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Theory of lineshapes in resonance scattering spectra

โœ Scribed by P.A. Hackett; R.A. Back


Publisher
Elsevier Science
Year
1976
Tongue
English
Weight
355 KB
Volume
37
Category
Article
ISSN
0009-2614

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โœฆ Synopsis


The form of the emission spectrum induced by scattering of a generalised light pulse from LI single resonance is calculated from the known time dependence of sxh scattering. It is shown that the intensity of the scattered light is given by IF(Y$ = Ic;,;(v)12 Ls(v)lZ, where F(v), S(V), and G,!<v) are the probability amplitudes of the scattered light, the excitation source and the resonance at frequency V. The implications of this equation in the interpretation of scattering experiments is discussed. In particular, defining resonance Raman sgtterir?g s that scattering in which the scattered Ii&t has the same bandwidth as the exciting light, it is concluded that although resonance Ramnn and resonance fluorescence spectra correspond to limiting cases of resonance scattering spectra. spectra in intermediate cases cannot be resolved into a sum of a Raman spectrum and a resonance fluorescence spectrum.


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A theory is presented that describes the time dependence bP scattering off an &omic or molecti "re~rznce" using tunabli: dye laser pulses. The main conclusion is that theie is n6,e'xponeatially deaying component which depends upon the frequency difference between the exciting pulse and the resonance