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The use of self-induced X-ray fluorescence in gamma-ray spectroscopy of uranium ore samples

机译:在铀矿石样品中使用自诱导X射线荧光

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Gamma logging for uranium exploration are currently based on total counting with Geiger Muller gas detectors or NaI (TI) scintillators. However, the total count rate interpretation in terms of uranium concentration may be impaired in case of roll fronts, when the radioactive equilibrium of the natural ~(238)U radioactive chain is modified by differential leaching of uranium and its daughter radioisotopes of thorium, radium, radon, etc. Indeed, in case of secular equilibrium, more than 95 % of gamma rays emitted by uranium ores come from ~(214)Pb and ~(214)Bi isotopes, which are in the back-end of ~(238)U chain. Consequently, these last might produce an intense gamma signal even when uranium is not present, or with a much smaller activity, in the ore. Therefore, gamma spectroscopy measurements of core samples are performed in surface with high-resolution hyper-pure germanium HPGe detectors to directly characterize uranium activity from the 1001 keV gamma ray of ~(234)mPa, which is in the beginning of ~(238)U chain. However, due to the low intensity of this gamma ray, i.e. 0.84 %, acquisitions of several hours are needed. In view to characterize uranium concentration within a few minutes, we propose here a method using both the 92 keV gamma ray of ~(234)Th and the 98.4 keV uranium X-ray. This last is due to uranium self-induced fluorescence caused by gamma radiations of ~(214)Pb and ~(214)Bi, which create a significant Compton scattering continuum acting as a fluorescence source and resulting in the emission of uranium fluorescence X-rays. The comparison of the uranium activity obtained with the 92 keV and 98.4 keV lines allows detecting a uranium heterogeneity in the ore. Indeed, in case of uranium nugget, the 92 keV line leads to underestimated uranium concentration due to gamma self-absorption, but on the contrary the 98.4 keV line leads to an overestimation because of increased fluorescence. In order to test this new approach, several tens of uranium ore samples have been measured with a handheld HPGe FALCON 5000 detector.
机译:用于铀勘探的伽玛测井目前是基于与Geiger Muller气体探测器或Nai(TI)闪烁体的总计数。然而,在卷面前的情况下,当天然〜(238)u放射性链的放射性平衡通过铀的差异浸出来改变铀的放射性平衡,可以损害铀浓度方面的总计数解释。 ,氡等,实际上,在世俗平衡的情况下,铀矿石发出的超过95%的γ射线来自〜(214)Pb和〜(214)Bi同位素,这是〜(238 )U链。因此,即使在矿石中不存在铀,或者在矿石中,铀的不存在较小的活性,这些最后可能产生强烈的γ信号。因此,具有高分辨率超纯锗HPGE探测器的表面上进行核心样品的γ光谱测量,以直接从1001keVγ射线的铀活动表征〜(234)MPa,这在〜(238)的开始时U链。然而,由于该伽马射线强度低,即0.84%,需要收购数小时。观点在几分钟内表征铀浓度,我们在此提出了一种使用〜(234)Th和98.4keV铀X射线的92keVγ射线的方法。最后是由于由γ(214)Pb和〜(214)Pb和〜(214)Bi引起的铀辐射引起的铀辐射,它产生了一种显着的康普顿散射连续体,其作为荧光源,导致铀荧光X射线的发射。用92keV和98.4KeV线获得的铀活性的比较允许检测矿石中的铀异质性。实际上,在铀核状物的情况下,由于γ自吸收,92keV线导致低估的铀浓度,但相反,由于荧光增加,98.4keV线导致高估估计。为了测试这种新方法,用手持HPGE Falcon 5000检测器测量了几十个铀矿石样本。

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