Problems in the General Theory of Relativity and Theory of Group Representations 1979
DOI: 10.1007/978-1-4684-0676-4_3
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Canonical Transformations and the Theory of Representations of Lie Groups

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Cited by 4 publications
(5 citation statements)
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“…As always, to pass from the classical expressions to the quantum ones it is necessary to order in some way the operators involved and replace the Poisson brackets by commutators. The equations (3) give us a hint about the very tempting possibility to rewrite them as…”
Section: Algebraic Casementioning
confidence: 99%
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“…As always, to pass from the classical expressions to the quantum ones it is necessary to order in some way the operators involved and replace the Poisson brackets by commutators. The equations (3) give us a hint about the very tempting possibility to rewrite them as…”
Section: Algebraic Casementioning
confidence: 99%
“…the constant term from the second equation ( 10) may be taken away. This corresponds to the transition from the algebra U(3) to SU (3).…”
Section: Classical Casementioning
confidence: 99%
See 1 more Smart Citation
“…Thus the components in each row characterize one of the possible irreducible representations of a specific subalgebra. The eigenvalues of the invariant (or Casimir) operators of so n+1 have been obtained by Perelomov, Popov [18] and Leznov, Malkin, and Man'ko [19] and are given by…”
Section: The Orthogonal Cayley-klein Algebrasmentioning
confidence: 99%
“…In fact, this quantum system is a particular case of systems with Hamiltonians linear in Lie algebra generators. Such systems in the general case (integrals of motion, evolution operator and propagators) were proposed many years ago; for more details, see [21]. Since the Hamiltonian (1.10) is explicitly time-dependent, it is also not possible to find the exact expression for either the wave function or the solution for the equations of motion in the Heisenberg picture.…”
Section: Introductionmentioning
confidence: 99%