Heaviside-step potential (QM)

From Wikipedia, the free encyclopedia

You have new messages (last change).
Please help improve this article or section by expanding it.
Further information might be found on the talk page or at requests for expansion.
This article has been tagged since January 2007.
This article may require cleanup to meet Wikipedia's quality standards.
Please discuss this issue on the talk page or replace this tag with a more specific message.
This article has been tagged since November 2006.

The Heaviside-step potential is a textbook problem of quantum mechanics and scattering theory. The problem consists of solving the time-independent Schrödinger equation for a particle with a step-like potential in one dimension.

Contents

[edit] Calculation

The time-independent Schrödinger equation for the wave function ψ(x) reads

H\psi(x)=[-\frac{\hbar^2}{2m}\frac{d^2}{dx^2}+V(x)]\psi(x)=E\psi(x),

where H is the Hamiltonian \hbar is the (reduced) Planck constant, m is the mass, E the energy of the particle and

V(x) = V0Θ(x)

is the potential step with height V0 > 0. \Theta(x)=0,\; x<0;\; \Theta(x)=1,\; x>0 is the Heaviside step-function. The barrier is positioned at x = 0. Without changing the results, any other shifted position was possible. The first term in the Hamiltonian, -\frac{\hbar^2}{2m}\frac{d^2}{dx^2}\psi is the kinetic energy.

The step divides the space in two parts (x < 0,x > 0). In any of these parts the potential is constant meaning the particle is quasi-free, and the solution of the Schrödinger equation can be written as a superposition of left and right moving waves (see free particle)

\psi_L(x)= \frac{1}{\sqrt{k_0}} \left(A_r e^{i k_0 x} + A_l e^{-ik_0x}\right)\quad x<0,
\psi_R(x)= \frac{1}{\sqrt{k_1}} \left(B_r e^{i k_1 x} + B_l e^{-ik_1x}\right)\quad x>0

where the wave vectors are related to the energy via

k_0=\sqrt{2m E/\hbar^2}, and
k_1=\sqrt{2m (V_0-E)/\hbar^2}.

The index r/l on the coefficients A and B denotes the direction of the velocity vector. Note that for energies E < V0, the wave function to the right of the step is exponentially decaying over a distance 1 / (ik1). Nevertheless we keep the notation r/l even though the waves are not propagating anymore in this case. The prefactor \frac{1}{\sqrt{k}} ensures a correct normalization of the probability flux.

The coefficients A,B have to be found from the boundary conditions of the wave function at x = 0. The wave function and its derivative have to be continuous everywhere, so.

Scattering at a finite potential step of height V0. The amplitudes and direction of left and right moving waves are indicated. In red, those waves used for the derivation of the reflection and transmission amplitude. E > V0 for this figure.
Scattering at a finite potential step of height V0. The amplitudes and direction of left and right moving waves are indicated. In red, those waves used for the derivation of the reflection and transmission amplitude. E > V0 for this figure.
ψL(0) = ψR(0),
\frac{d}{dx}\psi_L(0) = \frac{d}{dx}\psi_R(0).

Inserting the wave functions, the boundary conditions give the following restrictions on the coefficients

\sqrt{k_1}(A_r+A_l)=\sqrt{k_0}(B_r+B_l)
\sqrt{k_0}(A_r-A_l)=\sqrt{k_1}(B_r-B_l),

[edit] Transmission and reflection

At this point, it is instructive to compare the situation to the classical case. In both cases, the particle behaves as a free particle outside of the barrier region. A classical particle with energy E larger than the barrier height V0 does not feel the barrier at all, while a classical particle with E < V0 incident on the barrier from the left would always get reflected.

To study the quantum case, let us consider the following situation: a particle incident on the barrier from the left side (Ar). It may be reflected (Al) or transmitted (Br). Here and in the following assume E > V0

To find the amplitudes for reflection and transmission for incidence from the left, we put in the above equations Ar = 1 (incoming particle), Al = r (reflection), Bl=0 (no incoming particle from the right) and Br = t (transmission). We then solve the set of two linear equations for r,t.

The result is:

t=\frac{2\sqrt{k_0k_1}}{k_0+k_1}
r=\frac{k_0-k_1}{k_0+k_1}.

The model is symmetric with respect to a mirror transformation and at the same time exchange k_0\leftrightarrow k_1. For incidence from the right we have therefore the amplitudes for transmission and reflection

t'=t=\frac{2\sqrt{k_0k_1}}{k_0+k_1}
r'=-r=\frac{k_1-k_0}{k_0+k_1}.

[edit] Analysis of the obtained expressions.

[edit] E < V0

Quantum mechanics says that there is a finite probability that the incident particle will penetrate the potential barrier and exist to the right of the potential step. The probability of finding a particle at distance d in the region to the right of the step compared to that at x = 0 is given by

e^{-2K_1d}

This probability illustrates the differences between classical and quantum mechanics. The quantum mechanical penetration is not classically allowed

[edit] E > V0

In this energy range the transmission and reflection coefficient differ from the classical case. They are the same for incidence from the left and right and read

T=|t|^2=|t'|^2=\frac{4k_0k_1}{(k_0+k_1)^2}
R=|r|^2=|r'|^2=1-T=\frac{(k_0-k_1)^2}{(k_0+k_1)^2}

respectively. In the limit of large energies, E\gg V_0, the classical result (T=1, R=0) is recovered. Thus there is a finite probability for a particle with an energy larger than the step height to be reflected.

Reflection and transmission probability at a Heaviside-step potential. Dashed: classical result. Solid lines: quantum mechanics. For E < V0 the classical and quantum problem give the same result.
Reflection and transmission probability at a Heaviside-step potential. Dashed: classical result. Solid lines: quantum mechanics. For E < V0 the classical and quantum problem give the same result.

[edit] Remarks, application

The Heaviside-step potential mainly serves as an exercise in quantum mechanics classes as the solution requires the understanding of a variety of concepts of quantum physics like normalization, matching of wave functions, reflection/transmission amplitudes, and probabilities.

A similar problem to the one considered appears in the physics of normal-metal superconductor interfaces. Quasiparticles are scattered at the pair potential which in the simplest model may be assumed to have a step-like shape. The solution of the Bogoliubov-de Gennes equation resembles that of the discussed Heaviside-step potential. In the superconductor normal-metal case this gives rise to Andreev reflection.

[edit] See also

Retrieved from "http://en.wikipedia.org../../../h/e/a/Heaviside-step_potential_%28QM%29_a8a7.html"