2015
DOI: 10.1016/j.ultramic.2015.05.004
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On the electron vortex beam wavefunction within a crystal

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Cited by 9 publications
(6 citation statements)
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References 15 publications
(26 reference statements)
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“…When electron vortex beams interact with matter, the cylindrical symmetry is typically broken, and the beam evolves in a highly nontrivial way through the material. In this process, the electron OAM changes significantly for all but the thinnest sample and can even change its sign for certain thickness [238,239,240]. This process can be effectively simulated using standard multislice numerical calculations solving the nonrelativistic Schrödinger equation for a fast electron wavepacket travelling through the potential produced by the atoms.…”
Section: Elastic Interaction Of Vortex Electrons With Mattermentioning
confidence: 99%
“…When electron vortex beams interact with matter, the cylindrical symmetry is typically broken, and the beam evolves in a highly nontrivial way through the material. In this process, the electron OAM changes significantly for all but the thinnest sample and can even change its sign for certain thickness [238,239,240]. This process can be effectively simulated using standard multislice numerical calculations solving the nonrelativistic Schrödinger equation for a fast electron wavepacket travelling through the potential produced by the atoms.…”
Section: Elastic Interaction Of Vortex Electrons With Mattermentioning
confidence: 99%
“…3 . Previous studies using the Bloch waves method explored the elastic dynamic scattering of electron vortex beams in crystals 57 , 58 . Such studies showed that with higher semi-convergence angle (30 mrad, m = +1), a vortex beam remains strongly localized with in few (<10) nanometers.…”
Section: Resultsmentioning
confidence: 99%
“…Landau) beams in a uniform magnetic field in the zdirection, as well as Bessel beams, but not LG beams, which are approximate solutions to the paraxial Schrödinger equation [40]. These results however assume uniform electrostatic potential, and do not always hold in a crystal [42][43][44], so that our analysis is only applicable for weakly diffracting specimens. Integration along the electron trajectory with the assumption of a depth independent electron density leads to the quantisation condition 𝑞 𝑧 = 𝜔/2𝜋𝑣.…”
Section: Magnetic Energy Loss For a Vortex Electron Beam With Orbital...mentioning
confidence: 94%
“…𝑛 𝑣 (−𝐑, z) = 𝑛 𝑣 (𝐑, 𝑧); even parity of the electron density also implies that 𝑛 ̃𝑣(𝐪 ⊥ , 𝑧) is a real quantity. For a vortex beam in a crystalline specimen however this simple relationship breaks down due to dynamic diffraction [42][43][44].…”
Section: Magnetic Energy Loss For a Vortex Electron Beam With Orbital...mentioning
confidence: 99%