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Laser mirrors

Fig. 2. Representation of longitudinal modes ia a laser. Where line A = cj2D, c is the velocity of light, and D is the distance between the laser mirrors. Fig. 2. Representation of longitudinal modes ia a laser. Where line A = cj2D, c is the velocity of light, and D is the distance between the laser mirrors.
Surface modifications and surfiice roughness Cu, Mo, and Be laser mirrors atomic oxygen modified (corroded) surfaces and films, and chemically etched surfaces. [Pg.409]

Molybdenum is used for high energy laser mirrors which require water cooling. Corrosive action of the circulating cooling water can be prevented by coating the waterways with a thin film of tungsten by chemical vapour deposition. US Pat Application 308976 (1982). [Pg.850]

Coatings for high power laser mirrors using Reaction (3) and thermal annealing.t l... [Pg.158]

Carver, G. E., and Seraphin, B., Chemical Vapor Deposition Molybdenum Thin Films for High-Power Laser Mirrors, mLaser Induced Damage in Optical Materials, Publ. of National Bureau of Standards (Oct 1979)... [Pg.424]

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]

PROBLEM 21.7 Silica glasses used in lenses, laser mirrors, and other optical components can be made by the sol-gel method. One step in the process is the hydrolysis of Si(OCH3)4. Write a balanced equation for the reaction. [Pg.936]

For example, FT-Raman spectrometers have relatively large input apertures and etendue, and can often collect light reasonably efficiently from an unfocused laser spot. It is possible to position the smaller laser mirror in Figure 6.4A on the sample side of LI, allowing the laser to be unfocused or at least less tightly focused. If the laser spot is 1 mm instead of 100 pm, the power density decreases by a factor of 100 (Table 6.1). This procedure generally causes loss of signal compared to the focused case, but by a factor much smaller than 100. [Pg.119]

Molybdenum Semieonductor gate metallization, high-power laser mirrors, and coatings for solar converters. [Pg.447]

Fig. 8. Schematic diagram of ps fluorescence microprobe apparatus. PM Photomultiplier. D Diaphragm. XYS X-Y stage. F Filter. M Laser mirror. RS Rotating stage. Fig. 8. Schematic diagram of ps fluorescence microprobe apparatus. PM Photomultiplier. D Diaphragm. XYS X-Y stage. F Filter. M Laser mirror. RS Rotating stage.
Fig. 2. Diagram of the optical path of the bilateral laser scanning confocal microscope (InSIGHT). Real-time confocal imaging is obtained through the use of a double-sided mirror which simultaneously scans the sample and the oculars or detector at video rates. BSO, beam shaping optics LM, laser mirror D, dichroic M4, mirrors SM, scanning mirror G, galvonometer L1-L3 lenses S, variable slit. Fig. 2. Diagram of the optical path of the bilateral laser scanning confocal microscope (InSIGHT). Real-time confocal imaging is obtained through the use of a double-sided mirror which simultaneously scans the sample and the oculars or detector at video rates. BSO, beam shaping optics LM, laser mirror D, dichroic M4, mirrors SM, scanning mirror G, galvonometer L1-L3 lenses S, variable slit.
Ultraprecise surface figuring (e.g., optics with accuracy in the nm scale, i.e., stepper optics, x-ray-optics, infrared optics, diffractive optics, laser mirrors). [Pg.216]

Films for highly sophisticated optical applications, such as for special laser mirrors, should have no absorption losses because these obviously decrease the reflectivity and lower the damage threshold for high power radiation. It is very important in the deposition of such films to achieve complete oxidation, since traces of metal atoms or metal suboxides cause absorption. It has been shown by various researchers that better stoichiometric films can be achieved with activated oxygen gas containing ions and excited molecules, than by the use of ordinary neutral oxygen gas [390, 395, 396, 397, 429]. This holds especially true for the fabrication of fully oxidized compound films. [Pg.286]

J. Segner, Plasma Impuls Chemical Vapour Deposition - a Novel Technique for the Production of High-Power Laser Mirrors, Mat. Sci. Engin., A 140 (1991) 733. [Pg.315]

Figure 27 shows the spectral reflectance curve of a broadband laser mirror. [Pg.463]

In absence of laser mirrors, optical feedback at the both faces was only provided by the Fresnel reflection. Taking into account the refractive index of Nd YAG ceramics (no=1.8), and using Fresnel equations. [Pg.650]

C02-laser mirrors Range finders Phase plates... [Pg.394]

A KrF excimer laser (Lambda Physik LEXTRA 200, 248 nm, 30 ns fwhm) or a XeF excimer laser (ibid., 351 nm, 30 ns fwhm) was used as an excitation pulse for inducing expansion/contraction dynamics. The fluence was adjusted with partially transmitting laser mirrors, and was monitored shot-by-shot by a photodiode whose output was corrected with a joulemeter (Gentec, ED-200) with an oscilloscope (Hewlett-Packard, HP54522A). A c tral area of the excimer laser pattern with a homogeneous intensity distribution was chosen with an appropriate aperture and then focused onto the sample surface by using a quartz lens (f = 200 mm). Fresh surface of the sample film was used in every measurement. Etch depth was measured by a surface depth profiler (Sloan, Dektak 3). All experiments were done in air at room temperature. [Pg.214]

Glass matrix composites, in particular with carbon fibre reinforcement, have been also proposed for a variety of applications which require thermal dimensional stability, i.e. materials with multidimensional near zero thermal expansion coefficients such as support structures for laser mirrors [21, 22]. [Pg.463]

Fig. 3.7. MultiMode SPM head and major components laser (/) mirror (2) cantilever (3) tilt mirror (4) and photodetector (5). Reprinted from [9,13]... Fig. 3.7. MultiMode SPM head and major components laser (/) mirror (2) cantilever (3) tilt mirror (4) and photodetector (5). Reprinted from [9,13]...
Laser alignment There are two methods for ahgning the laser, mirror, and photodiode for all modes except STM, since STM does not use a laser. The first method uses a high-powered monocular magnifier to observe the laser spot s position on the cantilever. The second method uses a strip of paper to observe the laser s position. The choice of method is largely a matter of personal preference. [Pg.42]

Emmony DC, Howson RP, Willis LJ (1973) Laser mirror damage in germanium at 10.6 mm. Appl Phys Lett 23(11) 598-600... [Pg.1593]


See other pages where Laser mirrors is mentioned: [Pg.553]    [Pg.127]    [Pg.216]    [Pg.180]    [Pg.23]    [Pg.553]    [Pg.216]    [Pg.391]    [Pg.88]    [Pg.502]    [Pg.485]    [Pg.24]    [Pg.240]    [Pg.145]    [Pg.28]    [Pg.65]    [Pg.459]    [Pg.464]    [Pg.491]    [Pg.299]    [Pg.299]    [Pg.711]    [Pg.4213]   
See also in sourсe #XX -- [ Pg.286 , Pg.458 , Pg.463 ]




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