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Paul A. M. Dirac. Matchmaker: Relativity and Quantum Mechanics

Helge Kastrup, Jeffry V. Mallow A

Published Sep 27, 2022• 0 citations
Publisher

Abstract

Paul Dirac made contributions to theoretical physics that spanned quantum mechanics, relativity, gravity, and magnetism. Among these, the most important was arguably his connecting relativity and quantum mechanics. The Schrödinger equation is only correct for speeds much less than the speed of light. An equation correct for all speeds must include the energy associated with mass: E = mc2. The Dirac equation did just that. It also turned out to naturally include spin, which was an ad hoc addition to the wave functions obtained by the Schrödinger equation. He and Schrödinger shared the 1933 Nobel Prize.

DOI
10.1063/9780735421721_015

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Paul Dirac made contributions to theoretical physics that spanned quantum mechanics, relativity, gravity, and magnetism. Among these, the most important was arguably his connecting relativity and quantum mechanics. The Schrödinger equation is only correct for speeds much less than the speed of light. An equation correct for all speeds must include the energy associated with mass: E = mc2. The Dirac equation did just that. It also turned out to naturally include spin, which was an ad hoc addition to the wave functions obtained by the Schrödinger equation. He and Schrödinger shared the 1933 Nobel Prize.
Credible reasons are presented to reveal that many of the lingering century old enigmas, surrounding the behavior of at least an individual quantum particle, can be comprehended in terms of an objectively real specific wave function. This wave function is gleaned from the single particle energy-momentum eigenstate offered by the theory of space filling universal quantum fields that is an inevitable outcome of Dirac's pioneering masterpiece. Examples of these well-known enigmas are wave particle duality, the de Broglie hypothesis, the uncertainty principle, wave function collapse, and predictions of measurement outcomes in terms of probability instead of certainty. Paul Dirac successfully incorporated special theory of relativity into quantum mechanics for the first time. This was accomplished through his ingenious use of matrices that allowed the equations of motion to maintain the necessary first order time derivative feature necessary for positive probability density. The ensuing Dirac equation for the electron led to the recognition of the mystifying quantized spin and magnetic moment as intrinsic properties in contrast to earlier ad hoc assumptions. The solution of his relativistic equation for the hydrogen atom produced results in perfect agreement with experimental data available at the time. The most far reaching prediction of the celebrated Dirac equation was the totally unexpected existence of anti-particles, culminating in the eventual development of the quantum field theory of the Standard Model that reveals the deepest secrets of the universe known to date. Quanta 2019; 8: 88–100.
One of the reasons for 1933 Nobel Prize for physics is “for the discovery of new productive forms of atomic theory” (namely Schrodinger equation and Dirac equation). While, this paper points out that Schrodinger equation and Dirac equation are improper. According to Neutrosophy, Schrodinger equation and Dirac equation have three situations of truth, falsehood and indeterminacy respectively. Three reasons lead to Schrodinger equation and Dirac equation are improper: firstly, they are not derived by the principle of conservation of energy; secondly, the random (stochastic) concept could lead to absurd results; thirdly, they cannot solve many problems such as gravitation. Applying partial and temporary unified theory of natural science so including all the equations of natural science so far (in which, the theory of everything to express all of natural laws, described by Hawking that a single equation could be written on a T-shirt, is partially and temporarily realized in the form of partial and temporary unified variational principle of natural science so far), this paper presents partial and temporary unified theory of quantum mechanics so far, this unified theory can be used to make Schrodinger equation and Dirac equation tend to be proper (making Schrodinger equation and Dirac equation are restricted (or constrained) by principle of conservation of energy, and thus they can satisfy the principle of conservation of energy; also making they are restricted (or constrained) by a certain gravitational theory, and establish partial and temporary unified theory of quantum-gravitation so far).
I n the early 20th century, the groundbreaking theories of quantum mechanics and special relativity emerged at roughly the same time.At first, both theories appeared to be entirely incompatible with each other.While the quantum equations written out by Erwin Schrödinger and Wolfgang Pauli dealt with the behaviours of electrons, atoms, and molecules moving at speeds encountered in classical physics, the rules of special relativity first imagined by Albert Einstein described the behaviour of matter moving at close to the speed of light.Initially, this apparent clash of theories presented a crisis in physics.However, in the late 1920s, further theoretical work carried out by physicists including Paul Dirac, Oskar Klein, and Walter Gordon culminated in a new set of equations, which proved definitively that quantum mechanics and special relativity are compatible with each other after all. An educational challengeYet with this groundbreaking discovery came an entirely new problem.In adding a new layer of complexity to the equations of non-relativistic quantum mechanics, the more complete theories of relativistic
This chapter introduces the concepts of the relativistic theory to basic problems of quantum physics, in particular, the extension of the Schrodinger equation to a relativistic form. Starting from the fundamental laws of relativity, the chapter evaluates the Klein–Gordon equation and investigates if the equation can be considered a generalization of the non-relativistic Schrodinger equation to the case of the relativistic energy. The chapter shows that the wave function, which is a solution to the Klein–Gordon equation, cannot be connected with the probability wave function. For this reason, the Dirac equation is used to solve the problems faced by the Klein–Gordon equation. The Dirac equation also includes the spin. The advantage of the Dirac equation over the Schrodinger and Klein–Gordon equations is that it naturally includes the spin. In the Schrodinger and Klein–Gordon equations, the spin is not present and has to be added to the wave function manually whenever the wave function determines a system with the spin.
The father of quantum mechanics, Erwin Schrodinger, was one of the most important figures in the development of quantum theory. He is perhaps best known for his contribution of the wave equation, which would later result in his winning of the Nobel Prize for Physics in 1933. The Schrodinger wave equation describes the quantum mechanical behaviour of particles and explores how the Schrodinger wave functions of a system change over time. This project is concerned about exploring the one-dimensional case of the Schrodinger wave equation in a harmonic oscillator system. We will give the solutions, called eigenfunctions, of the equation that satisfy certain conditions. Furthermore, we will show that this happens only for particular values called eigenvalues.
This paper re-examines the key aspects of Dirac's derivation of his relativistic equation for the electron in order advance our understanding of the nature of quantum field theory. Dirac's derivation, the paper argues, follows the key principles behind Heisenberg's discovery of quantum mechanics, which, the paper also argues, transformed the nature of both theoretical and experimental physics vis-a-vis classical physics and relativity. However, the limit theory (a crucial consideration for both Dirac and Heisenberg) in the case of Dirac's theory was quantum mechanics, specifically, Schrodinger's equation, while in the case of quantum mechanics, in Heisenberg's version, the limit theory was classical mechanics. Dirac had to find a new equation, Dirac's equation, along with a new type of quantum variables, while Heisenberg, to find new theory, was able to use the equations of classical physics, applied to different, quantum-mechanical variables. In this respect, Dirac's task was more similar to that of Schrodinger in his work on his version of quantum mechanics. Dirac's equation reflects a more complex character of quantum electrodynamics or quantum field theory in general and of the corresponding (high-energy) experimental quantum physics vis-a-vis that of quantum mechanics and the (low-energy) experimental quantum physics. The final section examines this greater complexity and its implications for fundamental physics.