TY - JOUR
T1 - Feasibility studies towards future self-sufficient supply of the 99Mo-99mTc isotopes with Japanese accelerators
AU - Nakai, Kozi
AU - Takahashi, Naruto
AU - Hatazawa, Jun
AU - Shinohara, Atsushi
AU - Hayashi, Yoshihiko
AU - Ikeda, Hayato
AU - Kanai, Yasukazu
AU - Watabe, Tadashi
AU - Fukuda, Mitsuhiro
AU - Hatanaka, Kichiji
N1 - Publisher Copyright:
© 2014 The Japan Academy.
PY - 2014
Y1 - 2014
N2 - In order to establish a self-sufficient supply of 99mTc, we studied feasibilities to produce its parent nucleus, 99Mo, using Japanese accelerators. The daughter nucleus, 99mTc, is indispensable for medical diagnosis. 99Mo has so far been imported from abroad, which is separated from fission products generated in nuclear reactors using enriched 235U fuel. We investigated 99mTc production possibilities based on the following three scenarios: (1) 99Mo production by the (n, 2n) reaction by spallation neutrons at the J-PARC injector, LINAC; (2) 99Mo production by the (p, pn) reaction at Ep = 50-80 MeV proton at the RCNP cyclotron; (3) 99mTc direct production with a 20MeV proton beam from the PET cyclotron. Among these three scenarios, scenario (1) is for a scheme on a global scale, scenario (2) works in a local area, and both cases take a long time for negotiations. Scenario (3) is attractive because we can use nearly 50 PET cyclotrons in Japan for 99mTc production. We here consider both the advantages and disadvantages among the three scenarios by taking account of the Japanese accelerator situation.
AB - In order to establish a self-sufficient supply of 99mTc, we studied feasibilities to produce its parent nucleus, 99Mo, using Japanese accelerators. The daughter nucleus, 99mTc, is indispensable for medical diagnosis. 99Mo has so far been imported from abroad, which is separated from fission products generated in nuclear reactors using enriched 235U fuel. We investigated 99mTc production possibilities based on the following three scenarios: (1) 99Mo production by the (n, 2n) reaction by spallation neutrons at the J-PARC injector, LINAC; (2) 99Mo production by the (p, pn) reaction at Ep = 50-80 MeV proton at the RCNP cyclotron; (3) 99mTc direct production with a 20MeV proton beam from the PET cyclotron. Among these three scenarios, scenario (1) is for a scheme on a global scale, scenario (2) works in a local area, and both cases take a long time for negotiations. Scenario (3) is attractive because we can use nearly 50 PET cyclotrons in Japan for 99mTc production. We here consider both the advantages and disadvantages among the three scenarios by taking account of the Japanese accelerator situation.
KW - Accelerator production
KW - J-PARC
KW - Mo-Tc
KW - PET-cyclotron
KW - Tc generator
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U2 - 10.2183/pjab.90.413
DO - 10.2183/pjab.90.413
M3 - Article
C2 - 25504230
AN - SCOPUS:84923839474
SN - 0386-2208
VL - 90
SP - 413
EP - 421
JO - Proceedings of the Japan Academy Series B: Physical and Biological Sciences
JF - Proceedings of the Japan Academy Series B: Physical and Biological Sciences
IS - 10
ER -