Hodille E A, Byggmästar J, Safi E, Nordlund K
Department of Physics, University of Helsinki, PO Box 43, FI-00014, Finland.
J Phys Condens Matter. 2019 May 8;31(18):185001. doi: 10.1088/1361-648X/ab04d7. Epub 2019 Feb 6.
The sputtering and reflection properties of wurtzite beryllium oxide (BeO) subjected to deuterium (D) ions bombardment at 300 K with ion energy between 10 eV and 200 eV is studied by classical molecular dynamics. Cumulative irradiations of wurtzite BeO show a D concentration threshold above which an 'unphysical dramatic' sputtering is observed. From the cumulative irradiations, simulation cells with different D concentrations are used to run non-cumulative irradiations at different concentrations. Using a D concentration close to the experimentally determined saturation concentration (0.12 atomic fraction), the simulations are able to reproduce accurately the experimental sputtering yield of BeO materials. The processes driving the sputtering of beryllium (Be) and oxygen (O) atoms as molecules are subsequently determined. At low irradiation energy, between 10 eV and 80 eV, swift chemical sputtering (SCS) is dominant and produces mostly OD molecules. At high energy, the sputtered molecules are mostly Be O molecules (mainly BeO dimer). Four different processes are associated to the formation of such molecules: the physical sputtering of BeO dimer, the delayed SCS not involving D ions and the detachment-induced sputtering. The physical sputtering of BeO dimer can be delayed if the sputtering event implies two interactions with the incoming ion (first interaction in its way in the material, the other in its way out if it is backscattered). The detachment-induced sputtering is a characteristic feature of the 'dramatic' sputtering and is mainly observed when the concentration of D is close to the threshold leading to this sputtering regime.
采用经典分子动力学方法研究了纤锌矿型氧化铍(BeO)在300 K下受到能量在10 eV至200 eV之间的氘(D)离子轰击时的溅射和反射特性。纤锌矿型BeO的累积辐照显示出一个D浓度阈值,高于该阈值时会观察到“非物理性剧烈”溅射。根据累积辐照情况,使用具有不同D浓度的模拟单元在不同浓度下进行非累积辐照。使用接近实验确定的饱和浓度(0.12原子分数)的D浓度,模拟能够准确再现BeO材料的实验溅射产率。随后确定了作为分子驱动铍(Be)和氧(O)原子溅射的过程。在低辐照能量下,即在10 eV至80 eV之间,快速化学溅射(SCS)占主导,主要产生OD分子。在高能量下,溅射的分子主要是BeO分子(主要是BeO二聚体)。此类分子形成涉及四个不同过程:BeO二聚体的物理溅射、不涉及D离子的延迟SCS以及脱附诱导溅射。如果溅射事件意味着与入射离子有两次相互作用(第一次在其进入材料的过程中,另一次在其背散射时离开材料的过程中),则BeO二聚体的物理溅射可能会延迟。脱附诱导溅射是“剧烈”溅射的一个特征,主要在D浓度接近导致这种溅射状态的阈值时观察到。