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Springer series in optical sciences/SPringer series in optical sciences

Four-Wave Processes in Spectroscopy of Vibrational Molecular States

Sergey S. Alimpiev, V S Nersisyan, С. М. Никифоров, A M Prokhorov, Boris G. Sartakov

Published Jan 1, 1987• 0 citations
Publisher
DOI
10.1007/978-3-540-47973-4_65

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Recent research has expanded the capabilities of four-wave mixing by providing it with component selectivity, site selectivity, and mode selectivity. The selectivity is achieved by taking advantage of the three resonance enhancements that occur in a four-wave mixing process. New spectral scanning strategies allow one to scan a single resonance while maintaining the other two resonances at constant values. The constant resonances can be used to select a specific component, a specific site within an inhomogeneously broadened envelope of a component, and/or a specific vibrational or vibronic mode of that site. The scanned resonance will then contain enhanced features corresponding to the particular component, site, and/or mode that was chosen by the constant resonances. These component and site selective capabilities of the four-wave mixing complement the single vibronic level fluorescence methods. The relative transition intensities from a specific component or site reflect the mode coupling between the vibrational and vibronic modes. Since the four-wave mixing is fully resonant in these experiments, saturation effects play a dominant role and cannot be ignored. This review presents a complete discussion of the theoretical and experimental factors that control the fully resonant four-wave mixing. It shows examples of the component selectivity and the line narrowing capabilities. It also provides examples of how mode selection can identify mode coupling through the relative intensities of different vibrational features.
Control of coherence and population transfer between the ground and excited states is reported using three-pulse four-wave mixing. The inherent vibrational dynamics of the system are utilized in timing the pulse sequence that controls the excitation process. A slight alteration in the pulse sequence timing causes a change in the observed signal from coherent vibration in the ground state to coherent vibration in the excited state. This control is demonstrated experimentally for molecular iodine. The theoretical basis for these experiments is discussed in terms of the density matrix for a multilevel system.
A new variant of coherent spectroscopy is proposed for investigating the excitation of molecular vibration overtones which do not obey the alternative forbiddenness. Estimates obtained for the CH4 and HCl molecules show that the resonant susceptibility describing an optical process of the type ωα=2ω+ωL (ω is the frequency of infrared pumping radiation tuned to the frequency Ω of a molecular vibration and ωL is the frequency of a probe beam) is considerably greater than the nonresonant background susceptibility. A distinguishing feature of this process is the absence (in an isotropic medium) of the competing process of repeated scattering of a probe beam by the fundamental harmonic of the molecular vibration.