Impact of helium ion implantation on deuterium plasma induced microstructure evolution and deuterium retention in tungsten

IF 2.8 2区 工程技术 Q3 MATERIALS SCIENCE, MULTIDISCIPLINARY
Honghui Zhang , Tongjun Xia , Yongzhi Shi , Zhengyu Jiang , Xingyu Ren , Lisha Liang , Kaigui Zhu
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Abstract

Surface blistering and internal microstructure evolutions as well as deuterium retention in tungsten with helium ion implanted followed by deuterium plasma exposure were investigated. The helium ion implantation was taken with 40 keV with a flux of 1.6 × 1017 He+/(m2s) to a fluence of 6.0 × 1020 He+/m2 at room temperature. The following deuterium plasma exposure was taken with a flux of 5.96 × 1019 D/(m2s) at a bias of 100 eV at 340 K. The deuterium plasma exposure was designed with two different durations. One is about 19 h (h) which corresponds a fluence of 4.07 × 1024 D/m2, while another is nearly 96 h corresponds a fluence of 2.06 × 1025 D/m2. The helium ion implantation itself did not induce surface blister nor detectable internal helium bubble. After subsequent deuterium exposure of 19 h, dense surface blisters appeared on the reference tungsten, while no blister was formed on the helium implanted tungsten, indicating the helium ion implantation can efficiently suppress the surface blistering. However, when the deuterium irradiation time was increased up to 96 h, sparse deuterium blisters appeared on the surface of the helium ion pre-implanted W, indicating D could pass through the helium implantation layer as the exposure time was long enough. TEM results revealed that no bubble can be observed in the reference tungsten only exposed to deuterium plasma, while bubbles can be confirmed in the helium ion pre-implanted tungsten after deuterium irradiation, suggesting that the growth of helium bubbles can be enhanced by the subsequent deuterium plasma exposure. For the deuterium plasma exposure with 19 h, the total deuterium retention in the helium ion pre-implanted tungsten was three times that of the reference tungsten, indicating the helium ion implantation could increase the deuterium retention in tungsten.
氦离子植入对氘等离子体诱导的钨微观结构演变和氘保留的影响
研究了氦离子注入后氘等离子体暴露对钨表面起泡、内部微观结构演变及氘潴留的影响。在室温条件下,以40 keV、1.6 × 1017 He+/(m2s)注入,注入量为6.0 × 1020 He+/m2。下面的氘等离子体暴露在5.96 × 1019 D/(m2s)的通量下,在100 eV的偏置下,在340 K。氘等离子体暴露时间设计为两种不同的持续时间。一个约为19 h (h),对应的影响为4.07 × 1024 D/m2,另一个约为96 h,对应的影响为2.06 × 1025 D/m2。氦离子注入本身没有引起表面起泡,也没有检测到内部氦泡。随后氘暴露19 h后,参比钨表面出现致密的水泡,而注入氦的钨表面未形成水泡,说明注入氦离子能有效抑制表面水泡。然而,当氘辐照时间增加到96 h时,预注入氦离子的W表面出现稀疏的氘泡,说明随着辐照时间足够长,D可以穿过氦注入层。透射电镜结果显示,仅暴露在氘等离子体中的参比钨未观察到气泡,而氘辐照后氦离子预注入的钨则可以证实气泡的存在,说明后续的氘等离子体暴露可以促进氦气泡的生长。在氘等离子体暴露19 h时,预注入氦离子的钨中总氘保留量是参比钨的3倍,说明氦离子注入可以增加钨中的氘保留量。
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来源期刊
Journal of Nuclear Materials
Journal of Nuclear Materials 工程技术-材料科学:综合
CiteScore
5.70
自引率
25.80%
发文量
601
审稿时长
63 days
期刊介绍: The Journal of Nuclear Materials publishes high quality papers in materials research for nuclear applications, primarily fission reactors, fusion reactors, and similar environments including radiation areas of charged particle accelerators. Both original research and critical review papers covering experimental, theoretical, and computational aspects of either fundamental or applied nature are welcome. The breadth of the field is such that a wide range of processes and properties in the field of materials science and engineering is of interest to the readership, spanning atom-scale processes, microstructures, thermodynamics, mechanical properties, physical properties, and corrosion, for example. Topics covered by JNM Fission reactor materials, including fuels, cladding, core structures, pressure vessels, coolant interactions with materials, moderator and control components, fission product behavior. Materials aspects of the entire fuel cycle. Materials aspects of the actinides and their compounds. Performance of nuclear waste materials; materials aspects of the immobilization of wastes. Fusion reactor materials, including first walls, blankets, insulators and magnets. Neutron and charged particle radiation effects in materials, including defects, transmutations, microstructures, phase changes and macroscopic properties. Interaction of plasmas, ion beams, electron beams and electromagnetic radiation with materials relevant to nuclear systems.
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