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Generalized Mechanics

J. Math. Phys. 13, 796 (1972); doi:10.1063/1.1666053

Issue Date: May 1972

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Herbert Tesser
Department of Physics, Pratt Institute, Brooklyn, New York
The quantization scheme for generalized Hamiltonians recently proposed by Hayes is shown to be inconsistent. The theory of constraints developed by Dirac is used and leads to a consistent theory. ©1972 The American Institute of Physics
History: Received 29 April 1970; revised 10 December 1970
Permalink: http://link.aip.org/link/?JMAPAQ/13/796/1
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ISSN:
0022-2488 (print)   1089-7658 (online)
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REFERENCES (5)

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  1. See, for example, M. Borneas, Phys. Rev. 186, 1299 (1969), and references contained therein.
  2. C. F. Hayes, J. Math. Phys. 10, 1555 (1969).
  3. P. A. M. Dirac, Can. J. Math. 2, 129 (1950);
  4. 3, 1 (1951).
  5. E. T. Whittaker, Analytical Dynamics (Cambridge U.P., Cambridge, 1937), p. 265.
  6. This form of the Hamiltonian is unique. The ambiguities demonstrated by C. F. Hayes and J. M. Jankowski [Nuovo Cimento 58, 494 (1968)] arise because they make transformations on the Hamiltonian which are not canonical.

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