2D Harmonic Oscillator Quantum numbers

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SUMMARY

The discussion focuses on the differences between the Cartesian and polar representations of the 2D Harmonic Oscillator, specifically regarding quantum numbers and energy levels. It is established that while both representations yield the same energy levels, their quantum numbers are not directly interchangeable; for instance, in polar coordinates, the quantum numbers are represented as (n, |l|) while in Cartesian coordinates they are (n_x, n_y). The relationship between these quantum numbers is defined by the equation n = n_x + n_y. The polar representation exhibits circular symmetry, whereas the Cartesian representation displays mirroring symmetry, leading to distinct eigenstates in each coordinate system.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically the 2D Harmonic Oscillator.
  • Familiarity with quantum numbers and their significance in different coordinate systems.
  • Knowledge of energy eigenvalues in both Cartesian and polar coordinates.
  • Basic proficiency in plotting functions and interpreting graphical representations of quantum states.
NEXT STEPS
  • Study the relationship between quantum numbers in different coordinate systems, focusing on the 2D Harmonic Oscillator.
  • Learn about the linear combinations of eigenstates in quantum mechanics.
  • Explore the implications of symmetry in quantum systems, particularly circular and mirroring symmetries.
  • Investigate the mathematical derivation of energy eigenvalues for the 2D Harmonic Oscillator in both Cartesian and polar coordinates.
USEFUL FOR

Students of quantum mechanics, physicists analyzing harmonic oscillators, and educators teaching advanced physics concepts will benefit from this discussion.

Tabasko633
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Homework Statement


In the exercise, we solved the 2D Harmonic Oscillator in kartesian (x,y) and polar (r,φ) coordinates.
We found out that both have the same energy levels, but they look very different, when I plot them.
What am I missing? The polar solution seems more like it.

Homework Equations


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?temp_hash=fe2f5b418ec92066cdfe609b11e44886.png

The Attempt at a Solution


Two examples:

Unbenannt3.PNG
Unbenannt4.PNG


If needed, I can give you more details about the formulas or plots!
 

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What are the corresponding quantum numbers ##(n_x,n_y)## in the case of Cartesian and ##(n,|l|)## in the case of polar of the picture you plot there?
 
They correspond to the formulas above.
n_{x} and n_{y} are the quantum numbers from the 1D solution.
In the polar case, n_{r} corresponds to the energy and l to the angular momentum.
 
Last edited:
Tabasko633 said:
They correspond to the formulas above.
nx and ny are the quantum numbers from the 1D solution.
In the polar case, n corresponds to the energy and l to the angular momentum.
What I asked is what values of ##(n_x,n_y)## you used for plotting
unbenannt4-png.94564.png

and what values of ##(n,l)## for
unbenannt3-png.94563.png
?
 
Oh, sry.. (1,1) in both cases!
They look the same for the ground state.
Should I upload the file?
 
Tabasko633 said:
Oh, sry.. (1,1) in both cases!
That's the first mistake you made. Polar and Cartesian representations of 2D harmonic oscillator are different sets of bases, the one in polar coordinate is invariant under rotation while the one in Cartesian is not. This means, you should not assume that two pair of quantum numbers in polar and Cartesian representations having identical numerical values to be identically equal to each other. However, they are indeed connected if the energy eigenvalue are the same in both representation, in particular one eigenstate in one representation will be a linear combination of the eigenstates in the other representation. See the table in the last page in this link http://www.physics.rutgers.edu/~steves/501/Lectures_Final/Lec17_Polar%20Coordinates.pdf.
You can find there too that in polar coordinate the energy eigevalue is given by
$$
E_n = \hbar\omega(n+1)
$$
while in Cartesian coordinate by
$$
E_{n_x,n_y} = \hbar\omega(n_x+n_y+1)
$$
Here you can see that for the same energy in polar and Cartesian coordinates, the quantum numbers are related by ##n=n_x+n_y##. Using your program, try plotting the real part of ##(n,l) = (1,1)## for polar and ##(n_x,n_y) = (1,0)## in Cartesian.
 
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Actually, it is n=n_{x}+n_{y}=2n_{r}+l.
But I tried many different combinations, they behave very different in general.
(The polar solution has circular symmetry and the cartesian has mirroring symmetry)
 
Tabasko633 said:
But I tried many different combinations, they behave very different in general.
Indeed, they should be different. You can't find any pair of eigenfunctions in polar and in Cartesian which look identical as an eigenstate in one coordinate is a linear combination of eigenstates in the other coordinates, as I have mentioned in my previous comment. The only identical pair is the ground state because this energy level has no degeneracy. In fact, the eigenstate in polar is complex on the other hand the one in Cartesian is always real, no way to compare them one-on-one.
Tabasko633 said:
(The polar solution has circular symmetry and the cartesian has mirroring symmetry)
I have also pointed out this point in my previous comment. The polar representation is also eigenstate of angular momentum operator, which means it must indeed have circular symmetry. The Cartesian representation is eigenstate of ##x## and ##y## parity operators, so they will have mirror symmetry as you already observed.
 
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blue_leaf77 said:
Indeed, they should be different. You can't find any pair of eigenfunctions in polar and in Cartesian which look identical as an eigenstate in one coordinate is a linear combination of eigenstates in the other coordinates, as I have mentioned in my previous comment.

I guess it took two comments for me to understand, but now I got it.
In order to connect these two solutions, I will try to find the linear combination!
Thank you a lot for your help, blue_leaf77
 

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