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机译:讨论了Au的光中子截面:激光康普顿散射γ射线的测量和最小二乘法的数据缩减
Department of Physics, Konan University, 8-9-1 Okamoto, Higashinada, Kobe 658-8501, Japan;
Department of Physics, Konan University, 8-9-1 Okamoto, Higashinada, Kobe 658-8501, Japan;
Department of Physics, Konan University, 8-9-1 Okamoto, Higashinada, Kobe 658-8501, Japan;
Department of Physics, Konan University, 8-9-1 Okamoto, Higashinada, Kobe 658-8501, Japan;
Department of Physics, Konan University, 8-9-1 Okamoto, Higashinada, Kobe 658-8501, Japan;
Department of Physics, Konan University, 8-9-1 Okamoto, Higashinada, Kobe 658-8501, Japan;
National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan;
Japan Atomic Energy Agency, Tokai-mura, Naka, Ibaraki 319-1195, Japan;
Japan Atomic Energy Agency, Tokai-mura, Naka, Ibaraki 319-1195, Japan;
Japan Atomic Energy Agency, Tokai-mura, Naka, Ibaraki 319-1195, Japan;
Institut fuer Strahlenphysik, Forschungszentrum Dresden-Rossendorf, D-01314 Dresden, Germany;
Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA;
(γ; n) cross sections; au; laser compton-scattering y-rays; direct neutron counting;
机译:用激光康普顿散射y射线和光子差分法测量〜(152)Sm(γ,n)截面
机译:59.536 keVγ射线的瑞利,康普顿和共振拉曼散射截面的测量
机译:59.536 keVγ射线的瑞利,康普顿和共振拉曼散射截面的测量
机译:2.5.3使用激光逆康普顿γ射线测量〜(94)Zr的光中子截面
机译:用于X射线自由电子激光器的电子束的相位空间操纵和逆符合Compton散射源
机译:在强束缚K壳电子的情况下理论和实验康普顿散射截面在1.12 MeV
机译:使用激光 - 康普顿散射γ射线测量80se(γ,n)横截面