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instrumental techniques applied to mineralogy and geochemistry

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62<br />

Biliana Gasharova<br />

Even though Raman spectroscopy probes vibrational transitions indirectly by light<br />

scattering, the Raman shift has the same energy range as IR absorption.<br />

Selection rules<br />

Different vibrational modes have different relative intensities in IR <strong>and</strong> Raman<br />

spectra – some modes are active in one <strong>and</strong> not the other, <strong>and</strong> some modes are not<br />

observed at all. The IR <strong>and</strong> Raman activities of particular modes are determined by the<br />

quantum mechanical selection rules for the vibrational transitions, <strong>and</strong> by the mode<br />

symmetry. In a simple model, the selection rules can be rationalized by considering the<br />

interaction between the oscillating electric field vec<strong>to</strong>r of the light beam <strong>and</strong> a changing<br />

molecular dipole moment associated with the vibration. In an IR experiment, the light<br />

interacts directly with an oscillating molecular dipole, so for a vibrational mode <strong>to</strong> be IR<br />

active, it must be associated with a changing dipole moment. In general, asymmetric<br />

vibrations tend <strong>to</strong> give stronger IR absorption than symmetric species, since they are<br />

associated with larger dipole moment changes. Similarly, highly polar (“more ionic”)<br />

molecules <strong>and</strong> crystals have stronger IR spectra than non-polar samples. In Raman<br />

scattering, the light beam induces an instantaneous dipole moment in the molecule by<br />

deforming its electronic wave function. The a<strong>to</strong>mic nuclei tend <strong>to</strong> follow the deformed<br />

electron positions, <strong>and</strong> if the nuclear displacement pattern corresponds <strong>to</strong> that of a<br />

molecular vibration, the mode is Raman active. The magnitude of the induced dipole<br />

moment is related <strong>to</strong> the ease with which the electron cloud may be deformed, described<br />

by the molecular polarizability a.<br />

The classification of the vibrational quantum states <strong>and</strong> the description of the<br />

spectroscopic interaction are greatly simplified by exploiting the symmetry of the<br />

vibrating a<strong>to</strong>mic groups. The mathematical framework of the group theory is the basis of<br />

the quantitative description of the symmetry relations possessed by the vibrating groups,<br />

finally giving rise <strong>to</strong> the formulation of the symmetry-based selection rules. As the<br />

symmetry of the a<strong>to</strong>mic group increases, the number of different energy levels decreases.<br />

The degeneracy, i.e. the number of vibrational states, which have the same energy<br />

increases with increasing symmetry. The more symmetric the a<strong>to</strong>mic group, the fewer<br />

different energy levels it has, <strong>and</strong> the greater the degeneracy of those levels. The<br />

symmetry must be compatible in order that the molecule may absorb light <strong>and</strong> the

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