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arXiv:1206.1084quant-ph

Overview of Bohmian Mechanics

Xavier Oriols, Jordi Mompart

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Abstract

This chapter provides a comprehensive overview of the Bohmian formulation of quantum mechanics. It starts with a historical review of the difficulties found by Louis de Broglie, David Bohm, and John S. Bell to convince the scientific community about the validity and utility of Bohmian mechanics. Then, a formal explanation of Bohmian mechanics for nonrelativistic, single-particle quantum systems is presented. The generalization to many-particle systems, where the exchange interaction and the spin play an important role, is also presented. After that, the measurement process in Bohmian mechanics is discussed. It is emphasized that Bohmian mechanics exactly reproduces the mean value and temporal and spatial correlations obtained from the standard, that is the Copenhagen or orthodox, formulation. The ontological characteristics of Bohmian mechanics provide a description of measurements as another type of interaction without the need for introducing the wave function collapse. Several solved problems are presented at the end of the chapter, giving additional mathematical support to some particular issues. A detailed description of computational algorithms to obtain Bohmian trajectories from the numerical solution of the Schrodinger or the Hamilton-Jacobi equations are presented in an appendix. The motivation of this chapter is twofold: first, as a didactic introduction to Bohmian formalism, which is used in the subsequent chapters, and second, as a self-contained summary for any newcomer interested in using Bohmian mechanics in his or her daily research activity.

arXiv comments
87 pages. This paper includes the two prefaces, the introduction and the first chapter of the second edition of the book: Applied Bohmian Mechanics: From Nanoscale Systems to Cosmology (Print ISBN: 9789814800105). The whole book, with nine additional chapters, has been published by Pan Stanford editorial and it can be ordered and it can be ordered at: sales@panstanford.com
Journal reference
DOI
Subjects
quant-phQuantum Physics

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    • > This is exactly what I was talking about, you consider that your atom has energy levels and then you plug in classical EM fields, sometimes that's good enough to get somewhere. But it can never be classical because there's no way to have energy levels in a classical atom. And…

      naaskingView on HNParent context

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