Spectroscopic absorption contours of condensed systems appear to be described by one of several frequency functions, i.e., Gaussian, Lorentzianlpar;T1rpar;, orTn, where1thinsp;thinsp;nthinsp;le;thinsp;3. A phenomenological explanation is given in terms of a statistical model involving random perturbations on energy levelslpar;lang;psgr;mverbar; H verbar; psgr;nrang;,lang;psgr;nverbar; H verbar; psgr;nrang;rpar;and orthogonal coupling matrix elementslpar;lang;psgr;mverbar; Mqverbar; psgr;nrang;rpar;, whereMqis the lighthyphen;coupling operator andnandmare the two states between which transitions occur. If the matrix elements are well shielded from perturbation or strong complexes exist such that only a few relaxations of the same order of duration can occur, Gaussian functions result. If, along with the energy levels, one of the orthogonal components is strongly perturbed by a statistically orientated environment, a Lorentzian functionlpar;T1rpar;results. If two such components are perturbed, the predicted function isT2, and if all three components are significantly perturbed, thenT3results.
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