Experiment of positron generation using a crystal target at the KEK electron/positron linac / M. Inoue, S. Takenaka, I. Endo [et al.]

Уровень набора: Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms, Scientific Journal = 1984-Альтернативный автор-лицо: Inoue, M.;Takenaka, S.;Endo, I.;Yoshida, K.;Takahashi, T.;Iinuma, M.;Bogdanov, A. V., physicist, Senior Lecturer of Tomsk Polytechnic University, 1974-, Aleksey Viktorovich;Кольчужкин, А. М., российский физик-ядерщик, профессор кафедры экспериментальной ядерной физики Томского политехнического университета, 1935-, Анатолий Михайлович;Potylitsyn, A. P., Russian physicist, Professor of the TPU, 1945-, Alexander Petrovich;Vnukov, I. E.;Okuno, H.;Anami, S.;Enomoto, A.;Furukawa, K.;Kamitani, T.;Ogawa, Y.;Ohsawa, S.Язык: английский.Страна: .Резюме или реферат: We have performed an experiment of positron generation using a crystal target at an electron/positron linac at KEK. The target consists of a tungsten crystal to emit photons and an amorphous tungsten for pair creation, whose thicknesses are 0.5 and 2.0 radiation length, respectively. When the ?1 1 1? crystal axis is oriented parallel to the 3 GeV incident electron beam, the positron yield is enhanced by 40% compared to values for the disoriented crystal. No effect of injecting intense ultra-short electron bunches on the crystalline structure is observed. The crystal orientation dependence of the positron yield as well as the enhancement factor can be explained by a simulation assuming a coherent bremsstrahlung process of the electron in the crystal..Аудитория: .Тематика: труды учёных ТПУ | электронный ресурс Ресурсы он-лайн:Щелкните здесь для доступа в онлайн
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We have performed an experiment of positron generation using a crystal target at an electron/positron linac at KEK. The target consists of a tungsten crystal to emit photons and an amorphous tungsten for pair creation, whose thicknesses are 0.5 and 2.0 radiation length, respectively. When the ?1 1 1? crystal axis is oriented parallel to the 3 GeV incident electron beam, the positron yield is enhanced by 40% compared to values for the disoriented crystal. No effect of injecting intense ultra-short electron bunches on the crystalline structure is observed. The crystal orientation dependence of the positron yield as well as the enhancement factor can be explained by a simulation assuming a coherent bremsstrahlung process of the electron in the crystal.

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