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Rydberg, type experiment

Therefore, the energy separation between 5 i and Ti is 1 eV. For Rydberg-type excitations, the separation is, as a rule, 0.1 eV for valence-type excitations, it is 1-2 eV [22]. The separation of 1 eV is in favor of valence excitations in agreement with the results of those quenching experiments in which the kinetic distance was found to be comparable with the molecule diameter (Sec. 3.1). [Pg.368]

Using an apparatus of the type shown in Fig. 7.1, Bayfield and Koch (1974) conducted an ionization experiment with hydrogen Rydberg atoms that were prepared in the band 63 < tiq < 69 and exposed to electromagnetic radiation of three different frequencies Wj = 2nfi, with fi = 30 MHz,... [Pg.183]

In the early 1970s, when it had been recognized that experiments of beam-foil specfroscopy could produce lifetimes for many types of atomic transitions, we carried out a number of computations and analyses of transifion probabilities in atoms, with and without heavy valence-Rydberg state mixing. As we wrote in Ref. [26b], fhaf work revealed that (non int) corresponds to correlation vectors with small coefficients which are reasonably well decoupled from T and (int). This implies A) Their direct contribution to (, D /) is very small. I.e., the last three terms of eq. (12) are negligible because of the small... [Pg.56]


See other pages where Rydberg, type experiment is mentioned: [Pg.36]    [Pg.36]    [Pg.170]    [Pg.263]    [Pg.114]    [Pg.1230]    [Pg.52]    [Pg.58]    [Pg.387]    [Pg.382]    [Pg.155]    [Pg.220]    [Pg.492]    [Pg.24]    [Pg.126]    [Pg.22]    [Pg.135]    [Pg.5]    [Pg.197]    [Pg.28]    [Pg.269]    [Pg.123]    [Pg.268]    [Pg.296]    [Pg.742]    [Pg.190]    [Pg.391]    [Pg.63]    [Pg.85]    [Pg.514]    [Pg.27]    [Pg.318]    [Pg.265]    [Pg.270]    [Pg.185]   
See also in sourсe #XX -- [ Pg.36 ]




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