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NEUTRON EFFECTS ON RADIOISOTOPE IDENTIFIERS (RIIDs)

机译:中子对放射性同位素标识符(RIID)的影响

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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:我们正在进行一项多年计划,以评估COTS RIID仪器的检测和识别(ID)能力。在本次会议的配套文件中简要介绍了针对DTRA进行的测试程序的框架。在评估RIID的性能的过程中,有时我们会使其经受异常的测试条件,以模拟可能的应用场景,或者仅仅是出于完整性考虑。在我们的测试场景中偶尔会出现中子。在本报告中,我们重点关注在某些测试条件下可见的单一现象-由中子与测试环境以及RIID自身相互作用产生的伽马射线。根据测试条件,这些中子诱发的伽马射线会给测试源的光谱特征添加意想不到的谱线。这样的一个例子是由中子与钢的相互作用产生的847-keV线,钢是我们测试中经常使用的屏蔽材料。该光峰出现在测试光谱的区域中,其背景本底较低。因此,它是可见的,有时甚至是突出的。最近,我们已经确定了中子与三种检测材料-HPGe,Nal和LaBr_3的中子相互作用产生的谱线。主要关注线出现在50-300 keV范围内,并导致RIID的识别报告不正确。例如,一条来自〜(75m)Ge的139.9 keV的线是由于与〜(74)Ge的中子相互作用而产生的(正如先前其他人所报道的那样),并且由于基于〜(99m)Tc而被基于HPGe的RIIDs错误地识别出来。 ,其主线为140.5 keV。类似地,57.6 keV的谱线是由〜(127)I引起的中子非弹性散射引起的(其他人较早的报道),并且经常被基于Nal的RIID与〜(241)Am的59.5-keV谱线混淆。中子与基于LaBr3的RIID的相互作用产生了复杂的光谱结构,但迄今为止,仅约166 keV的谱线导致了错误的报告(〜(201)T1)。我们对中子对RIID的影响的面向应用的检查的重点是了解仪器测试光谱中此类外来线的起源,而不是其他人已经检查过的相关核结构现象学。我们的目标是减少不正确的RIID标识,并促进各个制造商适当改进仪器。

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