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E_p≤200 MeV能区p+^(58)Ni反应的计算与分析 被引量:1
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作者 梁春恬 蔡崇海 《原子能科学技术》 EI CAS CSCD 北大核心 2007年第1期1-10,共10页
以现有质子诱发58Ni的各种核反应截面、能谱、双微分截面、弹性散射角分布等实验数据为基础,利用自行研制的大型核模型计算程序MEND计算质子能量在200 MeV能区内58Ni(p,x)反应的截面、能谱、角分布和n、p、α、dt、3、He 6种出射轻粒子... 以现有质子诱发58Ni的各种核反应截面、能谱、双微分截面、弹性散射角分布等实验数据为基础,利用自行研制的大型核模型计算程序MEND计算质子能量在200 MeV能区内58Ni(p,x)反应的截面、能谱、角分布和n、p、α、dt、3、He 6种出射轻粒子的双微分截面。MEND程序的理论框架基于球形光学模型、核子的核内级联发射模型、以激子模型为基础的预平衡发射理论、蒸发模型和带宽度涨落修正的Hauser-Feshbach统计理论。光学模型中的势参数由APMN程序通过符合p+58Ni反应的去弹截面和弹性散射角分布获得。出射粒子的双微分截面则利用MEND程序输出的能谱再通过Kalbach系统学公式计算。将计算结果与实验数据及ENDF/B6评价库进行了比较,计算结果与实验数据基本一致,与ENDF/B6相比,增加了3He的计算,且将能区上推至200 MeV。 展开更多
关键词 ^^58Ni靶核 质子诱发反应 截面 能谱 双微分截面
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压水堆核电站氧化停堆过程一回路冷却剂中^(58)Co活度浓度分析 被引量:3
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作者 张丽莹 邢继 毛亚蔚 《辐射防护》 CAS CSCD 北大核心 2016年第4期206-210,共5页
压水堆核电站氧化停堆过程中,一回路冷却剂中^(58)Co的停堆释放峰值可达上百个GBq/t,对工作人员的职业照射剂量及停堆进程都有很大影响。本文介绍了压水堆核电站氧化停堆过程,分析了对^(58)Co活度浓度变化有显著影响的因素,如一回路水... 压水堆核电站氧化停堆过程中,一回路冷却剂中^(58)Co的停堆释放峰值可达上百个GBq/t,对工作人员的职业照射剂量及停堆进程都有很大影响。本文介绍了压水堆核电站氧化停堆过程,分析了对^(58)Co活度浓度变化有显著影响的因素,如一回路水化学、蒸汽发生器传热管材料、循环中停堆、化学和容积控制系统的净化等,同时提出了相关建议。 展开更多
关键词 氧化停堆 一回路冷却剂 58co峰值 水化学
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^(58)Ni(p,γ)^(59)Cu反应的天体热核反应率
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作者 刘绍湘 刘兆远 +3 位作者 马树勋 蔡晓红 柳纪虎 冯嘉祯 《兰州大学学报(自然科学版)》 CAS CSCD 北大核心 1991年第1期35-40,共6页
用能量为1.2MeV—3.4MeV的质子轰击纯镍厚靶,测得了~958)Ni(p,γ)^(59)Cu反应的产额,给出了测量方法.由测得的产额计算出爆发式核素合成时相应温度下的天体热核反应率,所得结果与理论预期值及他人实验结果作了比较.并对结果作了讨论.
关键词 天体 热核反应率 ^^58Ni ^^59Cu 厚靶
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Comprehensive analysis of uncertainty quantification for the^(58)Ni(n,p)^(58)Co reaction cross section
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作者 Mahesh Choudhary Aman Sharma +15 位作者 Namrata Singh Mahima Upadhyay Punit Dubey A.Gandhi Akash Hingu G Mishra Sukanya De L.S.Danu Ajay Kumar R.G.Thomas Saurav Sood Sajin Prasad S.Mukherjee I.N.Ruskov Yu.N.Kopatch A.Kumar 《Chinese Physics C》 SCIE CAS CSCD 2024年第9期170-175,共6页
In this study,we measured the^(58)Ni(n,p)^(58)Co reaction cross section with neutron energies of 1.06,1.86,and 2.85 MeV.The cross section was measured using neutron activation techniques andγ-ray spectroscopy,and it ... In this study,we measured the^(58)Ni(n,p)^(58)Co reaction cross section with neutron energies of 1.06,1.86,and 2.85 MeV.The cross section was measured using neutron activation techniques andγ-ray spectroscopy,and it was compared with cross section data available in the EXFOR.Furthermore,we calculated the covariance matrix of the measured cross section for the aforementioned nuclear reaction.The uncertainties of the theoretical calculation for^(58)Ni(n,p)^(58)Co reaction cross section were calculated via Monte Carlo method.In this study,we used uncertainties in the optical model and level density parameters to calculate uncertainties in the theoretical cross sections.The theoretical calculations were performed by using TALYS-1.96.In this study,we aim to analyze the effect of uncertainties of the nuclear model input as well as different experimental variables used to obtain the values of reaction cross section. 展开更多
关键词 ^^(58)Ni(n ^p)^(58)Co reaction γ-ray spectroscopy uncertainty quantification of cross section covariance analysis
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STUDY ON THE SEQUENCE STRUCTURE OF SBR BY ^(13)C—NMR METHOD Ⅰ. ASSIGNMENT FOR UNSATURAT CARBONS SPECTRA
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作者 焦书科 陈晓农 +1 位作者 胡力平 严宝珍 《Chinese Journal of Polymer Science》 SCIE CAS CSCD 1990年第1期17-24,共8页
The sequence structures of emulsion-processed SBR and solution-processed (by lithium catalyst) SBR were investigated by ^(13)C-NMR spectroscopy. Seventeen peaks within unsaturated carbon region were recorded under the... The sequence structures of emulsion-processed SBR and solution-processed (by lithium catalyst) SBR were investigated by ^(13)C-NMR spectroscopy. Seventeen peaks within unsaturated carbon region were recorded under the adopted experimental conditions. Assignments for these peaks were made by empirical-parameter-evaluation method. 展开更多
关键词 Sequence distribution ^^(13)C-NMR spectra of SBR peak assignment for olefinic car- bon atoms.
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中能中子与^(58)Ni反应的理论计算
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作者 黄小龙 《高能物理与核物理》 EI CSCD 北大核心 2006年第4期306-309,共4页
在中子与58Ni反应的总截面、去弹性散射截面和弹性散射角分布的实验数据基础上,获得了入射中子能量从0.825-150MeV的一组普适的中子与58Ni反应的光学模型势参数.利用光学模型、宽度涨落修正的Hauser-Feshbach理论、预平衡反应的激子... 在中子与58Ni反应的总截面、去弹性散射截面和弹性散射角分布的实验数据基础上,获得了入射中子能量从0.825-150MeV的一组普适的中子与58Ni反应的光学模型势参数.利用光学模型、宽度涨落修正的Hauser-Feshbach理论、预平衡反应的激子模型和核内级联模型的中能核反应计算程序 MEND,计算了中子与58Ni反应的所有截面、角分布和能谱,并将理论计算结果与实验数据和评价数据进行了分析比较. 展开更多
关键词 光学模型 中能核反应 MEND ^^58Ni
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Cross-section measurements for the^(58,60,61)Ni(n,α)^(55,57,58)Fe reactions at 8.50,9.50 and 10.50 MeV neutron energies
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作者 Haoyu Jiang Zengqi Cui +13 位作者 Yiwei Hu Jie Liu Haofan Bai Jinxiang Chen Guohui Zhang Yu.M.Gledenov E.Sansarbayar G.Khuukhenkhuu L.Krupa I.Chuprakov Xichao Ruan Hanxiong Huang Jie Ren Qiwen Fan 《Chinese Physics C》 SCIE CAS CSCD 2022年第2期70-78,共9页
Cross sections of the^(58,60,61)Ni(n,α)^(55,57,58)Fe reactions were measured at 8.50,9.50 and 10.50 MeV neutron energies based on the HI-13 tandem accelerator of China Institute of Atomic Energy(CIAE)with enriched^(5... Cross sections of the^(58,60,61)Ni(n,α)^(55,57,58)Fe reactions were measured at 8.50,9.50 and 10.50 MeV neutron energies based on the HI-13 tandem accelerator of China Institute of Atomic Energy(CIAE)with enriched^(58)Ni,^(60)Ni,and^(61)Ni foil samples with backings.A twin gridded ionization chamber(GIC)was used as the charged particle detector,and an EJ-309 liquid scintillator was used to obtain the neutron energy spectra.The relative and absolute neutron fluxes were determined via three highly enriched^(238)U_(3)O_(8)samples inside the GIC.The uncertainty of the present data of the^(58)Ni(n,α)^(55)Fe reaction is smaller than most existing measurements.The present data of^(60)Ni(n,α)^(57)Fe and^(61)Ni(n,α)^(58)Fe reactions are the first measurement results above 8 MeV.The present experimental data could be reasonably reproduced by calculations with TALYS-1.9 by adjusting several default values of theoretical model parameters. 展开更多
关键词 cross-section measurements ^^(58 60 61)Ni(n ^α)^(55 57 58) GIC CIAE
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A study of the strong pulses detected from PSR B0656+14 using the Urumqi 25-m radio telescope at 1540 MHz 被引量:2
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作者 Guo-Cun Tao Ali Esamdin +3 位作者 Hui-Dong Hu Mao-Fei Qian Jing Li Na Wang 《Research in Astronomy and Astrophysics》 SCIE CAS CSCD 2012年第12期1649-1654,共6页
We report on the properties of strong pulses from PSR B0656+14 by analyzing the data obtained using the Urumqi 25-m radio telescope at 1540 MHz from August 2007 to September 2010.In 44 h of observational data,a total... We report on the properties of strong pulses from PSR B0656+14 by analyzing the data obtained using the Urumqi 25-m radio telescope at 1540 MHz from August 2007 to September 2010.In 44 h of observational data,a total of 67 pulses with signal-to-noise ratios above a 5σthreshold were detected.The peak flux densities of these pulses are 58 to 194 times that of the average profile,and their pulse energies are 3 to 68 times that of the average pulse.These pulses are clustered around phases about 5-ahead of the peak of the average profile.Compared with the width of the average profile,they are relatively narrow,with the full widths at half-maximum ranging from 0.28 ° to 1.78 °.The distribution of pulse-energies follows a lognormal distribution.These sporadic strong pulses detected from PSR B0656+14 have different characteristics from both typical giant pulses and its regular pulses. 展开更多
关键词 stars:neutron-pulsars-pulsars:individual(B0656+14)Options: Encrypt Page Allow Cookies Remove Scripts Remove Objects 收藏本站首页期刊全文库学位论文库会议论文库学术百科吾喜杂志工具书优先出版注册|登录|我的账户基础科学|工程科技I辑|工程科技II辑|医药卫生科技|信息科技|农业科技|哲学与人文科学|社会科学I辑|社会科学II辑|经济管理高级搜索: 用" stars neutron-pulsars—pulsars "到知网平台检索 点击这里搜索更多...《Research in Astronomy and Astrophysics》 2012年12期 加入收藏 获取最新 A study of the strong pulses detected from PSR B0656+14 using the Urumqi 25-m radio telescope at 1540 MHzAli Esamdin 【摘要】: We report on the properties of strong pulses from PSR B0656+14 by analyzing the data obtained using the Urumqi 25-m radio telescope at 1540 MHz from August 2007 to September 2010.In 44 h of observational data a total of 67 pulses with signal-to-noise ratios above a 5σthreshold were detected.The peak flux densities of these pulses are 58 to 194 times that of the average profile and their pulse energies are 3 to 68 times that of the average pulse.These pulses are clustered around phases about 5-ahead of the peak of the average profile.Compared with the width of the average profile they are relatively narrow with the full widths at half-maximum ranging from 0.28 ° to 1.78 °.The distribution of pulse-energies follows a lognormal distribution.These sporadic strong pulses detected from PSR B0656+14 have different characteristics from both typical giant pulses and its regular pulses.【作者单位】 Xinjiang
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Interaction of Hsp40 with influenza virus M2 protein: implications for PKR signaling pathway 被引量:13
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作者 Zhenhong Guan Di Liu +5 位作者 Shuofu Mi Jie Zhang Qinong Ye Ming Wang George F.Gao Jinghua Yan 《Protein & Cell》 SCIE CSCD 2010年第10期944-955,共12页
Influenza virus contains three integral membrane proteins:haemagglutinin,neuraminidase,and matrix protein(M1 and M2).Among them,M2 protein functions as an ion channel,important for virus uncoating in endosomes of viru... Influenza virus contains three integral membrane proteins:haemagglutinin,neuraminidase,and matrix protein(M1 and M2).Among them,M2 protein functions as an ion channel,important for virus uncoating in endosomes of virus-infected cells and essential for virus replication.In an effort to explore potential new functions of M2 in the virus life cycle,we used yeast two-hybrid system to search for M2-associated cellular proteins.One of the positive clones was identified as human Hsp40/Hdj1,a DnaJ/Hsp40 family protein.Here,we report that both BM2(M2 of influenza B virus)and A/M2(M2 of influenza A virus)interacted with Hsp40 in vitro and in vivo.The region of M2-Hsp40 interaction has been mapped to the CTD1 domain of Hsp40.Hsp40 has been reported to be a regulator of PKR signaling pathway by interacting with p58^(IPK) that is a cellular inhibitor of PKR.PKR is a crucial component of the host defense response against virus infection.We therefore attempted to understand the relationship among M2,Hsp40 and p58^(IPK) by further experimentation.The results demonstrated that both A/M2 and BM2 are able to bind to p58^(IPK)in vitro and in vivo and enhance PKR autophosphorylation probably via forming a stable complex with Hsp40 and P58^(IPK),and consequently induce cell death.These results suggest that influenza virus M2 protein is involved in p58^(IPK)mediated PKR regulation during influenza virus infection,therefore affecting infected-cell life cycle and virus replication. 展开更多
关键词 M2 protein of influenza virus Hsp40 ^P58^(IPK) protein interaction PKR signal pathway
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