Abstract
The present computational work analyzes singlet fission (SF) as a pathway for multiplication of photogenerated excitons in crystalline polyacenes. Our study explores the well-known crystalline pentacene (C22H14) and the prospective and potentially interesting doped B,N-pentacene (BC20NH14). At the molecular level, the singlet fission process involves a pair of neighboring molecules and is based on the coupling between an excited singlet state (S1S0) and two singlet-coupled triplets (1T1T1), which, typically, is influenced by an intermolecular charge transfer state. Taking data from periodic density functional theory and ab initio wave function calculations, we applied the non-orthogonal configuration interaction method to determine electronic coupling parameters. The comparison of the results for both equilibrium structures reveal smaller SF coupling for pentacene than for B,N-pentacene by a factor of ∼5. Introduction of the dynamic behavior to the crystals (vibrations, thermal motion) provides a more realistic picture of the effect of the disorder at the molecular level on the SF efficiency. The coupling values associated to out-of-equilibrium structures show that most of the S1S0/1T1T1 couplings remain virtually constant or slightly increase for pentacene when molecular disorder is introduced. Homologous calculations on B,N-pentacene show a generalized decrease in the coupling values, notably if large phonon displacements are considered. A few of the structures analyzed feature much larger SF coupling if some distortion results in (nearly) degenerate charge transfer and excited singlet and triplet states. For these particular situations, an acceleration of the SF process could occur although in competition with electron-hole separation as an alternative pathway.
Original language | English |
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Pages (from-to) | 16249-16258 |
Number of pages | 10 |
Journal | Journal of Physical Chemistry C |
Volume | 127 |
Issue number | 33 |
DOIs | |
State | Published - Aug 24 2023 |
Funding
Financial support was granted by the Spanish Ministry of Science and Innovation (Project PID2020-113187GB-I00) and the Generalitat de Catalunya (2021SGR00110). X.L. thanks Evgenii Strugovshchikov for help on the VASP program. This work used resources of the Oak Ridge Leadership Computing Facility (OLCF) at the Oak Ridge National Laboratory, which is supported by the Office of Science of the U.S. Department of Energy (DOE) under Contract DE-AC05-00OR22725 through the Director’s Discretionary Program and INCITE Project CHM154. Access to computational resources at the Jülich Supercomputer Center (JSC) were provided through the PRACE Project 2021240033/pra129. This article was authored in part by UT-Battelle, LLC, under Contract DE-AC05-00OR22725 with DOE. By accepting this article for publication, the publisher acknowledges that the U.S. Government retains a nonexclusive, paid-up, irrevocable, worldwide license to publish or reproduce the published form of this article or allow others to do so for U.S. Government purposes. DOE will provide public access to these results of federally sponsored research in accordance with the DOE Public Access Plan (http://energy.gov/downloads/doe-public-access-plan). Financial support was granted by the Spanish Ministry of Science and Innovation (Project PID2020-113187GB-I00) and the Generalitat de Catalunya (2021SGR00110). X.L. thanks Evgenii Strugovshchikov for help on the VASP program. This work used resources of the Oak Ridge Leadership Computing Facility (OLCF) at the Oak Ridge National Laboratory, which is supported by the Office of Science of the U.S. Department of Energy (DOE) under Contract DE-AC05-00OR22725 through the Director’s Discretionary Program and INCITE Project CHM154. Access to computational resources at the Jülich Supercomputer Center (JSC) were provided through the PRACE Project 2021240033/pra129. This article was authored in part by UT-Battelle, LLC, under Contract DE-AC05-00OR22725 with DOE. By accepting this article for publication, the publisher acknowledges that the U.S. Government retains a nonexclusive, paid-up, irrevocable, worldwide license to publish or reproduce the published form of this article or allow others to do so for U.S. Government purposes. DOE will provide public access to these results of federally sponsored research in accordance with the DOE Public Access Plan ( http://energy.gov/downloads/doe-public-access-plan ).
Funders | Funder number |
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DOE Public Access Plan | |
INCITE | CHM154 |
U.S. Government | |
U.S. Department of Energy | DE-AC05-00OR22725 |
Office of Science | |
Generalitat de Catalunya | 2021SGR00110 |
Ministerio de Ciencia e Innovación | PID2020-113187GB-I00 |