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Manna AK. Thiocarbonyl-Bridged N-Heterotriangulenes for Energy Efficient Triplet Photosensitization: A Theoretical Perspective. Chemphyschem 2024; 25:e202400371. [PMID: 38700483 DOI: 10.1002/cphc.202400371] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 03/31/2024] [Revised: 05/02/2024] [Accepted: 05/03/2024] [Indexed: 05/05/2024]
Abstract
Structurally-rigid metal-free organic molecules are of high demand for various triplet harvesting applications. However, inefficient intersystem crossing (ISC) due to large singlet-triplet gap (Δ E S - T ${\Delta {E}_{S-T}}$ ) and small spin-orbit coupling (SOC) between lowest excited singlet and triplet often limits their efficiency. Excited electronic states, fluorescence and ISC rates in several thiocarbonyl-bridged N-heterotriangulene ( m ${m}$ S-HTG) with systematically increased thione content (m = ${m=}$ 0-3) are investigated implementing polarization consistent time-dependent optimally-tuned range-separated hybrid. All m ${m}$ S-HTGs are dynamically stable and also thermodynamically feasible to synthesize. Relative energies of several low-lying singlets (S n ${{S}_{n}}$ ) and triplets (T n ${{T}_{n}}$ ), and their excitation nature (i. e.,n π * ${n{\pi }^{^{\ast}}}$ orπ π * ${\pi {\pi }^{^{\ast}}}$ ) and SOC are determined for these m ${m}$ S-HTGs in dichloromethane. Low-energy optical peak displays gradual red-shift with increasing thione content due to relatively smaller electronic gap resulted from greater degree of orbital delocalization. Significantly large SOC due to different orbital-symmetry and heavy-atom effect produces remarkably high ISC rates (k I S C ${{k}_{ISC}}$ ~1012 s-1) for enthalpically favouredS 1 n π * → T 2 ${{S}_{1}\left(n{\pi }^{^{\ast}}\right)\to {T}_{2}}$ (π π * ${\pi {\pi }^{^{\ast}}}$ ) channel in these m ${m}$ S-HTGs, which outcompete radiative fluorescence rates (~108 s-1) even directly from higher lying optically brightπ π * ${\pi {\pi }^{^{\ast}}}$ singlets. Importantly, high energy triplet excitons of ~1.7 eV resulting from such significantly large ISC rates from non-fluorescentS 1 n π * ${{S}_{1}\left(n{\pi }^{^{\ast}}\right)}$ make these thiocarbonylated HTGs ideal candidates for energy efficient triplet harvest including triplet-photosensitization.
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Affiliation(s)
- Arun K Manna
- Department of Chemistry, Indian Institute of Technology Tirupati, 517619, Tirupati, Andhra Pradesh, India
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Hawly T, Streller F, Johnson M, Miguez-Lago S, Hammer N, Hampel F, Vivod D, Zahn D, Kivala M, Branscheid R, Spiecker E, Fink RH. Tailored Solution-Based N-heterotriangulene Thin Films: Unravelling the Self-Assembly. Chemphyschem 2021; 22:1079-1087. [PMID: 33792107 PMCID: PMC8251884 DOI: 10.1002/cphc.202100164] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 03/02/2021] [Revised: 03/31/2021] [Indexed: 11/22/2022]
Abstract
The ability of a series of bridged triarylamines, so‐called N‐heterotriangulenes, to form multilayer‐type 2D‐extended films via a solution‐based processing method was examined using complementary microscopic techniques. We found that the long‐range order, crystallinity, and layer thickness decisively depend on the nature of the substituents attached to the polycyclic backbone. Owing to their flat core unit, compounds exhibiting a carbonyl unit at the bridge position provide a superior building block as compared to thioketone‐bridged derivatives. In addition, nature and length of the peripheral substituents affect the orientation of the aromatic core unit within highly crystalline films. Hence, our results stress the significance of a suitable molecular framework and provide deeper understanding of structure formation in 2D‐confined surroundings for such compounds.
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Affiliation(s)
- Tim Hawly
- Friedrich-Alexander-Universität Erlangen-Nürnberg, Chair of Physical Chemistry II, Egerlandstraße 3, 91058, Erlangen, Germany
| | - Fabian Streller
- Friedrich-Alexander-Universität Erlangen-Nürnberg, Chair of Physical Chemistry II, Egerlandstraße 3, 91058, Erlangen, Germany
| | - Manuel Johnson
- Friedrich-Alexander-Universität Erlangen-Nürnberg, Chair of Physical Chemistry II, Egerlandstraße 3, 91058, Erlangen, Germany
| | - Sandra Miguez-Lago
- Friedrich-Alexander-Universität Erlangen-Nürnberg, Chair of Organic Chemistry I, Nikolaus-Fiebiger-Str. 10, 91052, Erlangen, Germany
| | - Natalie Hammer
- Friedrich-Alexander-Universität Erlangen-Nürnberg, Chair of Organic Chemistry I, Nikolaus-Fiebiger-Str. 10, 91052, Erlangen, Germany
| | - Frank Hampel
- Friedrich-Alexander-Universität Erlangen-Nürnberg, Chair of Organic Chemistry I, Nikolaus-Fiebiger-Str. 10, 91052, Erlangen, Germany
| | - Dustin Vivod
- Friedrich-Alexander-Universität Erlangen-Nürnberg, Chair of Theoretical Chemistry, Nägelsbachstraße 25, 91052, Erlangen, Germany
| | - Dirk Zahn
- Friedrich-Alexander-Universität Erlangen-Nürnberg, Chair of Theoretical Chemistry, Nägelsbachstraße 25, 91052, Erlangen, Germany
| | - Milan Kivala
- Ruprecht-Karls-Universität Heidelberg, Institute of Organic Chemistry & Centre of Advanced Materials, Im Neuenheimer Feld 270 & 225, 69120, Heidelberg, Germany
| | - Robert Branscheid
- Institute of Micro- and Nanostructure Research & Center for Nanoanalysis and Electron Microscopy (CENEM), Friedrich-Alexander-Universität Erlangen-Nürnberg, IZNF, Cauerstraße 3, 91058, Erlangen, Germany
| | - Erdmann Spiecker
- Institute of Micro- and Nanostructure Research & Center for Nanoanalysis and Electron Microscopy (CENEM), Friedrich-Alexander-Universität Erlangen-Nürnberg, IZNF, Cauerstraße 3, 91058, Erlangen, Germany
| | - Rainer H Fink
- Friedrich-Alexander-Universität Erlangen-Nürnberg, Chair of Physical Chemistry II, Egerlandstraße 3, 91058, Erlangen, Germany
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