A Passive Shield for the RED-100 Neutrino Detector / D. Yu. Akimov, I. S. Aleksandrov, V. A. Belov [et al.]

Уровень набора: Instruments and Experimental TechniquesАльтернативный автор-лицо: Akimov, D. Yu., Dmitry Yurjevich;Aleksandrov, I. S., Physicist, Junior Researcher of Tomsk Polytechnic University, Candidate of physical and mathematical sciences, 1986-, Ivan Sergeevich;Belov, V. A., Vladimir Aleksandrovich;Efremenko, Yu. V., Yury Valentinovich;Etenko, A. V., Aleksandr VladimirovichКоллективный автор (вторичный): Национальный исследовательский Томский политехнический университет, Физико-технический институт, Кафедра прикладной физики (№ 12), Международная научно-образовательная лаборатория "Рентгеновская оптика"Язык: английский.Страна: .Резюме или реферат: A combined passive shield of the RED-100 two-phase emission neutrino detector has been developed and built for suppressing the background of external γ rays and neutrons. The shield is composed of a 5-cm-thick copper layer (the inner layer is adjacent to the detector) and a water layer with a total thickness of approximately 70 cm (including the water inside the copper shield). The Monte Carlo simulation of the shielding efficiency has been performed. The obtained attenuation factor of the copper shield for the γ-ray background has been experimentally verified in a laboratory test using a NaI(Tl) scintillator detector. The γ-ray background rejection factor of the full shield has also been calculated..Примечания о наличии в документе библиографии/указателя: [References: 28 tit.].Аудитория: .Тематика: электронный ресурс | труды учёных ТПУ Ресурсы он-лайн:Щелкните здесь для доступа в онлайн
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[References: 28 tit.]

A combined passive shield of the RED-100 two-phase emission neutrino detector has been developed and built for suppressing the background of external γ rays and neutrons. The shield is composed of a 5-cm-thick copper layer (the inner layer is adjacent to the detector) and a water layer with a total thickness of approximately 70 cm (including the water inside the copper shield). The Monte Carlo simulation of the shielding efficiency has been performed. The obtained attenuation factor of the copper shield for the γ-ray background has been experimentally verified in a laboratory test using a NaI(Tl) scintillator detector. The γ-ray background rejection factor of the full shield has also been calculated.

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