Angular Momentum Eigenvalues in Two Dimensions Suppose we have a particle moving in a circle on the $xy$ plane. Then the angular momentum operator will be just $L_z = ε_{3jk} x_jp_k$ and $L^2 = L_z ^2$. Then if $m$ are the eigenvalues of $L_z$ we'll have $m^2$ as the eigenvalues of $L^2$ so we'll have 1 quantum number, instead of $l$ and $m_l$ as in the 3D case. However we can't even define creation and annihilation operators as usual ($L_{\pm}= L_x \pm i L_y $), since $L_x$, $L_y$ aren't even defined, so how are we to find the eigenvalues of $L_z$? 
 A: Let us start from the fact that $L^2(\mathbb R^2, dxdy)$ is isomorphic to $L^2(\mathbb R_+, rdr)\otimes L^2(\mathbb S^1, d\theta)$, the unitary identification being the unique linear continuous extension of $$U : L^2(\mathbb R_+, rdr)\otimes L^2(\mathbb S^1, d\theta) \ni  u_n(r) \otimes \frac{e^{i  m \theta}}{\sqrt{2\pi}}\mapsto u_n(r)\frac{e^{i  m \theta}}{\sqrt{2\pi}} \in L^2(\mathbb R^2, dxdy) \quad n \in \mathbb N\:, m \in \mathbb Z$$
with $dxdy = rdr d\theta$ and $x= r\cos \theta$, $y = r \sin \theta$ and where 
$\{u_n\}_{n\in \mathbb N}$ is a Hilbert basis of $L^2(\mathbb R_+, rdr)$.
$U$ does not depend on the choice of this basis.
Restrict $X_j$ and $P_j$ to the Schwartz space $\cal S(\mathbb R^2)$ that is a dense invariant core for them, that is equivalent to saying that they are essentially self adjoint thereon: they are symmetric on $\cal S(\mathbb R^2)$ and their closures are selfadjoint so that restricting to that space preserves the full information on these selfadjoint operators.
It is possible to construct a Hilbert basis of $L^2(\mathbb R^2, dxdy)$ whose elements stay in $\cal S(\mathbb R^2)$ and have the form $u_n(r) \frac{e^{i  m \theta}}{\sqrt{2\pi}}$ where $u_n \in C^\infty_0((0,+\infty))$.
Next define on   $\cal S(\mathbb R^2)$ the operator
$$L := XP_y -YP_x$$ 
By direct inspection, using the basis written above, one sees that 
$$U L U^{-1} = -i\hbar I\otimes \frac{d}{d\theta}\:.$$
With this expression, it turns out that the full set of functions $u_n(\cdot) \frac{e^{i  m \cdot}}{\sqrt{2\pi}}$ is a Hilbert basis of eigenvectors of $L$ with eigenvalues $\hbar m$.
As a consequence of Nelson's theorem, the symmetric densely defined operator $L$ is therefore


*

*essentially self-adjoint on $\cal S(\mathbb R^2)$, 

*its spectrum is a pure point-spectrum with eigenvalues $\hbar m \in \mathbb Z$.
Another more indirect approach, exploiting Peter-Weyl's theorem,  would concern the theory of strongly-continuous irreducible representations of $SO(2)$ giving rise to the same result.  
