论文标题
通过喷雾热解方法对钙钛矿太阳能电池的氧化石墨烯薄膜的沉积沉积
Deposition of Reduced Graphene Oxide Thin Film by Spray Pyrolysis Method for Perovskite Solar Cell
论文作者
论文摘要
钙钛矿吸收层,电子传输层(ETL),孔传输层(HTL)和透明导电氧化物层(TCO)是构成钙钛矿太阳能电池的主要组件。在ETL和HTL之间,将吸收层夹杂,在吸收太阳辐射后,在其上产生了电子孔对。尽管朝着效率取得了长足的进步,但长期稳定仍然是一个严重的关注。目前的工作着重于通过将二氧化钛(TIO2)作为ETL和减少氧化石墨烯(RGO)作为HTL来贡献以后的问题。具体而言,在目前的工作中,我们报告了我们在制备紧凑型二氧化钛(C-TIO2)和介孔二氧化钛(M-TIO2)层作为ETL和减少石墨烯氧化物薄膜作为HTL的努力。 C-Tio2膜是在FTO玻璃上旋转的,然后使用刀片技术铸造M-Tio2膜。同样,RGO膜是通过在玻璃基板上喷涂的。通过测量其光学特性(薄膜的透射率和反射率)来表征所示的ETL和HTL层。然后,从ETL和HTL分别从反射率和透射曲线中提取带隙。在RGO的情况下,我们发现EG的值为2.1 eV,根据先前报道的值的降低水平,在2.7EV和0.02EV之间变化。同样,添加M-TIO2后,C-TIO2的带隙为4.51 eV,降低至4.12 eV,比以前报道的值高0.9至1.1 eV。但是,在C-TIO2上使用M-TIO2后,带隙显示出趋势下降。在钙钛矿太阳能电池中,将研究ETL和HTL。
The Perovskite absorber layer, the electron transport layer (ETL), the hole transport layer (HTL), and the transparent conducting oxide layer (TCO) are the major components that make up a Perovskite solar cell. Between ETL and HTL, the absorber layer is sandwiched, on which electron-hole pairs are created after absorption of solar radiation. Despite substantial progress toward efficiency, long-term stability still remains a serious concern. Present work focuses toward contributing on the later issue by adopting Titanium dioxide (TiO2) as ETL and reduced graphene oxide (rGO) as HTL. Specifically, in the present work, we report our efforts on the preparation of compact titanium dioxide (C-TiO2) and mesoporous titanium dioxide (M-TiO2) layers as an ETL and a reduced graphene oxide thin film as a HTL. The C-TiO2 film was spin casted on FTO glass followed by casting of M-TiO2 film using Doctor Blading technique. Similarly, the rGO film was produced by spray casting over the glass substrate. The as-prepared ETL and HTL layers were characterized by measuring their optical properties (transmittance and reflectance of thin films). Then, the bandgap, Eg was extracted from reflectance and transmittance curves for ETL and HTL respectively. In the case of rGO, we found the value of Eg to be 2.1 eV, which varies between 2.7eV and 0.02eV depending upon its reduction level based on the previously reported values. Similarly, the bandgap of the C-TiO2 was 4.51 eV which was reduced to 4.12 eV after the addition of M-TiO2, which are 0.9 to 1.1 eV higher than previously reported values. However, bandgap shows decreasing trend after employing M- TiO2 over C-TiO2. In a Perovskite solar cell, both ETL and HTL will be investigated.