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Figure
2.
XRD
patterns
of
glass
substrates
with
vapor
deposition
of
(A)
a
layer
of
PbI2;
and
(B)
a
layer
of PbI2 followed by a layer of MAI, repeating this step 7 times; XRD pattern of the (C) annealed
7‐time deposited PbI2/MAI
layer; (D) 1‐time deposited PbI2 (50 nm thickness)/MAI (50 nm
thickness)
layer; and (E) 1‐time deposited PbI2 (150 nm thickness)/MAI (150 nm thickness) layer. Reprinted
from reference
[77], Copyright © 2015, Royal
Society
of Chemistry.
Figure 3. Crystallographic (lattice) planes (in gray) of tetragonal MAPbI3. Reprinted from reference [78],
Copyright © 2015, American Chemical Society.
For
PbCl2,
Cl−
was
detached
from
PbCl2
when
the
PbCl2
was
evaporated
on
the
MAI
substrate
[79]
and all the atoms of lead halide were dissociated during the crystal formation of the perovskite [80].
Figure 3. Crystallographic (lattice) planes (in gray) of tetragonal MAPbI3.
Reprintedfromreference [78],Copyright©2015,AmericanChemicalSociety.
For PbCl2, Cl´was detached from PbCl2 when the PbCl2 was evaporated on
the MAI substrate [79] and all the atoms of lead halide were dissociated during
the crystal formation of the perovskite [80]. Thus, except the speed and the way
of breaking the lead halide, the following steps should be similar with the one
stepmethod(Section3.3) forconvertingPbI2 orPbCl2 withMAIto theperovskite.
However, thesituation in thepresenceofMAClmaybedifferent. As lessenergy is
neededforMAClthanMAItoundergophasetransitionfromsolidtogas[69], itmay
be easier for MACl than MAI to diffuse into the PbI2 and cause the crystallization
of perovskite [81]. However, as Cl´ cannot be incorporated into MAPbI3 crystal
structure, theMAIandMAClmaycompetewitheachother todetermine theresult
crystal, because only MAPbI3 or MAPbCl3 was formed when PbI2 was soaked in
80mMMAI+40mMMAClorin40mMMAI+80mMMACl,respectively[80]. Thus,
the incorporation of some amountof MACl managed to modify the morphology of
theperovskiteandresulted inbetterperformanceof thesolarcells.
3.3.OneStepDepositionofMAPbI3-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],
howevernosuchphase transitionwasobservedforMAPbI3-xClx [83]. Toexplain the
102
Photovoltaic Materials and Electronic Devices
- Titel
- Photovoltaic Materials and Electronic Devices
- Autor
- Joshua M. Pearce
- Herausgeber
- MDPI
- Ort
- Basel
- Datum
- 2016
- Sprache
- englisch
- Lizenz
- CC BY-NC-ND 4.0
- ISBN
- 978-3-03842-217-4
- Abmessungen
- 17.0 x 24.4 cm
- Seiten
- 216
- Schlagwörter
- Perovskite, Plasmonics, Nanostructured Materials, Anti-Reflection Coatings, Transparent Conductive Oxides, Amorphous Silicon, Dye-sensitized Solar Cells (DSSCs) Materials, Organic Photovoltaic Materials, Solar Energy Materials
- Kategorien
- Naturwissenschaften Physik
- Technik