Zeng Guanggen, Harrison Paul, Kidman Ali, Al-Mebir Alaa, Feng Lianghuan, Wu Judy
Department of Physics and Astronomy, University of Kansas, Kansas, USA College of Materials Science and Engineering, Sichuan University, China
Department of Physics and Astronomy, University of Kansas, Kansas, USA.
Appl Spectrosc. 2016 Sep;70(9):1555-60. doi: 10.1177/0003702816643545. Epub 2016 May 11.
Raman spectra specific to CdS and CdTe were obtained on the CdS/CdTe heterojunction interface by employing two excitation wavelengths of λ1 = 488 nm and λ2 = 633 nm, respectively, from the glass side of Glass/FTO/CdS/CdTe/HgTe:Cu:graphite/Ag solar cells fabricated using pulsed-laser deposition (PLD). This two-wavelength Raman spectroscopy approach, with one wavelength selected below the absorption edge of the window layer (λ2 in this case), allows nondestructive characterization of the CdS/CdTe heterojunction and therefore correlation of the interfacial properties with the solar cell performance. In this study, the evolution of the interfacial strain relaxation during cell fabrication process was found to be affected not only by the inter-diffusion of S and Te corresponding to the formation of CdSxTe1-x ternary alloy with a various x from ∼0.01 to ∼0.067, but also by the variation in misfit dislocations (MDs) at CdS/CdTe interface from Raman TO/LO ratio ∼2.85 for as-deposited sample to TO/LO ∼4.44 for the cells post treatment. This is consistent with the change of the Urbach energy from 0.03 eV to 0.09 eV, indicative of the deterioration of crystalline quality of CdTe at interface although improved CdTe crystalline quality was observed away from the interface after the CdCl2 annealing. This difference crucially impacted on the rectification characteristics of the CdS/CdTe heterojunction and therefore the solar cell performance.
通过使用脉冲激光沉积(PLD)制备的Glass/FTO/CdS/CdTe/HgTe:Cu:石墨/Ag太阳能电池的玻璃侧,分别采用λ1 = 488 nm和λ2 = 633 nm的两个激发波长,在CdS/CdTe异质结界面获得了特定于CdS和CdTe的拉曼光谱。这种双波长拉曼光谱方法,其中一个波长选择在窗口层的吸收边缘以下(在这种情况下为λ2),允许对CdS/CdTe异质结进行无损表征,从而将界面特性与太阳能电池性能相关联。在本研究中,发现电池制造过程中界面应变弛豫的演变不仅受到对应于形成x从0.01到0.067变化的CdSxTe1-x三元合金的S和Te的相互扩散的影响,还受到CdS/CdTe界面处失配位错(MDs)变化的影响,从沉积态样品的拉曼TO/LO比2.85到处理后电池的TO/LO4.44。这与Urbach能量从0.03 eV变化到0.09 eV一致,表明尽管在CdCl2退火后远离界面处观察到CdTe晶体质量有所改善,但界面处CdTe的晶体质量仍在恶化。这种差异对CdS/CdTe异质结的整流特性以及因此对太阳能电池性能产生了至关重要的影响。