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Level excitation

The figure shows the migration of energy between excited levels of the ultimately reactive C-C oscillator, the... [Pg.1080]

Clebsch-Gordan coefficients coupling ground and excited levels that = transitions coupled by linearly... [Pg.2466]

If the collision starts on the excited level, the long-range dipole-dipole interaction produces an interatomic... [Pg.2473]

Thus, we can use the approximate quantum number m to label such levels. Moreover, it may be shown [11] that (1) 3/m is one-half of an integer for the case with consideration of the GP effect, while it is an integer or zero for the case without consideration of the GP effect (2) the lowest level must have m = 0 and be a singlet with Ai symmetry in 53 when the GP effect is not taken into consideration, while the first excited level has m = 1 and corresponds to a doublet E conversely, with consideration of the GP effect, the lowest level must have m = j and be a doublet with E symmetry in S, while the first excited level corresponds to m = and is a singlet Ai. Note that such a reversal in the ordering of the levels was discovered previously by Hancock et al. [59]. Note further thatj = 3/m has a meaning similar to thej quantum numbers described after Eq. (59). The full set of quantum numbers would then be... [Pg.594]

The state may decay by radiative (r) or non-radiative (nr) processes, labelled 5 and 7, respectively, in Figure 9.18. Process 5 is the fluorescence, which forms the laser radiation and the figure shows it terminating in a vibrationally excited level of Sq. The fact that it does so is vital to the dye being usable as an active medium and is a consequence of the Franck-Condon principle (see Section 7.2.5.3). [Pg.360]

Figure 9.50(a) illustrates the ionization process in a UPS experiment. In this type of experiment the incident radiation always has much more energy than is necessary to ionize the molecule M into either the zero-point level or a vibrationally excited level of M. The excess energy is then removed as kinetic energy of the photoelectron. [Pg.402]

Half-Lives and Decay Constants. Each nuclear state, whether an unstable ground state or an excited level, has a characteristic probabiUty... [Pg.445]

Although protons and neutrons are not emitted from the ground states of these isotopes, there are many cases where particles are emitted from excited states. For example, Cs decays by electron capture and -emission to excited levels ia and ia 7% of these cases protons are emitted from... [Pg.451]

Radiometry. Radiometry is the measurement of radiant electromagnetic energy (17,18,134), considered herein to be the direct detection and spectroscopic analysis of ambient thermal emission, as distinguished from techniques in which the sample is actively probed. At any temperature above absolute zero, some molecules are in thermally populated excited levels, and transitions from these to the ground state radiate energy at characteristic frequencies. Erom Wien s displacement law, T = 2898 //m-K, the emission maximum at 300 K is near 10 fim in the mid-ir. This radiation occurs at just the energies of molecular rovibrational transitions, so thermal emission carries much the same information as an ir absorption spectmm. Detection of the emissions of remote thermal sources is the ultimate passive and noninvasive technique, requiring not even an optical probe of the sampled volume. [Pg.315]

At low p.f.s the generator operates at a low level of excitations (armature reaction demagnetizing). During a fault, therefore, when the p.f. of the circuit falls it will also cause a fall in the excitation level and in turn in the terminal voltage. A low voltage, however, would reduce the severity of the fault. [Pg.503]

The resulting PL intensity depends on the absorption of the incident light and the mechanism of coupling between the initial excited states and the relaxed excited states that take part in emission. The spectrum is similar to an absorption spectrum and is useful because it includes higher excited levels that normally do not appear in the thermalized PL emission spectra. Some transitions are apparent in PLE spectra from thin layers that would only be seen in absorption data if the sample thickness were orders of magnitude greater. [Pg.379]

What is a typical size of the CI matrix Consider a small system, H2O with a 6-31G(d) basis. For the purpose of illustration, let us for a moment return to the spinorbital description. There are 10 electrons and 38 spin-MOs, of which 10 are occupied and 28 are empty. There are possible ways of selecting n electrons out of the 10 occupied orbitals, and K2s,n ways of distributing them in the 28 empty orbitals. The number of excited states for a given excitation level is thus Kiq. K2s,n, and the total number of... [Pg.105]

Table 4.1 Number of singlet CSFs as a function of excitation level for H2O with a 6-31G(d) basis... Table 4.1 Number of singlet CSFs as a function of excitation level for H2O with a 6-31G(d) basis...
Excitation level n Number of nth excited CSFs Total number of CSFs... [Pg.106]

The number of excited determinants thus grows factorially with the size of the basis set. Many of these excited determinants will of course have different spin multiplicity (triplet, quintet etc. states for a singlet HF determinant), and can therefore be left out in the calculation. Generating only the singlet CSFs, the number of configurations at each excitation level is shown in Table 4.1. [Pg.106]

The weight is the sum of coefficients at the given excitation level, eq. (4.2). The Cl method determines the coefficients from the variational principle, thus Table 4.2 shows that the doubly excited determinants are by far the most important in terms of energy. The singly excited determinants are the second most important, then follow the quadruples and triples. Excitations higher than 4 make only very small contributions, although there are actually many more of these highly excited determinants than the triples and quadruples, as illustrated in Table 4,1. [Pg.108]

Coupled cluster is closely connected with Mpller-Plesset perturbation theory, as mentioned at the start of this section. The infinite Taylor expansion of the exponential operator (eq. (4.46)) ensures that the contributions from a given excitation level are included to infinite order. Perturbation theory indicates that doubles are the most important, they are the only contributors to MP2 and MP3. At fourth order, there are contributions from singles, doubles, triples and quadruples. The MP4 quadruples... [Pg.137]

So far everything is exact. A complete manifold of excitation operators, however, means that all excited states are considered, i.e. a full Cl approach. Approximate versions of propagator methods may be generated by restricting the excitation level, i.e. tmncating h. A complete specification furthermore requires a selection of the reference, normally taken as either an HF or MCSCF wave function. [Pg.259]

One of the possible mechanisms of the intensity decrease is related to the change in occupancy of the base and excited levels [374]. The magnitude of the contribution of the occupancy change in to the intensity variation was estimated in [373]. Table 57 presents experimental and calculated values of coefficient p. [Pg.197]

Moser, C. M., and Lef bvre, R., J. Chem. Phys. 23, 598, "Lowest singlet excited levels of C10HS." Limited configurational interaction. [Pg.344]

We have found for polypropynoic acid that this series of polymers reveals selective fluorescence spectra together with nonselective absorption. To account for this phenomenon, a scheme was proposed according to which PCSs are characterized by energy transfer from excited levels of some conjugation sections to the lower levels of other sections, followed by luminescence from the latter40 41,246,248,249,253. ... [Pg.22]


See other pages where Level excitation is mentioned: [Pg.802]    [Pg.2050]    [Pg.3006]    [Pg.361]    [Pg.1]    [Pg.8]    [Pg.319]    [Pg.412]    [Pg.202]    [Pg.519]    [Pg.786]    [Pg.374]    [Pg.375]    [Pg.52]    [Pg.84]    [Pg.1272]    [Pg.106]    [Pg.107]    [Pg.108]    [Pg.134]    [Pg.1143]    [Pg.172]    [Pg.173]    [Pg.486]    [Pg.487]    [Pg.487]    [Pg.263]    [Pg.265]    [Pg.327]    [Pg.995]   
See also in sourсe #XX -- [ Pg.91 , Pg.93 , Pg.96 ]

See also in sourсe #XX -- [ Pg.564 ]

See also in sourсe #XX -- [ Pg.541 ]




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Approximate excitation level

Atomic level excitation

Configuration interaction excitation level truncation

Coordinate-dependent level approximation excitation

Core electron excitation energy level diagram

Core level excitation

Electronically excited levels

Electronically excited molecule energy level diagrams

Energy Levels of Excited Molecules

Energy level diagram first excited singlet state

Energy level diagram second singlet excited state

Energy level excitation, nonadiabatic

Energy levels metastable excited

Excitation of levels

Excited level

Excited level, fluorescence spectrum

Excited level, steady-state rate equation

Excited levels in atoms

Excited state level, electronic quenching

Excited state levels

Excited vibrational level population

Excited vibrational levels

Lifetime of excited level

Molecule lowest excitation level

Optical Double-Resonance and Level-Crossing Experiments with Laser Excitation

Photo-excitation Fermi level

Population of excited level

Pump-Dump Control Few-Level Excitation

Pump-Dump Excitation with Many Levels Tannor-Rice Scheme

Reduced excitation level

Resonant excitation of a two-level system free from relaxation

Resonant excitation of a two-level system with relaxations

Sensitization energy level, triplet excited

Space excitation level truncation

Triplet, energy levels, determination excitation

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