机译:测量〜(235)u和〜(238)U的累积光散产率和16mev Bremsstrahlung光子束
CEA DES IRESNE DTN SMTA Nuclear Measurement Laboratory F-13108 St Paul-lez-Durance France;
CEA DES IRESNE DTN SMTA Nuclear Measurement Laboratory F-13108 St Paul-lez-Durance France;
CEA DES IRESNE DTN SMTA Nuclear Measurement Laboratory F-13108 St Paul-lez-Durance France;
CEA DES IRESNE DTN SMTA Nuclear Measurement Laboratory F-13108 St Paul-lez-Durance France;
CEA DES IRESNE DTN SMTA Nuclear Measurement Laboratory F-13108 St Paul-lez-Durance France;
CEA DES IRESNE DTN SMTA Nuclear Measurement Laboratory F-13108 St Paul-lez-Durance France;
CEA DES IRESNE DTN SMTA Nuclear Measurement Laboratory F-13108 St Paul-lez-Durance France;
CEA DES IRESNE DTN SMTA Nuclear Measurement Laboratory F-13108 St Paul-lez-Durance France;
Unlversitie Paris-Saclay CEA UST F-91120 Palaiseau France;
Universite Grenoble Alpes CNRS Grenoble INP LPSC-IN2P3 38000 Grenoble France;
Photofission; Uranium; Delayed gamma rays; Bremsstrahlung; Fission yield; Photon activation analysis; MCNP;
机译:〜(235)U和〜(237)Np的光致裂变光子低于20 MeV的光致裂变:中子屈服量和时间谱的测量
机译:来自$ ^ {235} {rm U} $和$ ^ {239} {rm Pu} $的热裂变以及来自$ ^ {235} {rm U} $和$ ^ {的光裂变的累积产量的新实验结果238} {rm U} $由Bremsstrahlung诱发
机译:使用能量范围为9.0-16.6 MeV的单能光子测量〜(235)U /〜(238)U的光裂变截面比
机译:延迟中子和延迟的光电特征来自〜(232)Th,〜(235'238)U,〜(237)NP,巨型偶极子谐振区域中的终点Bremsstrahlung光子。
机译:裂变产物产生的能量依赖于0.5 MeV和14.8 MeV之间的入射中子能从235 U,238U和239Pu
机译:多收集器电感耦合等离子体质谱法对铀进行化学分离和土壤样品中234U / 238U和235U / 238U比的精确测量
机译:使用单元光子在9.0-16.6 meV的能量范围内的光缺口横截面比率测量235U / 238U