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better transport properties [22]. Little difference of electronic properties was
represent among orthorhombic, tetragonal and cubic phases of MAPbI3 [23],
however, the valance-band-maximum and conduction-band-minimum states can
be mainly derived from iodine ions at some unique positions, Cl´ substitution
can strengthen the unique position of the ions and result in more localized
charge density [24]. Thus, lower carrier recombination rate and enhanced carrier
transport ensued. For the interface, the (001) and (110) surfaces tend to favor hole
injection to 2,21,7,71-tetrakis(N,N-di-p-methoxyphenylamine)-9,91-spirobifluorene
(Spiro-MeOTAD), while the (100) surface facilitates electron transfer to [6,6]-phenyl
C61-butyric acid methyl ester (PCBM) [25]. A better structural matching between
adjacent rows of perovskite surface halides and TiO2 under coordinated titanium
maybethereasonfor the (110)-orientedgrowthofMAPbI3-xClx andMAPbI3 [26].
InterfacialCl´maythus furtherstabilize the (110)surfaceandmodify the interface
electronicstructurebetweenMAPbI3 andTiO2 [26].
Despite the absence of Cl´ in the perovskite, it still played an important role
in the crystallization process. For instance, the morphology of MAPbI3-xClx was
compared with MAPbI3 [27] and a model in which the Cl´ rich phase modifies the
morphologies of perovskite was proposed and fit well with the results from scanning
electronmicroscopy(SEM)[27]. Inaddition, thetransmissionelectronmicroscopy(TEM)
offreeze-driedperovskiteMAPbI3-xClx precursorsolutionshowedthepresenceofPbCl2
nanoparticles [28] and this is in agreement with the dynamic light scattering (DLS)
investigations of MAPbI3-xClx precursor solution [29]. Thus, references [28,29] further
proved the model of the heterogeneous nucleation by PbCl2 nanoparticles proposed
in reference [27]. However, the formation mechanism of the crystal structure remains
underminedandthiswillbediscussedinthefollowingpartsofthisarticle.
2. MethodsforFabricatingMAPbI3-xClx
In Section 3, we discuss the crystal structure of MAPbI3-xClx according to the
depositionmethod. Asthefabricationmethodswerediscussedindetail inreference[30],
here we add a brief introduction about the preparation methods of MAPbI3-xClx.
For the one-step deposition method, MAI:PbI2/PbCl2 (molar ratio 1:1 or 3:1) [31,32]
were dissolved in γ-butyrolactone (GBL) or DMF, spin-coated on the substrates
and annealed to form perovskite. Different annealing conditions result in different
morphology of the MAPbI3-xClx layer. While a rapid thermal annealing at 130 ˝C
resulted in micron-sized perovskite grains [33], two-step annealing, such as 90 ˝C
for 30 min then at 100 ˝C for 2 min [34] or 60 ˝C then ramping to 90 ˝C [35],
resultedinoptimalPCEonpoly(3,4-ethylenedioxythiophene)poly(styrene-sulfonate)
(PEDOT:PSS) substrates. A full coverage of perovskite can be achieved by rapid
cooling after annealing [36]. To increase the solubility of Cl´, 1,8-diiodooctane [37]
orotheralkylhalideadditives[38]ordimethylsulfoxide[9]canbeemployed. Adding
98
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