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When you have increasing energy levels in 2 or 3 dimensions how does the values of quantum numbers $n$ increase for each dimension?

For example if you have ground state $E_1$ then you have for $(n_x,n_y,n_z)$ is $(1,1,1)$ in 3 dimensions.

So does this mean for energy $E_2$ you have $(2,2,2)$ ?

I've only learnt it in 1 dimension so i don't understand how it works in higher dimensions?

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    $\begingroup$ For which class of systems? What is the Hamiltonian? What are $n_{x,y,z}?$ $\endgroup$
    – user87745
    Commented Nov 15, 2020 at 5:20
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    $\begingroup$ Oh this was in relation to an infinite square (cube) well. I was just unclear on how the quantum numbers increase as energy levels increase. $\endgroup$
    – WDUK
    Commented Nov 15, 2020 at 5:24

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For a particle in a box (also known as a particle in an infinite potential well) in $d$ dimensions, the Hamiltonian inside the box is given by $$\hat{H}=\frac{1}{2m}\sum_{i=1}^d{p}^2_i$$where $p_i$ is the momentum operator in the $i^{\text{th}}$ direction. As you already know (I infer so from your question) that using the boundary conditions, we arrive at the conclusion that $p_i$ must be of the form $$p_i=\frac{n_i\pi}{L_i}$$where $L_i$ is the length of the box in the $i^{\text{th}}$ direction and $n_i\in\mathbb{N}$. Thus, the energy of an eigenstate is given by $$E=\frac{\pi^2}{2m}\sum_{i=1}^d\frac{n_i^2}{L_i^2}$$.

Now, in the case of one--dimensional box, $E$ only depends on $n_x$ and is monotonically increasing with $n_x$. This means that the spectrum of a one--dimensional particle in a box is non--degenerate, and the value of the energy depends only on one quantum number, namely, $n_{x}$. One can simply write that $E=E_{n_x}$

However, in the case of a multidimensional box, $E$ depends on the multiple quantum numbers, namely, $\{n_i\}$ where $i>1$. And, we have to write $E=E_{\{n_i\}}$ to signify that $E$ depends on multiple quantum numbers.

Moreoever, multiple different sets of values of $n_i$ can produce the same value of energy. For example, let's consider the case where $L_i=L$ and $i=3$. All the following configurations of $n_i$ produce the same value of energy:$$n_x=2,n_y=1,n_z=1$$ $$n_x=1,n_y=2,n_z=1$$ $$n_x=1,n_y=1,n_z=2$$ Thus, we see that the spectrum of a particle in a box can be degenerate in a higher dimension.

So, to answer your question, the first excited energy state in a three-dimensional particle in a box (with equal sides) can correspond to all of the above configurations of quantum numbers.

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  • $\begingroup$ When i read this article: tinyurl.com/yxpvz8br Table 3.9.1 about half way down seems to suggest you cannot have $n=0$ in any of the dimensions for $E_1$ that you are suggesting ? It starts at $(1,1,1)$ $\endgroup$
    – WDUK
    Commented Nov 15, 2020 at 6:04
  • $\begingroup$ @WDUK Yes, I apologize, my bad. As I already had written, the $n$s should be natural numbers. If any of them is $0$ then the eigenfunction is just zero which is not normalizable and thus, not physical. I have corrected my examples. $\endgroup$
    – user87745
    Commented Nov 15, 2020 at 6:08
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So does this mean for energy $E_2$ you have $(2,2,2)$?

This is wrong! The 3-Dimensional box (and 2-Dimensional) have degeneracy is energy state that there 2 or more level for which the energy is same. Like for $E_2$, We have $(2,1,1),(1,2,1),(1,1,2)$.

Note that for 3-D box, The energy given by $$E_{n_1,n_2,n_3}=(n^2_1+n^2_2+n^2_3)\frac{\pi^2\hbar^2}{2mL^2}$$

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  • $\begingroup$ So is the general rule that for an increase in $E_n$ you get only one increase in quantum number but it can be in any combination of those 3 dimensions as a degeneracy ? So the sum of quantum numbers in $d$ dimensions for some energy $E_n = d+(n-1)$ ? $\endgroup$
    – WDUK
    Commented Nov 15, 2020 at 5:46

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