Please use this identifier to cite or link to this item: https://ir.swu.ac.th/jspui/handle/123456789/11880
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dc.contributor.authorThongnum A.
dc.contributor.authorPinsook U.
dc.date.accessioned2021-04-05T03:01:21Z-
dc.date.available2021-04-05T03:01:21Z-
dc.date.issued2020
dc.identifier.issn20403364
dc.identifier.other2-s2.0-85088486636
dc.identifier.urihttps://ir.swu.ac.th/jspui/handle/123456789/11880-
dc.identifier.urihttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85088486636&doi=10.1039%2fd0nr03432k&partnerID=40&md5=256add5a215f7b930e96b1d3d420a2d5
dc.description.abstractA comprehensive study of the transport properties of a prototypical CH3NH3PbI3 thin film is presented. The polaron-longitudinal optical (LO) phonon scattering mechanism, based on Low-Pines's polaron mobility, was studied to elucidate the charge-carrier mobility. We found that the calculated mobilities showed very good quantitative agreement with the experimental data measured in thin film samples using photoconductivity techniques. In THz mobility, the calculated results yielded room-temperature (RT) mobilities of ~650 cm2 V-1 s-1 (single crystal) and ~220 cm2 V-1 s-1 (disordered thin film) at a low quantum yield (?) and 32 cm2 V-1 s-1 (high-quality thin film) at ? = 1. The dynamic disorder due to organic reorientation was included in the calculations. Its effect provided a power law mobility of µ ? Tm and satisfactorily supported temperature-dependent mobility over the temperature range of 80-370 K. In the orthorhombic and tetragonal phases, the charge-carrier mobilities with dynamic disorder were approximately 47% and 22% lower than those obtained from phases without dynamic disorder. The RT mobility was 26 cm2 V-1 s-1 at ? = 1. In the low-temperature orthorhombic phase, the structural phase transition was considered. The mobility followed a power law with m = -1.7. In the tetragonal and cubic phases, the mobility also followed a power law, but with m = -1.1, which is an intermediate range in optical phonon scattering. When combined with recent theoretical analysis, we also found three limitations of power law mobility with exponents between -0.46 and -1.1 for polaron-LO phonon scattering, -1.2 and -1.6 for bare carrier-LO phonon scattering, and -1.7 and -2.0 for carrier scattering off optical phonons and lattice fluctuations. This work not only provides a description of temperature-dependent mobility in CH3NH3PbI3 thin films, but also gives new insights into THz photoconductivity and the relationship between LO phonon scattering and power law mobility. © 2020 The Royal Society of Chemistry.
dc.subjectHall mobility
dc.subjectHole mobility
dc.subjectOptical lattices
dc.subjectPhonon scattering
dc.subjectPhonons
dc.subjectPhotoconductivity
dc.subjectPolarons
dc.subjectSingle crystals
dc.subjectTemperature
dc.subjectDisordered thin films
dc.subjectLattice fluctuations
dc.subjectLongitudinal optical phonons
dc.subjectOptical phonon scattering
dc.subjectOrthorhombic phase
dc.subjectQuantitative agreement
dc.subjectStructural phase transition
dc.subjectTemperature dependent
dc.subjectThin films
dc.subjectarticle
dc.subjectcalculation
dc.subjectcrystal
dc.subjectlow temperature
dc.subjectphase transition
dc.subjectphonon
dc.subjectquantitative analysis
dc.subjectquantum yield
dc.subjectroom temperature
dc.titlePolaron transport in hybrid CH3NH3PbI3perovskite thin films
dc.typeArticle
dc.rights.holderScopus
dc.identifier.bibliograpycitationNanoscale. Vol 12, No.26 (2020), p.14112-14119
dc.identifier.doi10.1039/d0nr03432k
Appears in Collections:Scopus 1983-2021

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