依据实验组前期对CU2O薄膜沉积的实验,选择-0.4mA进行两电极的恒流沉积,并用椭偏仪进行在位监测,每沉积180s后进行300nm到800nm的椭偏测试。即在沉积180s、360s、540s、720s、900s、1080s后分别进行了椭偏仪全谱测试,测试角度为70°。
展示全部
椭偏仪在位表征电化学沉积的系统搭建(二十八)- 中心能量的演变
1.短波范围
图4-13是CU2O激迁图(b)和300nm-500nm拟合得到的不同沉积时间中心能量值(a)。从图4-1(a)中看到,在有自旋能级分裂时,一部分CU2O激子跃迁将如图所示。图(a)是在300nm-500nm波段用四振子Lorentz Oscillator+Drude模型拟合得到的不同沉积时间下的中心能量以及代表了不同类型的激子激发相应的能量线。可以看到180 s和900s得到了三个拟合中心能量,其余时间得到了四个中心能量。从中心能量与横线的对比中看出,在沉积时间为180s时的三个中心能量分别为EOA/EOB(EOA/EOB表示该能量是EOA或者EOB激子吸收峰)、EOC/EOD和E1A激子吸收峰;360s出现的前两个能量为EOA/EOB激子吸收峰,后两个能量分别为EOC/EOD和E1A激子吸收峰;540s前两个能量分别为EOC/EOD和E1A激子吸收峰,后两个能量可能是E1B激子吸收峰,同时也可能是E2能级上的电子跃迁吸收峰;720s第1个能量为EOC/EOD激子吸收峰,中间两个为E1A激子吸收峰,zui后一个能量超过在16eV,可引发E0、E1及E2能带的跃迁,具体属于哪个激子吸收峰有待进一步验证;900s时的三个中心能量分别为EOC/EOD、E1A和E1B激子吸收峰;1080s的四个中心能量分别属于EODA、EOC、EOD 和E1A激子吸收峰。
图4-13 (a)300nm-500nm拟合得到的不同沉积时间中心能量值;
(b)CU2O激子跃迁图
2.长波范围
由于对0s时和其他沉积时间用的拟合方法是逐点拟合,所以不能得到相应的中心能量值,但是可以通过把拟合得到的值和对应的能量相关联,画出0s时300nm-800nm及其余时间500nm-800nm的图,在对曲线线性部分进行拟合,得到的E轴的截距即为中心能量,如4-14所示。图4-14(a)是不同时间得到的在能量为1.55-2.48eV范围曲线,可以看到0s于2.1eV后增加较快,且存1处的线性变化段。其余不同沉积时间得到的图线变化不大,在1.55-2.1eV段与0s的重合;在2.1-2.48eV段180s的增加后基本稳定,720s的介于180s和其余时间之间。整体上认为1.55-2.4eV段更多反映的是基底的信息,没有线性变化的阶段。图4-14(b)是0s时1.55eV-4.13eV的图线,可看到除了前面提到的线性拟合段,在后面2.48-4.13eV段又存在两个线性变化的区域,拟合如图。
图4-14(c)是0s时3段线性拟合得到的E轴截距,对应于材料的能隙或电子的跃迁光吸收。从图可知前两个截距在2-3eV之间,zui后一个在3-4eV之间,所以0s时对应三个能量。前两个可能对应Au基底的表面等离子体共振吸收峰,zui后一个可能对应3d、4d和6sp的带间跃迁吸收以及6sp到7sp的导带间跃迁吸收。
图4-14 随E的变化及不同波段拟合
(a) 不同时间1.55-2.48eV;
(b)0s对应的1.55eV-4.13eV;
(c)0s对应的拟合得到的E轴截距
了解更多椭偏仪详情,请访问上海昊量光电的官方网页:
https://www.auniontech.com/three-level-56.html
更多详情请联系昊量光电/欢迎直接联系昊量光电
关于昊量光电:
上海昊量光电设备有限公司是光电产品专业代理商,产品包括各类激光器、光电调制器、光学测量设备、光学元件等,涉及应用涵盖了材料加工、光通讯、生物医疗、科学研究、国防、量子光学、生物显微、物联传感、激光制造等;可为客户提供完整的设备安装,培训,硬件开发,软件开发,系统集成等服务。
您可以通过我们昊量光电的官方网站www.auniontech.com了解更多的产品信息,或直接来电咨询4006-888-532。
参考文献
[1] WONG H S P, FRANK D J, SOLOMON P M et al. Nanoscale cmos[J]. Proceedings of the IEEE, 1999, 87(4): 537-570.
[2] LOSURDO M, HINGERL K. ellipsometry at the nanoscale[M]. Springer Heidelberg New York Dordrecht London. 2013.
[3] DYRE J C. Universal low-temperature ac conductivity of macroscopically disordered nonmetals[J]. Physical Review B, 1993, 48(17): 12511-12526. DOI:10.1103/PhysRevB.48.12511.
[4] CHEN S, KÜHNE P, STANISHEV V et al. On the anomalous optical conductivity dISPersion of electrically conducting polymers: Ultra-wide spectral range ellipsometry combined with a Drude-Lorentz model[J]. Journal of Materials Chemistry C, 2019, 7(15): 4350-4362.
[5] 陈篮,周岩. 膜厚度测量的椭偏仪法原理分析[J]. 大学物理实验, 1999, 12(3): 10-13.
[6] ZAPIEN J A, COLLINS R W, MESSIER R. Multichannel ellipsometer for real time spectroscopy of thin film deposition from 1.5 to 6.5 eV[J]. Review of Scientific Instruments, 2000, 71(9): 3451-3460.
[7] DULTSEV F N, KOLOSOVSKY E A. Application of ellipsometry to control the plasmachemical synthesis of thin TiONx layers[J]. Advances in Condensed Matter Physics, 2015, 2015: 1-8.
[8] DULTSEV F N, KOLOSOVSKY E A. Application of ellipsometry to control the plasmachemical synthesis of thin TiONx layers[J]. Advances in Condensed Matter Physics, 2015, 2015: 1-8.
[9] YUAN M, YUAN L, HU Z et al. In Situ Spectroscopic Ellipsometry for Thermochromic CsPbI3 Phase Evolution Portfolio[J]. Journal of Physical Chemistry C, 2020, 124(14): 8008-8014.
[10] 焦杨景.椭偏仪在位表征电化学沉积的系统搭建.云南大学说是论文,2022.
[11] CANEPA M, MAIDECCHI G, TOCCAFONDI C et al. Spectroscopic ellipsometry of self assembLED monolayers: Interface effects. the case of phenyl selenide SAMs on gold[J]. Physical Chemistry Chemical Physics, 2013, 15(27): 11559-11565. DOI:10.1039/c3cp51304a.
[12] FUJIWARA H, KONDO M, MATSUDA A. Interface-layer formation in microcrystalline Si:H growth on ZnO substrates studied by real-time spectroscopic ellipsometry and infrared spectroscopy[J]. Journal of Applied Physics, 2003, 93(5): 2400-2409.
[13] FUJIWARA H, TOYOSHIMA Y, KONDO M et al. Interface-layer formation mechanism in (formula presented) thin-film growth studied by real-time spectroscopic ellipsometry and infrared spectroscopy[J]. Physical Review B - Condensed Matter and Materials Physics, 1999, 60(19): 13598-13604.
[14] LEE W K, KO J S. Kinetic model for the simulation of hen egg white lysozyme adsorption at solid/water interface[J]. Korean Journal of Chemical Engineering, 2003, 20(3): 549-553.
[15] STAMATAKI K, PAPADAKIS V, EVEREST M A et al. Monitoring adsorption and sedimentation using evanescent-wave cavity ringdown ellipsometry[J]. Applied Optics, 2013, 52(5): 1086-1093.
[16] VIEGAS D, FERNANDES E, QUEIRÓS R et al. Adapting Bobbert-Vlieger model to spectroscopic ellipsometry of gold nanoparticles with bio-organic shells[J]. Biomedical Optics Express, 2017, 8(8): 3538.
[17] ARWIN H. Application of ellipsometry techniques to biological materials[J]. Thin Solid Films, 2011, 519(9): 2589-2592.
[18] ZIMMER A, VEYS-RENAUX D, BROCH L et al. In situ spectroelectrochemical ellipsometry using super continuum white laser: Study of the anodization of magnesium alloy [J]. Journal of Vacuum Science & Technology B, 2019, 37(6): 062911.
[19] ZANGOOIE S, BJORKLUND R, ARWIN H. Water Interaction with Thermally Oxidized Porous Silicon Layers[J]. Journal of The Electrochemical Society, 1997, 144(11): 4027-4035.
[20] KYUNG Y B, LEE S, OH H et al. Determination of the optical functions of various liquids by rotating compensator multichannel spectroscopic ellipsometry[J]. Bulletin of the Korean Chemical Society, 2005, 26(6): 947-951.
[21] OGIEGLO W, VAN DER WERF H, TEMPELMAN K et al. Erratum to ― n-Hexane induced swelling of thin PDMS films under non-equilibrium nanofiltration permeation conditions, resolved by spectroscopic ellipsometry‖ [J. Membr. Sci. 431 (2013), 233-243][J]. Journal of Membrane Science, 2013, 437: 312..
[22] BROCH L, JOHANN L, STEIN N et al. Real time in situ ellipsometric and gravimetric monitoring for electrochemistry experiments[J]. Review of Scientific Instruments, 2007, 78(6).
[23] BISIO F, PRATO M, BARBORINI E et al. Interaction of alkanethiols with nanoporous cluster-assembled Au films[J]. Langmuir, 2011, 27(13): 8371-8376.
[24] 李广立. 氧化亚铜薄膜的制备及其光电性能研究[D]. 西南交通大学, 2016.
[25] 董金矿. 氧化亚铜薄膜的制备及其光催化性能的研究[D]. 安徽建筑大学, 2014.
[26] 张桢. 氧化亚铜薄膜的电化学制备及其光催化和光电性能的研究[D]. 上海交通大学材料科 学与工程学院, 2013.
[27] DISSERTATION M. Cellulose Derivative and Lanthanide Complex Thin Film Cellulose Derivative and Lanthanide Complex Thin Film[J]. 2017.
[28] NIE J, YU X, HU D et al. Preparation and Properties of Cu2O/TiO2 heterojunction Nanocomposite for Rhodamine B Degradation under visible light[J]. ChemistrySelect, 2020, 5(27): 8118-8128.
[29] STRASSER P, GLIECH M, KUEHL S et al. Electrochemical processes on solid shaped nanoparticles with defined facets[J]. Chemical Society Reviews, 2018, 47(3): 715-735.
[30] XU Z, CHEN Y, ZHANG Z et al. Progress of research on underpotential deposition——I. Theory of underpotential deposition[J]. Wuli Huaxue Xuebao/ Acta Physico - Chimica Sinica, 2015, 31(7): 1219-1230.
[31] PANGAROV n. Thermodynamics of electrochemical phase formation and underpotential metal deposition[J]. Electrochimica Acta, 1983, 28(6): 763-775.
[32] KAYASTH S. ELECTRODEPOSITION STUDIES OF RARE EARTHS[J]. Methods in Geochemistry and Geophysics, 1972, 6(C): 5-13.
[33] KONDO T, TAKAKUSAGI S, UOSAKI K. Stability of underpotentially deposited Ag layers on a Au(1 1 1) surface studied by surface X-ray scattering[J]. Electrochemistry Communications, 2009, 11(4): 804-807.
[34] GASPAROTTO L H S, BORISENKO N, BOCCHI N et al. In situ STM investigation of the lithium underpotential deposition on Au(111) in the air- and water-stable ionic liquid 1-butyl-1-methylpyrrolidinium bis(trifluoromethylsulfonyl)amide[J]. Physical Chemistry Chemical Physics, 2009, 11(47): 11140-11145.
[35] SARABIA F J, CLIMENT V, FELIU J M. Underpotential deposition of Nickel on platinum single crystal electrodes[J]. Journal of Electroanalytical Chemistry, 2018, 819(V): 391-400.
[36] BARD A J, FAULKNER L R, SWAIN E et al. Fundamentals and Applications[M]. John Wiley & Sons, Inc, 2001.
[37] SCHWEINER F, MAIN J, FELDMAIER M et al. Impact of the valence band structure of Cu2O on excitonic spectra[J]. Physical Review B, 2016, 93(19): 1-16.
[38] XIONG L, HUANG S, YANG X et al. P-Type and n-type Cu2O semiconductor thin films: Controllable preparation by simple solvothermal method and photoelectrochemical properties[J]. Electrochimica Acta, 2011, 56(6): 2735-2739.
[39] KAZIMIERCZUK T, FRÖHLICH D, SCHEEL S et al. Giant Rydberg excitons in the copper oxide Cu2O[J]. Nature, 2014, 514(7522): 343-347.
[40] RAEBIGER H, LANY S, ZUNGER A. Origins of the p-type nature and cation deficiency in Cu2 O and related materials[J]. Physical Review B - Condensed Matter and Materials Physics, 2007, 76(4): 1-5.
[41] 舒云. Cu2O薄膜的电化学制备及其光电化学性能的研究[D]. 云南大学物理与天文学院,2019.
展示全部