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Cooling atoms

The use of lasers to cool atomic translational motion has been one of the most exciting developments in atomic physics in the last 15 years. For excellent reviews, see [66, 67]. Here we give a non-orthodox presentation, based on [68]. [Pg.275]

The second tenn is tire spontaneous force, sometimes called tire cooling force, Fq, because it is a dissipative force and can be used to cool atoms. [Pg.2459]

A predissociation, which may or may not be related to the one just discussed, is observed in hot flames147 and in cool atomic flames148. For rotationless states the predissociating curve appears to cross the bound 2E+ state very near v = 2. The corresponding inverse predissociation has been proposed149,150 as an explanation for the observed overpopulation of the first and second vibrational levels of OH(2E+) in flames where there is a considerable excess population (over thermodynamic equilibrium) of O and H atoms. This process may produce a population inversion in nozzle expansion of a dissociated gas 15 x. [Pg.148]

The development of new, highly efficient nebulizers, described in detail in the section on ICP-OES (Section 12.2.4.4.1), has meant that a more concentrated aerosol and a more sensitive FAAS determination is achievable. Similarly, the use of slotted tube atom traps (STATs) and water-cooled atom traps (WCAT)10 11—the latter have undergone modification in recent years12—enhances sensitivity with regard to volatile elements like Cd and Pb because of the long residence time of these atoms in the tube. [Pg.267]

Similarly, Are momentum transfer associated with a collision of photons with atoms is used regularly to cool atoms [242], that is, to alter the translational energy of an atom. Indeed, the momentum of large numbers of photons (over 140-photon momenta) have been successfully transferred coherently to atoms [243], This suggests the possibility of preparing an initial superposition of internal states of a molecule, followed by tire state-specific absorption of photon momenta of one of the internal states in order to form the required entangled supeiposition of the translational and internal states. [Pg.154]

Figure 1 Schematic representation of the cloud of cool atoms which escapes from the centre of the hollow cathode at high lamp operating currents... Figure 1 Schematic representation of the cloud of cool atoms which escapes from the centre of the hollow cathode at high lamp operating currents...
G. Raithel, S. L. Rolston, R. J. C. Spreeuw, and C. I. Westbrook. I also want to remember and acknowledge Richard N. Watts, who died in November 1996 at the age of 39. His pioneering work on laser cooling with diode lasers, sub-Doppler laser cooling and localization of laser cooled atoms prepeired the way for all the subsequent work on optical lattices. [Pg.36]

In the examples described in Section III it was shown that a particular choice of the LCT field is able to steadily increase the internal energy of molecules, which eventually leads to fragmentation. In what follows we address the question if a field is able to induce the opposite process, namely, to reduce the energy of two colliding atoms to build a stable molecule. Many theoretical studies on such photoassociation processes have been presented [154-165], mostly involving more than a single electronic state. Also, with the modern technology of cooled atoms and molecules, photoassociation has become an important issue (see, e.g., Refs. 161-164). [Pg.47]

USE Corrosion inhibitor for water-cooled atomic reactors. Soln as low temp heat transfer medium. [Pg.871]

As the universe expanded and cooled, atoms clumped into the first hydrogen-rich stars. The largest of these luminous masses underwent dramatic... [Pg.3]

S. Trajmar and J. C. Nickel The Dissociative Ionization of Simple, Molecules by Fast Ions, Colin J. Latimer Theory of Collisions between Laser Cooled Atoms, P S. Julienne, A. M. Smith, and K. Burnett... [Pg.421]

R. Y. Chio, P. G. Kwiai, and A. M. Steinberg Classical and Quantum Chaos in Atomic Systems, Dominique Delande and Andrease Buchleitner Measurements of Collisions between Laser-Cooled Atoms, Thad Walker and Paul Feng The Measurement and Analysis of Electric Fields in Glow Discharge Plasma,... [Pg.422]

Figure 6.28 Distortion of spectral line shape in an HCL due to self-reversal, (a) Shape of the spectral line entitled hy the HCL. (h) Shape of the spectral energy hand absorbed by cool atoms inside the HCL. (c) Shape of the net signal emerging from an HCL, showing self-absorption of... Figure 6.28 Distortion of spectral line shape in an HCL due to self-reversal, (a) Shape of the spectral line entitled hy the HCL. (h) Shape of the spectral energy hand absorbed by cool atoms inside the HCL. (c) Shape of the net signal emerging from an HCL, showing self-absorption of...
A schematic of the SCSI-MS technique is presented in Figure 10.1. The technique relies on the measurement of the resonant excitation frequency of one of the two oscillatory modes of a trapped and crystallized linear two-ion system consisting of one laser-cooled atomic ion of known mass and the a priori unknown atomic or molecular ion, whose mass is to be determined. From this measured frequency, the mass of the unknown ion can be deduced from a simple relation between the frequency and the relative masses of the two ions (see Section 10.3). [Pg.293]

It is interesting first to note that in contrast to standard mass measurement techniques, a strong Coulomb coupling between ions (the ion of interest and the laser-cooled atomic ion) is essential, rather than being problematical. However, as is discussed in Section 12.5, the non-linear nature of the Coulomb interaction between the two ions can lead to unwanted systematic errors in the mass measurements. [Pg.295]

A limitation of the SCSI-MS technique in its present linear RF trap version is the requirement that the mass of the unknown singly-charged ion be within the range (ca 0.3-3)ma, ion, where is the mass of the laser-cooled atomic ion, in order to achieve stable operating conditions with respect to the dynamical confining potential (see Section 10.3.1). With the availability of more atomic ion species that can be laser cooled, it will be possible to extend the range of masses that can be measured with the present complex experimental arrangement beyond the Mg and Ca ions that are... [Pg.295]

Recently, the axial alignment of two ions in a Penning trap has been demonstrated [13]. When a sufficiently general procedure can be realized such that any two simultaneously-trapped ions can be so aligned, the above-mentioned mass range for a single laser-cooled atomic ion species may be increased also. [Pg.296]


See other pages where Cooling atoms is mentioned: [Pg.218]    [Pg.2462]    [Pg.361]    [Pg.363]    [Pg.701]    [Pg.915]    [Pg.1586]    [Pg.118]    [Pg.296]    [Pg.51]    [Pg.54]    [Pg.281]    [Pg.133]    [Pg.49]    [Pg.52]    [Pg.243]    [Pg.62]    [Pg.667]    [Pg.161]    [Pg.21]    [Pg.315]    [Pg.218]    [Pg.2462]    [Pg.292]    [Pg.294]   
See also in sourсe #XX -- [ Pg.44 ]




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Applications of Cooled Atoms

Applications of Cooled Atoms and Molecules

Atom Cooling and Trapping

Atom confinement cooling

Atomic ions laser cooling

Atoms Doppler cooling

Cooling of atoms

Laser cooling of atoms

Lithium atoms, cooling

Optical Cooling and Trapping of Atoms

Three-dimensional Cooling of Atoms Optical Molasses

Threedimensional Cooling of Atoms Optical Mollasses

Water-cooled atom traps

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