Parametric x-ray radiation from 500-MeV electrons in a tungsten single crystal with a surface mosaicity less than 1.5′ / Yu. N. Adischev [et al.]

Уровень набора: Physics of Atomic Nuclei = 1965-Альтернативный автор-лицо: Adischev, Yu. N.;Vnukov, I. E.;Zabaev, V. N., physicist, associate professor of Tomsk Polytechnic University, 1946-, Viktor Nikolaevich;Kalinin, В. N.;Kiryakov, А. А.;Kunashenko, Yu. P., physicist, professor of Tomsk Polytechnic University, 1958-, Yuriy Petrovich;Pivovarov, Yu. L., physicist, professor of Tomsk Polytechnic University, 1953-, Yuriy Leonidovich;Potylitsyn, A. P., Russian physicist, Professor of the TPU, 1945-, Alexander Petrovich;Uglov, S. R., physicist, senior research fellow at Tomsk Polytechnic University, 1958-, Sergey RomanovichЯзык: английский.Страна: Россия.Резюме или реферат: The yield of parametric x-ray radiation from a tungsten single crystal irradiated with a E=500 MeV electron beam from the Tomsk Sirius synchrotron was studied experimentally in Bragg geometry. The tungsten sample was 1.7 mm thick and had a surface mosaicity less than 1.5′; it was oriented in such a way that the (111) face was at the Bragg angle of θ B=45° with respect to the electron-beam direction. The x-ray photons were detected at the angle of 2θ B=90° with respect to the electron beam. The angular distributions of parametric x rays are compared with those calculatedwith allowance for actual experimental conditions..Примечания о наличии в документе библиографии/указателя: [References: p. 955 (5 tit.)].Аудитория: .Тематика: труды учёных ТПУ | электронный ресурс Ресурсы он-лайн:Щелкните здесь для доступа в онлайн
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XXX International Conference On The Physics Of Interaction Of Fast Charged Particles With Matter

[References: p. 955 (5 tit.)]

The yield of parametric x-ray radiation from a tungsten single crystal irradiated with a E=500 MeV electron beam from the Tomsk Sirius synchrotron was studied experimentally in Bragg geometry. The tungsten sample was 1.7 mm thick and had a surface mosaicity less than 1.5′; it was oriented in such a way that the (111) face was at the Bragg angle of θ B=45° with respect to the electron-beam direction. The x-ray photons were detected at the angle of 2θ B=90° with respect to the electron beam. The angular distributions of parametric x rays are compared with those calculatedwith allowance for actual experimental conditions.

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