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Limit laser spectroscopy

The different sensitive techniques of Doppler-limited laser spectroscopy discussed in the previous sections supplement each other in an ideal way. In the visible and ultraviolet range, where electronic states of atoms or molecules are excited by absorption of laser photons, excitation spectroscopy is generally the most suitable technique, particularly at low molecular densities. Because of the short spontaneous lifetimes of most excited electronic states E, the quantum efficiency tjk reaches... [Pg.76]

Particularly for polyatomic molecules with their complex visible absorption spectra, the reduction of the Doppler width is essential for the resolution of single lines [392]. This is illustrated by a section from the excitation spectrum of the SO2 molecule, excited with a single-mode frequency-doubled dye laser tunable around X = 304 nm (Fig. 4.4b). For comparison the same section of the spectrum as obtained with Doppler-limited laser spectroscopy in an SO2 cell is shown in Fig. 4.4a [391]. [Pg.187]

The different sensitive techniques of Doppler-limited laser spectroscopy, discussed in the previous sections, supplement each other in an ideal way. [Pg.404]

The visible spectrum of most polyatomic molecules is generally so complex that resolution of single lines is only seldom possible with conventional absorption spectroscopy. Even Doppler-limited laser spectroscopy may leave many partially overlapping lines. A good example where the transition region from a medium to a high line density has been studied in detail is the band head of the (1,00) (0,00) band in the 3/2... [Pg.408]

As described above, classical infrared spectroscopy using grating spectrometers and gas cells provided some valuable infonnation in the early days of cluster spectroscopy, but is of limited scope. However, tire advent of tunable infrared lasers in tire 1980s opened up tire field and made rotationally resolved infrared spectra accessible for a wide range of species. As for microwave spectroscopy, tunable infrared laser spectroscopy has been applied botli in gas cells and in molecular beams. In a gas cell, tire increased sensitivity of laser spectroscopy makes it possible to work at much lower pressures, so tliat strong monomer absorjDtions are less troublesome. [Pg.2442]

Photolysis of DMDAF in benzene containing methyl alcohol gives the ether expected from the reaction of the singlet carbene. Monitoring this reaction by laser spectroscopy reveals that the detected transient reacts with the alcohol with a bimolecular rate constant very near the diffusion limits. In contrast, the transient reacts with triethylamine at least 100 times more slowly than it does with alcohol (Table 7). This behavior is inconsistent with identification of the transient as the cation or radical and points to its assignment as the singlet carbene. [Pg.344]

Infrared diode laser spectroscopy has been used for the measurement of hydrocarbon and CO concentrations in exhaust (13, 14, 15). The adsorption path length, and thus the absorption cell volume, required for hydrocarbon measurement is rather large, limiting the time-resolution of the measurement. The absorption path length required for CO measurement, however, is relatively short and approximately equal to the diameter of a standard exhaust pipe. This allows CO to be measured with high time-resolution by an infrared laser beam passed through an... [Pg.66]

Although exceedingly useful, the application of OS is not without problems. Optical spectra in condensed media consist of broad bands without identifying features structural information can be derived by comparison with known species, or by high-resolution laser spectroscopy. The TR-OS is often limited to wavelengths >300 nm, excluding some prototypes of the most interesting species. [Pg.212]

Accuracy of the radiofrequency measurements of the classic 2S — 2P Lamb shift [15, 16, 23, 24, 25] is limited by the large (about 100 MHz) natural width of the 2P state, and cannot be significantly improved. New perspectives in reducing the experimental error bars of the classic 2S — 2P Lamb shift were opened with the development of the Doppler-free two-photon laser spectroscopy for measurements of the transitions between the energy levels with different principal quantum numbers. Narrow linewidth of such transi-... [Pg.237]

Laser state-to-state techniques include both the application of highly sensitive laser spectroscopy for internal state-resolved detection of molecules in the gas phase, e.g., desorbing or scattering from a surface, and second, for laser pumping an initial state prior to interaction with a surface. To date, laser detection of internal states has been widely applied in gas-surface dynamics experiments, while those involving optical state preparation techniques have only been applied in a limited fashion. [Pg.174]

Wall-coated flow tube reactors have been used to study the uptake coefficients onto liquid and solid surfaces. This method is sensitive over a wide range of y (10" to 10 1). For liquids this method has the advantage that the liquid surface is constantly renewed, however if the uptake rate is fast, the liquid phase becomes saturated with the species and the process is limited by diffusion within the liquid, so that corrections must be applied [70,72,74]. Many experiments were designed to investigate the interaction of atmospheric species on solid surfaces. In this case the walls of the flow tube were cooled and thin films of substrate material were frozen on the wall. Most of the reaction probabilities were obtained from studies on flow tubes coated with water-ice, NAT or frozen sulfate. Droplet train flow tube reactors have used where liquid droplets are generated by means of a vibrating orifice [75]. The uptake of gaseous species in contact with these droplets has been measured by tunable diode laser spectroscopy [41]. [Pg.273]

The wavelength dependence of laser-stimulated recombination could be used to perform spectroscopy. The recombination rate is closely related to the distribution of positrons in energy and also to the population of bound levels close to the ionization threshold [17]. The spectral resolution for the first step of laser-stimulated recombination is thus limited by the energy distribution of the positrons. Laser-induced two-step recombination, first into a high-lying state with the subsequent stimulation of a bound-bound transition into a lower lying state, offers a first possibility for precise laser spectroscopy [18]. [Pg.522]

This Doppler width can be avoided by typical sub-Doppler laser spectroscopy techniques. Laser saturation spectroscopy with a resolution close to the natural line width was used for a test of Special Relativity at the ESR. For such sub-Doppler resolution one must also take into account the small additional broadening and shift arising from the angle 0 between laser beam and ion beam in the Doppler formula. At an interaction length of 10 meters and more, angles are easily controlled to be better than 1 mrad. This limits a possible shift, which enters by... [Pg.676]

This article will outline the experimental techniques we have used in the laser spectroscopy of these atoms and briefly indicate current plans for the refinement of these measurements. As Fig. 1 shows, the laser spectroscopy of positronium and muonium is not competitive with comparable measurements in hydrogen, largely due to the low density sources of these atoms. In the case of positronium, the first measurements were done at peak densities of a few atoms/cm3 during a laser pulse. The muonium work was limited by atom densities 10 2 atom/cm3 per laser pulse. As feeble as these sources might seem to spectroscopisis of less exotic atoms, one must remember that these instantaneous densities represent many orders of magnitude improvement of above pre-existing sources of thermal positronium and muonium. Clearly, improved sources will lead to more precise measurements. [Pg.951]

The main disadvantages of Fourier transform methods are usually discussed with reference to laser spectroscopy. A laser may be as much as 106 times more sensitive mostly due to its high photon flux. Thus, weak absorbers may be impossible to see with an FT device but it is often easy to study these species with a laser. The lines from a laser are also much narrower and so they allow one to get resolution of at least a factor of 10 better than that available with Fourier transform methods. The limit of resolution for Fourier transform techniques with commercially available spectrometers is approximately 0.001 cm-1 in the IR [14],... [Pg.170]

Thermal reaction mixtures in this work were analyzed by FTIR spectroscopy, tunable diode laser spectroscopy and vibrational circular dichroismA pair of representative VCD spectra are shown in Figure 1. The more intense spectrum is an optically pure reference sample of the (25, 35) isomer at 53.59 torr the other is a thermal reaction product mixture from this isomer after 360 min at 407 °C and gas chromatographic isolation, recorded at 81.30 torr . From the measured Ay4/A 4ref absorption intensity ratio and the pressures, one may calculate that the sample retains 51.65% of its original optical activity, which compares well with the value calculated from the value obtained from the least-squares fit of all five VCD experimental points (51.2%). These spectra, obtained in the gas phase with a few mg of chromatographically purified labeled cyclopropanes, demonstrate the promise of VCD for assessing enantiomeric excess in situations where classical polari-metric methods would be of limited utility. [Pg.476]


See other pages where Limit laser spectroscopy is mentioned: [Pg.99]    [Pg.406]    [Pg.408]    [Pg.99]    [Pg.406]    [Pg.408]    [Pg.40]    [Pg.614]    [Pg.334]    [Pg.378]    [Pg.269]    [Pg.160]    [Pg.238]    [Pg.394]    [Pg.419]    [Pg.915]    [Pg.4]    [Pg.141]    [Pg.112]    [Pg.88]    [Pg.271]    [Pg.19]    [Pg.529]    [Pg.672]    [Pg.848]    [Pg.857]    [Pg.902]    [Pg.951]    [Pg.54]    [Pg.137]    [Pg.17]    [Pg.529]    [Pg.672]   
See also in sourсe #XX -- [ Pg.734 , Pg.740 ]




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