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Classes of Spectroscopic Experiment

For lmW of detected radiation at 500 nm, (Abackground)1 2 2 x 109 in a 1 second detection period (1 Hz bandwidth), which would be an astonishingly large SBR (corresponding to a minimum detectable fractional absorption of [Pg.27]

There is another important difference between direct absorption and LIF spectroscopies. This difference reflects a fundamental distinction between direct and indirect detection schemes. In a direct absorption spectrum, the signal integrated over the absorption line is determined by a fundamental molecular property, the integrated absorption cross section, oA (see Eqs. 6.1.11 and 6.1.13), times the number density (molecules/cm3) of molecules in the lower level of the absorption transition. In an LIF spectrum, the detected signal is reduced by the product of the fluorescence quantum yield [Pg.28]

LIF (Ezekiel and Weiss, 1968 Cruse, et al., 1973 Zare and Dagdigian, 1974 Kinsey, 1977) is an example of an indirect technique for the detection of a one-photon resonant upward transition. There are many other indirect detection techniques (optogalvanic, optothermal, photoacoustic, cavity ringdown), but Multi-Photon Ionization (MPI) is a special type of indirect technique uniquely well suited for combining absorption detection with other useful functionalities (see Section 1.2.1.1). In MPI, photo-ion detection replaces photon detection. The one-color, singly-resonant-enhanced (n + m) REMPI f process consists of an n-photon resonant e, v, J — e ,v ,J excitation, followed by a further nonresonant m-photon excitation into the ionization continuum [Pg.29]

Nevertheless, the resonance enhanced production of AB+ and e at the t = 0 arrival time of the excitation pulse, combined with the high efficiency [Pg.29]

Emission spectra axe usually much more complicated than Direct Absorption spectra, because an absorption spectrum contains all possible upward transitions from a single initial vibration-electronic state, typically the ground state, whereas an emission spectrum contains all possible downward transitions from [Pg.33]


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Spectroscopic Experiments

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