2D Bragg high power microwave source driven by an annular electron beam

The first successful cold microwave measurements of a 2D Bragg coaxial mirror were discussed. An important difference between 1D and 2D Bragg structures was demonstrated concerning the dependence of their reflection coefficient on the parameter αlz, where α denotes wave coupling coefficient and lz r...

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Egile Nagusiak: Konoplev, I, Cross, A, He, W, Ginzburg, N, Peskov, N, Phelps, A, Robb, G, Ronald, K, Sergeev, A, Whyte, C
Formatua: Journal article
Hizkuntza:English
Argitaratua: 2000
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author Konoplev, I
Cross, A
He, W
Ginzburg, N
Peskov, N
Phelps, A
Robb, G
Ronald, K
Sergeev, A
Whyte, C
author_facet Konoplev, I
Cross, A
He, W
Ginzburg, N
Peskov, N
Phelps, A
Robb, G
Ronald, K
Sergeev, A
Whyte, C
author_sort Konoplev, I
collection OXFORD
description The first successful cold microwave measurements of a 2D Bragg coaxial mirror were discussed. An important difference between 1D and 2D Bragg structures was demonstrated concerning the dependence of their reflection coefficient on the parameter αlz, where α denotes wave coupling coefficient and lz represents length. The minimum of the transmission was found to be the same for the 2D structures. The possibility of achieving single mode operation was also demonstrated for the Free Electron Masers (FEM) when driven by an oversized electron beam with D/λ∼25, where D denotes diameter of the microwave system used and λ stands for wavelength of radiation.
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spelling oxford-uuid:0a155d93-dffc-4877-89a2-298c9eb0b96a2022-03-26T09:21:50Z2D Bragg high power microwave source driven by an annular electron beamJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:0a155d93-dffc-4877-89a2-298c9eb0b96aEnglishSymplectic Elements at Oxford2000Konoplev, ICross, AHe, WGinzburg, NPeskov, NPhelps, ARobb, GRonald, KSergeev, AWhyte, CThe first successful cold microwave measurements of a 2D Bragg coaxial mirror were discussed. An important difference between 1D and 2D Bragg structures was demonstrated concerning the dependence of their reflection coefficient on the parameter αlz, where α denotes wave coupling coefficient and lz represents length. The minimum of the transmission was found to be the same for the 2D structures. The possibility of achieving single mode operation was also demonstrated for the Free Electron Masers (FEM) when driven by an oversized electron beam with D/λ∼25, where D denotes diameter of the microwave system used and λ stands for wavelength of radiation.
spellingShingle Konoplev, I
Cross, A
He, W
Ginzburg, N
Peskov, N
Phelps, A
Robb, G
Ronald, K
Sergeev, A
Whyte, C
2D Bragg high power microwave source driven by an annular electron beam
title 2D Bragg high power microwave source driven by an annular electron beam
title_full 2D Bragg high power microwave source driven by an annular electron beam
title_fullStr 2D Bragg high power microwave source driven by an annular electron beam
title_full_unstemmed 2D Bragg high power microwave source driven by an annular electron beam
title_short 2D Bragg high power microwave source driven by an annular electron beam
title_sort 2d bragg high power microwave source driven by an annular electron beam
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