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Lasers, use

Apart from the obvious property of defining pulses within short time intervals, the pulsed laser radiation used in reaetion kineties studies ean have additional partieular properties (i) high mtensity, (ii) high monoehromatieity, and (iii) eoherenee. Depending on the type of laser, these properties may be more or less pronouneed. For instanee, the pulsed CO2 lasers used in IR laser ehemistry easily reaeh intensities between... [Pg.2136]

MW em and GW em Speeial lasers used in nuelear frision experiments may even reaeh 10 W em [78, 79]. Ideally the monoehromatieity, Av, is related to the pulse length. At, tlirough... [Pg.2136]

Schematic diagrams of modem experimental apparatus used for IR pump-probe by Payer and co-workers [50] and for IR-Raman experiments by Dlott and co-workers [39] are shown in figure C3.5.3. Ultrafast mid-IR pulse generation by optical parametric amplification (OPA) [71] will not discussed here. Single-colour IR pump-probe or vibrational echo experiments have been perfonned with OP As or free-electron lasers. Free-electron lasers use... Schematic diagrams of modem experimental apparatus used for IR pump-probe by Payer and co-workers [50] and for IR-Raman experiments by Dlott and co-workers [39] are shown in figure C3.5.3. Ultrafast mid-IR pulse generation by optical parametric amplification (OPA) [71] will not discussed here. Single-colour IR pump-probe or vibrational echo experiments have been perfonned with OP As or free-electron lasers. Free-electron lasers use...
For many lasers used in scientific work, the light is emitted in a short pulse lasting only a few nanoseconds, but the pulses can be repeated at very short intervals. Other lasers produce a continuous output of light. [Pg.384]

A remarkable feature of these spectra is the resolution of individual rotational lines in such large molecules. [Note that the expanded specttum in, for example. Figure 9.47(a) covers only 5000 MFIz (0.17 cm )]. This is due partly to the very low rotational temperature (3.0 K for aniline and 2.2 K for aniline Ar), partly to the reduction of the Doppler broadening and partly to the very high resolution of the ring dye laser used. [Pg.398]

The efficiency of a helium—neon laser is improved by substituting helium-3 for helium-4, and its maximum gain curve can be shifted by varying the neon isotopic concentrations (4). More than 80 wavelengths have been reported for pulsed lasers and 24 for continuous-wave lasers using argon, krypton, and xenon lasing media (111) (see Lasers). [Pg.15]

The GaAs laser used as light source emits at about 820 nm. Thus dyes in the actual sense are not needed rather, ir-absorbers for the spectmm between 750—850 nm Httie experience is available on this class of dyes, especially as far as their stabiHty is concerned, although much work has been done in this area. Also, infrared sensitive dyes and pigments, used in electrophotography, may be very suitable for WORM disks (8). [Pg.140]

Krypton lasers are also ionized gas lasers and are very similar in general characteristics to argon lasers (27). Krypton lasers having total multiline output up to 16 W are available commercially. The strongest line at 0.6471 p.m is notable because it is in the red portion of the spectmm, and thus makes the krypton laser useful for appHcations such as display and entertainment. [Pg.6]

Isotope shifts for most elements are small in comparison with the bandwidth of the pulsed lasers used in resonance ionization experiments, and thus all the isotopes of the analyte will be essentially resonant with the laser. In this case, isotopic analysis is achieved with a mass spectrometer. Time-of flight mass spectrometers are especially well-suited for isotopic analysis of ions produced by pulsed resonance ionization lasers, because all the ions are detected on each pulse. [Pg.135]

Different lasers use different materials as the active medium. The medium can be either solid, liquid, or gas, and there are advantages for each in the amount of energy that can be stored, ease of handling and storage, secondary safety hazards, cooling properties, and physical characteristics of the laser output. [Pg.705]

Gas lasers are not unlike fluorescent light bulbs and neon signs. Gas is confined to a hollow tube, and electricity passing through it excites the atoms. The most common gas lasers use carbon dioxide, argon, and helium-neon. Gas lasers are relatively inexpensive and can produce very high-powered beams. [Pg.705]

Excimer lasers use gases, but because of their special properties are usually considered as a class of their own. Excimer is short for excited dimer, which consists of two elements, such as argon and fluorine, that can be chemically combined in an excited state only. These lasers typically emit radiation with veiy small wavelengths, in the ultraviolet region of the electromagnetic spectrum. This shorter wavelength is an enormous advantage for many applications. [Pg.705]

Time-resolved microwave conductivity measurements with electrodes in electrochemical cells can conveniently be made with pulsed lasers (e.g., an Nd-YAG laser) using either normal or frequency-doubled radiation. Instead of a lock-in amplifier, a transient recorder is used to detect the pulse-induced microwave reflection. While transient microwave experiments with semiconducting crystals or powders have been performed... [Pg.447]

Arsenic and antimony are metalloids. They have been known in the pure state since ancient times because they are easily obtained from their ores (Fig. 15.3). In the elemental state, they are used primarily in the semiconductor industry and in the lead alloys used as electrodes in storage batteries. Gallium arsenide is used in lasers, including the lasers used in CD players. Metallic bismuth, with its large, weakly bonded atoms, has a low melting point and is used in alloys that serve as fire detectors in sprinkler systems the alloy melts when a fire breaks out nearby, and the sprinkler system is activated. Like ice, solid bismuth is less dense than the liquid. As a result, molten bismuth does not shrink when it solidifies in molds, and so it is used to make low-temperature castings. [Pg.745]

Advances in laser technology now allow for solid-state lasers of high beam quality. These beams may be projected from a much smaller auxiliary telescope, which negates the need for optical switching and completely eliminates any main telescope fluorescence. Solid-state YAG lasers are the most common type of lasers commercially available. These lasers use a crystal as the lasing... [Pg.221]

Ruby lasers use crystals of AI2O3. The crystals contain small amounts of Cr ions, which absorb light... [Pg.458]

Richeboeuf, L., Pasquiers, S., Legentil, M. et al. (1998) The influence of H2 and C2H6 molecules on discharge equilibrium and F-atom production in a phototriggered HF laser using SF6, J. Phys. D Appl. Phys. 31, 373-89. [Pg.393]

Weber FIP (1967) Method for pulsewidth measurement of ultrashort light pulses generated by phase-locked lasers using nonlinear optics. J Appl Phys 38 2231-2234... [Pg.146]

Another difference in these FRET methods is the cost of the microscopes. The two-photon microscope and its mode-locked laser used for sRET and FLIM-FRET cost approximately an order of magnitude more than the E-FRET system. Clearly, if cost is a limiting factor then the E-FRET approach is superior. [Pg.397]

A lot of features of MALDI are conveyed by its name it is a desorption ionization, produced by a laser beam, and assisted by a matrix (Figure 2.5). The analyte (1 pmol or less) is mixed with a suitable matrix in a 1 1000 or higher molar ratio. The matrix is composed of a compound with a strong absorption at the wavelength of the laser used. These two factors, matrix excess and its strong absorption, ensure that the energy from the laser pulse is absorbed by the matrix and not by the analyte, thus avoiding its decomposition. Nicotinic acid, sinapinic acid (SA), 2,5-dihydroxy benzoic acid (2,5-DHB) and 2-(4-hydroxyphenylazo)benzoic acid (HABA) are some of the most commonly used matrices for MALDI. [Pg.51]

Solid-state lasers using substitutional neodymium (Nd3+ ions) as the active defects are widely available. Practical lasers contain about 1% Nd3+ dopant. The most common host materials are glass, yttrium aluminum garnet (YAG), Y3A15012, and calcium tungstate, CaW04. In the crystalline host structures, the defects responsible for amplification are NdY and Ndca-... [Pg.430]


See other pages where Lasers, use is mentioned: [Pg.235]    [Pg.2955]    [Pg.132]    [Pg.217]    [Pg.2]    [Pg.2]    [Pg.6]    [Pg.8]    [Pg.8]    [Pg.704]    [Pg.705]    [Pg.1143]    [Pg.128]    [Pg.178]    [Pg.145]    [Pg.60]    [Pg.415]    [Pg.133]    [Pg.93]    [Pg.285]    [Pg.48]    [Pg.280]    [Pg.378]    [Pg.94]    [Pg.424]    [Pg.430]    [Pg.473]    [Pg.173]    [Pg.232]    [Pg.373]   
See also in sourсe #XX -- [ Pg.463 , Pg.464 ]




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Atmospheric gas monitoring using tuneable diode laser absorption spectroscopy

Biosensors Using Lasers

Breath diagnostics using laser spectroscopy

Detection using laser-induced

Detection using laser-induced fluorescence

Fast beam experiments using laser

Field Experiments Using Femtosecond Laser Filamentation

Flash using laser

Infrared lasers, time-resolved measurements using

Initiating method using plasma laser

Interfaces Using Laser Light

Isotope separation, using lasers

Laser ablation plumes used in thin film

Laser desorption/ionization mass spectrometry organic material analysis using

Laser flash photolysis use

Laser ionization sources using

Lasers uranium isotopes separated using

Matrix-assisted laser desorption ionisation matrices used

Matrix-assisted laser desorption ionization mass analyzers used with

Matrix-assisted laser desorption/ionization matrices used

Measurement of texture profile using laser sensors

Metal carbides, synthesis using laser

Metal oxides, synthesis using laser

Microstructuring Glasses Using Lasers

Microstructuring using Short-Pulse Lasers

Mixed oxides, synthesis using laser

Nuclear Activation Using Electron Bunches from Laser Plasmas

Optical Methods Using a Laser for Fouling Characterization

Phase fluorometers using the harmonic content of a pulsed laser

Photochemical aspects of photoinitiation using NIR lasers

Platelet Micro- and Macro-Aggregation Using Laser Scattering

Quantitative analysis using laser ablation

Raman spectra using laser

Ruby laser, flash photolysis using

Solid sample analysis using laser ablation

Surface Analysis Using Laser Ablation with ICP-OES

The use of lasers to improve knot security

Trajectories of Multiple People in Crowds Using Laser Range Scanner

Use of diode laser

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