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利用厚靶产生的轫致辐射,测量作为电子束能量和相对于电子束角度的函数的\(^{12}C(\gamma,n)^{11}C\)、\(^{14}N(\gamma,n)^{13}N\)和\(^{16}O(\gamma,n)^{15}O\)反应的活度产额。

Measurement of activity yields for 12C(gamma, n)11C, 14N(gamma, n)13N, and 16O(gamma, n)15O reactions as a function of electron beam energy and angle from the electron beam using thick target produced bremsstrahlung.

作者信息

Piltingsrud H V

出版信息

Med Phys. 1983 Mar-Apr;10(2):147-54. doi: 10.1118/1.595295.

Abstract

The calculation of activity yields from practical photonuclear target systems designed to produce short-lived positron emitting radionuclides for nuclear medicine purposes requires certain basic information. These include a knowledge of the photon source (bremsstrahlung energy spectrum and intensity as a function of angle from the electron beam) and the gamma, n activation cross section of the secondary target element. A lack of adequate information concerning these parameters motivated the present study in which activity yields for the reactions 12C(gamma, n)11C, 14N(gamma, n)13N, and 16O(gamma, n)15O were measured as a function of energy of and angle from the electron beam between 16 and 30 MeV and 0 degree and 30.5 degrees, respectively. The data indicate highly complex relationships between the activity yield and the experimental variables. Also indicated are possible applications of the data to indicate the energy of an electron beam producing a given bremsstrahlung field in which activation measurements are made.

摘要

为核医学目的设计的用于生产短寿命发射正电子放射性核素的实际光核靶系统的活度产额计算需要某些基本信息。这些信息包括光子源的知识(轫致辐射能谱以及作为与电子束夹角函数的强度)和次级靶元素的γ,n活化截面。由于缺乏关于这些参数的足够信息,激发了本研究,其中测量了反应12C(γ,n)11C、14N(γ,n)13N和16O(γ,n)15O的活度产额,它们分别是16至30 MeV电子束能量以及0度至30.5度与电子束夹角的函数。数据表明活度产额与实验变量之间存在高度复杂的关系。还指出了这些数据在确定产生给定轫致辐射场(在此场中进行活化测量)的电子束能量方面的可能应用。

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