Abstract

In this paper we introduce a simple procedure for computing the macroscopic quantum behaviour of periodic quantum systems in the high energy regime. The macroscopic quantum coherence is ascribed to a one-particle state, not to a condensate of a many-particle system; and we are referring to a system of high energy but with few degrees of freedom. We show that, in the first order of approximation, the quantum probability distributions converge to its classical counterparts in a clear fashion, and that the interference effects are strongly suppressed. The harmonic oscillator provides a testing ground for these ideas and yields excellent results.

Highlights

  • The superposition principle lies at the heart of quantum mechanics, and it is one of its features that most distinctly marks the departure from classical concepts [1]

  • In this paper we introduce a simple procedure to compute the high energy regime of a general density matrix for periodic quantum systems

  • To this end we extend the Fourier expansion in Equation (2) to the spatial components of the matrix density (7)

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Summary

Introduction

The superposition principle lies at the heart of quantum mechanics, and it is one of its features that most distinctly marks the departure from classical concepts [1]. A widely accepted explanation nowadays for the appearance of classical like features from an underlying quantum world is the environment induced decoherence approach [3,4,5,6]. This problem has been considered before by Cabrera and Kiwi [7] In this work, they use purely quantum-mechanical results to analyze (by inspection) the amplitude of the oscillations and the spatial autocorrelation function for large quantum numbers. They use purely quantum-mechanical results to analyze (by inspection) the amplitude of the oscillations and the spatial autocorrelation function for large quantum numbers They conclude that even for arbitrarily high quantum numbers, a superposition of (a few) eigenstates retains quantum effects.

General Procedure
Macroscopic Density Matrix of the Harmonic Oscillator
Final Remarks
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