H. Bhuyan , M. Escalona , R. Villegas , E. Mal , M. Cisternas , P. Saikia , B. Bora , S.S. Kausik , E. Wyndham , M. Favre
{"title":"Effect of RF acetylene plasma on the composition and dynamics of a titanium plasma plume in a plasma enhanced pulsed laser deposition system","authors":"H. Bhuyan , M. Escalona , R. Villegas , E. Mal , M. Cisternas , P. Saikia , B. Bora , S.S. Kausik , E. Wyndham , M. Favre","doi":"10.1016/j.optlastec.2024.111803","DOIUrl":null,"url":null,"abstract":"<div><p>We report the effect of radio frequency (RF) acetylene plasma on the dynamics and composition of titanium (Ti) plasma plume in a plasma-enhanced pulsed laser deposition (PEPLD) system. The titanium target, mounted inside a capacitively coupled RF discharge, was ablated by using a nanosecond Nd:YAG pulsed laser at 1064 nm with a power density of 2.65 GW/cm<sup>2</sup>. The experiments were performed at different operating pressures of acetylene. Fast imaging and optical emission spectroscopy were employed to study the physics behind the pulsed laser deposition in both (PLD) and PEPLD systems. A nonlinear dependence of the plasma plume evolution was observed over a range of pressure. Different expansion regimes correspond to the pressure of the experiments. The plume expansion velocity ranges between 6 × 10<sup>3</sup> m/s and 30 × 10<sup>3</sup> m/s. Emission spectra reveal the presence of C II and Ti II lines depending on the experimental conditions. The presence of background RF plasma leads to substantial enhancement of the emission intensity of the C II spectral lines. In addition, with increasing RF power and background pressure, the intensities of the C II spectral lines increase; whereas the intensities of the Ti II spectral lines decrease with the increase in RF power. Plasma temperature was estimated from the Ti II lines using the Boltzmann plot method, whereas the electron density was estimated from the Stark-broadened Ti II line at 454.9 nm. The calculated densities and temperatures lie between 10<sup>17</sup>–10<sup>18</sup> cm<sup>−3</sup> and 0.8–2.0 eV, respectively. These results show the effects of the different backgrounds (either neutral or RF plasma) on the propagation of the laser-produced plasma (LPP), which we propose to be useful in the thin film deposition process using PLD.</p></div>","PeriodicalId":4,"journal":{"name":"ACS Applied Energy Materials","volume":null,"pages":null},"PeriodicalIF":5.4000,"publicationDate":"2024-09-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Energy Materials","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0030399224012611","RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0
Abstract
We report the effect of radio frequency (RF) acetylene plasma on the dynamics and composition of titanium (Ti) plasma plume in a plasma-enhanced pulsed laser deposition (PEPLD) system. The titanium target, mounted inside a capacitively coupled RF discharge, was ablated by using a nanosecond Nd:YAG pulsed laser at 1064 nm with a power density of 2.65 GW/cm2. The experiments were performed at different operating pressures of acetylene. Fast imaging and optical emission spectroscopy were employed to study the physics behind the pulsed laser deposition in both (PLD) and PEPLD systems. A nonlinear dependence of the plasma plume evolution was observed over a range of pressure. Different expansion regimes correspond to the pressure of the experiments. The plume expansion velocity ranges between 6 × 103 m/s and 30 × 103 m/s. Emission spectra reveal the presence of C II and Ti II lines depending on the experimental conditions. The presence of background RF plasma leads to substantial enhancement of the emission intensity of the C II spectral lines. In addition, with increasing RF power and background pressure, the intensities of the C II spectral lines increase; whereas the intensities of the Ti II spectral lines decrease with the increase in RF power. Plasma temperature was estimated from the Ti II lines using the Boltzmann plot method, whereas the electron density was estimated from the Stark-broadened Ti II line at 454.9 nm. The calculated densities and temperatures lie between 1017–1018 cm−3 and 0.8–2.0 eV, respectively. These results show the effects of the different backgrounds (either neutral or RF plasma) on the propagation of the laser-produced plasma (LPP), which we propose to be useful in the thin film deposition process using PLD.
我们报告了射频(RF)乙炔等离子体对等离子体增强脉冲激光沉积(PEPLD)系统中钛(Ti)等离子体羽流的动力学和组成的影响。使用功率密度为 2.65 GW/cm2 的纳秒级 1064 纳米 Nd:YAG 脉冲激光对安装在电容耦合射频放电管内的钛靶进行烧蚀。实验在不同的乙炔工作压力下进行。快速成像和光学发射光谱被用来研究脉冲激光沉积(PLD)和 PEPLD 系统背后的物理原理。在一定的压力范围内,观察到等离子体羽流演变的非线性依赖性。不同的膨胀状态与实验压力相对应。等离子体膨胀速度介于 6 × 103 m/s 和 30 × 103 m/s 之间。发射光谱显示,根据实验条件,存在 C II 和 Ti II 线。背景射频等离子体的存在导致 C II 光谱线的发射强度大幅增强。此外,随着射频功率和背景压力的增加,C II 光谱线的强度也会增加;而 Ti II 光谱线的强度则会随着射频功率的增加而降低。等离子体温度是利用玻尔兹曼图法从 Ti II 光谱线估算出来的,而电子密度则是根据波长为 454.9 纳米的斯塔克展宽 Ti II 光谱线估算出来的。计算得出的密度和温度分别介于 1017-1018 cm-3 和 0.8-2.0 eV 之间。这些结果显示了不同背景(中性或射频等离子体)对激光产生的等离子体(LPP)传播的影响,我们建议将其用于使用 PLD 的薄膜沉积过程。
期刊介绍:
ACS Applied Energy Materials is an interdisciplinary journal publishing original research covering all aspects of materials, engineering, chemistry, physics and biology relevant to energy conversion and storage. The journal is devoted to reports of new and original experimental and theoretical research of an applied nature that integrate knowledge in the areas of materials, engineering, physics, bioscience, and chemistry into important energy applications.