不同温度下D注入Ti的深度分布

J. Roth, W. Eckstein, J. Bohdansky
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引用次数: 25

摘要

用D(3He, α) H核反应研究了6.6 keV D+在140 ~ 500 K温度范围内注入钛的深度分布。在140 K时,低剂量捕获量接近100%,在约2 × 1018D/cm2时达到饱和,而在室温下,高达2 × 1019 D/cm2时无法达到饱和。在较高的温度下,数量减少,直到在500k以上的表层中无法检测到氘。深度剖面强烈依赖于温度。在140k时,氘在约2000a的表面层中发现,氘与金属原子的最大比率为2.5。在室温下形成TiD1.8的氢化物层。氢化物层厚度随氘剂量的增加而增大,在2 × 1019 D/cm2下可达1.5 μm。在较高的温度下,原子浓度较低,氘似乎深入扩散到物体内部。从氘i在Ti和氢化钛中的扩散角度讨论了这些结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Depth Profiling of D Implanted into Ti at Different Temperatures
Abstract Depth proliles of 6.6 keV D+ implanted into titanium in the temperature range between 140 K and 500 K have been studied using the D(3He, α) H nuclear reaction. At 140 K the trapped amount is close to 100% at low doses and reaches saturation at about 2 × 1018D/cm2, whereas at room temperature no saturation could be reached up to 2 × 1019 D/cm2. At higher temperatures the amount decreases until no deuterium could be detected in the surface layer above 500 K. The depth profiles are strongly dependent on temperature. At 140 K the deuterium is found in a surface layer of about 2000 A with a maximum ratio of deuterium to metal atoms of 2.5. At room temperature a hydride layer of TiD1.8, forms. The thickness of the hydride layer depends on deuterium dose and extends to 1.5 μm at 2 × 1019 D/cm2. At higher temperatures the atom concentrations are lower and the deuterium seems to diffuse deeply into the bulk. These results are discussed in terms of diffusion of deuterium i n Ti and titanium hydride.
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