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Virtual levels

It is important to recall that the virtual levels in Figure 1.16 do not correspond to real stationary eigenstates of our quantum system. As a result, Raman spectra are much weaker than fluorescence spectra (by an efficiency factor of about 10 -10 ),... [Pg.31]

If the active metal becomes highly diluted the minimum polarity model leads to the virtual bound-state model (127, 128, 129). This model has also been applied to highly diluted Ni-Cu alloys (121a). The nickel d-states are then found to form not a common band with the copper d-states but narrow virtual levels between the copper d-states and the Fermi level. The levels are in resonance with the s,p-band of the metal. [Pg.104]

In order to keep the amount of substrate (or virtual level) constant in a three phase system, the whole reactor was placed with flexible tubing on a Mettler scale with a special resolution of 0.1 g. This signal was used as the input to the weight (level) controller. The substrate feed was kept at a constant value by controlling the feed pump. [Pg.40]

Figure 9-4. The Raman and resonance Raman scattering processes. In this figure, i > and f > refer to the initial and final states, respectively, in the Raman or resonance Raman scattering process. (A) In the Raman process, the molecule is initally in its ground vibrational level of the ground electronic state. An excitation photon (up arrow) carries the molecule to a virtual level (dashed line) from which it immediately scatters inelastically (down arrow), leaving die molecule in an excited vibrational level of the ground state. The difference between die excitation and scattered photon is measured. (B) Resonance Raman scattering follows the same process, except that die virtual level (dashed line) is coincident with a real excited vibronic level of the molecule. Again, die difference between the excitation and scattered photon is measured... Figure 9-4. The Raman and resonance Raman scattering processes. In this figure, i > and f > refer to the initial and final states, respectively, in the Raman or resonance Raman scattering process. (A) In the Raman process, the molecule is initally in its ground vibrational level of the ground electronic state. An excitation photon (up arrow) carries the molecule to a virtual level (dashed line) from which it immediately scatters inelastically (down arrow), leaving die molecule in an excited vibrational level of the ground state. The difference between die excitation and scattered photon is measured. (B) Resonance Raman scattering follows the same process, except that die virtual level (dashed line) is coincident with a real excited vibronic level of the molecule. Again, die difference between the excitation and scattered photon is measured...
The NAO basis usually contains all the occupied orbitals of the atom, plus some unoccupied level(s) very close in energy. For example, transition metals will include all occupied levels up to nd, (n + l)s and also the virtual level (n + l)p. Some additional features make it possible to further improve the basis. If the atom has a negative charge, or if additional virtual orbitals of higher energy are to be included as very diffuse functions, the atomic SCF calculation may be performed in the presence of a potential well . This well may also be employed when it is desirable to contract the valence atomic basis functions, as is often the case with solids. The well is best described by the following diagram ... [Pg.63]

The nuclear reactions are described as taking place in two steps (1) the formation of a compound nucleus in a highly excited virtual level, and (2) the dissociation of this compound nucleus leading to a state of high excitation of the product nucleus. The product nucleus, which decays promptly by electromagnetic transitions, ends up in the ground state or in some low-lying metastable level called an isomer. [Pg.358]


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See also in sourсe #XX -- [ Pg.57 , Pg.237 , Pg.310 ]

See also in sourсe #XX -- [ Pg.62 , Pg.290 ]




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