# Orbital angular momentum eigenstates in the $|\mathbf{r}\rangle$ representation

Consider the orbital angular momentum operators $$L^2$$ and $$L_z$$. In the $$|\mathbf{r}\rangle$$ representation using spherical coordinates those operators actions are given by

$$L^2\varphi(\mathbf{r})=-\hbar^2\left(\dfrac{\partial^2}{\partial\theta^2}+\dfrac{1}{\tan \theta} \dfrac{\partial}{\partial \theta}+\dfrac{1}{\sin^2\theta}\dfrac{\partial^2}{\partial\phi^2}\right)\varphi(\mathbf{r})$$

$$L_z\varphi(\mathbf{r})=-i\hbar \dfrac{\partial}{\partial \phi}\varphi(\mathbf{r}).$$

Now, we know that $$[L^2,L_z]=0$$ so that it is possible to construct a basis of state space of simultaneous eigenstates of both $$L^2$$ and $$L_z$$. We also know that the eigenvalues of $$L^2$$ are of the form $$l(l+1)\hbar^2$$ with $$l$$ integral or half-integral. On the other hand the eigenvalues of $$L_z$$ are of the form $$m\hbar$$ and with fixed $$l$$ we have that $$m$$ can only take on the values $$-l,-l+1,\dots,l-1,l$$. The simultaneous eigenvalue equations are then

$$L^2\psi(r,\theta,\phi)=l(l+1)\hbar^2\psi(r,\theta,\phi)$$

$$L_z\psi(r,\theta,\phi)=m\hbar \psi(r,\theta,\phi)$$

Now, the book I'm studying (Cohen's Quantum Mechanics book) states the following:

In the eigenvalue equations, $$r$$ does not appear in any differential operator, so we can consider it to be a parameter and *take into account only the $$\theta$$- and $$\phi$$-dependence of $$\psi$$. Thus, we denote by $$Y_l^m(\theta,\phi)$$ a common eigenfunction of $$L^2$$ and $$L_z$$ which corresponds to the eigenvalues $$l(l+1)\hbar^2$$ and $$m\hbar$$.

$$L^2Y^m_l(\theta,\phi) = l(l+1)\hbar^2Y^m_l(\theta,\phi)$$

$$L_zY^m_l(\theta,\phi)=m\hbar Y^m_l(\theta,\phi)$$

That equations give the $$\theta$$- and $$\phi$$-dependence of the eigenfunctions of $$L^2$$ and $$L_z$$. Once the solutions $$Y^m_l(\theta,\phi)$$ of these equations has been found, these eigenfunctions will be obtained in the form:

$$\psi_{l,m}(r,\theta,\phi)=f(r)Y^m_l(\theta,\phi)$$

where $$f(r)$$ is a function of $$r$$ which appears as na integration constant for the partial differential equation.

Now, I don't see how the author concludes that given $$l$$ and $$m$$ the eigenfunction $$\psi_{l,m}$$ is of the form $$\psi_{l,m}(r,\theta,\phi) = f(r)Y^m_l(\theta,\phi)$$. This conclusion to come out from thin air. By the way things are written it seems that $$Y^m_l$$ is by definition the eigenfunction corresponding to $$l$$ and $$m$$. But then the author states that the eigenfunction is really $$\psi_{l,m}(r,\theta,\phi)=f(r)Y^l_m(\theta,\phi)$$.

Indeed the equations defining the eigenfunctions of $$L^2$$ and $$L_z$$ are differential equations. Viewing from this point, $$\psi_{l,m}$$ is the form of a separable solution. But there are the ones which are not separable.

In general, considering the way the author presented things, how does he conclude the general form of eigenfunctions and what is his point on calling $$Y^m_l$$ the angular dependence of the eigenfunctions

• I'm not sure what exactly is unclear to you here. You know the spectrum fo $L_z$ and $L^2$. The $\psi_{l,m}$ are eigenfunctions for each possible eigenvalue. So why do you claim that there could be non-separable eigenfunctions? Writing a general non-separable function as $\sum_i f_i(r) Y^{l_i}_{m_i}(\theta,\phi)$, you should be able to see that only the separable ones are eigenfunctions. Feb 6, 2016 at 20:22
• The author is talking first and foremost of the eigenfunction of $\nabla^2$ in spherical coordinates which involves all 3 coordinates $(r,\theta,\phi)$. This eigenfunction he is denoting as $\psi(r,\theta,\phi)$. Next, he is using the explicit form of $\nabla^2$ in spherical coordinates and showing that it can be broken up into a piece that's purely $r$ dependent and a piece that's purely $(\theta,\phi)$ dependent. The latter turns out to be simply $L^2$. He concludes that the full eigenfunction $\psi$ can be constructed out of eigenfunctions of $L^2$, namely $Y^m_l$. Feb 6, 2016 at 22:04

## 1 Answer

We know that $\psi_{l,m}$ satisfies, for each $l$ and $m$, the equations

$$L^2\psi_{l,m}(r,\theta,\phi)=l(l+1)\hbar^2\psi_{l,m}(r,\theta,\phi),$$

$$L_z\psi_{l,m}(r,\theta,\phi)=m\hbar \psi_{l,m}(r,\theta,\phi).$$

But we also know that, by definition, $Y_{l, m}(\theta, \phi)$ satisfy the same equations.

Then, unless the eigenvalue equations for $Y_{l,m}$ are degenerate, which can proved to be not by solving the differential equations, we must conclude that $\psi_{l,m}$ and $Y_{l,m}$ are the same, apart from a "constant" factor which does not depend on $\theta$ or $\phi$, but does depend on $r$. The author then simply proceeds in calling this still unknown factor $f(r)$.