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Anticrossing spectroscopy

In practice there are several factors which complicate anticrossing spectroscopy. The four anticrossings of Fig 18.4 apparently occur at the same field, given... [Pg.389]

Beyer, H.J. and Kleinpoppen, H. (1979). Applications of anticrossing spectroscopy, Proc. VI Intern. Conf. Atomic Phys., Zinatne, Plenum Press, Riga, New York, London, pp. 435-461. [Pg.271]

Radford (1961, 1962) and Radford and Broida (1962) presented a complete theory of the Zeeman effect for diatomic molecules that included perturbation effects. This led to a series of detailed investigations of the CN B2E+ (v — 0) A2II (v = 10) perturbation in which many of the techniques of modern high-resolution molecular spectroscopy and analysis were first demonstrated anticrossing spectroscopy (Radford and Broida, 1962, 1963), microwave optical double resonance (Evenson, et at, 1964), excited-state hyperfine structure with perturbations (Radford, 1964), effect of perturbations on radiative lifetimes and on inter-electronic-state collisional energy transfer (Radford and Broida, 1963). A similarly complete treatment of the effect of a magnetic field on the CO a,3E+ A1 perturbation complex is reported by Sykora and Vidal (1998). The AS = 0 selection rule for the Zeeman Hamiltonian leads to important differences between the CN B2E+ A2II and CO a/3E+ A1 perturbation plus Zeeman examples, primarily in the absence in the latter case of interference effects between the Zeeman and intramolecular perturbation terms. [Pg.418]

Miller, et al., (1974) used MOMRIE (Microwave Optical Magnetic Resonance Induced by Electrons) complementarily with anticrossing spectroscopy in experiments on He, H2, and other molecules. Small differences in electron bombardment excitation cross-sections combined with different radiative lifetimes lead to steady-state population differences between initial and final levels of the microwave transition. By monitoring fluorescence from one of the two involved electronic states, a change in fluorescence intensity signals a microwave resonance. Electron bombardment excitation tends to produce smaller population differences than the chemical pumping scheme exploited in the CN experiments, but the MOMRIE technique is more generally applicable. [Pg.436]

The level-crossing and anticrossing phenomena have been observed for the first time for hyperfine components of atomic energy levels.The level-anticrossing spectroscopy was then applied to the study of very weak singlet-triplet (or doublet-quadruplet) coupling in atoms" and in diatomic molecules (see, e.g.. Refs. 124 and 125 and references therein). [Pg.374]

H.J. Beyer, H. Kleinpoppen, Anticrossing spectroscopy, in Progr. Atomic Spectroscopy, ed. by W. Hanle, H. Kleinpoppen (Plenum, New York, 1978), p. 607... [Pg.718]

A perturbation acts as a window through which normally unobservable states may be viewed. Anticrossing, quantum-beat, and MODR spectroscopies are capable of examining the states in the immediate vicinity of the perturbed level. Optical-optical double resonance (OODR) allows systematic exploration of states far above and below the perturbed level. Gottscho, (1979) utilized an... [Pg.438]


See other pages where Anticrossing spectroscopy is mentioned: [Pg.168]    [Pg.387]    [Pg.390]    [Pg.419]    [Pg.423]    [Pg.428]    [Pg.430]    [Pg.437]    [Pg.318]    [Pg.950]    [Pg.529]    [Pg.499]    [Pg.9]    [Pg.168]    [Pg.387]    [Pg.390]    [Pg.419]    [Pg.423]    [Pg.428]    [Pg.430]    [Pg.437]    [Pg.318]    [Pg.950]    [Pg.529]    [Pg.499]    [Pg.9]    [Pg.288]    [Pg.315]    [Pg.753]    [Pg.35]    [Pg.361]    [Pg.351]    [Pg.367]   
See also in sourсe #XX -- [ Pg.66 ]




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Anticrossings

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