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arXiv:cond-mat/0311479

Quantum Wave Resistance of Schrodinger functions

Timir Datta, Raphael Tsu

Published Nov 20, 2003• 5 citations
arXivHTMLPDF

Abstract

The new concept of quantum wave-impedance (QWI), Z is introduced to answer the question whether there is impedance to a Schrodinger wave. Z will be an analogue of Maxwell's free space impedance (376.7 ohm) for electromagnetic waves. We show, for free particle wave function, the value of Z is in general not zero and purely real (resistive). As in quantum hall (QHE), Z can be expressed in terms of the fine structure constant, the electromagnetic permittivity and permeability of free space. Z is a determinant of the partitioning and flow of charge and energy transported by the quantum system. The scale factor of Z is about 12.9 kilo-ohms (per spin), so the corresponding wave conductance G is (77.5 micro-mho, per spin) double the unit of Landaur conductance. As functions of the quantum numbers (l,m,n) Z shows, peaks, valleys and plateaus; also as in QHE, both integer and fractional steps may be obtained. In microwave and optical technology, conventional impedance is an essential parameter. The quantum impedance defined here will be no exception in future technology.

DOI
10.48550/arxiv.cond-mat/0311479

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The new concept of quantum wave-impedance (QWI), Z is introduced to answer the question whether there is impedance to a Schrodinger wave. Z will be an analogue of Maxwell's free space impedance (376.7 ohm) for electromagnetic waves. We show, for free particle wave function, the value of Z is in general not zero and purely real (resistive). As in quantum hall (QHE), Z can be expressed in terms of the fine structure constant, the electromagnetic permittivity and permeability of free space. Z is a determinant of the partitioning and flow of charge and energy transported by the quantum system. The scale factor of Z is about 12.9 kilo-ohms (per spin), so the corresponding wave conductance G is (77.5 micro-mho, per spin) double the unit of Landaur conductance. As functions of the quantum numbers (l,m,n) Z shows, peaks, valleys and plateaus; also as in QHE, both integer and fractional steps may be obtained. In microwave and optical technology, conventional impedance is an essential parameter. The quantum impedance defined here will be no exception in future technology.
The quantum microscopic world view: I promised an explanation of quantum theory in two steps. In the first step Schrödinger’s wave is something that moves in familiar threedimensional space. You could almost believe, as Schrödinger himself did at first, that there is something real waving that corresponds to the fundamental stuff of matter (electrons, quarks, photons, . . . ), something like Maxwell’s dynamical field of electromagnetism that in the old theory carries what we perceive as light. But alas, the Schrödinger wave function is not even an ordinary number. Its symbol stands for a whole array of numbers, including an amplitude at each point whose square is the probability that a detector will click there, and components in a set of “internal dimensions” that are new features of Nature. Worse, the Schrödinger wave for two detectors moves in six spatial dimensions, three to locate each detector. Adding more detectors requires more dimensions. Whatever it is, the Schrödinger wave is not a “real” field like Maxwell’s.
An application of the quantum wave impedance method for the analytical study of quantum-mechanical systems containing a set of delta-wells and delta-barriers is considered in this study.The algorithm for determining both transmission and reflection coefficients for a set of delta-barriers was proposed.Similarly, the scheme for analytically deriving the expressions for energy levels and wave functions of bound states for a set of delta-wells was developed.In both cases, the solution for the quantum wave impedance function in the region with a constant potential [1] and the matching conditions at the origins of deltafunctions were used.As an illustration of the application of the proposed approach, the quantum-mechanical systems with symmetric double-barrier potential and double-well potential were investigated.In the case of a single delta-well, the eigenenergy value as well as the expression for the eigenfunction were obtained directly using the non-linear differential equation for the quantum wave impedance function.The results demonstrate the effectiveness of the quantum wave impedance method in handling quantum-mechanical systems with deltalike potentials, offering a robust framework for further studies in this area.
The quantum principles that establish the energy levels and degeneracies needed to evaluate the partition functions are explored. The uncertainty principle is associated with the dual wave-particle nature of the model used to describe quantized gas particles. The Schroedinger wave equation is presented as a generalization of Maxwell's wave equation; the former applies to all particles while the Maxwell equation applies to the special case of photon particles. The size of the quantum cell in phase space and the representation of momentum as a space derivative operator follow from the uncertainty principle. A consequence of this is that steady-state problems that are space-time dependent for the classical model become only space dependent for the quantum model and are often easier to solve. The partition function is derived for quantized free particles and, at normal conditions, the result is the same as that given by the classical phase integral. The quantum corrections that occur at very low temperatures or high densities are derived. These corrections for the Einstein-Bose gas qualitatively describe the condensation effects that occur in liquid helium, but are unimportant for most practical purposes otherwise. However, the corrections for the Fermi-Dirac gas are important because they quantitatively describe the behavior of high-density conduction electron gases in metals and explain the zero point energy and low specific heat exhibited in this case.
An effort is made to review the Yang potential. The ground state and the wave function by using Bethe’s Ansatz are found. The Laughlin’s potential is studied and its various properties are investigated. The number of particles in cluster of electrons determines the angular momentum which is used to define the filling factor of the lowest Landau level. A flux factor is added to it so that it gives the desired denominators. The Laughlin state is obtained for any value of the filling factor, p. In all cases, the ground state belongs to nonphysical many-body Hamiltonians. The composite fermion wave function is not the ground state of any known single Hamiltonian. From the angular momentum, we construct the filling factor and then look for the wave function rather than for the Hamiltonian. In this approach the Hamiltonians found are unrealistic. It is possible to make the filling factors agree with the experimental values but the Hamiltonian are not the usual type. The relative angular momentum of two particles L2 is found to define a projection operator. The filling factor is defined for the state of two particles. The number of particles is g. If another particle approaches it to form a cluster, the modified filling factor is defined. In this methodology the flux quanta cannot be attached to the electron and the projection operator is not linked to the Coulomb Hamiltonian. A monolayer of carbon is called graphene. It exhibits unusual properties in the Hall effect and in the cyclotron resonance. Hence, the Kohn's theorem, which shows that the interactions do not play much role in determining the cyclotron resonance, becomes operative. The Hubbard model has been very successful in explaining the ground state of several electron systems. By using the spin in a particular way, we can obtain new features in the Hubbard model. There is a doubling in the Peierls-Luttinger phase factor and eigen values acquire higher multiplicities than are known for the usual treatment of spin. The flux is distributed on the area of the triangle. The graphene consists of hexagons of carbon atoms but the Hall effect shows that there are defects on which electrons form clusters so that there is spin wave type behaviour. The Hall resistivity as a function of magnetic field is not a linear function. Hence a suitable theory to understand the Hall effect is formulated. We find that there are phase transitions as a function of temperature. There are lots of fractions of charge which are explained on the basis of spin and orbital angular momentum of the electron. The nano meter size films of graphite also show that the Hall resistivity is non-linear and shows steps as a function of magnetic field. We make an effort to understand the steps in the Hall effect resistivity of graphite with quantum wells formed on the surface. The spin in the clusters is polarized so that it becomes NS which is not 1/2 but depends on the number N, of electrons in a cluster.
A method for determining the quantum wave impedance function for a quantum-mechanical system with an arbitrary piecewise constant potential has been developed.Using this method, both the well-known iterative formula [A.N. Khondker, M. R. Khan, A. F. M. Anwar, J. Appl.Phys.63, 5191 (1988)] and an alternative approach for calculating quantum wave impedance were derived.This approach was applied to both scattering and bound state cases.The general form of the wave functions for bound states, as well as the transmission and reection coecients in the scattering case, were obtained for systems with a potential consisting of an arbitrary number of rectangular barriers and wells.The application of the developed method was demonstrated by describing symmetric rectangular double-well and double-barrier quantum-mechanical systems.