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Energy degeneracy

Let us consider a general energy degeneracy, which may be described by an auxiliary operator A commuting with H, so that... [Pg.285]

Figure 6. Energy splitting of the d orbitals in octahedral and tetrahedral coordination. The numbers at each level indicate the energy degeneracy that still remains after ligand-field splitting. Note that the energy barycenter (i.e., center of energy ) need not be the same in octahedral and tetrahedral coordination as pictured. Figure 6. Energy splitting of the d orbitals in octahedral and tetrahedral coordination. The numbers at each level indicate the energy degeneracy that still remains after ligand-field splitting. Note that the energy barycenter (i.e., center of energy ) need not be the same in octahedral and tetrahedral coordination as pictured.
Reactions having Q-states provide mechanistic pathways to achieving the electronic interconversion which can be modulated by external electromagnetic fields such as, for instance, microwaves as well as thermal blackbody radation, due to the quasi energy degeneracy. In non-stationary situations, the operator... [Pg.44]

Here the eigenfunctions are denoted En), with the understanding that the notation will be extended to include additional quantum numbers when energy degeneracies exist.)... [Pg.12]

As constructed, Eq, (7.14) is composed of four independent noninterfering inci-Jf dent states since each has a different center-of-mass wave vector Ky. However, we can set conditions so that interference, and hence control, is allowed. That is, we require the equality of the center-of-mass motion of two components, plus energy degeneracy 1... [Pg.152]

The plot of the energy along 2xi and 2 3 in the second order picture is shown in Fig. 4b. In this case, the seam of intersection is a curved tine. The energy degeneracy is kept by combined displacements along and 2x3, and the first condition of von Neumann and Wigner (Equation 2) becomes ... [Pg.174]

Centrifugal barriers have a profound effect on the physics of many-electron atoms, especially as regards subvalence and inner shell spectra. One aspect not discussed above is how energy degeneracies arising from orbital collapse can lead to breakdown of the independent electron approximation and the appearance of multiply excited states. Similarly, we have not discussed multiple ionisation (the ejection of several electrons by a single photon) enhanced by a giant resonance. Both issues will be considered in chapter 7. [Pg.185]

When Ei,Vi E2,Vj, it is necessary before applying Eq. (5.1.12) to vertically shift one of the potentials to ensure strict energy degeneracy. The new curve crossing point obtained in this way is called a pseudo-crossing point (Miller, 1968). [Pg.285]

Table 2.7. Carbon Is and Oxygen Is Binding Energies, Degeneracy-Weighted Average C—0 Stretching Frequencies, and Number-Weighted Average C—0 Force Constants ... Table 2.7. Carbon Is and Oxygen Is Binding Energies, Degeneracy-Weighted Average C—0 Stretching Frequencies, and Number-Weighted Average C—0 Force Constants ...
Make a table similar to Table 2.1 for two particles with distinguishable quantum numbers in a three-dimensional cubical box, giving energies, degeneracies, and quantmn nmnbers for the lowest five energy values. The lowest energy state, for example, will be (1,1,1)(1,1,1). [Pg.102]

We have already seen (Chapters 8 and 13) that the orbital energies, degeneracies, and coefficients in benzene are to a great extent determined by symmetry. But these symmetry constraints can also be viewed as resulting from the cyclic periodicity of benzene, and this finite cyclic periodicity is, in essential ways, like the extended infinite periodicity of, say, regular polyacetylene or of graphite. It is reasonable, therefore, that some of the aspects of the energies and orbitals in these extended periodic stmctures are closely related to those in cyclic periodic systems. [Pg.526]


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