Investigation of the 66Zn(p,2pn)64Cu and 68Zn(p,x)64Cu nuclear processes up to 100 MeV:: Production of 64Cu

被引:57
|
作者
Szelecésnyi, F
Steyn, GF
Kovács, Z
Vermeulen, C
van der Meulen, NP
Dolley, SG
van der Walt, TN
Suzuki, K
Mukai, K
机构
[1] Hungarian Acad Sci, Cyclotron Dept, Inst Nucl Res, ATOMKI, H-4026 Debrecen, Hungary
[2] iThemba Lab Accelerator Based Sci, Radionuclide Prod Grp, ZA-7129 Somerset W, South Africa
[3] Natl Inst Radiol Sci, Radiopharmaceut Chem Sect, Dept Med Imaging, Inage Ku, Chiba 2638555, Japan
[4] Japan Steel Works, Ion Beam Grp, Kanazawa Ku, Yokohama, Kanagawa 2360004, Japan
基金
匈牙利科学研究基金会; 新加坡国家研究基金会;
关键词
enriched Zn; protons; Zn-66(p; 2pn)Cu-64; Zn-68(p; x)Cu-64; reactions; Cu-64; production;
D O I
10.1016/j.nimb.2005.05.057
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
Cross-sections of the Zn-66(p,2pn)Cu-64 and Zn-68(p,X)64Cu nuclear processes were measured on highly enriched zinc targets using the stacked-foil activation technique up to 100 MeV. The new cross-sections were compared to literature data. The optimum energy range for production of Cu-64 was found to be 70 -> 35 MeV on Zn-66 and 37 -> 20 MeV on Zn-68. The thick-target yields were determined as 777 MBq/mu Ah (21.0 mCi/mu Ah) and 185 NtBq/mu Ah (5.0 mCi/mu Ah), respectively. The yields of the longer-lived contaminant copper radioisotopes (i.e. Cu-61 when using Zn-66 as target material and both Cu-61 and Cu-67 in the case of Zn-68 target material) were also calculated. The results obtained from the present study indicate that both reactions are suited for the production of Cu-64 at a medium energy cyclotron. The optimum energy ranges are also complementary therefore the potential to utilize tandem targetry exists. (c) 2005 Elsevier B.V. All rights reserved.
引用
收藏
页码:625 / 637
页数:13
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