Development of High Intensity D-T fusion NEutron Generator (HINEG)

A high intensity D-T fusion neutron generator (HINEG) is keenly needed for the research and development (R&D) of nuclear technology and safety of the advanced nuclear energy system, especially for the radiation protection and shielding. The R&D of HINEG includes two phases: HINEG-I and HINEG...

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Main Authors: Wu Yican, Liu Chao, Song Gang, Wang Yongfeng, Li Taosheng, Jiang Jieqiong, Song Yong, Ji Xiang
Format: Article
Language:English
Published: EDP Sciences 2017-01-01
Series:EPJ Web of Conferences
Subjects:
Online Access:https://doi.org/10.1051/epjconf/201715303006
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spelling doaj-1a517573728b4463bb8e79fa098110622021-08-02T10:20:27ZengEDP SciencesEPJ Web of Conferences2100-014X2017-01-011530300610.1051/epjconf/201715303006epjconf_icrs2017_03006Development of High Intensity D-T fusion NEutron Generator (HINEG)Wu YicanLiu ChaoSong GangWang YongfengLi TaoshengJiang JieqiongSong YongJi XiangA high intensity D-T fusion neutron generator (HINEG) is keenly needed for the research and development (R&D) of nuclear technology and safety of the advanced nuclear energy system, especially for the radiation protection and shielding. The R&D of HINEG includes two phases: HINEG-I and HINEG-II. HINEG-I is designed to have both the steady beam and pulsed beam. The neutron yield of the steady beam is up to 1012 n/s. The width of pulse neutron beam is less than 1.5 ns. HINEG-I is used for the basic neutronics study, such as measurement of nuclear data, validation of neutronics methods and software, validation of radiation protection and so on. HINEG-II aims to generate a high neutron yield of 1013 n/s neutrons by adopting high speed rotating tritium target system integrated with jet/spray array enhanced cooling techniques, and can further upgrade to obtain neutron yield of 1014~1015n/s by using of accelerators-array in a later stage. HINEG-II can be used for fundamentals research of nuclear technology including mechanism of materials radiation damage and neutronics performance of components, radiation shielding as well as other nuclear technology applications.https://doi.org/10.1051/epjconf/201715303006FusionAccelerator Based Neutrons SourceHigh IntesityRadiation Shielding
collection DOAJ
language English
format Article
sources DOAJ
author Wu Yican
Liu Chao
Song Gang
Wang Yongfeng
Li Taosheng
Jiang Jieqiong
Song Yong
Ji Xiang
spellingShingle Wu Yican
Liu Chao
Song Gang
Wang Yongfeng
Li Taosheng
Jiang Jieqiong
Song Yong
Ji Xiang
Development of High Intensity D-T fusion NEutron Generator (HINEG)
EPJ Web of Conferences
Fusion
Accelerator Based Neutrons Source
High Intesity
Radiation Shielding
author_facet Wu Yican
Liu Chao
Song Gang
Wang Yongfeng
Li Taosheng
Jiang Jieqiong
Song Yong
Ji Xiang
author_sort Wu Yican
title Development of High Intensity D-T fusion NEutron Generator (HINEG)
title_short Development of High Intensity D-T fusion NEutron Generator (HINEG)
title_full Development of High Intensity D-T fusion NEutron Generator (HINEG)
title_fullStr Development of High Intensity D-T fusion NEutron Generator (HINEG)
title_full_unstemmed Development of High Intensity D-T fusion NEutron Generator (HINEG)
title_sort development of high intensity d-t fusion neutron generator (hineg)
publisher EDP Sciences
series EPJ Web of Conferences
issn 2100-014X
publishDate 2017-01-01
description A high intensity D-T fusion neutron generator (HINEG) is keenly needed for the research and development (R&D) of nuclear technology and safety of the advanced nuclear energy system, especially for the radiation protection and shielding. The R&D of HINEG includes two phases: HINEG-I and HINEG-II. HINEG-I is designed to have both the steady beam and pulsed beam. The neutron yield of the steady beam is up to 1012 n/s. The width of pulse neutron beam is less than 1.5 ns. HINEG-I is used for the basic neutronics study, such as measurement of nuclear data, validation of neutronics methods and software, validation of radiation protection and so on. HINEG-II aims to generate a high neutron yield of 1013 n/s neutrons by adopting high speed rotating tritium target system integrated with jet/spray array enhanced cooling techniques, and can further upgrade to obtain neutron yield of 1014~1015n/s by using of accelerators-array in a later stage. HINEG-II can be used for fundamentals research of nuclear technology including mechanism of materials radiation damage and neutronics performance of components, radiation shielding as well as other nuclear technology applications.
topic Fusion
Accelerator Based Neutrons Source
High Intesity
Radiation Shielding
url https://doi.org/10.1051/epjconf/201715303006
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