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Energy resolvation

Typically, the ratio of this to the incident flux detennines the transition probability. This infonnation will be averaged over the energy range of the initial wavepacket, unless one wants to project out specific energies from the solution. This projection procedure is accomplished using the following expression for the energy resolved (tune-independent) wavefunction in tenns in tenns of its time-dependent counterpart ... [Pg.981]

The last stage is the extraction of energy-resolved infomiation, obtamed automatically and simultaneously at many energies, by Fourier transfomiing the wavefiinction to produce an energy-resolved state ... [Pg.2301]

Energy-resolved observables can be inferred with knowledge of just the real part of a wave packet. [Pg.3]

Consider T(f) generated by Eq. (1). Energy-resolved observables are obtained by Fourier transformation from time (f) into energy E) space. An energy-resolved scattering state, from which such observables can be computed, is of the form... [Pg.6]

Since all energy-resolved observables can be inferred from appropriate expectation values of an energy-resolved wavefunction, Eq. (21) shows that the RWP method can be used to infer observables. Specific formulas for S matrix elements or reaction probabilities are given in Refs. [1] and [13]. See also Section IIIC below. [Pg.7]

Energy-resolved CID can be used to measure bond dissociation energies directly, and therefore is readily applicable for the determination of ion affinities. However, Graul and Squires have also described a method for measuring gas-phase acidities using CID of carboxylates. ° Upon CID, carboxylate ions, RCO2, undergo decarboxylation to form the alkyl anions, R, ... [Pg.215]

Threshold CID can be used to measure the energy required for decarboxylation, in order to determine the enthalpy of formation of R, which can be used to calculate the gas-phase acidity. While nominally straight-forward, the decarboxylation approach is limited to systems that have a bound anion, R, and requires an instrument with the capability of carrying out energy-resolved CID. However, it does have an advantage of being a regiospecific approach. [Pg.215]

The combination of state-of-the-art first-principles calculations of the electronic structure with the Tersoff-Hamann method [38] to simulate STM images provides a successful approach to interpret the STM images from oxide surfaces at the atomic scale. Typically, the local energy-resolved density of states (DOS) is evaluated and isosurfaces of constant charge density are determined. The comparison between simulated and measured high-resolution STM images at different tunneling... [Pg.151]

These plots show the projections on the (y, E) and (x, E) planes of the distribution of all the X-ray photons identified according to their position in the (x, y, E) space, that is, the energy resolved image of the source. Clearly visible in the plots are the contributions of the main fluorescence lines of each target layer. In most cases, the emission is centered at a common position (corresponding to the expected position of the source). In contrast, the emission around 900 ADC levels (corresponding approximately to 22.IkeV)... [Pg.133]

Electron beam divergence, 173 Electron beam pointing, 173 Electron density, 91 Electronic softening, 32 Emittance, 152 Energy resolved images, 134 Excimers, 20... [Pg.209]

Future developments. It seems probable that a considerable increase in electron energy resolving power can be achieved without great loss in... [Pg.44]

Figure 25 Schematic illustration for a system based on energy-dispersive coherent X-ray scatter (CXRS). Observation of the scattered photons is restricted to a fixed angle via a pinhole collimator. The spectrum from a highly energy resolving detector will show peaks at particular energies that are characteristic of the polycrystalline target. Computerized identification techniques can be used to identify the target substance. Figure 25 Schematic illustration for a system based on energy-dispersive coherent X-ray scatter (CXRS). Observation of the scattered photons is restricted to a fixed angle via a pinhole collimator. The spectrum from a highly energy resolving detector will show peaks at particular energies that are characteristic of the polycrystalline target. Computerized identification techniques can be used to identify the target substance.
In several studies, we have combined TRPD data with results obtained over a broader energy range by the time-resolved photoionization mass spectrometer (TPIMS) technique of Lifshitz s group," which is not fully energy resolved but provides a successful complementary technique to TRPD, as shown in the examples below. [Pg.93]


See other pages where Energy resolvation is mentioned: [Pg.643]    [Pg.196]    [Pg.199]    [Pg.199]    [Pg.477]    [Pg.153]    [Pg.490]    [Pg.10]    [Pg.17]    [Pg.332]    [Pg.477]    [Pg.229]    [Pg.230]    [Pg.150]    [Pg.74]    [Pg.264]    [Pg.323]    [Pg.129]    [Pg.130]    [Pg.131]    [Pg.134]    [Pg.135]    [Pg.149]    [Pg.359]    [Pg.206]    [Pg.239]    [Pg.10]    [Pg.275]    [Pg.137]    [Pg.124]    [Pg.125]    [Pg.225]    [Pg.14]    [Pg.423]   
See also in sourсe #XX -- [ Pg.23 , Pg.24 , Pg.30 , Pg.36 ]




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