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Referencias:

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• The geometrical symmetry we are considering should be distinguished from the dynamical symmetries that lead to the unexpected degeneracies of the energy levels of the hydrogen atom and the isotropic harmonic oscillator; Fock, V., (1935) Z. Phys, 98, p. 145. , (a)
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• We implicitly are restricting our considerations on the 0 (4) generators to bound states. For continuum states, it turns out that the dynamical symmetry group is isomorphic to the group of Lorenz transformations in one time and three space dimensions rather than to the group of rotations in four space dimensions. See Ref. 17; Runge, C., (a), Vectoranalysis (Hirzel, Leipzig, 1919), Vol. 1, p. 70; Lenz, W., (1924) Z. Phys, 24, p. 197. , (b)
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