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Interactions forbidden transition

The transition probability R is related to selection mles in spectroscopy it is zero for a forbidden transition and non-zero for an allowed transition. By forbidden or allowed we shall mostly be referring to electric dipole selection mles (i.e. to transitions occurring through interaction with the electric vector of the radiation). [Pg.33]

As the isoquinoline molecule reorients in the order listed above, the absorption of infrared radiation by the in-plane vibrational modes would be expected to increase, while that of the out-of-plane modes would be predicted to decrease (in accordance with the surface selection rule as described above). In the flat orientation there is no component of the dipole moment perpendicular to the surface for the in-plane modes, and under the surface selection rule these modes will not be able to absorb any of the incident radiation. However, as mentioned above, infrared active modes (and in some cases infrared forbidden transitions) can still be observed due to field-induced vibronic coupled infrared absorption (16-20). We have determined that this type of interaction is present in this particular system. [Pg.342]

For allowed transitions on D and A the Coulombic interaction is predominant, even at short distances. For forbidden transitions on D and A (e.g. in the case of transfer between triplet states (3D + 3A —> 1D + 3A ), in which the transitions Ti —> S0 in D and So —> Ti in A are forbidden), the Coulombic interaction is negligible and the exchange mechanism is found, but is operative only at short distances (< 10 A) because it requires overlap of the molecular orbitals. In contrast, the Coulombic mechanism can still be effective at large distances (up to 80-100 A). [Pg.114]

Hall, R. R. (1984), Laser Photoacoustic Spectroscopy of Forbidden Transitions Acetylene and Alkyne High Energy Vibrational States and their Interactions, Ph.D. Thesis, Rice University, Houston. [Pg.226]

We then turn to the question of how to eliminate the spin-orbit interaction in four-component relativistic calculations. This allows the assessment of spin-orbit effects on molecular properties within the framework of a single theory. In a previous publication [13], we have shown how the spin-orbit interaction can be eliminated in four-component relativistic calculations of spectroscopic properties by deleting the quaternion imaginary parts of matrix representations of the quaternion modified Dirac equation. We show in this chapter how the application of the same procedure to second-order electric properties takes out spin-forbidden transitions in the spectrum of the mercury atom. Second-order magnetic properties require more care since the straightforward application of the above procedure will extinguish all spin interactions. After careful analysis on how to proceed we... [Pg.402]

Symmetry forbidden transition can be made partially Mowed by vibronic interactions. [Pg.89]

CsNiCl3-type). Table 6 summarizes results on electronic spectra. The three spin-allowed transitions are usually observed and extensive vibrational contribution has been observed in single crystal spectra.120,121 Intense spin-forbidden transitions may also be observed122 due to exchange interactions in the solid phase. The diiodide123,124 and the complex halides121 show trigonal distortion. [Pg.468]

However, the Ne(2s2) state has some triplet character due to mixing with Ne(2s4). It is of considerable interest to investigate the restrictive effect of an overall spin-change in any electronic process. It has been noted that, of the inert gases, only Xe induces collisional deactivation of 0(2 lD) to 0(2 3P), which may be due either to chemical interaction, or to the spin-orbit coupling in the heavy atom. Most gases will induce the spin forbidden transition... [Pg.262]


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See also in sourсe #XX -- [ Pg.183 , Pg.184 , Pg.192 ]




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