A Spontaneous Statistical Solution of Schrödinger's Partial Differential Equation


Authors : Dr. Ismail Abbas

Volume/Issue : Volume 9 - 2024, Issue 2 - February

Google Scholar : http://tinyurl.com/5k77kntc

Scribd : http://tinyurl.com/y95t8sy5

DOI : https://doi.org/10.5281/zenodo.10691330

Abstract : In previous articles we have shown that the solution of the heat diffusion equation is stimulated and forced by the boundary conditions and the material tested, while the solution of the Schrödinger SE equation or quantum mechanics problems in general is generated spontaneously in the space of the isolated object. object. This object is called a quantum system. While quantum mechanics and classical mechanics are distinct frameworks applicable to different scales and types of physical systems, only B-matrix string mechanics effectively applies to both scales. In this article we solve SE in three different situations 1D, 2D, 3D via the spontaneous chains of the B matrix of the Cairo technique. The validity and accuracy of numerical statistical solutions undoubtedly confirm that quantum mechanical systems operate spontaneously rather than stimulated.

In previous articles we have shown that the solution of the heat diffusion equation is stimulated and forced by the boundary conditions and the material tested, while the solution of the Schrödinger SE equation or quantum mechanics problems in general is generated spontaneously in the space of the isolated object. object. This object is called a quantum system. While quantum mechanics and classical mechanics are distinct frameworks applicable to different scales and types of physical systems, only B-matrix string mechanics effectively applies to both scales. In this article we solve SE in three different situations 1D, 2D, 3D via the spontaneous chains of the B matrix of the Cairo technique. The validity and accuracy of numerical statistical solutions undoubtedly confirm that quantum mechanical systems operate spontaneously rather than stimulated.

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