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The Journal of Nuclear Medicine Vol. 13 No. 10 729-732
© 1972 by Society of Nuclear Medicine
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Production of Carrier-Free 123I Using the 127I(p,5n)123Xe Reaction

M. A. Fusco, N. F. Peek, J. A. Jungerman, F. W. Zielinski, S. J. DeNardo and G. L. DeNardo

University of California at Davis, Davis, California

Correspondence: For reprints contact: Neal Peek, Crocker Nuclear Laboratory, University of California, Davis, Calif. 95616.

ABSTRACT

A cyclotron procedure for the production of high-purity, carrier-free 123I suitable for immediate radio-pharmaceutical use has been developed. Proton irradiation of natural elemental iodine results in the production of 123Xe which subsequently decays to 123I. The primary reaction for 57-MeV protons is 127I(p,5n)123Xe; other reactions yield 125Xe and the neutron-deficient radioisotopes of iodine. At the end of bombardment, the target iodine is dissolved in aqueous KI, and helium gas is bubbled through the solution, sweeping the xenon through a recirculating system. The xenon gas is collected in a liquid nitrogen-cooled trap. The isolated xenon is contained for 6 hr during which time the 123Xe (T1/2, 2.1 hr) decays to 123I. The 123I may be recovered by adding a small volume of physiological saline.

An irradiation on the Crocker Nuclear Laboratory isochronous cyclotron of 1 hr, using a 1 gm/cm2 thickness of iodine (7-MeV proton energy loss in the target) and 57.5-MeV protons at 6 µA, resulted in 24 isolable mCi of 123I. The only detectable contaminant in the final product was 125I which was about 0.1% of the 123I activity.

A reasonable extrapolation of our irradiation experience indicates that a yield of 89 mCi can be obtained in practice. This production figure is based on a target thickness of 1 gm/cm2 and an irradiation time of 3 hr at 10 µA.

The advantages of this method over existing methods are (A) readily available, inexpensive, isotopically pure targets; (B) multimillicurie yields of carrier-free 123I, and (C) significantly reduced radio-nuclidic contamination. When used in vivo the radiation dose to the patient is reduced and optimal spatial resolution is possible for imaging procedures. This method, however, requires 50–60-MeV protons which are not universally available.







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Copyright © 1972 by the Society of Nuclear Medicine.