Particle in an Infinite Circular Well
Particle in an Infinite Circular Well
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 , equal to the number of angular nodes, determines the angular momentum . The radially excited state energies depend on the zeros of the Bessel function (kr).
m
mℏ
J
m
Details
Details
The solutions are of the form (kr)sin(mθ) and (kr)cos(mθ) with the quantized energy levels
J
|m|
J
|m|
E
n,m
2
ℏ
2
k
n,m
2μ
where is the Planck constant, is the mass and is the zero of the Besssel function (k,r).
ℏ
μ
k
n,m
th
n
J
m
References
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
External Links
Permanent Citation
Permanent Citation
Enrique Zeleny, Michael Trott
"Particle in an Infinite Circular Well"
http://demonstrations.wolfram.com/ParticleInAnInfiniteCircularWell/
Wolfram Demonstrations Project
Published: August 14, 2013

