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作 者:F.A.Rasulova N.V.Aksenov S.I.Alekseev R.A.Aliev S.S.Belyshev I.Chuprakov N.Yu.Fursova A.S.Madumarov J.H.Khushvaktov A.A.Kuznetsov B.S.Yuldashev
机构地区:[1]Joint Institute for Nuclear Research,Dubna,Russia [2]Institute of Nuclear Physics of the Academy of Sciences of the Republic of Uzbekistan,Tashkent,Uzbekistan [3]Faculty of Chemistry of Lomonosov Moscow State University,Moscow,Russia [4]National Research Center"Kurchatov Institute",Moscow,Russia [5]Skobeltsyn Institute of Nuclear Physics of Lomonosov Moscow State University,Moscow,Russia [6]Faculty of Physics of Lomonosov Moscow State University,Moscow,Russia [7]Institute of Nuclear Physics,Almaty,Republic of Kazakhstan
出 处:《Chinese Physics C》2024年第2期91-103,共13页中国物理C(英文版)
摘 要:In this study,experiments were performed at bremsstrahlung end-point energies of 10-23 MeV with the beam from the MT-25 microtron using theγ-activation technique.The experimental values of relative yields were compared with theoretical results obtained on the basis of TALYS with the standard parameters and the combined model of photonucleon reactions.Including isospin splitting in the combined model of photonucleon reactions allows describing experimental data on reactions with proton escape in the energy range from 10 to 23 MeV.Therefore,taking into account isospin splitting is necessary for a correct description of the decay of the giant dipole resonance.
关 键 词:bremsstrahlung photon cross section isospin splitting giant dipole resonance
分 类 号:O571[理学—粒子物理与原子核物理]
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