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首页> 外文期刊>Nuclear Instruments & Methods in Physics Research >SIMS analysis of xenon and krypton in uranium dioxide: A comparison of two models of gas-phase ionisation
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SIMS analysis of xenon and krypton in uranium dioxide: A comparison of two models of gas-phase ionisation

机译:二氧化铀中氙和rypto的SIMS分析:两种气相电离模型的比较

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Reasonable detection limits in secondary ion mass spectrometry (SIMS) analysis of inert gases in solids may be achieved by gas-phase ionisation. For Xe in UO_2 Desgranges and Pasquet (D&P) have recently reported that the ion intensity I_(Xe)~+ can be enhanced significantly using O_2~+ ion bombardment in combination with an oxygen jet directed at the sputtered area. A similar effect was reported by Portier et al. for Kr in UO_2. The enhancement was attributed to ionisation by an interaction with oxygen atoms and molecules (D&P model). The proposed mechanism is at variance with a recently outlined model of gas-phase ionisation involving charge transfer between the ejected atoms and the incoming primary ions. The purpose of this study was to clarify these contradictory views by a reanalysis of the original data. Access to all relevant original data was kindly provided by L Desgranges. In contrast to expectation based on the D&P model, step-wise increases in the flow rate of the oxygen jet did not result in an immediate response of I_(xe+). Instead, transient yield changes were observed, with characteristic rise times that were even longer for Xe* than for uranium specific signals. This observation invalidates the idea that ionisation of Xe atoms is due to interaction with oxygen molecules of the jet. Recalling well known transient phenomena in ion-bombardment induced photon emission, it is argued that the enhancement effect may be associated with the increase in the oxidation state of the sample, as a result of which the fraction of Xe (or Kr) atoms leaving the sample in an electronically excited state is presumably increasing, thus enlarging the effective cross section for charge transfer. Alternatively, the enhancement may be due to a lowering of the ejection velocity of rare gas atoms, possibly caused by the increase in near-surface sample oxidation. A second problem with the D&P study is the use of I_U~+ as a reference signal. Literature data as well as new results reveal that UO_2~+ and UO~+ secondary ions dominate the SIMS spectrum of oxidised uranium at energies <60eV, the U+ fraction amounting to only 1% or less. Other issues are (ⅰ) the significant variation of the sample erosion rate that occurred upon deliberate changes of the mean primary ion current density, (ⅱ) the associated bombardment induced, progressive oxygen depletion of the sample, (ⅲ) the presence of a background superimposed on the Xe+ signals, a significant effect at low current densities and (iv) the space-charge broadening of the primary ion beam at high beam currents. Eliminating all these interfering factors, the (reduced) ionisation probabilities of Xe+ were found to be in accordance with gas-phase ionisation by charge exchange, even in the pressure of excessive oxygen flooding.
机译:通过气相电离可以实现对固体中惰性气体的二次离子质谱(SIMS)分析中的合理检测限。对于UO_2中的Xe,Desgranges和Pasquet(D&P)最近报道,使用O_2〜+离子轰击结合指向溅射区域的氧气喷射,可以显着提高离子强度I_(Xe)〜+。 Portier等报道了类似的效果。 UO_2中的Kr。增强归因于与氧原子和分子相互作用的电离(D&P模型)。所提出的机理与最近概述的气相电离模型有关,该模型涉及在喷射的原子和进入的初级离子之间的电荷转移。本研究的目的是通过对原始数据的重新分析来弄清这些矛盾的观点。 L Desgranges友好地提供了对所有相关原始数据的访问。与基于D&P模型的预期相反,氧气射流流量的逐步增加并未导致I_(xe +)的即时响应。取而代之的是,观察到瞬时的产量变化,Xe *的特征上升时间甚至比铀特定信号的特征上升时间更长。这种观察使认为Xe原子的电离是由于与射流中的氧分子的相互作用而无效。回顾离子轰击引起的光子发射中众所周知的瞬态现象,有人认为增强效应可能与样品氧化态的增加有关,其结果是Xe(或Kr)原子的一部分离开了原子。处于电子激发态的样品可能会增加,从而增大了电荷转移的有效截面。可替代地,这种增强可能是由于稀有气体原子的喷射速度的降低,可能是由于近表面样品氧化的增加所致。 D&P研究的第二个问题是使用I_U〜+作为参考信号。文献数据和新的结果表明,在能量<60eV时,UO_2〜+和UO〜+次级离子在氧化铀的SIMS光谱中占主导地位,U +分数仅为1%或更少。其他问题是(ⅰ)故意改变平均一次离子电流密度时发生的样品腐蚀速率的显着变化;(ⅱ)伴随轰击引起的样品的逐步氧耗竭;(ⅲ)背景的存在叠加在Xe +信号上,在低电流密度下会产生显着影响,并且(iv)在高束电流下初级离子束的空间电荷展宽。消除所有这些干扰因素,发现Xe +的(降低的)电离几率与通过电荷交换进行的气相电离一致,即使在氧气溢流过多的压力下也是如此。

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