Particle in an Infinite Circular Well

​
m
1
k
1
plot
density
3D
contour
This Demonstration solves the quantum-mechanical problem of a particle confined to a disk, which can be called an infinite 2D circular well. The probability densities for several energy eigenstates are plotted. The azimuthal quantum number
m
, equal to the number of angular nodes, determines the angular momentum
mℏ
. The radially excited state energies depend on the zeros of the Bessel function
J
m
​
(kr)
.

Details

The solutions are of the form
J
|m|
(kr)sin(mθ)
and
J
|m|
(kr)cos(mθ)
with the quantized energy levels
E
n,m
=
2
ℏ
2
k
n,m
2μ
,
where
ℏ
is the Planck constant,
μ
is the mass and
k
n,m
is the
th
n
zero of the Besssel function
J
m
(k,r)
.

References

[1] R. W. Robinett, "Visualizing the Solutions for the Circular Infinite Well in Quantum and Classical Mechanics," American Journal of Physics, 64(4), ‎1996 pp. 440–446.
[2] R. W. Robinett, Quantum Mechanics, Classical Results, Modern Systems and Visualized Examples, 2nd ed., Oxford: Oxford University Press, 2006.
[3] R. W. Robinett, "Quantum Mechanics of the Two-Dimensional Circular Billiard Plus Baffle System and Half-Integral Angular Momentum." arxiv.org/pdf/quant-ph/0307035.pdf.

External Links

Bessel Function of the First Kind (Wolfram MathWorld)
Planck's Constant (ScienceWorld)
Quantum Numbers (ScienceWorld)
Magnetic Quantum Number (ScienceWorld)
Schrödinger Equation (ScienceWorld)

Permanent Citation

Enrique Zeleny, Michael Trott
​
​"Particle in an Infinite Circular Well"​
​http://demonstrations.wolfram.com/ParticleInAnInfiniteCircularWell/​
​Wolfram Demonstrations Project​
​Published: August 14, 2013