TY - JOUR
T1 - Carrier Recombination and Diffusion in Wet-Cast Tin Iodide Perovskite Layers under High Intensity Photoexcitation
AU - Ščajev, Patrik
AU - Aleksiejū Nas, Ramū Nas
AU - Baronas, Paulius
AU - Litvinas, Džiugas
AU - Kolenda, Marek
AU - Qin, Chuanjiang
AU - Fujihara, Takashi
AU - Matsushima, Toshinori
AU - Adachi, Chihaya
AU - Juršėnas, Saulius
N1 - Funding Information:
Vilnius University team acknowledges the financial support provided by Research Council of Lithuania under the project no. S-MIP-17-71. Additionally, this work was supported by the Japan Science and Technology Agency (JST), ERATO, Adachi Molecular Exciton Engineering Project (grant number JPMJER1305), JSPS KAKENHI (grant nos. JP15K14149 and JP16H04192), and The Canon Foundation.
Publisher Copyright:
Copyright © 2019 American Chemical Society.
PY - 2019/8/15
Y1 - 2019/8/15
N2 - Tin iodide perovskite CH3NH3SnI3 is often considered as a replacement for toxic lead halide perovskites. Tin iodide is not only suitable for production of solar cells, but also it emits in the near-infrared spectral region, which is unique among the metal halide perovskites. On the downside, the CH3NH3SnI3 layers tend to be of high unintentional p-type doping, which significantly limits the solar cell efficiency. On the other hand, it is little known how this doping could affect other optical and electrical properties important for light-emitting applications. Here, we present an optical study of carrier diffusion and recombination pathways by time-resolved photoluminescence, differential transmission, and light induced transient grating techniques at excitations close to the lasing regime. We investigate several CH3NH3SnI3 layers formed by a solvent bathing method and using different antisolvents, causing different structural quality and doping level of the layers. We observe the amplified spontaneous emission with a threshold excitation as low as 5 μJ/cm2 however, the threshold is sensitive to structural quality and increases significantly in the layers with larger surface roughness. We present an all-optical method to determine the equilibrium density of holes, which varies in the range of 0.7-5.0 × 1018 cm-3, depending on the antisolvent used for production of a particular layer. Finally, we observe band-like diffusion of carriers with high values of ambipolar diffusion coefficient: it grows from 0.5 to 1.5 cm2/s with excitation due to carrier degeneracy. High diffusivity, large quantum yield even at low densities, and low stimulated emission threshold allow us to argue that unintentional p-type doping can be beneficial for light emitting applications.
AB - Tin iodide perovskite CH3NH3SnI3 is often considered as a replacement for toxic lead halide perovskites. Tin iodide is not only suitable for production of solar cells, but also it emits in the near-infrared spectral region, which is unique among the metal halide perovskites. On the downside, the CH3NH3SnI3 layers tend to be of high unintentional p-type doping, which significantly limits the solar cell efficiency. On the other hand, it is little known how this doping could affect other optical and electrical properties important for light-emitting applications. Here, we present an optical study of carrier diffusion and recombination pathways by time-resolved photoluminescence, differential transmission, and light induced transient grating techniques at excitations close to the lasing regime. We investigate several CH3NH3SnI3 layers formed by a solvent bathing method and using different antisolvents, causing different structural quality and doping level of the layers. We observe the amplified spontaneous emission with a threshold excitation as low as 5 μJ/cm2 however, the threshold is sensitive to structural quality and increases significantly in the layers with larger surface roughness. We present an all-optical method to determine the equilibrium density of holes, which varies in the range of 0.7-5.0 × 1018 cm-3, depending on the antisolvent used for production of a particular layer. Finally, we observe band-like diffusion of carriers with high values of ambipolar diffusion coefficient: it grows from 0.5 to 1.5 cm2/s with excitation due to carrier degeneracy. High diffusivity, large quantum yield even at low densities, and low stimulated emission threshold allow us to argue that unintentional p-type doping can be beneficial for light emitting applications.
UR - http://www.scopus.com/inward/record.url?scp=85071699686&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85071699686&partnerID=8YFLogxK
U2 - 10.1021/acs.jpcc.9b03226
DO - 10.1021/acs.jpcc.9b03226
M3 - Article
AN - SCOPUS:85071699686
SN - 1932-7447
VL - 123
SP - 19275
EP - 19281
JO - Journal of Physical Chemistry C
JF - Journal of Physical Chemistry C
IS - 32
ER -