TY - JOUR
T1 - Thermally Activated Delayed Fluorescence Sensitization for Highly Efficient Blue Fluorescent Emitters
AU - Abroshan, Hadi
AU - Zhang, Yadong
AU - Zhang, Xiaoqing
AU - Fuentes-Hernandez, Canek
AU - Barlow, Stephen
AU - Coropceanu, Veaceslav
AU - Marder, Seth R.
AU - Kippelen, Bernard
AU - Brédas, Jean Luc
N1 - Funding Information: This work was funded by the Department of Energy (Award DE-EE0008205) and the University of Arizona. The authors acknowledge the use of the computing facilities of the Partnership for an Advanced Computing Environment (PACE) at the Georgia Institute of Technology and the support of the PACE team. The project or effort depicted was or is sponsored by the Department of the Defense, Defense Threat Reduction Agency (Award HDTRA 11810033). The content of the information does not necessarily reflect the position or the policy of the federal government, and no official endorsement should be inferred. Funding Information: This work was funded by the Department of Energy (Award DE‐EE0008205) and the University of Arizona. The authors acknowledge the use of the computing facilities of the Partnership for an Advanced Computing Environment (PACE) at the Georgia Institute of Technology and the support of the PACE team. The project or effort depicted was or is sponsored by the Department of the Defense, Defense Threat Reduction Agency (Award HDTRA 11810033). The content of the information does not necessarily reflect the position or the policy of the federal government, and no official endorsement should be inferred. Publisher Copyright: © 2020 Wiley-VCH GmbH
PY - 2020/12/22
Y1 - 2020/12/22
N2 - Hyperfluorescence is emerging as a powerful strategy to develop optoelectronic devices with high-color purity and enhanced stability. It requires appropriate integration of a sensitizer displaying efficient thermally activated delayed fluorescence (TADF) and an emitter displaying strong, narrow-band fluorescence. Here, through a joint computational and experimental approach, an unprecedented, end-to-end systems level description of the electronic and optical processes that take place in a hyperfluorescent emissive layer composed of a TADF sensitizer, 2,5-bis(2,6-di(9H-carbazol-9-yl)phenyl)-1,3,4-oxadiazole (4CzDPO), and a fluorescent emitter, 2,5,8,11-tetra-tert-butylperylene (TBPe) is provided. The photophysical properties measurement of the emissive layer is combined with the computational determination of the electronic properties, film morphology, and excitation transfer phenomena. The Förster resonance energy transfer rates from 4CzDPO to TBPe are on the order of 1011 s−1, considerably higher than the radiative and nonradiative recombination rates for 4CzDPO. These features ensure nearly complete energy transfer to TBPe, leading to a five-fold increase in the photoluminescence quantum yields in the 4CzDPO:TBPe system in comparison to neat films of 4CzDPO. This approach highlights the factors that can provide efficient energy transfer from TADF molecules to fluorescent emitters, suppress energy transfer among TADF molecules, and avoid the need for a host material within the emissive layer.
AB - Hyperfluorescence is emerging as a powerful strategy to develop optoelectronic devices with high-color purity and enhanced stability. It requires appropriate integration of a sensitizer displaying efficient thermally activated delayed fluorescence (TADF) and an emitter displaying strong, narrow-band fluorescence. Here, through a joint computational and experimental approach, an unprecedented, end-to-end systems level description of the electronic and optical processes that take place in a hyperfluorescent emissive layer composed of a TADF sensitizer, 2,5-bis(2,6-di(9H-carbazol-9-yl)phenyl)-1,3,4-oxadiazole (4CzDPO), and a fluorescent emitter, 2,5,8,11-tetra-tert-butylperylene (TBPe) is provided. The photophysical properties measurement of the emissive layer is combined with the computational determination of the electronic properties, film morphology, and excitation transfer phenomena. The Förster resonance energy transfer rates from 4CzDPO to TBPe are on the order of 1011 s−1, considerably higher than the radiative and nonradiative recombination rates for 4CzDPO. These features ensure nearly complete energy transfer to TBPe, leading to a five-fold increase in the photoluminescence quantum yields in the 4CzDPO:TBPe system in comparison to neat films of 4CzDPO. This approach highlights the factors that can provide efficient energy transfer from TADF molecules to fluorescent emitters, suppress energy transfer among TADF molecules, and avoid the need for a host material within the emissive layer.
KW - TADF
KW - energy transfer
KW - fluorescence
KW - hyperfluorescence
KW - sensitizers
UR - http://www.scopus.com/inward/record.url?scp=85091272778&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85091272778&partnerID=8YFLogxK
U2 - 10.1002/adfm.202005898
DO - 10.1002/adfm.202005898
M3 - Article
SN - 1616-301X
VL - 30
JO - Advanced Functional Materials
JF - Advanced Functional Materials
IS - 52
M1 - 2005898
ER -