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Further investigation on the fusion of ^(6)Li with ^(209)Bi target at near-barrier energies

作     者:张高龙 焦振威 张广鑫 M.R.Cortes 胡世鹏 钱建强 D.Mengoni 屈卫卫 李聪博 郑云 张焕乔 孙慧斌 王楠 张春雷 J.J.Valiente-Dobón D.Testov M.Mazzocco A.Gozzelino C.Parascandolo D.Pierroutsakou M.La Commara A.Goasduff D.Bazzacco D.R.Napoli F.Galtarossa F.Recchia A.Illana S.Bakes I.Zanon S.Aydin G.de Angelis M.Siciliano R.Menegazzo S.M.Lenzi J.L.Ferreira J.Rangel Serkan Akkoyun L.F.Canto J.Lubian G.L.Zhang;Z.W.Jiao;G.X.Zhang;M.R.Cortes;S.P.Hu;J.Q.Qian;D.Mengoni;W.W.Qu;C.B.Li;Y.Zheng;H.Q.Zhang;H.B.Sun;N.Wang;C.L.Zhang;J.J.Valiente-Dobón;D.Testov;M.Mazzocco;A.Gozzelino;C.Parascandolo;D.Pierroutsakou;M.La Commara;A.Goasduff;D.Bazzacco;D.R.Napoli;F.Galtarossa;F.Recchia;A.Illana;S.Bakes;I.Zanon;S.Aydin;G.de Angelis;M.Siciliano;R.Menegazzo;S.M.Lenzi;J.L.Ferreira;J.Rangel;Serkan Akkoyun;L.F.Canto;J.Lubian

作者机构:School of PhysicsBeihang UniversityBeijing 100191China Sino-French Institute of Nuclear Engineering and TechnologySun Yat-Sen UniversityZhuhai 519082China Instituto de FísicaUniversidade Federal Fluminense24210-340NiteróiRio de JaneiroBrazil Institute for Advanced Study in Nuclear Energy&SafetyShenzhen UniversityShenzhen 518060China Shenzhen Key Laboratory of Research and Manufacture of High Purity Germanium Materials and FetectorsShenzhen UniversityShenzhen 518060China INFNSezione di PadovaPadovaItaly Dipartimento di fisica Astronomia dell'Universita di padovaPadovaItaly State Key Laboratory of Radiation Medicine and ProtectionSchool of Radiation Medicine and ProtectionSoochow UniversitySuzhou 215123China China Institute of Atomic EnergyBeijing 102413China The Key Laboratory of Beam Technology and Material Modification of Ministry of EducationCollege of Nuclear Science and TechnologyBeijing Normal UniversityBeijing 100875China INFNLaboratori Nazionali di LegnaroI-35020 LegnaroItaly INFNSezione di NapoliI-80126 NapoliItaly Dipartimento di FarmaciaUniversitàdi Napoli"Federico II"I-80131 NapoliItaly Department of Natural and Mathematical SciencesFaculty of EngineeringTarsus University33480 MersinTurkiye Physics DivisionArgonne National LaboratoryLemont-ILUSA Departamento de MatemaéticaFísica e Computaç˜ao Universidade do Estado do Rio de JaneiroFaculdade de Tecnologia27537-000ResendeRio de JaneiroBrazil Department of PhysicsSivas Cumhuriyet UniversitySivasTurkey Instituto de FísicaUniversidade Federal do Rio de JaneiroCP 6852821941-972Rio de JaneiroBrazil 

出 版 物:《Chinese Physics C》 (中国物理C(英文版))

年 卷 期:2024年第48卷第7期

页      面:106-117页

核心收录:

学科分类:07[理学] 070202[理学-粒子物理与原子核物理] 0702[理学-物理学] 

基  金:Supported by the National Nature Science Foundation of China(U2167204,11975040,1832130) The Brazilian authors thank the partial financial support from CNPq,FAPERJ,and INCT-FNA(Instituto Nacional de Ciência e Tecnologia,Física Nuclear e Aplicações),research Project No.(464898/2014-5) supported by(M.S.)the U.S.Department of Energy,Office of Science,and Office of Nuclear Physics(DE-AC02-06CH11357) supported By the Key Research and Development Program of Guangdong Province,China(2020B040420005) the Basic and Applied Basic Research Foundation of Guangdong Province,China(2021B1515120027) LingChuang Research Project of China National Nuclear Corporation(20221024000072F6-0002-7) the Nuclear Energy Development and Research Project(HNKF202224(28)),and the'111'Center(B20065) 

主  题:cross section incomplete fusion suppression factor weakly bound nuclei 

摘      要:The complete and incomplete fusion cross sections for ^(6)Li+^(209)Bi were measured using the in-beamγ-ray method around the Coulomb *** cross sections of(deuteron captured)incomplete fusion(ICF)products were re-quantified experimentally for this reaction *** results reveal that the ICF cross section is equivalent to that of complete fusion(CF)above the Coulomb barrier and dominant near or below the Coulomb barrier.A theoretical calculation based on the continuum discretized coupled channel(CDCC)method was performed for the aforementioned CF and ICF cross sections;the result is consistent with the *** universal fusion function(UFF)was also compared with the measured CF cross section for different barrier parameters,demonstrating that the CF suppression factor is significantly influenced by the choice of potential,which can reflect both dynamic and static effects of breakup on the fusion process.

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