Moshe Shapiro 2008 J. Phys. A: Math. Theor. 41 175303 doi:10.1088/1751-8113/41/17/175303
Moshe Shapiro
Show affiliationsBased on (1) the spectral resolution of the energy operator; (2) the linearity of correspondence between physical observables and quantum self-adjoint operators; (3) the definition of conjugate coordinate–momentum variables in classical mechanics; and (4) the fact that the physical point in phase space remains unchanged under (canonical) transformations between one pair of conjugate variables to another, we are able to show that
, the proper-time rest-energy transformation matrices, are given as aexp(−iEsts/
), from which we obtain the proper-time rest-energy evolution equation
. For special relativistic situations this equation can be reduced to the usual
dynamical equations, where t is the 'reference time' and E is the total energy. Extension of these equations to accelerating frames is then provided.
03.65.Sq Semiclassical theories and applications
81R15 Operator algebra methods (See also 46Lxx, 81T05)
81Q10 Selfadjoint operator theory in quantum theory, including spectral analysis
81Q20 Semiclassical techniques including WKB and Maslov methods
Issue 17 (2 May 2008)
Received 8 February 2008, in final form 10 March 2008
Published 15 April 2008
Moshe Shapiro 2008 J. Phys. A: Math. Theor. 41 175303
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