Difference between revisions of "Sub-Quantum Physics 5: H Atom States: Constant Density Balls, and Degenerate Ellipses"

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==Abstract==
 
==Abstract==
  
Angular considerations of the quantum states of the hydrogen atom are here fully treated in terms of a new sub-quantum physics.  The methodology leads to excellent fits for Schrodinger 1S, 2P, 3D, and 4F position probability densities.  The 1S state is a superposition of concentric constant-probability-density balls.  The 2P, etc., states are superpositions of radial motions in degenerate ellipses, fanning out angularly from a central axis.[[Category:Scientific Paper]]
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Angular considerations of the quantum states of the hydrogen atom are here fully treated in terms of a new sub-quantum physics.  The methodology leads to excellent fits for Schrodinger 1S, 2P, 3D, and 4F position probability densities.  The 1S state is a superposition of concentric constant-probability-density balls.  The 2P, etc., states are superpositions of radial motions in degenerate ellipses, fanning out angularly from a central axis.
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[[Category:Scientific Paper|sub-quantum physics h atom states constant density balls degenerate ellipses]]

Latest revision as of 11:07, 1 January 2017

Scientific Paper
Title Sub-Quantum Physics 5: H Atom States: Constant Density Balls, and Degenerate Ellipses
Author(s) Alan McCone
Keywords {{{keywords}}}
Published 2001
Journal Galilean Electrodynamics
Volume 12
Number 4
Pages 63-69

Abstract

Angular considerations of the quantum states of the hydrogen atom are here fully treated in terms of a new sub-quantum physics. The methodology leads to excellent fits for Schrodinger 1S, 2P, 3D, and 4F position probability densities. The 1S state is a superposition of concentric constant-probability-density balls. The 2P, etc., states are superpositions of radial motions in degenerate ellipses, fanning out angularly from a central axis.