Piltingsrud H V, Robbins P J
Med Phys. 1985 Sep-Oct;12(5):613-8. doi: 10.1118/1.595753.
Described in this paper are what we believe to be the first practical photonuclear target systems for production of 11C containing CO and CO2 using bremsstrahlung produced from an electron linear accelerator similar to certain radiotherapy accelerators. This is a continuation of work reported earlier concerning a similar target system presently being used for production of 15O-O2. The 11C producing systems utilized liquid carbon dioxide, liquid cyclohexane, and liquid glacial acetic acid target materials. The carbon dioxide and glacial acetic acid target materials produced principally a 11C-CO product material. The cyclohexane target material produced a 11C-hydrocarbon product which was then oxidized to CO2. Target activity yields for these systems, normalized to a 20-cm-long by 10-cm-diam target chamber irradiated in a bremsstrahlung field produced by a 26-MeV, 100-microA electron beam, were 1.9 X 10(8) Bq (5 mCi) at 7.4 X 10(8) Bq g-1 (20 mCi g-1) for carbon dioxide, 1.4 X 10(8) Bq (3.8 mCi) at 3.7 X 10(10) Bq g-1 (1 Ci g-1) for cyclohexane, and 7.4 X 10(8) Bq (20 mCi) at 3.7 X 10(10) Bq g-1 (1 Ci g-1) for glacial acetic acid.
本文描述了我们认为的首批实用的光核靶系统,该系统使用类似于某些放射治疗加速器的电子直线加速器产生的轫致辐射来生产含(^{11}C)的(CO)和(CO_2)。这是早期报道的关于目前用于生产(^{15}O - O_2)的类似靶系统工作的延续。生产(^{11}C)的系统使用液态二氧化碳、液态环己烷和液态冰醋酸作为靶材料。二氧化碳和冰醋酸靶材料主要产生(^{11}C - CO)产物材料。环己烷靶材料产生(^{11}C) - 烃产物,然后将其氧化为(CO_2)。对于这些系统,将靶活度产率归一化为在由(26 MeV)、(100 μA)电子束产生的轫致辐射场中照射的(20 cm)长、(10 cm)直径的靶室,二氧化碳的靶活度产率为(1.9×10^8 Bq(5 mCi)),活度浓度为(7.4×10^8 Bq g^{-1}(20 mCi g^{-1}));环己烷的靶活度产率为(1.4×10^8 Bq(3.8 mCi)),活度浓度为(3.7×10^{10} Bq g^{-1}(1 Ci g^{-1}));冰醋酸的靶活度产率为(7.4×10^8 Bq(20 mCi)),活度浓度为(3.7×10^{10} Bq g^{-1}(1 Ci g^{-1}))。