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NEUTRON EFFECTS ON RADIOISOTOPE IDENTIFIERS (RIIDs)

机译:放射性同位素标识符(RIID)的中子作用

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We are engaged in a multi-year program to evaluate detection and identification (ID) capabilities of COTS RIID instruments. The framework of our testing program, conducted for DTRA, is briefly described in a companion paper in this conference. In the course of evaluating the performance of RIIDs, we sometimes subject them to unusual test conditions, either to simulate a possible application scenario, or simply for the sake of completeness. Neutrons are occasionally present in our test scenarios. In this report we focus on a single phenomenon that is visible under certain test conditions-gamma rays arising from neutron interactions with the test environment and with the RIIDs themselves. Depending on the test conditions, these neutron-induced gammas can add unexpected lines to the spectral signature of the test source. One such example is the 847-keV line generated from neutron interactions with steel, a shielding material frequently used in our testing. This photopeak occurs in a region of the test spectrum where the underlying background is relatively low. Thus it is visible, and at times even prominent. Recently, we have identified spectral lines that arise from neutron interactions with three detecting materials-HPGe, Nal, and LaBr_3. The lines of primary interest occur in the 50 - 300 keV range, and have led to incorrect identification reports from RIIDs. For example, a line at 139.9 keV from ~(75m)Ge arises from neutron interaction with ~(74)Ge (as reported by others earlier), and has been incorrectly identified by HPGe-based RIIDs as due to ~(99m)Tc, which has a primary line at 140.5 keV. Similarly, a line at 57.6 keV arises from neutron inelastic scattering by ~(127)I (per earlier reports by others), and has been frequently confused by Nal-based RIIDs with the 59.5-keV line of ~(241)Am. Neutron interactions with LaBr3-based RIIDs produce a complex spectral structure, but to date only a line at about 166 keV has led to incorrect reports (of ~(201)Tl). Our application-oriented examination of neutron effects on RIIDs has focused on understanding the origin of such extraneous lines in instrument test spectra, and not on the associated nuclear structure phenomenology, which others have examined. Our goal is to reduce incorrect RIID identifications and to facilitate appropriate instrument advances by the respective manufacturers.
机译:我们从事多年计划,以评估COTS RIID仪器的检测和识别(ID)功能。我们对DTRA进行的测试计划的框架在本会议的伴侣文件中简要介绍。在评估RIID的性能的过程中,我们有时将它们主题在不寻常的测试条件下,要么模拟可能的应用场景,要么只是为了完整性。中子偶尔出现在我们的测试场景中。在本报告中,我们专注于单一现象,该现象在某些测试条件下可见 - 从中​​子相互作用与测试环境和riid本身产生的伽马射线。根据测试条件,这些中子诱导的伽玛可以向测试源的光谱特征添加意外行。一个这样的例子是从中子相互作用与钢的847-keV线,常用于我们测试中的屏蔽材料。该PhotoPak发生在测试谱的区域中,其中底层背景相对较低。因此,它是可见的,有时甚至突出。最近,我们已经识别出从中子相互作用产生的光谱线与三种检测材料 - HPGE,NAL和LABR_3。主要兴趣线在50-300 keV范围内发生,并导致RIID的识别报告不正确。例如,来自〜(75米)Ge的139.9kev的线从中子相互作用与〜(74)GE(如其他人报告),并且由于〜(99米)TC而被基于HPGE的RIID被错误地识别,它在140.5 kev处具有主要线。类似地,57.6 kev的线产生从中子射击〜(127)i(其他人的报告),并且经常被NAL的RIID与〜(241)的59.5-keV线混淆。与基于Labr3的RIID的中子相互作用产生复杂的光谱结构,但迄今为止只有大约166keV的线路导致了不正确的报告(〜(201)T1)。我们对RIID的中子效果的面向应用的审查专注于理解仪器测试光谱中这种无关线的起源,而不是关于其他核结构现象学的起源,其他人已经研究过。我们的目标是减少不正确的RIID标识,并促进各自制造商的适当工具。

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