2020
DOI: 10.1002/adma.202002122
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Solution‐Processed Organic Solar Cells with High Open‐Circuit Voltage of 1.3 V and Low Non‐Radiative Voltage Loss of 0.16 V

Abstract: During the past decade, solution-processed bulk-heterojunction (BHJ) organic solar cells (OSCs) have made great strides and power conversion efficiencies (PCEs) over 16% have been achieved. [1-6] However, the PCEs of top-performing

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Cited by 191 publications
(143 citation statements)
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“…[19] Voltage loss was analyzed according to a previous report that investigated the origin of the high V OC of the PBQx-TCl:BTA3based device and the improved V OC of the ternary device as compared with the PBQx-TCl:BTP-eC9-based device. [20] The optical bandgap of the device was determined to be 1.81, 1.40, and 1.41 eV from the crossing point of EL and EQE spectra for PBQx-TCl:BTA3, PBQx-TCl:BTP-eC9, and PBQx-TCl:BTA3:BTP-eC9, respectively (Figure S9, Supporting Information). By fitting the reduced spectra of both EL and highly sensitive EQE, we estimated the energy of charge transfer (CT) states to be 1.77, 1.36, and 1.37 eV, indicating a negligible voltage loss of 0.04 V as caused by the exciton dissociation in all three devices (Figure S10, Supporting Information).…”
Section: Devicesmentioning
confidence: 99%
“…[19] Voltage loss was analyzed according to a previous report that investigated the origin of the high V OC of the PBQx-TCl:BTA3based device and the improved V OC of the ternary device as compared with the PBQx-TCl:BTP-eC9-based device. [20] The optical bandgap of the device was determined to be 1.81, 1.40, and 1.41 eV from the crossing point of EL and EQE spectra for PBQx-TCl:BTA3, PBQx-TCl:BTP-eC9, and PBQx-TCl:BTA3:BTP-eC9, respectively (Figure S9, Supporting Information). By fitting the reduced spectra of both EL and highly sensitive EQE, we estimated the energy of charge transfer (CT) states to be 1.77, 1.36, and 1.37 eV, indicating a negligible voltage loss of 0.04 V as caused by the exciton dissociation in all three devices (Figure S10, Supporting Information).…”
Section: Devicesmentioning
confidence: 99%
“…Consequently, the majority of photogenerated states will decay via the NFA singlet exciton, instead of progressing into free charge carriers via the CT state manifold. This analysis provides an important empirical insight into why the charge generation is severely compromised in a number of ultralow offset NFA OSCs, [29,127] including the previously discussed PTB7-Th:IOTIC-0F system; in PTB7-Th:IOTIC-0F, the HOMO offset was found to be just 40 meV. In contrast, charge generation was found to be efficient in the PTB7-Th:IOTIC-2F a and PTB7-Th:IOTIC-4F blends, where the HOMO offset was determined to be 140 and 240 meV, respectively.…”
Section: Charge Generationmentioning
confidence: 99%
“…As far as we know, ΔE 3 approaching 0.2 eV represents one of the lowest values of nonradiative E loss in OSCs to date. [63] NFAs that can enable devices to achieve high V oc is desirable because they can be combined with other materials with large J sc in ternary blend to further improve the efficiency of OSCs. The common practice in increasing the V oc of Y6-type NFAs is to replace the F atom of terminal groups with electron-donating units.…”
Section: Doi: 101002/aenm202003177mentioning
confidence: 99%