Twisting neutral particles with electric fields

February 8, 2021 10:15 am Published by

In our paper, twisting neutral particles with electric fields, 1  we demonstrate that a polarized neutron impinging on a longitudinally oriented electric field can obtain a unit of orbital angular momentum entangled to its spin degree of freedom. The coupling strength is proportional to the electric field strength and the transverse wavevector, which depends on the beam divergence. To obtain maximally entangled states the neutron must experience a voltage drop of roughly rad. While such fields are not feasible in laboratory environment they do appear naturally between the lattice planes of perfect crystals.

Here we show the cross-section of two Eigenstates of the cylindrical Schroedinger equation, one without orbital angular momentum and one with one unit of orbital angular momentum (see here for details of theory).


Perhaps more surprising is our prediction of so called transverse spin-orbit states, where the or- bital angular momentum of the neutron is oriented transversly to the propagation direction. This can be realized with an electric field oriented perpendicularly to the propagation direction of the neutron. In practice this coupling is much more pronounced than the longitudinal variant, since the electric field now couples to the longitudinal wavevector, which is usually 3-4 orders of magni- tude larger than the transverse wavevector. Transverse orbital angular momentum has not been explicitly observed in any particle system to our knowledge.

Below a figure can be seen depicting a planewave with no transverse orbital angular momen- tum. This planewave is multiplied by the transverse orbital angular momentum raising operator, thereby increasing the orbital angular momentum by one unit of . The wavefronts appear to show a forked pattern, with a phase singularity at the center. While this does not accurately represent the action of an electric field on a planewave, the figure does give an idea as to how transverse orbital angular momentum presents itself.


1. Niels Geerits and Stephan Sponar Phys. Rev. A 103, 022205 (2021). ↩