2013
DOI: 10.1021/jp4093089
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Small-Molecule Bulk Heterojunctions: Distinguishing Between Effects of Energy Offsets and Molecular Packing on Optoelectronic Properties

Abstract: We report on the dependence of time-resolved photoluminescence (PL) and photocurrent in small-molecule bulk heterojunctions on the donor–acceptor (D/A) LUMO offset, D/A separation, and acceptor domain structure. We chose a high-performance functionalized fluorinated anthradithiophene (ADT) derivative, ADT-TES-F, as the donor and two other fluorinated ADT derivatives, ADT-R-F (where R is a variable side group), as well as two functionalized fluorinated pentacene (Pn) derivatives, Pn-R-F8, as acceptors. The choi… Show more

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Cited by 19 publications
(40 citation statements)
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“…20 Similar trends were observed in ADT-TES-F/Pn-R-F8 blends, in which the emission efficiency and lifetime of exciplex significantly depended on the size of the acceptor's R-group, so that larger R groups led to a less emissive and shorter lived exciplex. 2,5 If the ADT-TES-F donor and Pn-R-F8 acceptor molecules are separated by a neutral spacer such as PMMA, FRET, with the FRET radius of 4.2-4.5 nm, depending on the side group R, dominates over the exciplex formation. FRET between ADT-TES-F donor and Pn-NODIPS-F8 acceptor molecules is illustrated in Fig.5 which shows fluorescence spectra from ADT-TES-F donor-only, Pn-NODIPS-F8 acceptor-only, and ADT-TES-F/Pn-NODIPS-F8 D/A pair in PMMA under a 490 nm excitation.…”
Section: Org/manuscriptsmentioning
confidence: 99%
“…20 Similar trends were observed in ADT-TES-F/Pn-R-F8 blends, in which the emission efficiency and lifetime of exciplex significantly depended on the size of the acceptor's R-group, so that larger R groups led to a less emissive and shorter lived exciplex. 2,5 If the ADT-TES-F donor and Pn-R-F8 acceptor molecules are separated by a neutral spacer such as PMMA, FRET, with the FRET radius of 4.2-4.5 nm, depending on the side group R, dominates over the exciplex formation. FRET between ADT-TES-F donor and Pn-NODIPS-F8 acceptor molecules is illustrated in Fig.5 which shows fluorescence spectra from ADT-TES-F donor-only, Pn-NODIPS-F8 acceptor-only, and ADT-TES-F/Pn-NODIPS-F8 D/A pair in PMMA under a 490 nm excitation.…”
Section: Org/manuscriptsmentioning
confidence: 99%
“…In the case of the ADT-TES-F/Pn-TIPS-F8 blend, strong PL emission due to the ADT-TES-F/Pn-TIPS-F8 CT state (exciplex) was observed, with a peak at ~ 710 nm (1.75 eV) (Fig. 2(b)) which closely matched the energy difference between the LUMO of Pn-TIPS-F8 and HOMO of ADT-TES-F. 9,10,12 No emissive CT states were observed in any other D/A blend studied. The fast decay component has been previously attributed to charge trapping and various recombination processes such as bimolecular and trap-assisted recombination; 15 for example, a faster decay in ADT-TES-F/PCBM blends as compared to pristine ADT-TES-F films was determined to be due to enhanced bimolecular recombination in these blends.…”
Section: Optical Absorption and Photoluminescence Propertiesmentioning
confidence: 53%
“…8 Addition of the Pn-TIPS-F8 acceptor to the ADT-TES-F donor has been shown to result in the formation of an emissive charge transfer state (exciplex), which was detrimental for charge photogeneration. 9 Photoinduced interactions between P3HT and Pn-TIPS-F8 and their effect on photoconductivity are not known; also not known is how charge carrier dynamics in P3HT-based D/A blends compare to those in ADT-TES-F-based D/A blends utilizing same acceptors, which is investigated here.…”
Section: Methodsmentioning
confidence: 99%
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