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Hole-burning experiments, ground state

R. de Vivie-Riedle and J. Manz Prof. Neumark s question about detecting the hole burning in the nuclear wavepacket of the electronic ground state is very stimulating. In this context, we have developed a scheme for detecting the hole in the wavepacket by a femtosecond chemistry laser experiment that involves two laser pulses Our explanation will be for the specific system K2, but more general applications for other systems are obvious ... [Pg.196]

We have adopted the excitonic band model not only because it describes conventional absorption spectroscopy (linear spectroscopy), but because it enables an extremely convenient description of nonlinear experiments, such as pump-probe, dynamical hole burning, or photon echoes. In these third-order experiments one has to consider not only transitions from the ground state to the one-excitonic states but also transitions from the one-excitonic to the two-excitonic states (see Fig. 13). These additional transitions reveal the required information to deduce, at least in principle, the complete coupling scheme. [Pg.321]

In contrast to the previous experiments with dilute rare-earth ions, quadrupole splittings in the ground ( F ) and excited ( Z>o) states of Eu " in the stoichiometric rare-earth compound EuPsOu were also determined by laser hole burning and optically detected... [Pg.35]


See other pages where Hole-burning experiments, ground state is mentioned: [Pg.81]    [Pg.256]    [Pg.338]    [Pg.228]    [Pg.89]    [Pg.394]    [Pg.67]    [Pg.458]    [Pg.1981]    [Pg.341]    [Pg.342]    [Pg.187]    [Pg.134]    [Pg.468]    [Pg.7]    [Pg.80]    [Pg.6]    [Pg.93]    [Pg.165]    [Pg.1981]    [Pg.17]    [Pg.237]    [Pg.252]    [Pg.288]    [Pg.37]    [Pg.112]    [Pg.267]    [Pg.286]    [Pg.360]    [Pg.133]    [Pg.939]   


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