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International Journal of Theoretical Physics

Classical Limit and Ehrenfest’s Theorem Versus Non-relativistic Limit of Noncommutative Dirac Equation in the Presence of Minimal Uncertainty in Momentum

Ilyas Haouam

Published Aug 22, 2023• 13 citations
Publisher
DOI
10.1007/s10773-023-05444-3

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This chapter introduces an elementary form of the fundamental axioms of quantum mechanics, focusing on the structure and interpretation of state functions within a vector space framework. The properties of linear operators acting on state functions are explored, along with the physical meaning of the state function itself. From this interpretation, boundary conditions and normalization requirements are derived. The chapter presents key results such as the normalization theorem, the time derivative of a physical observable, and Ehrenfest's theorem. It also defines probability density and probability current density, deriving the continuity equation for probability. The uncertainty principle is formally established, and energy conservation is addressed. The eigenvalues and eigenstates of the momentum operator are determined, and normalization using the Dirac delta function is introduced. The free particle wavefunction is derived, concluding with a discussion on the classical limit of quantum mechanics. Metadata/Keywords: quantum axioms, state function, linear operators, probability density, probability current, Ehrenfest's theorem, uncertainty principle, Dirac delta function, momentum eigenstates, classical limit

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In this article, we investigate Ehrenfest's theorem from the Dirac equation in a noncommutative phase-space where we calculate the time derivative of the position and the kinetic momentum operators for Dirac particles in interaction with electromagnetic field and within a noncommutative setting. This allows examining the effect of the phase-space noncommutativity on Ehrenfest's theorem. Knowing that with both the linear Bopp-Shift and Moyal-Weyl product, the noncommutativity is inserted.
The behaviour of wavepackets of the `Dirac oscillator' in (1 + 1) dimensions is examined. The Dirac oscillator is a relativistic extension of the harmonic oscillator. We construct a wavepacket in the usual Dirac representation and another one in the Foldy - Wouthuysen (FW) representation. In the nonrelativistic limit, these wavepackets are both reduced to Schrödinger's coherent wavepacket for the harmonic oscillator. The wavepacket in the Dirac representation exhibits Zitterbewegung whereas the one in the FW representation does not. We find that the wavepacket in the FW representation behaves much more like a classical particle than that of the Dirac representation. This gives insights into Ehrenfest's theorem for the Dirac equation.
This chapter introduces an elementary form of the fundamental axioms of quantum mechanics, focusing on the structure and interpretation of state functions within a vector space framework. The properties of linear operators acting on state functions are explored, along with the physical meaning of the state function itself. From this interpretation, boundary conditions and normalization requirements are derived. The chapter presents key results such as the normalization theorem, the time derivative of a physical observable, and Ehrenfest's theorem. It also defines probability density and probability current density, deriving the continuity equation for probability. The uncertainty principle is formally established, and energy conservation is addressed. The eigenvalues and eigenstates of the momentum operator are determined, and normalization using the Dirac delta function is introduced. The free particle wavefunction is derived, concluding with a discussion on the classical limit of quantum mechanics. Metadata/Keywords: quantum axioms, state function, linear operators, probability density, probability current, Ehrenfest's theorem, uncertainty principle, Dirac delta function, momentum eigenstates, classical limit