The Geometry of Quantum Mechanics: Difference between revisions
Imported from text file |
Imported from text file |
||
| Line 12: | Line 12: | ||
==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]] | 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 13:16, 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.