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Nuclear resonance fluorescence for nuclear materials assay.

机译:用于核材料测定的核共振荧光。

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摘要

This dissertation examines the measurement of nuclear resonance fluorescence gamma-rays as a technique to non-destructively determine isotopic compositions of target materials that are of interest for nuclear security applications. The physical processes that can result in non-resonant background to nuclear resonance fluorescence measurements are described and investigated using a radiation transport computer code that relies on the Monte Carlo technique, MCNPX. The phenomenon of nuclear resonance fluorescence is discussed with consideration of the angular distributions of resonance emissions, the effects of nuclear recoil, and the influence of thermal motion.;Models describing two ways of measuring nuclear resonance fluorescence rates in materials are considered. First the measurement of back-scattered photons is considered. In this type of measurement, the portion of the interrogating photon beam that is scattered into large relative angles is measured. When the radioactivity of the target can be overcome by shielding or by use of intense photon sources, direct measurement of gamma-rays, emitted during nuclear resonance fluorescence can provide quantitative signatures that appear to be useful for applications such as forensic age-dating of large radiological sources. However, if the target radioactivity is too intense, as in the case for most spent nuclear fuel, a second measurement type, where indirect measurement of transmitted resonant-energy photons can also provide quantitative information. This method allows radiation detectors to be better-shielded from target radioactivity, but suffers from a slower accrual rate of statistical confidence. The models described herein indicate that very intense photon sources and large high-resolution detector arrays would be needed to measure 239Pu content in spent fuel to precisions desired by nuclear safeguards organizations. However, the rates at which statistics accrue are strongly proportional to the strengths of the resonances, and measurement of a plutonium isotope with stronger resonances may provide more practical measurement rates.;The model for predicting relative detection rates of nuclear resonance fluorescence gamma-rays in the transmission measurement was experimentally tested using the 238U in a mixture of depleted uranium and lead as a surrogate for 239Pu in spent fuel. The experiment indicated that the model was approximately correct, but that the process of notch refilling, which was excluded from the initial model, appears to be visible. Data files of the computer code, MCNPX, were modified to allow for nuclear resonance fluorescence to be simulated and a bug in the code was repaired to allow the code to more accurately simulate non-resonant elastic photon scattering. Simulations using this modified version of MCNPX have indicated that the magnitude of the notch refill process is comparable to that of the difference between the analytical model and the experimental data.
机译:本论文探讨了核共振荧光伽玛射线的测量技术,该技术可无损确定目标材料的同位素组成,这是核安保应用所关注的。使用依赖于蒙特卡罗技术MCNPX的辐射传输计算机代码,描述和研究了可能导致核共振荧光测量产生非共振背景的物理过程。考虑了共振发射的角度分布,核后坐力的影响以及热运动的影响,讨论了核共振荧光现象。考虑了描述两种测量材料中核共振荧光率的方法的模型。首先考虑反向散射光子的测量。在这种类型的测量中,将测量询问光子束中散射成较大相对角度的部分。如果可以通过屏蔽或使用强光子源来克服目标的放射性,则直接测量在核共振荧光过程中发射的伽玛射线可以提供定量特征,这些特征似乎可用于诸如大法医年龄鉴定的应用放射源。但是,如果目标放射性太强(如大多数乏核燃料的情况一样),则是第二种测量类型,其中传输的共振能量光子的间接测量也可以提供定量信息。这种方法可以使辐射探测器更好地屏蔽目标放射性,但会降低统计置信度的累积率。本文所述的模型表明,将需要非常强的光子源和大型高分辨率探测器阵列来测量乏燃料中的239Pu含量,以达到核保障组织所需的精度。然而,统计的累积率与共振强度成正比,共振强度更高的a同位素的测量可能提供更实用的测量率。预测核磁共振荧光伽玛射线相对检测率的模型传输率的测量是在贫铀和铅的混合物中使用238U作为乏燃料中239Pu的替代物进行的。实验表明该模型是近似正确的,但是从原始模型中排除的缺口重新填充过程似乎是可见的。修改了计算机代码MCNPX的数据文件,以模拟核共振荧光,并修复了代码中的错误,以使代码可以更准确地模拟非共振弹性光子散射。使用此修改版的MCNPX进行的仿真表明,缺口重新填充过程的大小可与分析模型和实验数据之间的差异相媲美。

著录项

  • 作者

    Quiter, Brian Joseph.;

  • 作者单位

    University of California, Berkeley.;

  • 授予单位 University of California, Berkeley.;
  • 学科 Engineering Nuclear.
  • 学位 Ph.D.
  • 年度 2010
  • 页码 255 p.
  • 总页数 255
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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