Search for quantum systems with a given spectrum-generating algebra: detailed study of the case ofSO 2,1

Il Nuovo Cimento A (1965-1970) - Tập 2 - Trang 217-236 - 2007
P. Cordero1, G. C. Ghirardi2
1International Centre for Theoretical Physics, Trieste
2Istituto di Fisica Teorica dell'Università, Trieste

Tóm tắt

A method is introduced to determine the HamiltoniansH of the quantum-mechanical systems having a given Lie algebra as their spectrum-generating algebra (SGA). Application of this method to the particular case in which the SGA is assumed to be the Lie algebraSO 2,1 allows under several assumptions the determination of a general solutionH, for a system of two spinless particles, having this algebra as its SGA, and possessing both a discrete and a continuous spectrum. Velocity-dependent potentials have been included, the only restrictions imposed onH being that it be at most quadratic in the momentum, and rotationally and time-reversal invariant. The potential obtained as the general solution contains as an essential part a term which asymptotically is Coulomb-like and is more general than those which have been obtained previously in the same context. The requirement that the potential be angular-momentum independent reduces the possible Hamiltonian to that of the hydrogen atom, with an extra cubic force, which has already been solved. In the case in which a purely discrete spectrum is allowed, the general answer is not given, but still a sufficiently general Hamiltonian is obtained withSO 2,1 as its SGA, that includes as a particular case the known harmonic oscillator with an extra cubic force.

Tài liệu tham khảo

Y. Dothan, M. Gell-Mann andY. Ne’eman:Phys. Lett.,17, 148 (1965). A. O. Barut, P. Budini andC. Fronsdal:Proc. Roy. Soc., A291, 106 (1966). R. H. Pratt andT. F. Jordan:Phys. Rev.,148, 1276 (1966). R. Musto:Phys. Rev.,148, 1274 (1966). M. Bander andC. Itzykson:Rev. Mod. Phys.,38, 330 (1966). C. Fronsdal:Phys. Rev.,156, 1665 (1967). R. C. Hwa andJ. Nuyts:Phys. Rev.,145, 1188 (1966). P. Budini:Acta Phys. Austriaca, Suppl.,4, 118 (1967). J. Lánik:Nucl. Phys.,2 B, 263 (1967). J. Lánik:Nucl. Phys.,5 B, 523 (1968). P. Aldrovandi andP. Leal Ferreira:Lett. Nuovo Cimento,1, 317 (1969). P. Cordero:Lett. Nuovo Cimento,4, 164 (1970). The reader who is not familiar with the formalism can find a clear and detailed discussion on the definition and use of the tilting operator in ref. (13). A. O. Barut: inLectures in Theoretical Physics, Vol.10 B, edited byA. O. Barut andW. E. Brittin (New York, 1969), p. 377. R. Cirelli andG. M. Prosperi:Nuovo Cimento,37, 1049 (1965). R. Cirelli, E. Montaldi andG. M. Prosperi:Nuovo Cimento,45 A, 381 (1966). A. O. Barut andC. Fronsdal:Proc. Roy. Soc., A287, 532 (1965).