Electron-light interactions beyond the adiabatic approximation: recoil engineering and spectral interferometry

The adiabatic approximation has formed the basis for much of our understandings of the interaction of light and electrons. The classical nonrecoil approximation or quantum mechanical Wolkow states of free-electron waves have been routinely employed to interpret the outcomes of low-loss electron ener...

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Main Author: Nahid Talebi
Format: Article
Language:English
Published: Taylor & Francis Group 2018-01-01
Series:Advances in Physics: X
Subjects:
Online Access:http://dx.doi.org/10.1080/23746149.2018.1499438
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spelling doaj-d9d723cfd85c45bfbac3d1b99bac03a12020-11-24T21:09:02ZengTaylor & Francis GroupAdvances in Physics: X2374-61492018-01-013110.1080/23746149.2018.14994381499438Electron-light interactions beyond the adiabatic approximation: recoil engineering and spectral interferometryNahid Talebi0Stuttgart Center for Electron Microscopy, Max Planck Institute for Solid State ResearchThe adiabatic approximation has formed the basis for much of our understandings of the interaction of light and electrons. The classical nonrecoil approximation or quantum mechanical Wolkow states of free-electron waves have been routinely employed to interpret the outcomes of low-loss electron energy-loss spectroscopy (EELS) or electron holography. Despite the enormous success of semianalytical approximations, there are certainly ranges of electron–photon coupling strengths where more demanding self-consistent analyses are to be exploited to thoroughly grasp our experimental results. Slow-electron point-projection microscopes and many of the photoemission experiments are employed within such ranges. Here, we aim to classify those regimes and propose numerical solutions for an accurate simulation model. A survey of the works carried out within self-consistent Maxwell–Lorentz and Maxwell–Schrödinger frameworks are outlined. Several applications of the proposed frameworks are discussed, and an outlook for further investigations is also delivered. Abbreviations: CL: Cathodoluminescence CW: continuous – wave DLA: dielectric laser accelerator EDPHS: electron-driven photon source EEGS: electron energy-gain spectroscopy EELS: Electron energy-loss spectroscopy eV: electron-volt fs: femtosecond FDTD: finite-difference time-domain IR: infrared PIC: particle-in-cell PINEM: photon-induced near-field electron microscopy PLDOS: photonic local density of state PPM: point-projection electron microscopy SEM: scanning electron microscope SVA: slowly varying approximation TE: transverse electric TEM: transmission electron microscope THz: terahertz TM: transverse magnetic UV: ultraviolethttp://dx.doi.org/10.1080/23746149.2018.1499438Adiabatic approximationrecoilspectral interferometryself-consistent field theory
collection DOAJ
language English
format Article
sources DOAJ
author Nahid Talebi
spellingShingle Nahid Talebi
Electron-light interactions beyond the adiabatic approximation: recoil engineering and spectral interferometry
Advances in Physics: X
Adiabatic approximation
recoil
spectral interferometry
self-consistent field theory
author_facet Nahid Talebi
author_sort Nahid Talebi
title Electron-light interactions beyond the adiabatic approximation: recoil engineering and spectral interferometry
title_short Electron-light interactions beyond the adiabatic approximation: recoil engineering and spectral interferometry
title_full Electron-light interactions beyond the adiabatic approximation: recoil engineering and spectral interferometry
title_fullStr Electron-light interactions beyond the adiabatic approximation: recoil engineering and spectral interferometry
title_full_unstemmed Electron-light interactions beyond the adiabatic approximation: recoil engineering and spectral interferometry
title_sort electron-light interactions beyond the adiabatic approximation: recoil engineering and spectral interferometry
publisher Taylor & Francis Group
series Advances in Physics: X
issn 2374-6149
publishDate 2018-01-01
description The adiabatic approximation has formed the basis for much of our understandings of the interaction of light and electrons. The classical nonrecoil approximation or quantum mechanical Wolkow states of free-electron waves have been routinely employed to interpret the outcomes of low-loss electron energy-loss spectroscopy (EELS) or electron holography. Despite the enormous success of semianalytical approximations, there are certainly ranges of electron–photon coupling strengths where more demanding self-consistent analyses are to be exploited to thoroughly grasp our experimental results. Slow-electron point-projection microscopes and many of the photoemission experiments are employed within such ranges. Here, we aim to classify those regimes and propose numerical solutions for an accurate simulation model. A survey of the works carried out within self-consistent Maxwell–Lorentz and Maxwell–Schrödinger frameworks are outlined. Several applications of the proposed frameworks are discussed, and an outlook for further investigations is also delivered. Abbreviations: CL: Cathodoluminescence CW: continuous – wave DLA: dielectric laser accelerator EDPHS: electron-driven photon source EEGS: electron energy-gain spectroscopy EELS: Electron energy-loss spectroscopy eV: electron-volt fs: femtosecond FDTD: finite-difference time-domain IR: infrared PIC: particle-in-cell PINEM: photon-induced near-field electron microscopy PLDOS: photonic local density of state PPM: point-projection electron microscopy SEM: scanning electron microscope SVA: slowly varying approximation TE: transverse electric TEM: transmission electron microscope THz: terahertz TM: transverse magnetic UV: ultraviolet
topic Adiabatic approximation
recoil
spectral interferometry
self-consistent field theory
url http://dx.doi.org/10.1080/23746149.2018.1499438
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