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absence of the phase transition for MAPbI3-xClx, we first study the crystallization
processofMAPbI3-xClx byonestepdepositionmethod.
resulted
in better performance of the solar cells.
3.3.
One Step
Deposition of
MAPbI3‐xClx
The better crystallization of MAPbI3‐xClx along (110) and (220) plane of the tetragonal phase or
(100) and (200) planes of the cubic phase may be due to the lowered cubic‐tetragonal phase
transition temperature of MAPbI3−xClx after the incorporation of Cl− [82]. A clear cubic‐tetragonal
phase transition temperature of MAPbI3 was detected by differential scanning calorimeter (DSC)
analysis [65], however no such phase transition was observed for MAPbI3−xClx [83]. To explain the
absence of the phase transition for MAPbI3−xClx, we first study the crystallization process of
MAPbI3‐xClx by one
step deposition method.
Figure 4. XRD patterns and optical images (insets) of MAPbI3‐xClx film during annealing. Reprinted
from reference
[84], Copyright © 2015, American Chemical
Society.
Detail information about crystal formation process of MAPbI3 is summarized in reference [85].
For MAPbI3‐xClx, the transformation from the intermediate phase to the perovskite is determined as
Figure 4. XRD patterns and opt cal i ages (insets) of MAPbI3-xClx film
during annealing. Reprinted from reference [84], Copyright © 2015, American
ChemicalSociety.
Detail informationaboutcrystal formationprocessofMAPbI3 is summarized
inreference [85]. ForMAPbI3-xClx, the transformationfrom the intermediatephase
to the perovskite is determined as 80 ˝C by in situgrazing incidence wide-angle
X-ray scattering (GIWAXS) [86]. Figure 4 presents a clearer picture of the crystal
formationofMAPbI3-xClx. The15.7˝and31.5˝peaksareassociatedwiththe(100)
and (200) diffraction peaks of MAPbCl3 [82]. These peaks were also observed in
references [27,87,88]. In Figure 4, it is interesting to note that MAPbI3 was formed
first for theas-spincoatedfilmbutconvertedtoMAPbCl3 afterannealingat100˝C
for 10 min, and then MAPbCl3 was converted back to MAPbI3 after 45 min of
annealing[84]. Furtherannealingwouldresult in thedecompositionofMAPbI3 to
PbI2, but this occurred after conversion to the intermediate phase to MAPbI3 [89].
Because MAPbCl3 is in a cubic phase, we suppose that MAPbCl3 may cause a
templateeffect for thecubicMAPbI3 phase.
103
Photovoltaic Materials and Electronic Devices
- Title
- Photovoltaic Materials and Electronic Devices
- Author
- Joshua M. Pearce
- Editor
- MDPI
- Location
- Basel
- Date
- 2016
- Language
- English
- License
- CC BY-NC-ND 4.0
- ISBN
- 978-3-03842-217-4
- Size
- 17.0 x 24.4 cm
- Pages
- 216
- Keywords
- Perovskite, Plasmonics, Nanostructured Materials, Anti-Reflection Coatings, Transparent Conductive Oxides, Amorphous Silicon, Dye-sensitized Solar Cells (DSSCs) Materials, Organic Photovoltaic Materials, Solar Energy Materials
- Categories
- Naturwissenschaften Physik
- Technik