Difference between revisions of "The Geometry of Quantum Mechanics"
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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.[[Category:Scientific Paper]] | + | 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|geometry quantum mechanics]] | ||
Latest revision as of 11:16, 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.
