2016
DOI: 10.1002/aenm.201600742
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A Wide Bandgap Polymer with Strong π–π Interaction for Efficient Fullerene‐Free Polymer Solar Cells

Abstract: A wide bandgap polymer donor PBDTS‐DTBTO is designed and synthesized, which shows an optical bandgap of 1.76 eV and strong π–π interaction. By using a low‐bandgap acceptor ITIC, power conversion efficiency over 9% is achieved in the fullerene‐free polymer solar cells (PSC) device. Furthermore, the PSC devices fabricated by PBDTS‐DTBTO:ITIC show relatively small sensitivity to variations of the active layer thickness.

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Cited by 77 publications
(42 citation statements)
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“…Under the same device processing conditions, the two polymer donors yielded moderate PCEs when PC 71 BM or IEICO were used as acceptor materials (Supporting Information, Table S1). Furthermore,weselected another four polymers,i ncluding PBDTTT-E-T, [35] PBDTS-DTBTO, [36] PBQ-3, [37] and PBDB-T [38] (Supporting Information, Figure S4), as donor materials for the fabrication of IEICO-4F-based devices because of their good applicability in fullerene-free OSC devices.T hese polymers have varied optical absorption bands (E opt g ranging from 1.55 to 1.77 eV), and the four OSC devices show V OC values ranging from 0.689 to 0.771 V. As presented in Table S2 (Supporting Information), the four devices all yielded J SC values over 20 mA cm À2 even though they have relatively low energy losses from 0.469 to 0.551 eV.…”
Section: Angewandte Chemiementioning
confidence: 99%
“…Under the same device processing conditions, the two polymer donors yielded moderate PCEs when PC 71 BM or IEICO were used as acceptor materials (Supporting Information, Table S1). Furthermore,weselected another four polymers,i ncluding PBDTTT-E-T, [35] PBDTS-DTBTO, [36] PBQ-3, [37] and PBDB-T [38] (Supporting Information, Figure S4), as donor materials for the fabrication of IEICO-4F-based devices because of their good applicability in fullerene-free OSC devices.T hese polymers have varied optical absorption bands (E opt g ranging from 1.55 to 1.77 eV), and the four OSC devices show V OC values ranging from 0.689 to 0.771 V. As presented in Table S2 (Supporting Information), the four devices all yielded J SC values over 20 mA cm À2 even though they have relatively low energy losses from 0.469 to 0.551 eV.…”
Section: Angewandte Chemiementioning
confidence: 99%
“…Organic solar cells (OSCs) based on binary active layers have been intensively investigated in past decades . Nevertheless, the narrow optical absorption spectrum of organic semiconductors resulting from the electron hopping between the discontinuous energy bands makes it challenging to gain panchromatic absorption coverage in OSCs, even by combining a donor and an acceptor with complementary absorption bands . To solve this problem, tandem OSCs composed of multiple active layers have been designed, while the complicated fabrication processes of these types of devices may impede their practical applications .…”
Section: Photovoltaic Parameters For J52:it‐m:ieico With Various Ratiosmentioning
confidence: 99%
“…Polymer solar cells have many advantages, such as lightweight, flexibility, transparency, and ease of manufacturing (by rolling, coating, or printing techniques) for mass production . In addition, the performance of the polymer solar cells can be remarkably improved by designing the proper structure of polymer to be able to adjust the band gap and the energy level; also, it is easy to integrate polymer solar cells with other devices with different functions . Thus, the study on integration of a polymer solar cell and a supercapacitor into a single device, namely polymer solar cell type photo‐supercapacitor (PSPS), has been started after DSSCPSs.…”
Section: The Types Of Photo‐supercapacitorsmentioning
confidence: 99%