Finite potential barrier (QM)

In quantum mechanics, the finite potential barrier is a standard one-dimensional problem that demonstrates the phenomenon of quantum tunnelling. The problem consists of solving the time-independent Schrödinger equation for a particle with a finite size barrier potential in one dimension. Typically, a free particle impinges on the barrier from the left.

Although classically the particle would be reflected, quantum mechanics states that there is a finite probability that the particle will penetrate the barrier and continue travelling through to the other side. The likelihood that the particle will pass through the barrier is given by the transmission coefficient, while the likelihood that it is reflected is given by the reflection coefficient.

Calculation

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

:$Hpsi(x)=left\; [-frac\{hbar^2\}\{2m\}frac\{d^2\}\{dx^2\}+V(x)\; ight]\; psi(x)=Epsi(x),$

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

:$V(x)=V\_0\; [Theta(x)-Theta(x-a)]$

is the barrier potential with height $V\_0\; >$

0 and width $a$.

is the Heaviside step function.

The barrier is positioned between $x=0$ and $x=a$. Withoutchanging 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 barrier divides the space in three parts (). 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). If $E>V\_0$

:, :

where the wave numbers are related to the energy via

::

The index r/l on the coefficients A and B denotes the direction of the velocity vector. Note that if the energy of the particle is below the barrier height, $k\_1$ becomes imaginary and the wave function is exponentially decaying within the barrier. Nevertheless we keep the notation r/l even though the waves are not propagating anymore in this case. Here we assumed $E\; eq\; V\_0$. The case $E=V\_0$ is treated below.

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

:$psi\_L(0)=psi\_C(0)$,:$frac\{d\}\{dx\}psi\_L(0)\; =\; frac\{d\}\{dx\}psi\_C(0)$,:$psi\_C(a)=psi\_R(a)$,:$frac\{d\}\{dx\}psi\_C(a)\; =\; frac\{d\}\{dx\}psi\_R(a)$.

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

:$A\_r+A\_l=B\_r+B\_l$:$ik\_0(A\_r-A\_l)=ik\_1(B\_r-B\_l)$,:$B\_re^\{iak\_1\}+B\_le^\{-iak\_1\}=C\_re^\{iak\_0\}+C\_le^\{-iak\_0\}$,:$ik\_1(B\_re^\{iak\_1\}-B\_le^\{-iak\_1\})=ik\_0(C\_re^\{iak\_0\}-C\_le^\{-iak\_0\})$.

= "E" = "V"₀ =

If the energy equals the barrier height, the solutions of the Schrödinger equation in the barrier region are not exponentials anymore but linear functions of the space coordinate

:

The complete solution of the Schrödinger equation is found in the same way as above by matching wave functions and their derivatives at $x=0$ and $x=a$. That results in the following restrictions on the coefficients:

:$A\_r+A\_l=B\_1$:$ik\_0(A\_r-A\_l)=B\_2$,:$B\_1+B\_2a=C\_re^\{iak\_0\}+C\_le^\{-iak\_0\}$,:$B\_2=ik\_0(C\_re^\{iak\_0\}-C\_le^\{-iak\_0\})$.

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 $V\_0$ would "always" pass the barrier, and a classical particle with

To study the quantum case, consider the following situation: a particle incident on the barrier from the left side ($A\_r$). It may be reflected ($A\_l$) or transmitted ($C\_r$).

To find the amplitudes for reflection and transmission for incidence from the left, we put in the above equations $A\_r=1$ (incoming particle), $A\_l=r$ (reflection), $C\_l$=0 (no incoming particle from the right) and $C\_r=t$ (transmission). We then eliminate the coefficients $B\_l,\; B\_r$ from the equation and solve for $r,\; t$.

The result is:

:$t=frac\{4\; k\_0k\_1\; e^\{-i\; a(k\_0-k\_1)\{(k\_0+k\_1)^2-e^\{2ia\; k\_1\}(k\_0-k\_1)^2\}$:$r=frac\{(k\_0^2-k\_1^2)sin(ak\_1)\}\{2\; i\; k\_0k\_1\; cos(ak\_1)+(k\_0^2+k\_1^2)sin(ak\_1)\}.$

Due to the mirror symmetry of the model, the amplitudes for incidence from the right are the same as those from the left. Note that these expressions hold for any energy $E>0$.

Analysis of the obtained expressions

"E" < "V"₀

The surprising result is that for energies less than the barrier height,

for the particle to be transmitted through the barrier, being $k\_1=sqrt\{2m\; (V\_0-E)/hbar^\{2$. This effect which differs from the classical case is called quantum tunneling. The transmission is exponentially suppressed with the barrier width which can be understood from the functional form of the wave function: outside of the barrier it oscillates with wave vector $k\_0$, while within the barrier it is exponentially damped over a distance $1/k\_1$. If the barrier is much larger than this decay length, the left and right part are virtually independent and tunneling is consequently suppressed.

"E" > "V"₀

In this case:$T=|t|^2=\; frac\{1\}\{1+frac\{V\_0^2sin^2(k\_1\; a)\}\{4E(E-V\_0)$

Equally surprising is that for energies larger than the barrier height, $E>V\_0$, the particle may be reflected from the barrier with a non-zero probability :$,R=|r|^2=1-T.$

This reflection probability is in fact oscillating with $k\_1\; a$ and only in the limit $Egg\; V\_0$ approaches the classical result $r=0$, no reflection. Note that the probabilities and amplitudes as written are for any energy (above/below) the barrier height.

= "E" = "V"₀ =

The transmission probability at $E=V\_0$ evaluates to

:$T=frac\{1\}\{1+ma^2V\_0/2hbar^2\}$.

Remarks and applications

The calculation presented above may at first seem unrealistic and hardlyuseful. However it has proved to be a suitable model for a variety of real-lifesystems. One such example are interfaces between two conducting materials. In the bulk of the materials, the motion of the electrons is quasi free and can be described by the kinetic term in the above Hamiltonian with an effective mass $m$. Often the surfaces of such materials are covered with oxide layers or are not ideal for other reasons. This thin, non-conducting layer may then be modeled by a barrier potential as above. Electrons may then tunnel from one material to the other giving rise to a current.

The operation of a scanning tunneling microscope (STM) relies on this tunneling effect. In that case the barrier is due to the air between the tip of the STM and the underlying object. Since the tunnel current depends exponentially on the barrier width, this device is extremely sensitive to height variations on the examined sample.

The above model is one-dimensional while space is three-dimensional. One should solve the Schrödinger equation in three dimensions. On the other hand, many systems only change along one coordinate direction and are translationally invariant along the others. The Schrödinger equation may then be reduced to the case considered here by an ansatz for the wave function of the type: $Psi(x,y,z)=psi(x)phi(y,z)$.

For another, related model of a barrier see Delta potential barrier (QM) which can be regarded as a special case of the finite potential barrier. All results from this article immediately apply to the delta potential barrier taking the limits $V\_0\; oinfty,quad\; a\; o\; 0$ while keeping $V\_0\; a=frac\{lambda^2\}\{m^2\}$ constant.

ee also

*Pauli exclusion principle

References

*cite book | author=Griffiths, David J.|title=Introduction to Quantum Mechanics (2nd ed.) | publisher=Prentice Hall |year=2004 |id=ISBN 0-13-111892-7
*Cite book | author = Claude Cohen-Tannoudji, Bernard Diu et Frank Laloë| title = Mécanique quantique, vol. I et II | publisher = Paris: Collection Enseignement des sciences (Hermann)| year = 1977| id = ISBN 2-7056-5767-3

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