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DEUTERIUM RETENTION IN BERYLLIUM AND BERYLLIUM OXIDE

机译:铍和氧化铍中的氘保留

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Retention of deuterium in Be sample and BeO film implanted with D ions or exposed to D atoms at temperatures in the range 300 to 700 K have been studied using SIMS and RGA (residual gas analysis) measurements in the course of surface sputtering. The microstructure of implanted specimens was investigated by TEM. (1) Be and BeO implanted with (3-9) keV D-ions accumulate deuterium in the form of both D atoms and D_2 molecules. In Be irradiated with D ions up to high fluences at which maximum D concentration is reached, the fraction of deuterium trapped in the form of D2 molecules is approx 0.8 at irradiation temperature Tirr =300 K and approx 0 6 at Tirr =700 K. As for BeO, the majority of implanted deuterium is retained as D atoms both at 300 and 700 K. In Be sample and BeO film implanted with D ions at T_irr ?300 K, the D_2 molecules are present in tiny bubbles (Be and BeO) and in intercrystalline non-interconnected gaps (BeO) In Be irradiated at T_irr= 700 K, along with relatively small facetted bubbles (near the very surface), large oblate gas-filled cavities and channels forming extended labyrinths. The microstructure of BeO film subjected to D ion implantation at Tirr = 700 K is indistinguishable from that of BeO film irradiated at T_irr = 300 K. The high concentration of D atoms in the ion stopping zone of Be matrix and BeO film after implantation to saturated fluences at 7_irr = 300 and 700 K is attributed to deuterium (i) trapped in radiation vacancies, (ii) adsorbed on the walls of bubbles and channels and (iii) chemically bonded to O atoms adjacent to point defects in the BeO lattice. (2) Due to the presence of oxygen containing molecules as trace impurities, the beryllium oxide layer is formed on the surface of Be sample exposed to D atoms at elevated temperatures. It has been found mat the deuterium atom exposure leads to the deuterium retention in tins layer. The majority of deuterium (> 90 percent) retains as D atoms, the other part is accumulated in the form of D_2 molecules. After termination of D atom exposure D concentration in BeO layer decreases with time at room temperature. It is supposed that the formation of beryllium hydroxide Be(OD)_2 under D atoms exposure of growing BeO layer takes place. The decrease of deuterium concentration in time is explained by dehydration of Be(OD)_2.
机译:在表面溅射过程中,使用SIMS和RGA(残留气体分析)测量技术研究了注入D离子或暴露于D原子的Be样品和BeO膜中氘在300至700 K范围内的氘保留。透射电镜研究了植入标本的微观结构。 (1)注入了(3-9)keV D离子的Be和BeO以D原子和D_2分子的形式积累氘。在以最高通量达到最高通量的D离子辐照下,在辐照温度Tirr = 300 K时,以D2分子形式捕获的氘分数约为0.8,在Tirr = 700 K时约为0 6。对于BeO,大多数注入的氘在300和700 K时都保留为D原子。在Be样品和在T_irr?300 K下注入D离子的BeO膜中,D_2分子以微小气泡(Be和BeO)存在。晶间非互连间隙(BeO)中的T_irr = 700 K时,伴随着相对较小的多面气泡(非常靠近表面),较大的扁圆形充气腔和形成迷宫的通道。在Tirr = 700 K下进行D离子注入的BeO膜的微观结构与在T_irr = 300 K下辐照的BeO膜的微观结构没有区别。注入饱和后,Be基质和BeO膜的离子停止区中D原子的浓度很高。在7_irr = 300和700 K处的能量密度归因于氘(i)陷于辐射空位中;(ii)吸附在气泡和通道壁上;以及(iii)化学键合到与BeO晶格中的点缺陷相邻的O原子。 (2)由于存在作为痕量杂质的含氧分子,因此在高温下暴露于D原子的Be样品的表面上形成氧化铍层。已经发现,氘原子的暴露导致氘保留在锡层中。氘的大部分(> 90%)保留为D原子,其余部分以D_2分子的形式积累。在D原子暴露终止后,BeO层中的D浓度在室温下随时间降低。推测在成长的BeO层的D原子暴露下会发生氢氧化铍Be(OD)_2的形成。氘浓度随时间的降低可以通过Be(OD)_2的脱水来解释。

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