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Energy magnetic dipole transition

For absorbers with magnetic dipole transitions, the evanescent magnetic field H leads to absorption of electromagnetic energy. Assuming equal magnetic permeabilities at both sides of the interface, the components of the evanescent field H at z = 0 are... [Pg.294]

When energy equivalent to the difference between the energy levels is applied to the system, a transition from the lower to the higher energy level occurs. In NMR spectroscopy, the applied energy that allows this nuclear magnetic dipole transition to occur is a radio-frequency magnetic field, Hx, which is applied perpendicularly to H0. [Pg.169]

Figure 11.58. Hyperfine energy levels and magnetic dipole transitions for Hj in the N = 1 rotational level (not to scale). The dashed lines indicate magnetic-dipole allowed transitions which were not observed experimentally (see text). Figure 11.58. Hyperfine energy levels and magnetic dipole transitions for Hj in the N = 1 rotational level (not to scale). The dashed lines indicate magnetic-dipole allowed transitions which were not observed experimentally (see text).
Mavroyannis and Stephen [239] were the first to show that between freely rotating molecules there is a discrimination energy from terms in the total dispersion energy arising from virtual magnetic dipole transitions. A general theory, with this as a... [Pg.26]

Symmetry considerations have a profound effect on the interpretation of lanthanide spectra. We have already mentioned the effect of symmetry on selection rules for electric and magnetic dipole transitions and on the classification of crystal-field split energy levels. In this section, we consider the effect of symmetry on the crystal-field Hamiltonian itself. [Pg.483]

To analyze the recorded spectra, the spectrometer needs to be calibrated. The three main calibration parameters are the velocity scale, the center point of the spectrum and the nonlinearity of the velocity/time profile of the oscillation compared to a standard reference. The calibration is performed using a spectrum recorded from an a-iron foil at room temperature using the well defined line positions of the sextet from a-iron, which occur at 5.312mms , 3.076mms , and 0.840mms The center of this a-iron spectrum at room temperature is taken as the reference point (0.0 nun s ) for isomer shift values of sample spectra. The typical Mossbauer spectrum of the 14.4 keV transition of Fe in natural iron (Fig. 4.10) represents a simple example of pure nuclear Zeeman effect. Because of the cubic symmetry of the iron lattice, there is no quadrupole shift of the nuclear energy levels. The relative intensities of the six magnetic dipole transitions are... [Pg.198]

For crystals which are centrosymmetric, there are no odd components of the crystal field so transitions of type 1 cannot occur in this particular case. In fact for octahedral symmetry, the spectra are dominated by vibronic transitions, that is transitions which occur from the ground electronic and vibrational state to an excited electronic and vibrational state. In some cases, the 0-0 transition (from the ground state V 0 to the excited state v = 0) is not observed and its energy is determined by assignment of the vibronic lines. For crystals without a center of symmetry the 0-0 lines are usually dominant. Magnetic dipole transitions are occasionally observed, but quadrupole induced transitions have not been assigned. Detailed selection rules are determined by the site symmetries of the ions in the crystals. [Pg.249]


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See also in sourсe #XX -- [ Pg.336 ]




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