2016
DOI: 10.1007/978-3-319-28338-8_4
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Charge Separation at Nanostructured Molecular Donor–Acceptor Interfaces

Abstract: Planar and bulk heterojunctions of organic donor and acceptor molecules are used for understanding elementary processes in photovoltaic cells. Electronic structure, interface and film morphology, excitonic behaviour, device characteristics and correlations between those properties are reviewed here using a wide range of material combinations.

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Cited by 2 publications
(4 citation statements)
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“…The downward bending of the spectral profiles of the pristine donor compounds around 1.5 eV is an artifact due to the grating and detector changeover in the spectrometer. Note that the magnitude of k xy for DIP 51,52 and for 6T 21,53 compares very well with the literature. Ellipsometry.…”
Section: ■ Experimental Sectionsupporting
confidence: 85%
“…The downward bending of the spectral profiles of the pristine donor compounds around 1.5 eV is an artifact due to the grating and detector changeover in the spectrometer. Note that the magnitude of k xy for DIP 51,52 and for 6T 21,53 compares very well with the literature. Ellipsometry.…”
Section: ■ Experimental Sectionsupporting
confidence: 85%
“…polymer HJ from similar experiments [52,[108][109][110] using CV measurements or detection of charge transfer emission/absorption to determine an estimate for the photovoltaic gap ΔE PV [107,111,112]. This bandgap-voltage offset is significantly larger for OPVCs than for most inorganic pn-junction solar cells [113] as well as for the emerging perovskite cells [114] and one of the reasons for the lower performance of OPVCs [53]. A clear limitation for maximisation of the photovoltaic gap ΔE PV is given due to the necessary HOMO-HOMO and LUMO-LUMO offset.…”
Section: Concluding Remarks and Outlookmentioning
confidence: 99%
“…The clear discrimination between charge transfer from the substrate into the films of the PHJ can be achieved by careful analysis and considering electrostatic modelling [68,77,79]. The cases presented here were contact doping [69], long range charge transfer through an unpinned layer [53] or charge transfer at the interface of two pinned layers However, electrostatic modelling can be applied successfully only if the real morphology is known. As mentioned before, structural compatibility and related reorientation [54,55], structural disorder induced by the deposition process [87,128] and the surface/interface energies [55] have to be taken into account.…”
Section: Concluding Remarks and Outlookmentioning
confidence: 99%
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