Difference between revisions of "The Geometry of Quantum Mechanics"

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==Abstract==
 
==Abstract==
  
It is shown that the strange mathematics of quantum mechanics can be accounted for if it describes the interaction of three vector fields; nucleus, electron, and photon.  A state vector is formed as the combination of two of the three vector fields.  This yields an infi-nite number of possible solutions, the probability amplitudes.  The remaining vector field, or operator, is then applied to the state vec-tor to obtain an infinite number of possible values for the physical variable, the eigenvalues.  Combining the vector fields in a different order yields two distinct, but mathematically equivalent solutions, matrix mechanics and wave mechanics.[[Category:Scientific Paper]]
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It is shown that the strange mathematics of quantum mechanics can be accounted for if it describes the interaction of three vector fields; nucleus, electron, and photon.  A state vector is formed as the combination of two of the three vector fields.  This yields an infi-nite number of possible solutions, the probability amplitudes.  The remaining vector field, or operator, is then applied to the state vec-tor to obtain an infinite number of possible values for the physical variable, the eigenvalues.  Combining the vector fields in a different order yields two distinct, but mathematically equivalent solutions, matrix mechanics and wave mechanics.
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[[Category:Scientific Paper|geometry quantum mechanics]]

Latest revision as of 10:16, 1 January 2017

Scientific Paper
Title The Geometry of Quantum Mechanics
Read in full Link to paper
Author(s) Richard Oldani
Keywords {{{keywords}}}
Published 2008
Journal None
No. of pages 4

Read the full paper here

Abstract

It is shown that the strange mathematics of quantum mechanics can be accounted for if it describes the interaction of three vector fields; nucleus, electron, and photon. A state vector is formed as the combination of two of the three vector fields. This yields an infi-nite number of possible solutions, the probability amplitudes. The remaining vector field, or operator, is then applied to the state vec-tor to obtain an infinite number of possible values for the physical variable, the eigenvalues. Combining the vector fields in a different order yields two distinct, but mathematically equivalent solutions, matrix mechanics and wave mechanics.