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Elsevier eBooks

Differential equations in quantum mechanics

Valerio Magnasco

Published Jan 1, 2013• 1 citation
Publisher
DOI
10.1016/b978-0-444-62647-9.00003-8

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The symmetry study of main differential equations of mechanics and electrodynamics has shown, that differential equations, which are invariant under transformations of groups, which are symmetry groups of mathematical numbers (considered in the frame of the number theory) determine the mathematical nature of the quantities, incoming in given equations. It allowed to proof the main postulate of quantum mechanics, that to any mechanical quantity can be set up into the correspondence the Hermitian matrix by quantization. High symmetry of Maxwell equations allows to show, that to EM-field funcions, incoming in given equations, can be set up into the correspondence the Quaternion (twice-Hermitian) matrices by their quantization.
Action at distance in Newtonian physics is replaced by finite propagation speeds in classical post-Newtonian physics.As a result, the differential equations of motion in Newtonian physics are replaced by functional differential equations, where the delay associated with the finite propagation speed is taken into account.Newtonian equations of motion, with post-Newtonian corrections, are often used to approximate the functional differential equations.Are the finite propagation speeds the origin of the quantum mechanics?In this work a simple atomic model based on a functional differential equation which reproduces the quantized Bohr atomic model is presented.As straightforward application of the result the fine structure of the hydrogen atom is approached.