Authors:H. Aglan, S. Kandil, H. Hanafi, M. Mousa, and Z. Saleh
The radiochemical separation of no-carrier-added cerium from proton irradiated lanthanum was studied by solvent extraction
using DEE, TBP and TPPO, the latter reagent being employed for the first time for separation of radiocerium from bulk of lanthanum.
Distribution coefficients of cerium and lanthanum were investigated as a function of equilibrium time and concentration of
HNO3. A mixture of 0.05M K2Cr2O7 and 0.1M H2SO4 was used as an oxidizing agent to improve the separation efficiency of cerium. A comparative study of the three extractants
released that DEE is the best for separation of cerium from bulk of lanthanum oxide. The target was prepared by pressing.
The production of 139Ce of high radionuclidic purity and chemical purity via irradiation of lanthanum oxide target at MGC-20 cyclotron with protons
of energy 14.5 MeV is described. The experimental yield was found to be 153 kBq/μA·h.
Authors:S. Kandil, H. Hanafi, H. Aglan, and Z. Saleh
The adsorption behaviour of La/Ce system on Dowex 50W-X8 in different media, namely, nitric acid, acetate buffer and citrate
buffer was studied as a function of the concentration of nitric acid and buffer pH. In addition, in cation-exchange column
chromatography experiments, three different eluants, namely, citrate buffer of pH 5.5, 0.1 M EDTA and 0.2 M α-HIBA, were employed
for separation of Ce(III) from La(III). The optimum conditions for improvement of radiochemical separation of no-carrier-added
139Ce from proton irradiated lanthanum were applied using the most suitable chelating agent 0.2 M α-HIBA. The purification of
139Ce from macro amount of La(III) was done using two columns in a sequence. The target was prepared by pressing. The production
of high radionuclidic and chemical purity 139Ce via irradiation of lanthanum oxide target at MGC-20 cyclotron of proton energy 14.5 MeV was described. The experimental
yield was found to be 200 kBq/μA h.
Authors:K. Allan, M. Ali, H. Hanafi, and K. El-Azony
The activated carbon was prepared by using corncobs and characterized by sorpatometer for using as an exchanger material to
separate the generated 113mIn from 113Sn and 124,125Sb. To optimize the separation process, the different parameters like acetone percentage, HCl concentration were studied.
The exchange capacity of Sn(IV) is 7.6 meq/g onto the activated carbon and the elution efficiency of 113mIn > 80% by using 10 mL of 0.2 M HCl-80% acetone with flow rate 1 mL/min. The radionuclidic purity and radiochemical purity
of the eluted 113mIn were examined and clarified the presence of 124,125Sb with relatively high level as radio impurities, so further separation was carried out by using Dowex 1×8 as an anion exchanger
below the activated carbon matrix on the same separation column to adsorb the 113Sn and 124,125Sb, which escape from the activated carbon matrix.
Authors:S. Kandil, B. Scholten, K. Hassan, H. Hanafi, and S. Qaim
The radiochemical separation of 88Y from proton irradiated natSrCO3 and alpha-particle irradiated natRbCl, of 86Y from proton irradiated 86SrCO3, and of 87Y from alpha-particle irradiated natRbCl were studied at no-carrier-added levels by two techniques, namely, ion-exchange chromatography using Dowex 50W-X8 and
Dowex 21K resins, and solvent extraction using HDEHP. Out of all those methods, the ion-exchange chromatography using Dowex
50W-X8 (cation-exchanger) was found to be the best: the separation yield was high, the chemical impurity in the separated
radioyttrium (inactive Sr or Rb) was low (0.5 μg) and the final product was obtained in the form of citrate. The optimized
separation method using Dowex 50W-X8 was applied in practical production of 86Y and 88Y via proton irradiations of 86SrCO3 and natSrCO3, respectively, at 16 MeV as well as of 87Y and 88Y via α-particle irradiation of natRbCl at 26 MeV. The tangible experimental yields of 86Y and 87Y amounted to 150 and 5.7 MBq/μA·h, respectively. The yields of 88Y obtained were 0.06 MBq/μA·h and 1 MBq/μA·h for alpha-particle and proton irradiations, respectively. Each yield value corresponds
to more than 70% of the respective theoretical value.