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Complete Report - University of New South Wales

Complete Report - University of New South Wales

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ARCPHOTOVOLTAICSCENTRE OFEXCELLENCE2010/11ANNUAL REPORTRecent improvements in independently confirmedefficiency for small area (≤ 1cm 2 ) organic solar cells(extracted from Green et al. [4.4.2.2]).Figure 4.4.2.1<strong>University</strong> Staff• Dr Ashraf Uddin• Pr<strong>of</strong>. Martin Green• A/Pr<strong>of</strong>. Gavin ConibeerSenior FellowDr Dirk KönigResearch FellowDr Shujuan HuangResearch AssistantXiaohan YangPostgraduate Research Students• Lara Treiber• Xiaohan Yang• Miga Jung• Xiaolei Liu• Kim Taekyun• Fred Oi• Matthew WrightUndergraduate Thesis Students• Thoo Chee Hong• Matthew Wright• Xinda Yang• Jizhong Yao• Adam Sen Ann Ong• Lihui Song• Buyi Yan• Viren NathooTaste <strong>of</strong> Research StudentSolomon Freer4.4.2.1 IntroductionA new organic photovoltaic (OPV) researchlab has been established at Level-10 inthe UNSW Chemical Science Buildingto accommodate work on organicsemiconductor materials and OPV devices.Today this lab is equipped with basicfacilities organised with support from anARC Discovery Grant, UNSW equipmentgrant, a family grant from the Green family,a Faculty grant and with the support <strong>of</strong>the ARC Photovoltaic Centre <strong>of</strong> Excellence.Currently, the research team consists <strong>of</strong>three academics, two research fellows, oneresearch assistant, 6 PhD, one M.Eng. and 8honours students.We have already produced some meaningfuldata from our research work. Two journalpapers, three conference proceedingpapers and one patent are already inpreparation. The nanoscale texture or thinfilm morphology <strong>of</strong> the donor/acceptorblends used in most OPV devices is acritical variable that can dominate boththe performance <strong>of</strong> new materials beingoptimized in the lab and efforts to movefrom laboratory-scale to factory-scaleproduction. Although OPV conversionefficiencies (up to 8.3%) have improvedsignificantly in recent years, progress inmorphology optimization still occurs largelyby trial and error, in part because much <strong>of</strong>our basic understanding <strong>of</strong> how nanoscalemorphology affects the optoelectronicproperties <strong>of</strong> these heterogeneous organicsemiconductor films has to be inferredindirectly from macroscopic measurements.The morphology <strong>of</strong> the active film is avery important factor in producing highefficiency devices.Films spin-coated from blend solutionsundergo separation <strong>of</strong> the donor/acceptorphases. The scale <strong>of</strong> the phase separationdepends on the solvent, solubility <strong>of</strong> thematerials and parameters <strong>of</strong> the spincoatingprocess such as the spin speedand temperature. If the morphologycould be controlled on a molecularscale the efficiency <strong>of</strong> charge separationand transport could be expected to besubstantially higher. Now we are workingfor the morphology optimization <strong>of</strong>organic films for OPV devices in respect t<strong>of</strong>undamental issues such as light trapping,control <strong>of</strong> electronic structure at filmsinterfaces, exciton dissociation and carriertransport for photovoltaic operation toachieve our goals.The detailed physical understanding <strong>of</strong> OPVdevices still lags behind their application,on account <strong>of</strong> fundamental differences inthe optoelectronic properties <strong>of</strong> organicmaterials compared to conventionalsemiconductors. This lack <strong>of</strong> understandinglimits the scope <strong>of</strong> material and devicedesign. Among those features thatdistinguish OPV devices from inorganicsemiconductor based devices are: (i) thecharges and excited states are localizedon individual molecules or molecularsegments, with the result that charge andenergy transport processes are relativelyslow; (ii) the dielectric permittivity is low,leading to stronger space charge effects;(iii) the organic semiconductor materialsare electronically disordered, dispersingthe rates <strong>of</strong> charge transfer and transportprocesses; (iv) the active layers are <strong>of</strong>tenheterogeneous, either as multi-componentfilms or because <strong>of</strong> nonuniform molecularordering; and (v) the organic semiconductoris usually not doped, thus precluding theconditions that allow charge dynamics tobe linearized in the description <strong>of</strong> devicephysics. The need for appropriate device54

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