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Radioelectronics Nanosystems Information Technologies

HARMONIC OSCILLATOR AND RELATED STATES WITH LARGE VALUE OF UNCERTAINTY

V. A. Andreev

Published Jan 1, 2017• 1 citation
Publisher

Abstract

A review is given of the properties of two types of quantum states, which have great uncertainty in the coordinate and momentum.Both are obtained from the states of a harmonic oscillator by means of certain transformations.The first type is correlated states, they are obtained from coherent states with a help of the Bogolyubov transform.The variances of the coordinate and momentum of such a state depend on the Bogolyubov transform parameters and can, in general, take arbitrarily large values.Their specific values are determined by the physical processes with which the Bogolyubov transform is realized.A concrete example of such physical process is considered.Another type are stretched states.Formally, they arise when the n-partial state of a harmonic oscillator undergoes a transform associated with a scale transformation of the phase space.The dispersion of the coordinate and momentum of these states depends on the scale transformation parameter and can also take arbitrarily large values.Physically stretched states can be obtained by passing n-photon states through a quantum amplifier.The role of the scale transformation of the phase space is played by the gain of the quantum amplifier.

DOI
10.17725/rensit.2017.09.008

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A review is given of the properties of two types of quantum states, which have great uncertainty in the coordinate and momentum.Both are obtained from the states of a harmonic oscillator by means of certain transformations.The first type is correlated states, they are obtained from coherent states with a help of the Bogolyubov transform.The variances of the coordinate and momentum of such a state depend on the Bogolyubov transform parameters and can, in general, take arbitrarily large values.Their specific values are determined by the physical processes with which the Bogolyubov transform is realized.A concrete example of such physical process is considered.Another type are stretched states.Formally, they arise when the n-partial state of a harmonic oscillator undergoes a transform associated with a scale transformation of the phase space.The dispersion of the coordinate and momentum of these states depends on the scale transformation parameter and can also take arbitrarily large values.Physically stretched states can be obtained by passing n-photon states through a quantum amplifier.The role of the scale transformation of the phase space is played by the gain of the quantum amplifier.
We consider scale transformations (q, p) → (λq, λp) in phase space. They induce transformations of the Husimi functions H(q, p) defined in this space. We consider the Husimi functions for states that are arbitrary superpositions of n-particle states of a harmonic oscillator. We develop a method that allows finding so-called stretched states to which these superpositions transform under such a scale transformation. We study the properties of the stretched states and calculate their density matrices in explicit form. We establish that the density matrix structure can be described using negative binomial distributions. We find expressions for the energy and entropy of stretched states and calculate the means of the number-ofstates operator. We give the form of the Heisenberg and Robertson–Schrödinger uncertainty relations for stretched states.
In this paper, dynamics and quantum mechanical coherent states of a simple harmonic oscillator are considered in the framework of the Generalized Uncertainty Principle (GUP). Equations of motion for the simple harmonic oscillator are derived and some of their new implications are discussed. Then, coherent states of the harmonic oscillator in the case of the GUP are compared with the relative situation in ordinary quantum mechanics. It is shown that in the framework of GUP there is no considerable difference in definition of coherent states relative to ordinary quantum mechanics. But, considering expectation values and variances of some operators, based on quantum gravitational arguments, one concludes that although it is possible to have complete coherency and vanishing broadening in usual quantum mechanics, gravitational induced uncertainty destroys complete coherency in quantum gravity and it is not possible to have a monochromatic ray in principle.
Harmonic oscillators are important in physical applications and in demonstrating the working of the postulates of quantum formalism. A classical harmonic oscillator has a state space, i.e., its phase space, coordinated by the oscillator’s position x and momentum p . Observables correspond to real-valued functions on the state space. The evolution of the state is determined by Hamilton’s equations, which reduce to Eq. (27.12) . The time dependence of the state automatically determines the time dependence of observables.
We present a new method to study the eigenvalues and eigenfunctions of anharmonic oscillators. It involves a new class of Bogoliubov transformations and leads to the introduction of k-photon coherent states. We consider the Hamiltonians for the simple harmonic and anharmonic oscillators as the two generators of a Lie algebra, whose other generators may be found exactly, or up to any desired order of the perturbation parameter involved. An element of this Lie group, turning out to be the multi-photon operator, transforms the anharmonic Hamiltonian to the harmonic one, thus facilitating the calculation of the eigenvalues and eigenfunctions of the former. The transformation of the ordinary annihilation and creation operators leads to generalized ones, corresponding to generalized oscillation modes, and also helps us out to introduce multi-photon coherent states. We specifically consider four-photon coherent states in detail and study time dependent position and momentum uncertainties in these states.
Examples of Berry’s and WBBZ - (D.Wojcik, I.Bialynicki-Birula and K.Zyczkowski) quantum fractal constructions are considered. The behavior of fractal dimensions of these very special superpositions of basic states of a particle in a potential box and harmonic oscillator is investigated in going from coordinate representation to momentum and coherent state representations. The mean value of quanta and dispersion for isolated quantum harmonic oscillator prepared in “fractal” state and interacting with another oscillator are calculated.
This is a pedagogical paper where we present a physically motivated approach to introduce the coherent states of a harmonic oscillator from which it is simple to rigorously derive their mathematical definition. We do this in two different ways that turn out to be equivalent but emphasize two related but different aspects of classicality. First, we analyze which are the quantum states that are the closest one can get to a point in phase space and demonstrate the validity of the following theorem: (i) The product of the uncertainty in position and that of momentum saturates the bound imposed by Heisenberg uncertainty relations for all times if and only if the state is an eigenstate of the annihilation operator. Second, we analyze the way in which the difference between the expectation value of the energy and the energy associated with the expectation values of position and momentum depends on the state, and show the validity of the following theorem (ii) the difference between the expectation value of the energy and the energy associated with the expectation values is minimal if and only if the state is an eigenstate of the annihilation operator. We also show that the reason why coherent states are chosen as the most classical ones by the decoherence process induced by coupling the particle to an environment in the standard Quantum Brownian motion model, is precisely due to the validity of the two above theorems.