et al. 1984). The contribution of specular reflectance can be diminished by reducing the particle size and by increasing the sample dilution. For powder samples, as indicated above, the diluent is KBr or KCI. Good results are normally obtained with alkali halide powders that contain 1-2% of sample. In certain cases, the sample concentration may be increased up to 10%. [Pg.89]


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