2018
DOI: 10.1002/aenm.201800204
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Fused‐Ring Nonfullerene Acceptor Forming Interpenetrating J‐Architecture for Fullerene‐Free Polymer Solar Cells

Abstract: An interesting and important question emerges with the rapid advances of the highly efficient fused‐ring nonfullerene acceptors; that is, how the acceptor molecules form aggregates in its blended film with a donor polymer/small molecule so as to offer highly efficient exciton diffusion and electron transport? To answer this question, a new acceptor molecule, 3,9‐bis(5‐methylene‐4‐one‐6‐(1,1‐dicyanomethylene)‐cyclopenta[c]thiophen‐2,8‐dimethyl)‐5,5,11,11‐tetrakis(4‐n‐hexylphenyl)‐dithieno[2,3‐d:2′,3′‐d′]‐s‐inda… Show more

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Cited by 70 publications
(69 citation statements)
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References 73 publications
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“…For the PM6:IT‐4F system, the face‐on oriented π–π stacking signal appears around 1.78 Å −1 ( d ≈ 3.53 Å). The peak around 1.35 Å −1 ( d ≈ 0.46 Å) could be due to the packing ordering of the perpendicular side chains of IT‐4F, as observed previously by us from the ITCT‐DM molecule . Upon the mixing with 0.2 IDIC, the π–π stacking scattering signal is seen around 1.77 Å −1 ( d ≈ 3.55 Å), featuring the addition of the (010) signals of the IT4F binary and the IDIC binary.…”
Section: Resultssupporting
confidence: 71%
See 1 more Smart Citation
“…For the PM6:IT‐4F system, the face‐on oriented π–π stacking signal appears around 1.78 Å −1 ( d ≈ 3.53 Å). The peak around 1.35 Å −1 ( d ≈ 0.46 Å) could be due to the packing ordering of the perpendicular side chains of IT‐4F, as observed previously by us from the ITCT‐DM molecule . Upon the mixing with 0.2 IDIC, the π–π stacking scattering signal is seen around 1.77 Å −1 ( d ≈ 3.55 Å), featuring the addition of the (010) signals of the IT4F binary and the IDIC binary.…”
Section: Resultssupporting
confidence: 71%
“…The peak around 1.35 Å −1 (d ≈ 0.46 Å) could be due to the packing ordering of the perpendicular side chains of IT-4F, as observed previously by us from the ITCT-DM molecule. [53] Upon the mixing with 0.2 IDIC, the π-π stacking scattering signal is seen around 1.77 Å −1 (d ≈ 3.55 Å), featuring the addition of the (010) signals of the IT4F binary and the IDIC binary. The CCL reflecting the crystalline size of the π-π stacking is estimated to be 3.86 nm for both the IT-4F binary blend and its ternary blend with the addition of 0.2 IDIC.…”
Section: Film Morphologymentioning
confidence: 98%
“…[15,[26][27][28] So, the molecular conformation of the terminal region would directly influence the charge transport and the final photovoltaic performances. [15,[26][27][28] So, the molecular conformation of the terminal region would directly influence the charge transport and the final photovoltaic performances.…”
mentioning
confidence: 99%
“…The π-π stacking of terminal moieties is now recognized to be the main charge transport channel for A-D-A type FREAs. [15,[26][27][28] So, the molecular conformation of the terminal region would directly influence the charge transport and the final photovoltaic performances. In this contribution, A-π-D-π-A type FREAs IDTCN-O, IDTCN-C, and IDTCN-S were designed based on the same molecular skeleton of IDTT2F with hexyl, hexyloxy, and hexylthio side chain, respectively, incorporated at the outer site of the thiophene bridge to systematically investigate the influence of side chain type on the photo voltaic performance.…”
mentioning
confidence: 99%
“…To enhance spectral response, several methods have been performed to modify the IDT-based acceptors, such as increasing the conjugation lengths, [11,22,33,34] introducing electron-donating groups in the D units, [24,26,28,35] and using strong electron-withdrawing atoms in the A groups. [16,23,25,36] Accordingly, several narrow-bandgap (NBG) fused-ring nonfullerene acceptors (NFAs), such as BTOIC, [12] IHIC, [37] 4TIC, [38] F8IC, [31] IEICO, [24] ATT-2, [39] BT-CIC, [40] DTPCIC, [41] COi8DFIC, [42] and R12-4Cl, [43] were successfully developed. Although these acceptors presented satisfying J SC , nonideal open-circuit voltage (V OC ) and fill factor (FF) limit the Small molecule acceptors (SMAs) for polymer solar cells (PSCs) have become a hot topic due to the resulting breakthrough of power conversion efficiency (PCE).…”
Section: Doi: 101002/smtd201900280mentioning
confidence: 99%