首页> 外文OA文献 >Reactive pulsed laser ablation deposition (RPLAD) of indium tin oxide (ITO), titanium dioxide (TiO2) thin films and gold (AU) nanoparticles for dye sensitised solar cells (DSSC) applications
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Reactive pulsed laser ablation deposition (RPLAD) of indium tin oxide (ITO), titanium dioxide (TiO2) thin films and gold (AU) nanoparticles for dye sensitised solar cells (DSSC) applications

机译:铟锡氧化物(ITO),二氧化钛(TiO2)薄膜和金(AU)纳米粒子的反应性脉冲激光烧蚀沉积(RPLAD),用于染料敏化太阳能电池(DSSC)应用

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摘要

ABSTRACTudThe focus of this work was the study possible ways to improve the efficiency of solar cells. To this end, the main aim was to investigate the deposition process of Indium Tin Oxide (ITO), Titanium Dioxide (TiO2), multi-layers ITO/TiO2 on quartz SiO2 substrates under different conditions (oxygen pressure, laser fluence and wavelength, and temperature) and later gold nanoparticles by the Reactive Pulsed Laser Ablation Deposition (RPLAD) technique. It was intended to investigate their electrical structural and optical properties under selected conditions for possible application to Dye Sensitised Solar Cells (DSSC).udUnder optimised conditions, maximum deposition rates of 12nm/min for ITO and 21nm/min for TiO2 thin films were achieved. Rutherford Backscattering Spectrometry (RBS) with 2MeV He+ ions was used to measure the films thickness. Uniform thicknesses over a large area were found to be about 400nm and 800nm for ITO and TiO2 films, respectively. Crystalline properties were studied via x-ray diffraction and Raman spectroscopy. X-ray Diffraction (XRD) analysis revealed that the ITO films are highly orientated nanocrystals with their a-axis normal to the glass substrate surface. The average particle size of the precipitated nanocrystals was calculated to be 10-15nm.udThe structure of the films was characterised via Atomic Force Microscopy (AFM) imaging of the top surface of the film. The films have a rough surface with average roughness of 26-30nm. Pores were observed with a density of 144 and 125 pores/mm2 and average size of 150 and 110nm for ITO films deposited at 200 and 400°C, respectively. TiO2 films deposited on the prepared ITO films were less crystalline. Annealing was performed at 300 and 500°C for 3 consecutive hours and the XRD results show that the transformation of TiO2 film into anatase phase was almost complete with a crystal size of ~ 6-7nm.udScanning Transmission Electron Microscopy (STEM) of the surfaces was also performed. The TiO2 films deposited onto the prepared ITO films present a udrelatively high pore size with an average pore diameter of ~ 40nm and excellent uniformity. It is interesting to note that the pores are randomly arranged. The random arrangement of the pores network may actually be beneficial for producing a uniform electrode. In addition, STEM cross-sectional analysis of the films showed a columnar structure but no evidence of voids in the structure. The large surface area produced suggests applications in DSSC.udThe electrical properties of the films were investigated and an estimation of resistivity and Hall mobility was made. Low values of resistivity and high values of mobility were observed for ITO films. The resistivity of the film increases with increasing thickness while it decreases when increasing the deposition temperature. The lowest value was found to be 1.5x10-6Ωm for ITO films deposited at 400°C. Hall mobility was found to increase with substrate temperature. In this investigation, the highest Hall mobility at room temperature was estimated to be 22.3cm2/Vs under ambient O2 pressure (PO2) of 1Pa and 52.1 and 51.3cm2/Vs for films deposited at 200 and 400°C, respectively. But the best ITO film was deposited at 200°C, since this film combines good resistivity, good Hall mobility and good transmittance.udUV-VIS-IR transmission spectra were recorded on a Perkin Elmer Lambda 900. From the transmission data, the energy gap as well as the optical constant was estimated. A high transmission for ITO films in the visible (Vis) range was observed which was above 88% for films produced at room temperature and above 95% for those deposited at 200°C. The transmission for the films produced in oxygen was about 90% above 400nm, whereas it lies between 70 and 80% for films produced in rare gases. An increase in the band gap was observed by increasing the oxygen pressure and substrate temperature for ITO films. Increasing the quartz SiO2 substrate temperature from room temperature to 400 °C resulted in an increase of the transmission of TiO2 films, mostly in the Visible Near Infrared (Vis-NIR) from about 70% to 92%. After annealing at 500°C for 3 consecutive hours, the transmission of TiO2 film further sharply decreases toward shorter wavelengths. udAnalysis of the transmittance curve of TiO2/Au shows a decrease of about 6% of the transmission in the Ultraviolet Visible (UV-Vis) range.udOptical absorption edge analysis showed that the optical density could be used to detect the film growth conditions and to correlate the film structure and the absorption edge. The TiO2 films deposited present a direct band gap at 3.51eV and 3.37eV for TiO2 as deposited and after annealing, respectively, while the indirect band gap was found to be 3.55eV and 3.26eV for TiO2 films as deposited and after annealing, respectively. There was a shift of about 0.1eV between as deposited ITO monolayer films and ITO/TiO2 bilayers deposited at 200°C. A small shift towards shorter wavelengths has been observed for multilayer ITO/TiO2/Au. In this case, the increase of Eg was ascribed to a reduction of the oxygen vacancies with increasing substrate temperature at which the ITO film was deposited.udThe change in the shape of the fundamental absorption edge is considered to reflect the variation of density and the short range structural modifications undetected by structural characterisations. Enlargement of band-gap energies of semiconductors may be advantageous when used in DSSC to suppress the charge recombination between the reduced electrolytes and the photo-excited holes in the valence band of TiO2 substrates and enhance the open-circuit potential of the cell. When ITO/TiO2 bilayers were annealed before depositing Au, the gap energy remained constant.
机译:摘要 ud这项工作的重点是研究提高太阳能电池效率的可能方法。为此,主要目的是研究氧化铟锡(ITO),二氧化钛(TiO2),多层ITO / TiO2在石英SiO2基板上在不同条件(氧气压力,激光通量和波长以及温度和更高的金纳米粒子的反应脉冲激光烧蚀沉积(RPLAD)技术。旨在研究其在选定条件下的电结构和光学性能,以可能应用于染料敏化太阳能电池(DSSC)。 ud在最佳条件下,ITO的最大沉积速率为12nm / min,TiO2薄膜的最大沉积速率为21nm / min 。具有2MeV He +离子的卢瑟福背散射光谱(RBS)用于测量薄膜厚度。对于ITO和TiO 2膜,发现大面积上的均匀厚度分别为约400nm和800nm。通过X射线衍射和拉曼光谱研究了晶体性质。 X射线衍射(XRD)分析表明,ITO膜是高度取向的纳米晶体,其a轴垂直于玻璃基板表面。沉淀的纳米晶体的平均粒径经计算为10-15nm。ud通过膜的顶表面的原子力显微镜(AFM)成像来表征膜的结构。该膜具有粗糙的表面,其平均粗糙度为26-30nm。对于分别在200和400°C沉积的ITO膜,观察到的孔分别具有144和125孔/ mm2的密度以及150和110nm的平均尺寸。沉积在制备的ITO膜上的TiO2膜的结晶度较低。退火在300和500°C下连续进行了3个小时,XRD结果表明TiO2薄膜向锐钛矿相的转变几乎完成,晶体尺寸约为6-7nm。 ud扫描电子显微镜(STEM)还进行了表面处理。沉积在制备的ITO膜上的TiO2膜具有相对较高的孔径,平均孔径约为40nm,并且具有出色的均匀性。有趣的是,孔是随机排列的。孔网络的无规排列实际上可能对于产生均匀的电极是有益的。此外,薄膜的STEM横截面分析显示为柱状结构,但没有证据显示结构中有空隙。产生的大表面积表明其在DSSC中的应用。 ud研究了薄膜的电性能,并估算了电阻率和霍尔迁移率。对于ITO膜,观察到低电阻率值和高迁移率值。膜的电阻率随厚度增加而增加,而当沉积温度升高时电阻率则降低。发现在400℃下沉积的ITO膜的最低值为1.5×10-6Ωm。发现霍尔迁移率随衬底温度而增加。在这项研究中,室温下的最高霍尔迁移率在1Pa的环境O2压力(PO2)下估计分别为22.3cm2 / Vs,在200和400°C下沉积的薄膜分别为52.1和51.3cm2 / Vs。但是最好的ITO膜是在200°C时沉积的,因为该膜具有良好的电阻率,良好的霍尔迁移率和良好的透射率。 udUV-VIS-IR透射光谱记录在Perkin Elmer Lambda 900上。根据透射数据,能量估计间隙和光学常数。观察到的ITO膜在可见光(Vis)范围内的高透射率,在室温下生产的膜高于88%,在200°C沉积的膜高于95%。在400nm以上的氧气中生成的薄膜的透射率约为90%,而在稀有气体中生成的薄膜的透射率在70%至80%之间。通过增加ITO膜的氧气压力和衬底温度,可以观察到带隙的增加。将石英SiO2衬底的温度从室温提高到400°C,导致TiO2薄膜的透射率增加,大部分在可见近红外(Vis-NIR)中从大约70%增加到92%。在500°C下连续退火3小时后,TiO2薄膜的透射率进一步朝着更短的波长急剧下降。 ud对TiO2 / Au的透射率曲线的分析表明,在紫外可见(UV-Vis)范围内,透射率下降了约6%。 ud光学吸收边缘分析表明,光密度可用于检测膜的生长条件并使膜结构和吸收边缘相关。沉积的TiO2薄膜在沉积和退火后分别具有3.51eV和3.37eV的直接带隙,而在沉积的TiO2薄膜和退火后的间接带隙分别为3.55eV和3.26eV。, 分别。沉积的ITO单层薄膜和200°C沉积的ITO / TiO2双层薄膜之间存在约0.1eV的偏移。对于多层ITO / TiO2 / Au,已经观察到向较短波长的微小变化。在这种情况下,Eg的增加归因于随着沉积ITO膜的衬底温度的升高,氧空位的减少。 ud基本吸收边缘形状的变化被认为反映了密度和光吸收率的变化。结构特征未发现的短程结构修改。当在DSSC中使用时,半导体的带隙能的增大可能是有利的,以抑制还原的电解质与TiO 2衬底的价带中的光激发空穴之间的电荷复合,并增强电池的开路电势。当在沉积Au之前对ITO / TiO2双层进行退火时,间隙能保持恒定。

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    Fotsa-Ngaffo Fernande;

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