Version 2 2015-12-17, 10:46Version 2 2015-12-17, 10:46
Version 1 2015-11-11, 05:07Version 1 2015-11-11, 05:07
journal contribution
posted on 2015-12-17, 10:46authored byHui-Seon Kim, In-Hyuk Jang, Namyoung Ahn, Mansoo Choi, Antonio Guerrero, Juan Bisquert, Nam-Gyu Park
Mismatch
of current (<i>I</i>)-voltage (<i>V</i>) curves
with respect to the scan direction, so-called <i>I</i>–<i>V</i> hysteresis, raises critical issue in MAPbI<sub>3</sub> (MA = CH<sub>3</sub>NH<sub>3</sub>) perovskite solar cell.
Although ferroelectric and ion migration have been proposed as a basis
for the hysteresis, origin of hysteresis has not been apparently unraveled. We report here on the origin of <i>I</i>–<i>V</i> hysteresis of perovskite solar cell that was systematically
evaluated by the interface-dependent electrode polarizations. Frequency
(<i>f</i>)-dependent capacitance (C) revealed that the normal
planar structure with the TiO<sub>2</sub>/MAPbI<sub>3</sub>/spiro-MeOTAD
configuration showed most significant <i>I</i>–<i>V</i> hysteresis along with highest capacitance (10<sup>–2</sup> F/cm<sup>2</sup>) among the studied cell configurations. Substantial
reduction in capacitance to 10<sup>–3</sup> F/cm<sup>2</sup> was observed upon replacing TiO<sub>2</sub> with PCBM, indicative
of the TiO<sub>2</sub> layer being mainly responsible for the hysteresis.
The capacitance was intensively reduced to 10<sup>–5</sup> F/cm<sup>2</sup> and <i>C</i>–<i>f</i> feature
shifted to higher frequency for the hysteresis-free planar structures
with combination of PEDOT:PSS, NiO, and PCBM, which underlines the
spiro-MeOTAD in part contributes to the hysteresis. This work is expected
to provide a key to the solution of the problem on <i>I</i>–<i>V</i> hysteresis in perovskite solar cell.