Theory of electromagnetic insertion devices and the corresponding synchrotron radiation

Permanent magnet insertion devices (IDs), which are the main radiation generating devices in synchrotron light sources and free-electron lasers, use a time-invariant but space-periodic magnetic field to wiggle relativistic electrons for short-wavelength radiation generation. Recently, a high power m...

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Main Authors: Muhammad Shumail, Sami G. Tantawi
Format: Article
Language:English
Published: American Physical Society 2016-07-01
Series:Physical Review Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevAccelBeams.19.074001
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spelling doaj-8dcc1747154b49c2924a0d33829d44902020-11-24T23:40:04ZengAmerican Physical SocietyPhysical Review Accelerators and Beams2469-98882016-07-0119707400110.1103/PhysRevAccelBeams.19.074001Theory of electromagnetic insertion devices and the corresponding synchrotron radiationMuhammad ShumailSami G. TantawiPermanent magnet insertion devices (IDs), which are the main radiation generating devices in synchrotron light sources and free-electron lasers, use a time-invariant but space-periodic magnetic field to wiggle relativistic electrons for short-wavelength radiation generation. Recently, a high power microwave based undulator has also been successfully demonstrated at SLAC which promises the advantage of dynamic tunability of radiation spectrum and polarization. Such IDs employ transverse elecromagnetic fields which are periodic in both space and time to undulate the electrons. In this paper we develop a detailed theory of the principle of electromagnetic IDs from first principles for both linear and circular polarization modes. The electromagnetic equivalent definitions of undulator period (λ_{u}) and undulator deflection parameter (K) are derived. In the inertial frame where the average momentum of the electron is zero, we obtain the figure-8-like trajectory for the linear polarization mode and the circular trajectory for the circular polarization mode. The corresponding radiation spectra and the intensity of harmonics is also calculated.http://doi.org/10.1103/PhysRevAccelBeams.19.074001
collection DOAJ
language English
format Article
sources DOAJ
author Muhammad Shumail
Sami G. Tantawi
spellingShingle Muhammad Shumail
Sami G. Tantawi
Theory of electromagnetic insertion devices and the corresponding synchrotron radiation
Physical Review Accelerators and Beams
author_facet Muhammad Shumail
Sami G. Tantawi
author_sort Muhammad Shumail
title Theory of electromagnetic insertion devices and the corresponding synchrotron radiation
title_short Theory of electromagnetic insertion devices and the corresponding synchrotron radiation
title_full Theory of electromagnetic insertion devices and the corresponding synchrotron radiation
title_fullStr Theory of electromagnetic insertion devices and the corresponding synchrotron radiation
title_full_unstemmed Theory of electromagnetic insertion devices and the corresponding synchrotron radiation
title_sort theory of electromagnetic insertion devices and the corresponding synchrotron radiation
publisher American Physical Society
series Physical Review Accelerators and Beams
issn 2469-9888
publishDate 2016-07-01
description Permanent magnet insertion devices (IDs), which are the main radiation generating devices in synchrotron light sources and free-electron lasers, use a time-invariant but space-periodic magnetic field to wiggle relativistic electrons for short-wavelength radiation generation. Recently, a high power microwave based undulator has also been successfully demonstrated at SLAC which promises the advantage of dynamic tunability of radiation spectrum and polarization. Such IDs employ transverse elecromagnetic fields which are periodic in both space and time to undulate the electrons. In this paper we develop a detailed theory of the principle of electromagnetic IDs from first principles for both linear and circular polarization modes. The electromagnetic equivalent definitions of undulator period (λ_{u}) and undulator deflection parameter (K) are derived. In the inertial frame where the average momentum of the electron is zero, we obtain the figure-8-like trajectory for the linear polarization mode and the circular trajectory for the circular polarization mode. The corresponding radiation spectra and the intensity of harmonics is also calculated.
url http://doi.org/10.1103/PhysRevAccelBeams.19.074001
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