Smith-Purcell effect as resonant diffraction radiation

Podrobná bibliografie
Parent link:Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms.— , 1998
Vol. 145, Iss. 1-2.— 1998.— P. 60-66
Hlavní autor: Potylitsyn A. P. Alexander Petrovich
Shrnutí:The radiation of ultrarelativistic charged particle passing near a grating (Smith-Purcell radiation (SPR)) has been considered on the basis of a simple physical model, where SPR is treated as the resonant diffraction radiation (RDR). The apparent analogy between RDR and a well known resonant transition radiation has been used. The results have been compared with those obtained via other approaches. For an ultrarelativistic case it has been shown that the SPR intensity for a grating designed from strips separated by vacuum gaps sufficiently exceeds the one for traditional grating made up by a periodically deformed continuous surface.
В фонде НТБ ТПУ отсутствует
Jazyk:angličtina
Vydáno: 1998
Témata:
Médium: Kapitola
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=595873

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200 1 |a Smith-Purcell effect as resonant diffraction radiation  |f A. P. Potylitsyn 
330 |a The radiation of ultrarelativistic charged particle passing near a grating (Smith-Purcell radiation (SPR)) has been considered on the basis of a simple physical model, where SPR is treated as the resonant diffraction radiation (RDR). The apparent analogy between RDR and a well known resonant transition radiation has been used. The results have been compared with those obtained via other approaches. For an ultrarelativistic case it has been shown that the SPR intensity for a grating designed from strips separated by vacuum gaps sufficiently exceeds the one for traditional grating made up by a periodically deformed continuous surface. 
333 |a В фонде НТБ ТПУ отсутствует 
461 |t Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms  |d 1998 
463 |t Vol. 145, Iss. 1-2  |v P. 60-66  |d 1998 
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