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Tytuł artykułu

New method of pure 111In production by proton-induced nuclear reactions with enriched 112 Sn

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Języki publikacji
EN
Abstrakty
EN
We aimed at finding out a simple and reliable way of 111In production with the highest radionuclide purity from its grand parent 111Sb and parent 111Sn nuclei, produced by the 112Sn(p,2n)111Sb and 112Sn(p,pn)111Sn reactions, respectively. The target was a metallic 112Sn sample enriched to 84%. We have measured activation cross sections for seven reactions on an enriched 112Sn sample induced by 23.6 š 0.8 MeV energy protons. Gamma-ray spectroscopy with high-purity germanium detectors has been used. We also identified the activities of 55Co (T1/2 = 17.5 h) and 60Cu (T1/2 = 23.7 min) in proton beam monitoring Ni foils, induced in the natNi(p,X)55Co and natNi(p,X)60Cu reactions at 22.8 MeV proton energy. The cross sections determined for these reactions are: s[natNi(p,X)55Co] = 36.6 š 4 mb and s[natNi(p,X)60Cu] = 64.4 š 7 mb. The measured cross sections of reactions on tin isotopes are: sigma[112Sn(p,n)112Sb] = 4 š 0.8 mb; sigma[112Sn(p,2n)111Sb] = 182 š 26 mb; sigma[112Sn(p,pn)111Sn] = 307 š 35 mb; sigma[114Sn(p,2n)113Sb] = 442 š 52 mb; s[117Sn(p,n)117Sb] = 15 š 3 mb; sigma[117Sn(p,p’gamma)117mSn] = 0.37 š 0.06 mb; s[115Sn(p,2p)114m2In] = 0.01 š 0.002 mb. Our measurements indicated the expected yield of the 111In production to be 46 MBq/mAh (1.2 mCi/mi Ah). The contamination of 111In by the undesired nuclide 114m2In was determined and belongs to the smallest ones found in the literature. The measured cross sections were compared with theoretical calculations by two top-level nuclear reaction codes EMPIRE and TALYS.
Czasopismo
Rocznik
Strony
17--27
Opis fizyczny
Bibliogr. 32 poz., rys.
Twórcy
autor
autor
  • Institute of Physics, Slovak Academy of Sciences, 84511 Bratislava, Slovakia and Faculty of Philosophy and Sciences, Silesian University, 74601 Opava, Czech Republic, Tel.: +421 2 59410537, Fax: +421 2 54776085, betak@savba.sk
Bibliografia
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  • 4. Bìták E, Mikołajczak R, Staniszewska J, Mikołajewski S, Rurarz E (2005) Activation cross sections for reactions induced by 14 MeV neutrons on natural tin and enriched 112Sn targets with reference to 111In production via isotope generator 112Sn(n,2n)111Sn → 111In. Radiochim Acta 93:311−326
  • 5. Blosser HG, Handley TH (1955) Survey of (p,n) reactions at 12 MeV. Phys Rev 100:1340−1344
  • 6. Dahl JR, Tilbury RS (1972) The use of a compact, multiparticle cyclotron for the production of 52Fe, 67Ga,111In and 123I for medical purposes. Int J Appl Radiat Isot 23:431−437
  • 7. European Pharmacopoeia, 3rd ed. (2000) Supplement 2000. Council of Europe, Strasbourg
  • 8. EXFOR (2005) EXFOR-CINDA for applications.Database and retrieval systems, v. 1.63i (CD ROM).IAEA, Vienna (http://www-nds.iaea.or.at/exfor)
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  • 10. GENIE (2000) User’s manual, basic spectroscopy software and documentation for Genie 2000 software suite. Canberra Industries 800 Research Parkway, Meridan, Connecticut 06450, USA
  • 11. Grutter A (1982) Excitation functions for radioactive isotopes produced by proton bombardment of Cu and Al in the energy range of 16−70 MeV. Nucl Phys A 383:98−108
  • 12. Gul K (2001) Calculations for the excitation functions of the 63Cu(p,n)63Zn, 63Cu(p,n)62Zn and 65Cu(p,n)65Zn reactions. Appl Radiat Isot 54:147−151
  • 13. Herman M (2002) EMPIRE-II statistical model code for nuclear reaction calculations (version 2.18 Mondovi).IAEA, Vienna
  • 14. Herman M, Obložinský P, Capote R et al. (2005) EMPIRE modular system for nuclear reaction calculations (version 2.19 Lodi). NNDC BNL, Upton, USA
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  • 16. Kaufman S (1960) Reactions of protons with 58Ni and 60Ni. Phys Rev 117:1532−1538
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  • 18. Koning AJ, Hilaire S, Duijvestijn MC (2004) TALYS: a nuclear reaction program. Report 21297/04.62741/P FAI/AK/AK. NRG, Petten
  • 19. Kopecky P (1985) Proton beam monitoring via the Cu(p,x)58Co, 63Cu(p,2n)62Zn, and 65Cu(p,n)65Zn reaction in copper. Int J Appl Radiat Isot 36:657−661
  • 20. Michel R, Weigel H, Herr W (1978) Proton induced reaction on nickel with energies between 12 and 45 MeV.Z Phys A 286:393−400
  • 21. Novgorodov AF, Biełov AG, Zieliński A, Kołaczkowski A (1987) A simple method for high-temperature separation of 111In from massive tin targets. Radiochimiya 29:254−258 (in Russian) (also see: preprint P6-85-918,JINR Dubna)
  • 22. NuDat 2.1,http://www-nds.iaea.org/nudat2/index.jsp
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  • 26. Rurarz E, Mikołajewski S (1993) Model calculations of 111In production via the 112,114,115,116,117Sn(p,xnypza)111Sb &rarr111Sn &rarr 111In reactions. Report SINS 02147/II. Soltan Institute for Nuclear Studies, Świerk, Poland
  • 27. Schwerer O, Okamoto K (1989) Status report on cross sections on monitor reactions for radioisotope production Report INDC(NDS)-21 GZ+. IAEA, Vienna
  • 28. Tanaka S, Furukawa M, Chiba M (1972) Nuclear reactions of nickel with protons up to 56 MeV. J Inorg Nucl Chem 34:2419−2426
  • 29. Tarkányi F, Szelecsenyi F, Kopecky P (1991) Excitation functions of proton induced nuclear reactions on natural nickel for minitoring of beam energy and intensity. Appl Radiat Isot 42:513−517
  • 30. Tuli JK (2005) Nuclear wallet cards. BNL, Upton, NY
  • 31. Williamson CF, Bujot JP, Picard J (1966) Tables of range and stopping power of chemical elements for charged particles of energy 0.5 to 500 MeV. Report CEA-R-3042.CEA, Saclay
  • 32. Zaitseva NG, Knotek O, Kowalew A et al. (1990)Excitation functions and yields for 111In production using 113,114,natCd (p,xn)111In reaction with 65 MeV protons. Appl Radiat Isot 41:177−183
Typ dokumentu
Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-article-BUJ6-0011-0035
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