Modeling the response of a planar silicon detector when measuring the exposure dose rate in the energy range from 5 keV to 10MeV

The main advantages of using silicon semiconductor detectors in dosimetry in comparison with traditional detectors are considered. The shortcomings are analyzed and possible methods for their elimination are proposed. One of the proposed methods makes it possible to increase the efficiency of detect...

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Збережено в:
Бібліографічні деталі
Дата:2020
Автори: Dubina, V.N., Maslov, N.I., Shlyahov, I.N.
Формат: Стаття
Мова:English
Опубліковано: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2020
Назва видання:Вопросы атомной науки и техники
Теми:
Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/194575
Теги: Додати тег
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Modeling the response of a planar silicon detector when measuring the exposure dose rate in the energy range from 5 keV to 10MeV / V.N. Dubina, N.I. Maslov, I.N. Shlyahov // Problems of atomic science and tecnology. — 2020. — № 5. — С. 105-110. — Бібліогр.: 9 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
Опис
Резюме:The main advantages of using silicon semiconductor detectors in dosimetry in comparison with traditional detectors are considered. The shortcomings are analyzed and possible methods for their elimination are proposed. One of the proposed methods makes it possible to increase the efficiency of detecting gamma quantum in the energy range 0.1…10MeV. The requirements are formulated to optimize the design of detectors operating in a wide range of dose rates and gamma radiation energies by computer simulation. Mathematical calculations and computer simulations determine the dosimeter design, materials and thicknesses γ–converter. The mechanisms of modeling the absorbed dose in air and ambient dose in silicon detectors with a thickness of 300 μm, sizes (5×5)mm² and (1.8×1.8)mm², in the range of incident γ–ray energies from 5keV to 10 MeV are presented.