Fractional Angular Momenta, Gouy and Berry phases in Relativistic Bateman-Hillion-Gaussian Beams of Electrons
arXiv:1812.04957 · doi:10.1103/PhysRevLett.126.134803
Abstract
A new Bateman-Hillion solution to the Dirac equation for a relativistic Gaussian electron beam taking explicit account of the -position of the beam waist is presented. This solution has a pure Gaussian form in the paraxial limit but beyond it contains higher order Laguerre-Gaussian components attributable to the tighter focusing. One implication of the mixed mode nature of strongly diffracting beams is that the expectation values for spin and orbital angular momenta are fractional and are interrelated to each other by \textit{intrinsic spin-orbit coupling}. Our results for these properties align with earlier work on Bessel beams [Bliokh \textit{et al.} Phys. Rev. Lett. \textbf{107}, 174802 (2011)] and show that fractional angular momenta can be expressed by means of a Berry phase. The most significant difference arises, though, due to the fact that Laguerre-Gaussian beams naturally contain Gouy phase, while Bessel beams do not. We show that Gouy phase is also related to Berry phase and that Gouy phase fronts that are flat in the paraxial limit become curved beyond it.
arXiv comment6 pages, 5 figures
References in corpus (36)
- Goos-Hänchen and Imbert-Fedorov beam shifts: An overview
- Twisted Photons: New Quantum Perspectives in High Dimensions
- Twisted Light Transmission over 143 kilometers
- Theory and applications of free-electron vortex states
- Semiclassical Dynamics of Electron Wave Packet States with Phase Vortices
- Angular Momenta and Spin-Orbit Interaction of Nonparaxial Light in Free Space
- Relativistic Electron Vortex Beams: Angular Momentum and Spin-Orbit Interaction
- Ultrafast Generation and Control of an Electron Vortex Beam via Chiral Plasmonic Near Fields
- Spin and orbital angular momenta of acoustic beams
- Electron vortex beams in a magnetic field: A new twist on Landau levels and Aharonov-Bohm states
- Observation of the Larmor and Gouy Rotations with Electron Vortex Beams
- Atomic scale electron vortices for nanoresearch
- Colliding particles carrying non-zero orbital angular momentum
- Atomic ionization by twisted photons: Angular distribution of emitted electrons
- Realization of electron vortices with large orbital angular momentum using miniature holograms fabricated by electron beam lithography
- Relativistic electron wave packets carrying angular momentum
- Twisted electron in a strong laser wave
- Vacuum Faraday effect for electrons
- Elastic scattering of vortex electrons provides direct access to the Coulomb phase
- Propagation of Vortex Electron Wave Functions in a Magnetic Field
- Measuring the phase of the scattering amplitude with vortex beams
- Relativistic quantum dynamics of twisted electron beams in arbitrary electric and magnetic fields
- Position, spin and orbital angular momentum of a relativistic electron
- Doing spin physics with unpolarized particles
- Manipulating twisted electron beams
- Measuring geometric phase without interferometry
- Relativistic vortex electrons: paraxial versus non-paraxial regimes
- Radiative Capture of Twisted Electrons by Bare Ions
- Experimental proposal for measuring the Gouy phase of matter waves
- Radiative recombination of twisted electrons with bare nuclei: going beyond the Born approximation
- Nonuniform currents and spins of relativistic electron vortices in a magnetic field
- Bessel beams of two-level atoms driven by a linearly polarized laser field
- Quantum potential energy as concealed motion
- Acoustic vortex beams in synthetic magnetic fields
- Gouy Phase for Relativistic Quantum Particles
- Lorentz Covariant Quantum 4-Potential and Orbital Angular Momentum for the Transverse Confinement of Matter Waves
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