Orbital angular momentum of free electrons

An electron in free space travelling at non-relativistic speeds, follows the Schrödinger equation for a free particle, that is

${\displaystyle i\hbar {\frac {\partial }{\partial t}}\Psi (\mathbf {r} ,t)={\frac {-\hbar ^{2}}{2m}}\nabla ^{2}\Psi (\mathbf {r} ,t)}$,

where ${\textstyle \hbar }$ is the reduced Planck constant, ${\textstyle \Psi (\mathbf {r} ,t)}$ is the single-electron wave function, ${\textstyle m}$ its mass, ${\textstyle \mathbf {r} }$ the position vector, and ${\textstyle t}$ is time. This equation is a type of wave equation and when written in the Cartesian coordinate system (${\textstyle x}$,${\textstyle y}$,${\textstyle z}$), the solutions are given by a linear combination of plane waves, in the form of

${\displaystyle \Psi _{\mathbf {p} }(\mathbf {r} ,t)\propto e^{i(\mathbf {p} \cdot \mathbf {r} -E(\mathbf {p} )t)/\hbar }}$

where ${\textstyle \mathbf {p} }$ is the linear momentum and ${\textstyle E(\mathbf {p} )}$ is the electron energy, given by the usual dispersion relation ${\textstyle E(\mathbf {p} )={\frac {p^{2}}{2m}}}$. By measuring the momentum of the electron, its wave function must collapse and give a particular value. If the energy of the electron beam is selected beforehand, the total momentum (not its directional components) of the electrons is fixed to a certain degree of precision. When the Schrödinger equation is written in the cylindrical coordinate system (${\textstyle \rho }$,${\textstyle \theta }$,${\textstyle z}$), the solutions are no longer plane waves, but instead are given by Bessel beams,[2] solutions that are a linear combination of

$${\displaystyle \Psi _{p_{\rho },\,p_{z},\,\ell }(\rho ,\theta ,z)\propto J_{|\ell |}\left({\frac {p_{\rho }\rho }{\hbar }}\right)e^{i(p_{z}z-Et)/\hbar }e^{i\ell \theta },}$$

that is, the product of three types of functions: a plane wave with momentum ${\textstyle p_{z}}$ in the ${\textstyle z}$-direction, a radial component written as a Bessel function of the first kind ${\textstyle J_{|\ell |}}$, where ${\textstyle p_{\rho }}$ is the linear momentum in the radial direction, and finally an azimuthal component written as ${\textstyle e^{i\ell \theta }}$ where ${\textstyle \ell }$ (sometimes written ${\textstyle m_{z}}$) is the magnetic quantum number related to the angular momentum ${\textstyle L_{z}}$ in the ${\textstyle z}$-direction. Thus, the dispersion relation reads ${\textstyle E=(p_{z}^{2}+p_{\rho }^{2})/2m}$. By azimuthal symmetry, the wave function has the property that ${\textstyle \ell =0,\pm 1,\pm 2,\cdots }$ is necessarily an integer, thus ${\textstyle L_{z}=\hbar \ell }$ is quantized. If a measurement of ${\textstyle L_{z}}$ is performed on an electron with selected energy, as ${\textstyle E}$ does not depend on ${\textstyle \ell }$, it can give any integer value. It is possible to experimentally prepare states with non-zero ${\textstyle \ell }$ by adding an azimuthal phase to an initial state with ${\textstyle \ell =0}$; experimental techniques designed to measure the orbital angular momentum of a single electron are under development. Simultaneous measurement of electron energy and orbital angular momentum is allowed because the Hamiltonian commutes with the angular momentum operator related to ${\textstyle L_{z}}$.

Note that the equations above follow for any free quantum particle with mass, not necessarily electrons. The quantization of ${\displaystyle L_{z}}$ can also be shown in the spherical coordinate system, where the wave function reduces to a product of spherical Bessel functions and spherical harmonics.

There are a variety of methods to prepare an electron in an orbital angular momentum state. All methods involve an interaction with an optical element such that the electron acquires an azimuthal phase. The optical element can be material,[3][4][5] magnetostatic,[6] or electrostatic.[7] It is possible to either directly imprint an azimuthal phase, or to imprint an azimuthal phase with a holographic diffraction grating, where grating pattern is defined by the interference of the azimuthal phase and a planar[8] or spherical[9] carrier wave.

Electron vortex beams have a variety of proposed and demonstrated applications, including for mapping magnetization,[4][10][11][12] studying chiral molecules and chiral plasmon resonances,[13] and identification of crystal chirality.[14]

Interferometric methods borrowed from light optics also work to determine the orbital angular momentum of free electrons in pure states. Interference with a planar reference wave,[5] diffractive filtering and self-interference[15][16][17] can serve to characterize a prepared electron orbital angular momentum state. In order to measure the orbital angular momentum of a superposition or of the mixed state that results from interaction with an atom or material, a non-interferometric method is necessary. Wavefront flattening,[17][18] transformation of an orbital angular momentum state into a planar wave,[19] or cylindrically symmetric Stern-Gerlach-like measurement[20] is necessary to measure the orbital angular momentum mixed or superposition state.