Our system is currently under heavy load due to increased usage. We're actively working on upgrades to improve performance. Thank you for your patience.
2020
DOI: 10.1039/d0ta03016c
|View full text |Cite
|
Sign up to set email alerts
|

Extraordinarily long diffusion length in PM6:Y6 organic solar cells

Abstract: Simulated energy band diagrams of thin and thick PM6:Y6 devices.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

4
64
0

Year Published

2020
2020
2024
2024

Publication Types

Select...
10

Relationship

3
7

Authors

Journals

citations
Cited by 90 publications
(78 citation statements)
references
References 31 publications
(42 reference statements)
4
64
0
Order By: Relevance
“…Figure 1b showcases simulated J–V curves for the 400 nm device in three different scenarios: 1) parameters based on experimental data; 2) when the hole mobility is hypothesized to be four times higher than that measured; and 3) when k 2 is reduced by 50% and the hole mobility is also increased by a factor of 4. As demonstrated in Figure 1b, lowering k 2 by twofold to reach reduced‐Langevin recombination and a fourfold higher hole mobility, compared with what we have previously published for a thick PM6:Y6 system, [ 9,22 ] as input parameters, generates an FF in the range of 65–70% (see Table S1 and Figure S1, Supporting Information, for details).…”
Section: Resultssupporting
confidence: 69%
“…Figure 1b showcases simulated J–V curves for the 400 nm device in three different scenarios: 1) parameters based on experimental data; 2) when the hole mobility is hypothesized to be four times higher than that measured; and 3) when k 2 is reduced by 50% and the hole mobility is also increased by a factor of 4. As demonstrated in Figure 1b, lowering k 2 by twofold to reach reduced‐Langevin recombination and a fourfold higher hole mobility, compared with what we have previously published for a thick PM6:Y6 system, [ 9,22 ] as input parameters, generates an FF in the range of 65–70% (see Table S1 and Figure S1, Supporting Information, for details).…”
Section: Resultssupporting
confidence: 69%
“…The diffusion length of carriers in 100‐nm PM6:Y6 devices was recently reported to be comparable with the thickness of the active layer. [ 44 ] When the transporting layers which reduce the diffusion of the minority carriers towards the wrong electrodes are removed, the long diffusion lengths of carriers might enhance surface recombination. [ 45 ] These results are reproduced by corresponding simulations, shown by the solid black curves in Figure 3b, for a PM6:Y6 device with nonohmic contacts, exhibiting considerable injection barriers for holes at the anode and electrons at the cathode contacts, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…To achieve high performance in an OSC, it is critical to have proper film morphology in its photoactive layer in order to maintain a balance between exciton dissociation and charge transport. In the past few years, bulk heterojunction (BHJ) architecture has gained great success in OSC based on polymeric donors and fullerene-derived acceptors 4 , which circumvents the short exciton diffusion length in polymer donor materials (typically 5–10 nm) 5 , 6 by providing an interpenetrating donor/acceptor (D/A) network for electron- and hole-transport 7 . This approach has successfully increased the short-circuit current density ( J SC ) in OSCs.…”
Section: Introductionmentioning
confidence: 99%