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231225s2021 xx |||||o 00| ||eng c |
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|a 10.1107/S1600577521004318
|2 doi
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|a pubmed25n1091.xml
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|a (DE-627)NLM327595655
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|a (NLM)34212868
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|a DE-627
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|a eng
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|a Hadad, Mansour
|e verfasserin
|4 aut
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|a Elliptical plasma-filled waveguide as a new standard short-period undulator
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|c 2021
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|a Text
|b txt
|2 rdacontent
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|a ƒaComputermedien
|b c
|2 rdamedia
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|a ƒa Online-Ressource
|b cr
|2 rdacarrier
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|a Date Revised 02.07.2021
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|a published: Print-Electronic
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|a Citation Status PubMed-not-MEDLINE
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|a Undulators as the sources of high-brilliance synchrotron radiation are of widespread interest in new generations of light sources and free-electron lasers. Microwave propagation in a plasma-filled elliptical waveguide can be studied as a standard short-period undulator. This structure as a lucrative insertion device can be installed in the storage ring of third- and fourth-generation light sources to produce high-energy and high-brilliance synchrotron radiation. In this article, the propagation of the transverse electric modes in a plasma-filled waveguide with an elliptical cross-section is investigated, and the field components, the cut-off frequencies and the electron beam trajectory are calculated. With due consideration of the electron beam dynamics and in order to achieve a standard short-period undulator, parameters such as the dimensions of the waveguide elliptical cross-section, the microwave frequency and the plasma density are calculated
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|a Journal Article
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|a elliptical waveguide
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|a plasma-filled waveguide
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|a synchrotron radiation
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|a undulator
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|a Yousefnejad, Sirous
|e verfasserin
|4 aut
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|a Saeidi, Farhad
|e verfasserin
|4 aut
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|a Rahighi, Javad
|e verfasserin
|4 aut
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|a Shokri, Babak
|e verfasserin
|4 aut
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|i Enthalten in
|t Journal of synchrotron radiation
|d 1994
|g 28(2021), Pt 4 vom: 01. Juli, Seite 1050-1058
|w (DE-627)NLM09824129X
|x 1600-5775
|7 nnas
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|g volume:28
|g year:2021
|g number:Pt 4
|g day:01
|g month:07
|g pages:1050-1058
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|u http://dx.doi.org/10.1107/S1600577521004318
|3 Volltext
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|a AR
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|d 28
|j 2021
|e Pt 4
|b 01
|c 07
|h 1050-1058
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