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Low and medium energy deuteron-ind ced reactions on $^{63,65}$Cu nuclei
Low medium energy deuteron-ind ced reactions
2011/7/21
The activation cross sections of (d,p), (d,2n), (d,3n), and (d,2p) reactions on 63,65Cu were measured in the energy range from 4 to 20 MeV using the stacked-foils technique.
Low and medium energy deuteron-ind ced reactions on $^{63,65}$Cu nuclei
Low medium energy deuteron-ind ced reactions nuclei
2011/7/20
The activation cross sections of (d,p), (d,2n), (d,3n), and (d,2p) reactions on 63,65Cu were measured in the energy range from 4 to 20 MeV using the stacked-foils technique. Then, following the availa...
Nuclear spins, magnetic moments and quadrupole moments of Cu isotopes from N = 28 to N = 46: probes for core polarization effects
Nuclear spins magnetic moments quadrupole moments Cu isotopes probes core polarization effects
2010/12/31
Measurements of the ground-state nuclear spins, magnetic and quadrupole moments of the copper isotopes from 61Cu up to 75Cu are reported. The experiments were performed at the ISOLDE facility, using t...
Half-lives and branchings for β-delayed neutron emission for neutron-rich Co-Cu isotopes in the r-process
Half-lives branchings β-delayed neutron emission neutron-rich Co-Cu isotopes the r-process
2010/12/31
The {\beta} decays of very neutron-rich nuclides in the Co-Zn region were studied experimentally at the National Superconducting Cyclotron Laboratory using the NSCL {\beta}-counting station in conjunc...
Phobos results on charged particle multiplicity and pseudorapidity distributions in Au+Au, Cu+Cu, d+Au, and p+p collisions at ultra-relativistic energies
Phobos results on charged particle multiplicity pseudorapidity distributions Au+Au, Cu+Cu, d+Au p+p collisions ultra-relativistic energies
2011/1/4
Pseudorapidity distributions of charged particles emitted in $Au+Au$, $Cu+Cu$, $d+Au$, and $p+p$ collisions over a wide energy range have been measured using the PHOBOS detector at RHIC. The centralit...
测量了200A GeV 32S核与Cu作用产生的重碎片P,Si,Al和Mg的角分布,得出它们的横动量分布宽度σpt在130—270MeV/c的范围.
用阈探测器中子活化法测量了50MeV/u 18O离子轰击Be.Cu和Au厚靶的总中子产额和前向中子发射率. 实验结果表明,中子产额对靶核原子序数有一定的依赖性,较轻靶子的中子产额和中子发射率高于较重的靶子;当靶核(Cu)和入射离子单核能(50MeV)相同时,18O离子的中子产额约为12C离子的4倍.
用中子活化分析法对制造器件用的半导体硅中Na,Cu,Au含量的分析
半导体硅 制造器件 中子活化分析法
2008/12/23
本文介绍了用作器件的半导体硅片表面和本体中Na,Cu,Au含量的堆中子活化分析方法。给出了探测极限。除了常用的“相对比较法”外,着重介绍了“代用标准法”。为了适应常规分析的要求,我们以铁丝作Cu和Na的代用标准,使照后的标准处理摆脱了放射性溶液操作。
C,Al,Cu,Sn,Pb等原子核对高能π+,K+介子及质子的吸收截面
2007/12/13
在联合原子核研究所同步稳相加速器上,研究了高能π+、K+介子和原子核的相互作用。利用角度式气体契连科夫速度选择器,选择出纯度约达99％的K+介子束。测量了C,Al,Cu,Sn,Pb等原子核对动量为2.72,3.70,4.75Бэв/с的π+介子的吸收截面;C,Al,Cu等原子核对动量为4.75Бэв/с的K+介子的吸收截面;C,Sn,Pb等原子核对动量为2.72Бэв/с的质子的吸收截面。利用光学...
6.8MeV质子对Cr,Co,Ni,Cu,Zn的弹性散射
2007/12/12
本实验测量了6.8MeV质子对Cr,Co,Ni,Cu和Zn的弹性散射角分布。在其微分截面σe(θ)与库仑散射微分截面σR(θ)之比对θ的作图中显示:这几种元素A相近,也有大体相似的角分布曲线;其极大极小位置可以用kR′sinθm/2=常数表之,显示出核的粗糙结构的特征。但在大角度处,这几种质量数A相近的核,其(σe(θ))/(σR(θ))值却有显著的差异,而且偶z核的(σe(