The basic ideas in the theory of quantum mechanics on phase space are illustrated through an introduction of generalities, which seem to underlie most if not all such formulations and follow with examples taken primarily from kinematical particle model descriptions exhibiting either Galileian or Lorentzian symmetry. The structures of fundamental importance are the relevant (Lie) groups of symmetries and their homogeneous (and associated) spaces that, in the situations of interest, also possess Hamiltonian structures. Comments are made on the relation between the theory outlined and a recent paper by Carmeli, Cassinelli, Toigo, and Vacchini.
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Abdus Salam International Centre for Theoretical Physics,34100 Trieste,ItalyAbdus Salam International Centre for Theoretical Physics,34100 Trieste,Italy
A.E.F.Djema
H.Smail
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Département de Physique,Institut d'Hydraulique,Centre Universitaire Mustapha Stambouli,Mascara 29000,AlgeriaAbdus Salam International Centre for Theoretical Physics,34100 Trieste,Italy
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Univ Autonoma San Luis Potosi, Fac Ciencias, Campus Pedregal,Ave Parque Chapultepec 1610, San Luis Potosi 78217, San Luis Potosi, MexicoUniv Autonoma San Luis Potosi, Fac Ciencias, Campus Pedregal,Ave Parque Chapultepec 1610, San Luis Potosi 78217, San Luis Potosi, Mexico
Sanchez-Cordova, Mar
Berra-Montiel, Jasel
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Univ Autonoma San Luis Potosi, Fac Ciencias, Campus Pedregal,Ave Parque Chapultepec 1610, San Luis Potosi 78217, San Luis Potosi, Mexico
Univ Napoli Federico II, Dipartimento Fis Ettore Pancini, Complesso Univ Monte S Angelo, I-80126 Naples, ItalyUniv Autonoma San Luis Potosi, Fac Ciencias, Campus Pedregal,Ave Parque Chapultepec 1610, San Luis Potosi 78217, San Luis Potosi, Mexico