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Pump-probe and Photon-Echo Experiments

In the last chapter, we used a steady-state treatment to relate the shape of an absorption band to the dynamics of relaxations in the excited state. Because a period on the order of the electronic dephasing time will be required to establish a steady state, Eqs. (10.43) and (10.44) apply only on time scales longer than this. We need to escape this limitation if we hope to explore the relaxation dynamics themselves. Our first goal in this chapter is to develop a more general approach for analyzing spectroscopic experiments on femtosecond and picosecond time scales. This provides a platform for discussing how pump-probe and photon-echo experiments can be used to probe the dynamics of structural flucmations and the transfer of energy or electrons on these short time scales. [Pg.463]

These expressions apply to a variety of experiments that depend on the third-order polarization, including pump-probe and photon-echo experiments. Three-pulse photon echo experiments, for example, depend on R2. [Pg.477]


See other pages where Pump-probe and Photon-Echo Experiments is mentioned: [Pg.15]    [Pg.487]   


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