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Lasers laboratory experiments

In order to achieve coherent control in a laboratory experiment, three major requirements are to be met. Well-defined final states cannot be reached without the preparation of a well-defined initial state. Ultrashort, spectrally wide and intense laser pulses at different wavelengths must be produced for excitation and a good characterization of the final product states must be achieved. [Pg.51]

Other experimental and theoretical methods have been developed for the determination of the heat of sublimation of solid iodine these too are suitable for undergraduate laboratory experiments or variations on this experiment. Henderson and Robarts have employed a photometer incorporating a He-Ne gas laser, the beam from which (attenuated by a CUSO4 solution) has a wavelength of 632.8 nm, in a hot band near the long-wavelength toe of the absorption band shown in Fig. 3. Stafford has proposed a thermodynamic treatment in which a free-energy function ifef), related to entropy, is used in calculations based on the third law of thermodynamics. In this method either heat capacity data or spectroscopic data are used, and as in the present statistical mechanical treatment, the heat of sublimation can be obtained from a measurement of the vapor pressure at only one temperature. [Pg.536]

Neon is primarily used in luminous tubes (vacuum electric discharge tubes), airplane beacons, helium-neon lasers, high-voltage indicators, cryogenic refrigerant, and laboratory experiments. [Pg.1779]

The experiments described in this chapter can be carried out in any laser laboratory equipped for monitoring fast photochemical reactions. [Pg.3]

The support by the Office of Basic Energy Sciences, Division of Chemical Sciences, U.S. Department of Energy, under grant No. FG-05-92-ER14310, is gratefully acknowledged. All pulse radiolysis experiments described here were performed in collaboration with John R. Miller at the Argonne National Laboratory linac facility. Renata Kobetic and Timothy R. Schatz are thanked for their work on the laser photolysis experiments. [Pg.229]

CARS has been successfully used for the spectroscopy of chemical reactions (Sect. 8.4). The BOX CARS technique with pulsed lasers offers spectral, spatial, and time-resolved investigations of collision processes and reactions, not only in laboratory experiments but also in the tougher surroundings of factories, in the reaction zone of car engines, and in atmospheric research (Sect. 10.2 and [380, 381]). [Pg.180]

The formation and photo-dissociation of -ions plays an important role in astrophysics to explain the development and the collapse of molecular clouds. Therefore laboratory experiments are demanded to measure absolute cross sections for these processes. In Fig. 4.40 a possible experimental arrangement for such measurements is shown [498]. The ions are created in a special ion source, are accelerated and mass selected. The transmitted -ions are excited by one- or two-laser beams and the fragments are detected. [Pg.220]

The isotope I Cl can be selectively excited at A = 605 nm by a cw dye laser. The excited molecules react in collisions with bromine benzene and form the unstable radical ClC6H5Br, which dissociates rapidly into C6H5 C1 -f Br. In a laboratory experiment, several milligrams of C6H5CI were produced during a two hour exposure. Enrichment factors K = Cl/ Cl oi K = 6 have been achieved [1426]. [Pg.605]

Eibisch, M., Fuchs, B., Schiller, J., Su6, R., and Teuber, K. 2011. Analysis of phospholipid mixtures from biological tissues by matrix-assisted laser desorption and ionization time-of-flight mass spectrometry (MALDI-TOF MS) A laboratory experiment. J. Chem. Educat., 88 503-507. [Pg.229]

The limit of conventional, cryogenically cooled pulsed laser photolysis experiments is 80 K, and the technique suffers from the problem noted for flow tube experiments on ion + neutral reactions, viz. freezing out of reactants or precursors on the cold walls of the reaction cell or the pipes leading into the cell. The CRESU technique has been applied to neutral + neutral reactions by Smith and co-workers to overcome this problem. A diagram of the apparatus is shown in Fig. 3.3. Temperatures as low as 13 K have been obtained. An alternative approach is to introduce the gas mixture into the nozzle via a pulsed valve. This is less demanding on the pumping capacity, but produces less stable flows. It is employed in a number of laboratories. Mullen and Smith [55], for example, have studied NH - - NO at temperatures down to 53 K. [Pg.88]

The previous experiment was also inline monitored by photometric measurements. The pulse laser photometer used is well suited to characterize physical properties of emulsions like dispersed phase content or average droplet size [33]. The following results demonstrate that the pulse laser can not only be used in laboratory experiments but also for monitoring continuous emulsification processes. [Pg.295]


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See also in sourсe #XX -- [ Pg.119 ]




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