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poly-(vinylpyrrolidone) (PVP)canalso improvethesurfacecoverageofperovskite [39].
It is interestingtonotethat, forMAPbI3-xClx, asimpleannealingstepisenoughtoform
agoodcoverage[6,40], but forMAPbI3, a special step, suchasmulti-deposition[41],
adding N-cyclohexyl-2-pyrrolidone (CHP) [42], fast deposition [43–45], or air flow
duringspincoating[46,47], isneeded.
The sequential deposition method was mainly applied for MAPbI3 perovskite.
Inatypicalsynthesis, thesolutionofPbI2 inDMFwasspunonasubstrateas thefirst
step then the substrate was dipped in a solution of MAI in 2-propanol (IPA) to form
MAPbI3 crystalsas thesecondstep[48]. For the inclusionofchloride, in thefirst step
the PbCl2 can be mixed with PbI2 in DMF or dimethyl sulfoxide (DMSO) [49–52],
and/or the second step MACl can be added [53–55]. For vapor based deposition
methods, the MAPbI3-xClx can be formed by co-evaporating MAI and PbCl2 onto
thesubstrates [56,57]orbyreactingPbCl2 onsubstrateswithMAIvapor [58,59].
3. TheCrystalStructureFormandFormation
3.1. CrystalStructureofMAPbI3Layer
The parameters and transitions of phases of bulk MAPbI3 were included in
references [60,61]. Here, we focus on the tetragonal and cubic phases [62]. In fact,
therearenocriticaldifferencesbetweenthetwophases,exceptaslight rotationof
PbI6 octahedra alongthe c-axis. The atomicstructures of MAPbI3 of the two phases
areshowninFigure1A,B.Thus, the tetragonalphasecanbetreatedasapseudocubic
phase with a* = a/
?
2, c* = c/2 [63]. Below 54 ˝C, the cubic phase of MAPbI3 can
be transformed into the tetragonal phase [60], and the opposite transition occurs
by annealing at 100 ˝C for 15 min [41]. In Figure 1C, the X-ray diffraction (XRD)
patternsof the twophasesareshown. After transformationto the tetragonalphase,
the (100) and (200) peaks of cubic MAPbI3 split, also new (211) and (213) peaks show
up. Here, we use the peak splitting as indictor for phase transformation. Analysis of
theMAPbI3-xClx usuallyshowsthecubicphaseofMAPbI3,however,withamuch
more preference along (100) and (200). This will be discussed in the Sections 3.2
and3.3.
Anotherphasewhichshouldbenotedis theamorphousphase. Pairdistribution
functionanalysisofX-rayscatteringshowedthatafterannealingat100˝Cfor30min,
theMAPbI3 inmeso-porousTiO2 hasabout30atom%inmediumrangecrystalline
order and the other 70 atom% in a disordered state with a coherence length of
1.4 nm [66]. The poor crystallization of the MAPbI3 in meso-porous TiO2 was
studied by high-resolution TEM [67]. Quartz crystal microbalance measurements
suggest that during the sequential method only half of PbI2 is converted to MAPbI3
instantly, while the other half is involved in reversible transformation with MAPbI3.
Additionally, the amorphous character with a very small average crystallite size may
99
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