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Energy characterization

While each approach has its own peculiarities, one common obstacle arises due to the so-called intruder states. These are the states from the orthogonal complement Mo of Mo, whose energy falls within the interval of energies characterizing the reference configurations spanning Mo or lies... [Pg.17]

Gaseous Discharge Lamps. Gaseous discharge lamps consist of an electrically operated source of radiant energy characterized by the emission of radiation from a stream of ionized gas carrying current between electrodes in the lamp (See Fig G10). Lamps in common use include fluorescent, mercury-vapor and neon lamps. In general,... [Pg.662]

Ory developed to explain them, have yielded considerable insight into the variety of dynamical processes that occur subsequent to electronic excitation [1], From these studies, one hopes to obtain bond dissociation energies, characterize the symmetry of the excited state, measure the product branching ratios, and determine if the excited state undergoes direct dissociation on an excited-state surface, predissociation via another excited state, or internal conversion to the ground state followed by statistical decay to products. [Pg.730]

This is, however, by no means the case since the rate constants depend not only on temperature, but in a rather complex manner on the surface concentrations and mutual configurations of the reacting species. Thus, for example, the activation energy characterizing kA (LH step) was... [Pg.46]

Fig. 3. The dependence of energies, characterizing the vibronic process, on nuclear displacements according to the bending mode ra (A) (see equation (12)), for AsF3(above) and AsBr3(below) at the As-F(Br) spacing 1.85(2.47) A in D3h. Point-markings and solid lines refer to DFT data and their fitting (equation (8)), respectively. Fig. 3. The dependence of energies, characterizing the vibronic process, on nuclear displacements according to the bending mode ra (A) (see equation (12)), for AsF3(above) and AsBr3(below) at the As-F(Br) spacing 1.85(2.47) A in D3h. Point-markings and solid lines refer to DFT data and their fitting (equation (8)), respectively.
The chapters in this volume have been collected in order to chart a course toward a more holistic, thus more realistic, view of mineral reactivity than can be garnered from equilibrium modeling. Spectroscopies are the tools by which structure, dynamics, and reactivity can be most directly examined. Examples include numerous means of mineral spectroscopy applied to numerous ends, such as determination of composition, purify, interaction with energy, characterization of chemically and spectroscopically special (active) centers, and adsorbate interactions. Coverage of both spectroscopy and minerals is intended to be illustrative, not exhaustive. [Pg.5]

In the following years main attention was devoted to detailed elaboration of the concept of the cold dark matter dominated Universe. Here a central issue was the amount of dark matter. Initially opinions varied from a moderate density of the order of 0.2 critical density up to the critical density. Only a few years ago it was clarified that dark matter constitutes only 0.25 of the critical density, and the rest is mostly dark energy, characterized by the cosmological constant or the U A-term. [Pg.258]

Uhlmann P, Schneider S. 2002. Acid-base and eurface energy characterization of grafted polyethylene using inverse gas chromatography. J. Chromatogr. A 969 73-80. [Pg.325]

Thus, the resonance energy characterizes the insufficiency of structure 34 for accurately representing the ground state. It is clear therefore that this concept is best quantified by comparing the energy of the optimized ground state with that of the best possible wave function for 34, and this is meaningful... [Pg.220]

We consider the interaction of N monomers, X1 X2,..., XN. The interaction energy characterizing the interactions in the cluster is given by,... [Pg.73]

Bending magnet. The radiation spectrum emitted from a bending magnet (Fig. 1) is a smooth function of energy characterized by a critical or half-power energy given by... [Pg.290]

Fig. 4.1. Energy as a function of shear deformation in A1 (adapted from Mehl and Boyer (1991)). The lattice parameter a is fixed during the deformation and hence the energy characterizes a one-parameter family of deformations of the fee lattice, with the members of the family parameterized by b. Fig. 4.1. Energy as a function of shear deformation in A1 (adapted from Mehl and Boyer (1991)). The lattice parameter a is fixed during the deformation and hence the energy characterizes a one-parameter family of deformations of the fee lattice, with the members of the family parameterized by b.
For some parameters, the potential energy along the helical axis is essentially flat. This will probably be particularly true of die tubular fullerenes [36]. An infinite, flat channel is a one-dimensional ionic conductor for which the band of states has energies characterized simply by [33]... [Pg.66]


See other pages where Energy characterization is mentioned: [Pg.589]    [Pg.37]    [Pg.33]    [Pg.510]    [Pg.369]    [Pg.12]    [Pg.366]    [Pg.135]    [Pg.145]    [Pg.125]    [Pg.168]    [Pg.190]    [Pg.164]    [Pg.240]    [Pg.366]    [Pg.295]    [Pg.145]    [Pg.151]    [Pg.164]    [Pg.38]    [Pg.287]    [Pg.366]    [Pg.143]    [Pg.156]    [Pg.329]    [Pg.529]    [Pg.140]    [Pg.141]    [Pg.287]    [Pg.196]    [Pg.643]    [Pg.62]    [Pg.112]   
See also in sourсe #XX -- [ Pg.39 , Pg.307 ]




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