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dc.contributor.authorPonseca, Carlito S.
dc.date.accessioned2019-10-04 14:25:37
dc.date.accessioned2020-04-01T14:07:06Z
dc.date.accessioned2016-08-01 23:55
dc.date.accessioned2019-10-04 14:25:37
dc.date.accessioned2020-04-01T14:07:06Z
dc.date.accessioned2016-12-31 23:55:55
dc.date.accessioned2019-10-04 14:25:37
dc.date.accessioned2020-04-01T14:07:06Z
dc.date.available2020-04-01T14:07:06Z
dc.date.issued2016
dc.identifier612573
dc.identifierOCN: 1030817800en_US
dc.identifier.urihttp://library.oapen.org/handle/20.500.12657/32352
dc.description.abstractThis chapter presents the fate of the charge carriers from the moment of its photogeneration in the perovskite to injection and transport into electrodes. Time-resolved electrical measurement techniques, terahertz (THz) spectroscopy and microwave (MW) conductivity, are primarily used to deconvolute ultrafast processes and to directly access behavior of charged species from the ps to µs timescales. Transient absorption and photoluminescence spectroscopy were also utilized to gain insight on carrier population dynamics and radiatively recombining charges. Photogenerated charged species were converted into highly mobile charges (µe = 12.5 cm2V-1s-1 and µh = 7.5 cm2V-1s-1) almost instantaneously (< 0.2 ps), while the remaining loosely bounded excitons dissociate into mobile charges after 2-3 ps. This high mobility is maintained for at least 1 ns as obtained by THz spectroscopy, while its lifetime is at least few tens of µs as measured by the MW conductivity technique. Lowering the temperature increases carrier mobilities with T-1.6.Dependence and a 75 meV barrier energy is required for temperature-activated recombination. Finally, injection of hole from MAPbI3 to Spiro-OMeTAD was found to be ultrafast and the state and population of dark holes dictate its recombination.
dc.languageEnglish
dc.subject.classificationthema EDItEUR::P Mathematics and Science::PD Science: general issuesen_US
dc.subject.otherthz spectroscopy
dc.subject.othertime resolved electrical measurement
dc.subject.otherphotoconductivity
dc.subject.othermobility
dc.subject.otherthz spectroscopy
dc.subject.othertime resolved electrical measurement
dc.subject.otherphotoconductivity
dc.subject.othermobility
dc.subject.otherCarrier generation and recombination
dc.subject.otherCharge carrier
dc.subject.otherChemical kinetics
dc.subject.otherHertz
dc.subject.otherPerovskite
dc.subject.otherPhenyl-C61-butyric acid methyl ester
dc.subject.otherPicosecond
dc.subject.otherSolar cell
dc.titleChapter 11 Charge Carrier Dynamics in Organometal Halide Perovskite Probed by Time-Resolved Electrical Measurements
dc.typechapter
oapen.identifier.doi10.5772/61631
oapen.relation.isPublishedBy09f6769d-48ed-467d-b150-4cf2680656a1
oapen.relation.isPartOfBook2872576b-5633-4781-8179-aa676ca35865
oapen.relation.isFundedBy7292b17b-f01a-4016-94d3-d7fb5ef9fb79
oapen.collectionEuropean Research Council (ERC)
oapen.chapternumber1
oapen.grant.number226136
oapen.grant.acronymVISCHEM
oapen.grant.programFP7
oapen.remark.publicRelevant Wikipedia pages: Carrier generation and recombination - https://en.wikipedia.org/wiki/Carrier_generation_and_recombination; Charge carrier - https://en.wikipedia.org/wiki/Charge_carrier; Chemical kinetics - https://en.wikipedia.org/wiki/Chemical_kinetics; Electron - https://en.wikipedia.org/wiki/Electron; Hertz - https://en.wikipedia.org/wiki/Hertz; Perovskite - https://en.wikipedia.org/wiki/Perovskite; Phenyl-C61-butyric acid methyl ester - https://en.wikipedia.org/wiki/Phenyl-C61-butyric_acid_methyl_ester; Photoconductivity - https://en.wikipedia.org/wiki/Photoconductivity; Picosecond - https://en.wikipedia.org/wiki/Picosecond; Solar cell - https://en.wikipedia.org/wiki/Solar_cell
oapen.identifier.ocn1030817800


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