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Reflection cavity

Fig. 11. Chemical laser arrangement with flash initiation. 1 laser tube. 2 100% reflecting cavity mirror, 3 coupling mirror, 4 He-Ne laser for resonator alignment, 5 to gas manifold, 6 infrared detectors, 7 monochromator, 8 diode providing a triggering signal for the oscilloscope, 9 single spectral line, 10 total emission signal6)... Fig. 11. Chemical laser arrangement with flash initiation. 1 laser tube. 2 100% reflecting cavity mirror, 3 coupling mirror, 4 He-Ne laser for resonator alignment, 5 to gas manifold, 6 infrared detectors, 7 monochromator, 8 diode providing a triggering signal for the oscilloscope, 9 single spectral line, 10 total emission signal6)...
Fig. 21. Schematic representation of a subsonic C02 laser with purely chemical excitation (after Cool82)). A He and Fg injectors, H CO2 and NO inlet, C construction detail shown in B, L D2 mixing array, K part of the D2 inlet system which is shown in detail in J, D sodium chloride window, E totally reflecting cavity mirror with long focal length, M, F beam-folding (plane) mirrors, O partially reflecting cavity mirror for output coupling, N laser beam, G resonator housing flushed with nitrogen... Fig. 21. Schematic representation of a subsonic C02 laser with purely chemical excitation (after Cool82)). A He and Fg injectors, H CO2 and NO inlet, C construction detail shown in B, L D2 mixing array, K part of the D2 inlet system which is shown in detail in J, D sodium chloride window, E totally reflecting cavity mirror with long focal length, M, F beam-folding (plane) mirrors, O partially reflecting cavity mirror for output coupling, N laser beam, G resonator housing flushed with nitrogen...
Figure 2.7 Lumped circuit diagram for a reflection cavity... Figure 2.7 Lumped circuit diagram for a reflection cavity...
Next we may consider the sensitivity of the system to insertion of an analytical sample. This will act to increase the cavity loss, and so lower its Q (Equation 2.4). The optimum sensitivity will therefore occur when the derivative of the appropriate expression above with respect to k and to /Qc is a maximum. Choosing this appropriate expression is not, however, quite so straightforward as it may seem. For, with a reflection cavity we are observing not the signal inside the cavity, but that reflected from it. The most appropriate parameter to consider is therefore the derivative of the voltage reflection coefficient p with respect to... [Pg.31]

For this kind of cavity, there is no form of coupling that leads to zero power reflection as characterises the reflection cavity, but the optimum signal sensitivity still occurs at critical coupling. At this point only 11% of the incident power is... [Pg.34]

As a check, calculations were made for a 1-D equivalent of a U-fueled, DjO-reflected cavity reactor reported by Stratton. The transition to a 1-D system was done by albedo weighting the reflector to obtain an equfva-. lent slab reactor with one-half the cavity reaicfor s core. surface area. The experimental core thickness was given as 2 mil, while our calculated value for the equivalent.. stab was 2.5 mil. This result coupled with the earlier calculations Would indicate that there is a possibility of... [Pg.297]

Proceeding in a similar manner as in the nonretarded case, we now solve the Helmholtz equation in the presence of a single sphere, cylinder, or half-space j. Let the particle under investigation have the dielectric permeability Sj, the magnetic permeability fij, and the electrical conductivity Oj. Normalizability of the superpotential within a sphere or cylinder means that no Bessel functions of the second kind are permitted in the interior. In order to obtain normalizability within a half-space, we have to introduce a rear surface, which is situated at the intersection X = Xg of the half-space with the perfectly reflecting cavity. For the coefficients of the internal potentials we find in the case of... [Pg.76]

The mutual inversion of coordinates at spheres 1 and 2 entails accounting for the rotational symmetry by coupling inverted spherical harmonics P cos9i) exp in(pi) and P (cos92)exp(-i7<normal components of all fields to vanish on the surface of a perfectly reflecting cavity with radius r, yielding... [Pg.80]

A perfectly reflecting cavity with radius rg imposes the normalization condition... [Pg.81]

Figure 10.28 Textile slot spiral with shallow reflecting cavity (a) measured voltage standing wave ratio (VSWR) and circularly polarized gain and (b) measured radiation pattern across the band. Figure 10.28 Textile slot spiral with shallow reflecting cavity (a) measured voltage standing wave ratio (VSWR) and circularly polarized gain and (b) measured radiation pattern across the band.
Methods based on optical absorbance may also be used for air samples. For example, concentrations of gases such as methane and carbon dioxide may be measured by their optical absorbances at certain infrared wavelengths. A recent implementation of this principle for gases is cavity ring-down spectroscopy (CRDS), in which gas concentrations are inferred from fhe rate at which pulses of monochromatic light, tuned to the optical absorbance peak of fhe sample gas, die away in a reflective cavity. [Pg.61]


See other pages where Reflection cavity is mentioned: [Pg.346]    [Pg.347]    [Pg.1098]    [Pg.1098]    [Pg.28]    [Pg.29]    [Pg.32]    [Pg.32]    [Pg.33]    [Pg.35]    [Pg.115]    [Pg.127]    [Pg.439]    [Pg.297]    [Pg.93]    [Pg.227]    [Pg.202]   
See also in sourсe #XX -- [ Pg.29 ]




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