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Deuteron-induced reactions generated by intense lasers for PET isotope production

机译:强激光产生氘氘诱发的反应以生产PET同位素

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We investigate the feasibility of using laser accelerated protons/deuterons for positron emission tomography (PET) isotope production by means of the nuclear reactions ~(11)B(p, n)~(11)C and ~(10)B(d, n)~(11)C The second reaction has a positive Q-value and no energy threshold. One can, therefore, make use of the lower energy part of the laser-generated deuterons, which includes the majority of the accelerated deuterons. By assuming that the deuteron spectra are similar to the proton spectra, the ~(11)C produced from the reaction ~(10)B(d, n)~(11)C is estimated to be 7.4 x 10~9 per laser-shot at the Titan laser at Lawrence Livermore National Laboratory. Meanwhile a high-repetition table-top laser irradiation is estimated to generate 3.5 x 10~(711)C per shot from the same reaction. In terms of the ~(11)C activity, it is about 2 x 10~4 Bq per shot. If this laser delivers kHz, the activity is integrated to 1 GBq after 3 min. The number is sufficient for the practical application in medical imaeine for PET.
机译:我们研究了利用激光加速质子/氘核通过〜(11)B(p,n)〜(11)C和〜(10)B(d,)反应生成正电子发射断层扫描(PET)同位素的可行性, n)〜(11)C第二反应的Q值为正,没有能量阈值。因此,可以利用激光产生的氘核的较低能量部分,其中包括大部分加速氘核。通过假设氘核光谱与质子光谱相似,由〜(10)B(d,n)〜(11)C反应产生的〜(11)C估计为每个激光-7.4 x 10〜9。在劳伦斯·利弗莫尔国家实验室的泰坦激光器上拍摄。同时,估计高重复性台式激光照射可从同一反应中每次发射产生3.5 x 10〜(711)C。就〜(11)C活性而言,每发约为2 x 10〜4 Bq。如果此激光器提供kHz,则3分钟后将活动积分到1 GBq。该数量足以用于PET的医疗金丝氨酸的实际应用。

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