Emission brightness, photon yield, and radiation losses of ultrarelativistic electrons in oriented thick crystals

Bibliographische Detailangaben
Parent link:Russian Physics Journal
Vol. 34, iss. 6.— 1991.— [P. 479-489]
Weitere Verfasser: Amosov K. Yu., Vnukov I. E., Kalinin B. N., Naumenko G. A. Gennadiy Andreevich, Potylitsyn A. P. Alexander Petrovich, Sarychev V. P.
Zusammenfassung:Title screen
The brightness ΔErad/ΔΩ of γ-radiation produced in oriented single crystals and amorphous targets of various thicknesses by electrons with E0=900 MeV has been measured experimentally. Comparison with theoretical calculations reveals that the radiation channeled in the axial direction in diamond has the maximum brightness. The measured angular distributions and spectral composition of the radiation have been used to determine the photon yield in the cone with angle ⊖c=0.6 mrad and it is shown that diamond has no competitors in this respect. It is concluded that the use of targets made of single crystals with Z as small as possible (diamond and beryllium) is preferable.
Режим доступа: по договору с организацией-держателем ресурса
Sprache:Englisch
Veröffentlicht: 1991
Schlagworte:
Online-Zugang:http://dx.doi.org/10.1007/BF00895879
Format: Elektronisch Buchkapitel
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=647219

MARC

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200 1 |a Emission brightness, photon yield, and radiation losses of ultrarelativistic electrons in oriented thick crystals  |f K. Yu. Amosov [еt al.] 
203 |a Text  |c electronic 
300 |a Title screen 
320 |a [References: p. 489 (15 tit.)] 
330 |a The brightness ΔErad/ΔΩ of γ-radiation produced in oriented single crystals and amorphous targets of various thicknesses by electrons with E0=900 MeV has been measured experimentally. Comparison with theoretical calculations reveals that the radiation channeled in the axial direction in diamond has the maximum brightness. The measured angular distributions and spectral composition of the radiation have been used to determine the photon yield in the cone with angle ⊖c=0.6 mrad and it is shown that diamond has no competitors in this respect. It is concluded that the use of targets made of single crystals with Z as small as possible (diamond and beryllium) is preferable. 
333 |a Режим доступа: по договору с организацией-держателем ресурса 
461 |t Russian Physics Journal 
463 |t Vol. 34, iss. 6  |v [P. 479-489]  |d 1991 
610 1 |a электронный ресурс 
610 1 |a труды учёных ТПУ 
610 1 |a electrons 
610 1 |a radiation 
610 1 |a crystals 
701 1 |a Amosov  |b K. Yu. 
701 1 |a Vnukov  |b I. E. 
701 1 |a Kalinin  |b B. N. 
701 1 |a Naumenko  |b G. A.  |c physicist  |c senior research fellow, Professor of Tomsk Polytechnic University, Candidate of physical and mathematical sciences  |f 1947-  |g Gennadiy Andreevich  |3 (RuTPU)RU\TPU\pers\31524  |9 15685 
701 1 |a Potylitsyn  |b A. P.  |c Russian physicist  |c Professor of the TPU  |f 1945-  |g Alexander Petrovich  |3 (RuTPU)RU\TPU\pers\26306  |9 12068 
701 1 |a Sarychev  |b V. P. 
801 2 |a RU  |b 63413507  |c 20160329  |g RCR 
856 4 0 |u http://dx.doi.org/10.1007/BF00895879 
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