Louis-Charles Fortier , Martin Chicoine , Simon Chouteau , Mathilde Clausse , Émile Lalande , Alexandre W. Lussier , Sjoerd Roorda , Luc Stafford , Guy Terwagne , François Schiettekatte
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In addition, we observe a thin Mo layer building up at the surface, likely due to the sputtering of an electrode in the plasma source. Secondly, we etch in HF a crystalline Si (c-Si) sample with <span><math><mrow><mo><</mo><mn>100</mn><mo>></mo></mrow></math></span> surface orientation, which should leave 14 H/nm<span><math><msup><mrow></mrow><mrow><mn>2</mn></mrow></msup></math></span> bonded to the c-Si surface. The sample is then introduced in the chamber and exposed to a diffuse Ar plasma at low pressure. During plasma processing, the H surface concentration is monitored using a resonant nuclear reaction with a <sup>15</sup>N beam at 6.385 MeV. The initial H concentration is <span><math><mrow><mn>11</mn><mo>.</mo><mn>7</mn><mo>±</mo><mn>1</mn><mo>.</mo><mn>1</mn></mrow></math></span> H/nm<span><math><msup><mrow></mrow><mrow><mn>2</mn></mrow></msup></math></span>, and it decreases over a 3-minute timescale to an equilibrium concentration of <span><math><mrow><mn>6</mn><mo>.</mo><mn>0</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>8</mn></mrow></math></span> H/nm<span><math><msup><mrow></mrow><mrow><mn>2</mn></mrow></msup></math></span>. Over the range of experimental conditions investigated, the diffuse Ar plasma is therefore not able to entirely sputter the H from the c-Si surface.</p></div>","PeriodicalId":19380,"journal":{"name":"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms","volume":"554 ","pages":"Article 165439"},"PeriodicalIF":1.4000,"publicationDate":"2024-06-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0168583X2400209X/pdfft?md5=bd2a54e48ac7984501ea8664816ee10c&pid=1-s2.0-S0168583X2400209X-main.pdf","citationCount":"0","resultStr":"{\"title\":\"In Plasma ion beam analysis of polymer layer and adsorbed H monolayer etching\",\"authors\":\"Louis-Charles Fortier , Martin Chicoine , Simon Chouteau , Mathilde Clausse , Émile Lalande , Alexandre W. Lussier , Sjoerd Roorda , Luc Stafford , Guy Terwagne , François Schiettekatte\",\"doi\":\"10.1016/j.nimb.2024.165439\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>We present two experiments where a layer is plasma-etched while monitoring its evolution by <em>in plasma</em> ion beam analysis. First, we etch a photoresist with a diffuse O<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span> plasma at low pressure. Using a 4.335 MeV He beam, Rutherford Backscattering Spectrometry and Elastic Recoil Detection spectra are acquired every minute during 8 h. Etching of most elements follows a linear trend, but H desorbs faster at the beginning of the plasma process, which we ascribe to the ion beam-induced desorption. In addition, we observe a thin Mo layer building up at the surface, likely due to the sputtering of an electrode in the plasma source. Secondly, we etch in HF a crystalline Si (c-Si) sample with <span><math><mrow><mo><</mo><mn>100</mn><mo>></mo></mrow></math></span> surface orientation, which should leave 14 H/nm<span><math><msup><mrow></mrow><mrow><mn>2</mn></mrow></msup></math></span> bonded to the c-Si surface. The sample is then introduced in the chamber and exposed to a diffuse Ar plasma at low pressure. During plasma processing, the H surface concentration is monitored using a resonant nuclear reaction with a <sup>15</sup>N beam at 6.385 MeV. The initial H concentration is <span><math><mrow><mn>11</mn><mo>.</mo><mn>7</mn><mo>±</mo><mn>1</mn><mo>.</mo><mn>1</mn></mrow></math></span> H/nm<span><math><msup><mrow></mrow><mrow><mn>2</mn></mrow></msup></math></span>, and it decreases over a 3-minute timescale to an equilibrium concentration of <span><math><mrow><mn>6</mn><mo>.</mo><mn>0</mn><mo>±</mo><mn>0</mn><mo>.</mo><mn>8</mn></mrow></math></span> H/nm<span><math><msup><mrow></mrow><mrow><mn>2</mn></mrow></msup></math></span>. Over the range of experimental conditions investigated, the diffuse Ar plasma is therefore not able to entirely sputter the H from the c-Si surface.</p></div>\",\"PeriodicalId\":19380,\"journal\":{\"name\":\"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms\",\"volume\":\"554 \",\"pages\":\"Article 165439\"},\"PeriodicalIF\":1.4000,\"publicationDate\":\"2024-06-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://www.sciencedirect.com/science/article/pii/S0168583X2400209X/pdfft?md5=bd2a54e48ac7984501ea8664816ee10c&pid=1-s2.0-S0168583X2400209X-main.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0168583X2400209X\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"INSTRUMENTS & INSTRUMENTATION\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0168583X2400209X","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"INSTRUMENTS & INSTRUMENTATION","Score":null,"Total":0}
引用次数: 0
摘要
我们介绍了两项实验,在等离子体蚀刻一层的同时,通过等离子体离子束分析监控其演变过程。首先,我们在低压下使用弥散 O2 等离子体蚀刻光刻胶。大多数元素的蚀刻遵循线性趋势,但 H 在等离子过程开始时解吸较快,我们将其归因于离子束诱导的解吸。此外,我们还观察到表面形成了一层薄薄的 Mo 层,这可能是由于等离子源中的一个电极被溅射所致。其次,我们在高频中蚀刻了表面取向为 100 的晶体硅(c-Si)样品,这将使 14 H/nm2 与晶体硅表面结合。然后将样品引入腔室,在低压下暴露于弥散氩等离子体中。在等离子处理过程中,使用 6.385 MeV 的 15N 光束进行共振核反应,监测 H 的表面浓度。初始 H 浓度为 11.7±1.1 H/nm2,在 3 分钟的时间尺度内降至 6.0±0.8 H/nm2 的平衡浓度。因此,在所研究的实验条件范围内,扩散氩等离子体无法完全溅射出晶体硅表面的 H。
In Plasma ion beam analysis of polymer layer and adsorbed H monolayer etching
We present two experiments where a layer is plasma-etched while monitoring its evolution by in plasma ion beam analysis. First, we etch a photoresist with a diffuse O plasma at low pressure. Using a 4.335 MeV He beam, Rutherford Backscattering Spectrometry and Elastic Recoil Detection spectra are acquired every minute during 8 h. Etching of most elements follows a linear trend, but H desorbs faster at the beginning of the plasma process, which we ascribe to the ion beam-induced desorption. In addition, we observe a thin Mo layer building up at the surface, likely due to the sputtering of an electrode in the plasma source. Secondly, we etch in HF a crystalline Si (c-Si) sample with surface orientation, which should leave 14 H/nm bonded to the c-Si surface. The sample is then introduced in the chamber and exposed to a diffuse Ar plasma at low pressure. During plasma processing, the H surface concentration is monitored using a resonant nuclear reaction with a 15N beam at 6.385 MeV. The initial H concentration is H/nm, and it decreases over a 3-minute timescale to an equilibrium concentration of H/nm. Over the range of experimental conditions investigated, the diffuse Ar plasma is therefore not able to entirely sputter the H from the c-Si surface.
期刊介绍:
Section B of Nuclear Instruments and Methods in Physics Research covers all aspects of the interaction of energetic beams with atoms, molecules and aggregate forms of matter. This includes ion beam analysis and ion beam modification of materials as well as basic data of importance for these studies. Topics of general interest include: atomic collisions in solids, particle channelling, all aspects of collision cascades, the modification of materials by energetic beams, ion implantation, irradiation - induced changes in materials, the physics and chemistry of beam interactions and the analysis of materials by all forms of energetic radiation. Modification by ion, laser and electron beams for the study of electronic materials, metals, ceramics, insulators, polymers and other important and new materials systems are included. Related studies, such as the application of ion beam analysis to biological, archaeological and geological samples as well as applications to solve problems in planetary science are also welcome. Energetic beams of interest include atomic and molecular ions, neutrons, positrons and muons, plasmas directed at surfaces, electron and photon beams, including laser treated surfaces and studies of solids by photon radiation from rotating anodes, synchrotrons, etc. In addition, the interaction between various forms of radiation and radiation-induced deposition processes are relevant.