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Division Spotlight
Radiation Protection & Shielding
The Radiation Protection and Shielding Division is developing and promoting radiation protection and shielding aspects of nuclear science and technology — including interaction of nuclear radiation with materials and biological systems, instruments and techniques for the measurement of nuclear radiation fields, and radiation shield design and evaluation.
Meeting Spotlight
Conference on Nuclear Training and Education: A Biennial International Forum (CONTE 2025)
February 3–6, 2025
Amelia Island, FL|Omni Amelia Island Resort
Standards Program
The Standards Committee is responsible for the development and maintenance of voluntary consensus standards that address the design, analysis, and operation of components, systems, and facilities related to the application of nuclear science and technology. Find out What’s New, check out the Standards Store, or Get Involved today!
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Latest News
US, Korea sign MOU for nuclear cooperation
The U.S. departments of Energy and State have signed a memorandum of understanding with the Republic of Korea’s ministries of Trade, Industry and Energy and of Foreign Affairs for the two nations to partner on nuclear exports and cooperation.
Liu Xiaobo, Peng Xianjue, Lei Jiarong, Fan Xiaoqiang, Du Jinfeng, Gao Hui
Nuclear Science and Engineering | Volume 181 | Number 1 | September 2015 | Pages 96-104
Technical Paper | doi.org/10.13182/NSE14-100
Articles are hosted by Taylor and Francis Online.
Based on a new experimental method implemented for validating neutron initiation probability, a set of burst initiation probability experiments (128 bursts) that were initiated by simultaneously injecting pulsed neutrons just as the reactor achieves the prompt supercritical state of 0.042 $ has been carried out at the CFBR-II (Chinese Fast Burst Reactor–II). The experimental configuration and procedures remained the same throughout the entire set of experiments. Based on the measured data, each burst was tallied by judging whether or not the burst was initiated by the pulsed neutrons. With the injection of pulsed neutrons (the equivalent strength of the neutrons is 1230), the tallies of the burst initiated by pulsed neutrons were 44, and hence, the experimental result of initiation probability is 0.344, which is 27% more than the theoretical calculation result of 0.271. Some factors that influence the experimental results are discussed. The discrepancy is attributed mainly to neutrons that are scattered and returned from the environment during the injection of pulsed neutrons and the statistical deviation.