TY - JOUR
T1 - Singlet Fission in Quaterrylenediimide Thin Films
AU - Chen, Michelle
AU - Powers-Riggs, Natalia E.
AU - Coleman, Adam F.
AU - Young, Ryan M.
AU - Wasielewski, Michael R.
N1 - Funding Information:
This work was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences under Award DE-FG02-99ER14999 (M.R.W.). M.C. gratefully acknowledges support from the Ryan Fellowship and the Northwestern University International Institute for Nanotechnology. N.E.P.R. acknowledges funding from the National Science Foundation Graduate Research Fellowship Program under Grant No. DGE-1324585. We thank Professor Yi-Lin Wu and Dr. Aritra Mandal for valuable discussions and Dr. Stephen A. Miller and the Northwestern University Laser and Electronics Design Core Facility for assistance on instrumentation. This work made use of the IMSERC at Northwestern University, which has received support from the Soft and Hybrid Nanotechnology Experimental (SHyNE) Resource (NSF ECCS-1542205), the State of Illinois, and the International Institute for Nanotechnology (IIN). This work made use of the Jerome B. Cohen X-ray Diffraction Facility supported by the MRSEC program of the National Science Foundation (DMR-1720139) at the Materials Research Center of Northwestern University and the Soft and Hybrid Nanotechnology Experimental (SHyNE) Resource (NSF ECCS-1542205). This work made use of the Keck-II facility of Northwestern University’s NUANCE Center, which has received support from the Soft and Hybrid Nanotechnology Experimental (SHyNE) Resource (NSF ECCS-1542205); the MRSEC program (NSF DMR-1720139) at the Materials Research Center; the International Institute for Nanotechnology (IIN); the Keck Foundation; and the State of Illinois, through the IIN.
Publisher Copyright:
Copyright © 2020 American Chemical Society.
PY - 2020/2/6
Y1 - 2020/2/6
N2 - Singlet fission (SF) creates two triplet excitons following absorption of a photon by two electronically interacting chromophores. Quaterrylene-3,4:13,14-bis(dicarboximide) (QDI) is a strongly absorbing chromophore that readily fulfills the energetic requirements for SF, E(S1) > 2E(T1), and thus should undergo rapid and efficient SF. SF was studied in thin films of the QDI derivative N,N-bis(2,6-diisopropylphenyl)-QDI (ArQDI), which undergoes SF in <300 fs to form the correlated triplet pair state, 1(T1T1), which dissociates with a (7.3 ± 1.2 ns)-1 rate constant. The observed triplet yield for a thin film that has been solvent-vapor annealed with CH2Cl2 is 135 ± 20% instead of 200%, which is typically expected of chromophores that undergo ultrafast formation of the 1(T1T1) state. The lower SF yield in ArQDI results from the failure of the 1(T1T1) state to dissociate before returning to the ground state. In contrast to other molecules, like hexacene, which have low triplet energies, the SF rate in ArQDI is not limited by a multiphonon relaxation bottleneck, largely due to the fact that the S-T energy gap in the film is substantially smaller than that measured for monomeric ArQDI. The ability to maintain a favorable S-T energy gap in a film is a design consideration when chromophores are considered for use to enhance solar cell performance.
AB - Singlet fission (SF) creates two triplet excitons following absorption of a photon by two electronically interacting chromophores. Quaterrylene-3,4:13,14-bis(dicarboximide) (QDI) is a strongly absorbing chromophore that readily fulfills the energetic requirements for SF, E(S1) > 2E(T1), and thus should undergo rapid and efficient SF. SF was studied in thin films of the QDI derivative N,N-bis(2,6-diisopropylphenyl)-QDI (ArQDI), which undergoes SF in <300 fs to form the correlated triplet pair state, 1(T1T1), which dissociates with a (7.3 ± 1.2 ns)-1 rate constant. The observed triplet yield for a thin film that has been solvent-vapor annealed with CH2Cl2 is 135 ± 20% instead of 200%, which is typically expected of chromophores that undergo ultrafast formation of the 1(T1T1) state. The lower SF yield in ArQDI results from the failure of the 1(T1T1) state to dissociate before returning to the ground state. In contrast to other molecules, like hexacene, which have low triplet energies, the SF rate in ArQDI is not limited by a multiphonon relaxation bottleneck, largely due to the fact that the S-T energy gap in the film is substantially smaller than that measured for monomeric ArQDI. The ability to maintain a favorable S-T energy gap in a film is a design consideration when chromophores are considered for use to enhance solar cell performance.
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U2 - 10.1021/acs.jpcc.9b10397
DO - 10.1021/acs.jpcc.9b10397
M3 - Article
AN - SCOPUS:85079795406
SN - 1932-7447
VL - 124
SP - 2791
EP - 2798
JO - Journal of Physical Chemistry C
JF - Journal of Physical Chemistry C
IS - 5
ER -