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Effect of excitation

Figure 9.41 Potential energy curves for the two lowest electronic states of Nal showing avoided level crossing and the effect of excitation with a femtosecond laser pulse. (Reproduced, with permission, from Rose, T. S., Rosker, M. J. and Zewail, A. H., J. Chem. Phys., 91, 7415, 1989)... Figure 9.41 Potential energy curves for the two lowest electronic states of Nal showing avoided level crossing and the effect of excitation with a femtosecond laser pulse. (Reproduced, with permission, from Rose, T. S., Rosker, M. J. and Zewail, A. H., J. Chem. Phys., 91, 7415, 1989)...
The information available is discussed in light of the effects of excitation energy and the environment on the photofragmentation process of several transition metal cluster complexes. The photochemical information provides a data base directly relevant to electronic structure theories currently used to understand and predict properties of transition metal complexes (1,18,19). [Pg.75]

B) Calculated Ed (solid circles left axis) is seen to fluctuate significantly in time-lapse experiments. After 30 min a large intensity fluctuation in acceptor excitation was simulated by manually diminishing laser power with 60%. The open circles depict the correction factor y, calculated according to Eq. (7.6) from cells expressing acceptors only. Calculating Ed with the online-updated y-factor (solid squares) abolished the effects of excitation fluctuations. [Pg.328]

The implied capability of these plasma deposits to inhibit corrosion at metal surfaces may be of practical as well as of basic importance. An important consideration in this respect is the rapid rate of deposition for such protective coatings attainable at micro-wave frequencies. Since plasma technology is still in a process of evolution, optimum deposition kinetics cannot yet be stated however, the marked effect of excitation frequency on the deposition of organo-silicones can be documented (10), as in Fig. 3. Here, using terminology and comparative data due to Yasuda et al. (2). it is shown that deposition rates in microwave plasmas exceed those at lower (e.g. radio) frequencies by about an order of magnitude. [Pg.297]

The long lifetimes and high redox potentials of a range of ruthenium(II) complexes and in particular [Ru(bpy)3] " have important consequences for their use as photoactive redox catalysts. This area of research is extremely active and we now focus on the decay of the excited state of [Ru(bpy)3] + ( [Ru(bpy)3] " ) and its quenching. Braterman et al. have described the electronic absorption spectrum and structure of the emitting state of [Ru(bpy3] +, and the effects of excited state asymmetry. The effects of solvent on the absorption spectrum of [Ru(bpy)3] " have been studied. In H2O, MeCN and mixtures of these solvents, the value of e(450 nm) remains the same ((4.6 0.4) x 10 dm mol cm ). The ground state spectrum is essentially independent of... [Pg.576]

The CCSD calculations are similar, both in methodology and in the accuracy of the results obtained, to calculations performed with Pople s quadratic Cl method. Like CCSD calculations, QCISD calculations also explicitly include single and double excitations and the effects of quadruple excitation in QCISD are obtained from quadrature of the effects of double excitations. However, CCSD does contain terms for the effects of excitations beyond quadruples, which are absent from QCISD. [Pg.976]

Thus in the condensed phases the collision frequency, cage effect, primary excitation delocalization, and rapid excitation energy transfer will all tend to negate the chemical effects of excitation in saturated hydrocarbons. [Pg.189]

Effect of excitation wavelength on the charge recombination dynamics of excited donor acceptor complexes... [Pg.331]

One further point is that in our treatment there is a critical amount of energy required for the isomerization route to occur, although tunneling as pointed out by Robinson5 must be considered. Thus, the effect of exciting wavelength may be very marked. [Pg.332]

The rates km cover the km o accounting for the excited state decay of chromophore m (by radiative as well as non-radiative transitions) and the SC ) originated by inter-system crossing to triplet states (ISC rate). The simple km do not include the effect of excited state wave function delocalization and a possible decay out of exciton states [45], Therefore, we shortly demonstrate the computation of the photon emission part of the km including such a delocalization effect (determination of excitonic augment rates). It will be important for the mixed quantum classical simulations discussed in the following (for more details see also [11]). [Pg.51]

Effect of Excitation Wavelength on the Luminescence Spectrum of CdS/CuxS... [Pg.62]

Effect of Excitation Light Wavelength on the Rate of Photocatalytic Reaction... [Pg.80]

Varying other parameters, such as the width of the pulses, also has substantial effect on product control. For example, the effect of exciting more vib-rotational levels in the E electronic state by using a broader pump pulse is shown in Figure1, t 3.27, where AkfJ = 60 cm-1 and A2co = 100 cm-1. The superposition state prepared by the first pulse consists of the v = 14, 15 and J 21,23 levels, where the pulse is] centered at 2, = 803.88 nm, corresponding to the frequency halfway between the,... [Pg.74]

The above considerations were a starting point in the formulation of the problems in the series of investigations discussed in this chapter.14-24 The motive for elucidating the mechanochemical aspect of the radiation cryochemistry of solids was the discovery14 of the effect of excitation of a reaction in the irradiated, low-temperature-stabilized samples of reactants in response to a local fracture. [Pg.341]

The MO basis for this effect is seen quite simply in Fig. 3. Here it is seen that electron promotion is from MO 2 which is antibonding (having a negative bond order) between the orbitals at atoms 2 and 3 and, this promotion is to MO 3 which is bonding (i.e. with a positive and large bond order) between atoms 2 and 3. The net effect of excitation then is enhancement of the 2,3-bond order upon electronic excitation. [Pg.51]

Dynamic up-shift of the A (l) v(CO) band of the lowest excited state is the most pronounced IR effect of excited-state relaxation. Time-dependences of the A (l) v(CO) energies measured for various complexes in different media have revealed [37, 75, 76, 86] that relaxation involves four different lifetimes (Fig. 12) ... [Pg.95]

Fig. 2. Spectra of zeolite H-MFI showing the effects of excitation wavelength and calcination on the masking of Raman spectral features by background fluorescence (24). Fig. 2. Spectra of zeolite H-MFI showing the effects of excitation wavelength and calcination on the masking of Raman spectral features by background fluorescence (24).
In Section IV the computer simulation is extended to describe the effects of excitation in chiral molecules and racemic mixtures of enantiomers. The modification of the dynamical properties brought about by mixing two enantiomers in equimolar proportion may be explained in terms of rotation-translation coupling. The application of an external field in this context ai iplifies the difference between the field-on acf s and cross-correlation of enantiomer and racemic mixture and provides a method of studying experimentally the fundamental phenomenon of rotation-translation coupling in the molecular liquid state of matter. [Pg.186]

Figure 18. Computer simulation of the effects of excitation on the decay of the angular velocity u. Curve 1 denotes the equilibrium correlation function Curves 2... [Pg.272]

Figure 19. Theoretical calculations via the CFP applied to Eq. (5.69) (v being assumed as infinitely fast) of the effects of excitation on the decay of the angular velocity u. Curves 1 to 4 have the same meaning as in Fig. 18, and curves 2 and 3 correspond to the same excitation parameter as those of Fig. 18. The memory and nonlinearity parameters which best reproduce the experimental results are g = 1.45 and IF = 0.0680. Figure 19. Theoretical calculations via the CFP applied to Eq. (5.69) (v being assumed as infinitely fast) of the effects of excitation on the decay of the angular velocity u. Curves 1 to 4 have the same meaning as in Fig. 18, and curves 2 and 3 correspond to the same excitation parameter as those of Fig. 18. The memory and nonlinearity parameters which best reproduce the experimental results are g = 1.45 and IF = 0.0680.
In Table 12, the experimental results of Paic and Pecar [29] are also hsted for comparison. They observed almost 10% decrease for V and about 5% decrease for Cr. These results are much larger than the present theoretical values. Unfortunately there is no description about the chemical forms of the samples they used. It is possible that the chemical forms of their radioactive sources are different from those of the targets for PI. If the chemical forms of the samples are different, the relative ratios become a sum of two effects, the chemical effect and the effect of excitation modes, and can be larger values than those for the latter effect alone. For example, if we choose the smallest value for EC and the largest value for PI from... [Pg.320]


See other pages where Effect of excitation is mentioned: [Pg.153]    [Pg.376]    [Pg.200]    [Pg.162]    [Pg.468]    [Pg.483]    [Pg.485]    [Pg.25]    [Pg.450]    [Pg.348]    [Pg.63]    [Pg.28]    [Pg.162]    [Pg.381]    [Pg.495]    [Pg.510]    [Pg.512]    [Pg.173]    [Pg.68]    [Pg.316]   
See also in sourсe #XX -- [ Pg.1315 ]




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Excitation effects

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