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my 1 otherwise. 01, 2 1 x / o 9 2 + m2y + m c2 _+ s g n [ m ~ - 2 ] . J ( m2. + m y2+ m 2 ) 2 c% 2 2 4~,my. (18) Now, the original two-dimensional one-particle Hamiltonian Hxy which mixes the x- and y-directions via the angular momentum term has been transformed into the sum of two Hamiltonians of independent particles with masses Mx'and M2 in one-dimensional harmonic potentials with frequencies o91 and 092, respectively. The new masses and frequencies are given in terms of the original -qB frequencies mx, my, and the cyclotron frequency mc = - 7 - .

2 Q u a n t u m Mechanical Aspects of the Interaction of the Ionic Center of Mass and Electronic Motions . . . . . . . . . . . . . . . . . . 3 The classical Self-Stabilization and Self-Ionization Processes 49 49 4 Summary and Conclusions . . . . . . . . . . . . . . . . . . 60 5 References . . . . . . . . . . . . . . . . . . . . . . . 62 46 52 56 Structure and Bonding, Vol. 86 Springer-Verlag Berlin Heidelberg 1997 28 P.

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