2017
DOI: 10.1002/qua.25562
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N‐doped cycloparaphenylenes: Tuning electronic properties for applications in thermally activated delayed fluorescence

Abstract: We theoretically characterize a series of substituted cycloparaphenylene nanohoops to study the effect of incorporating an electron-withdrawing group into their cyclic structure. We systematically vary the nature, position, and number of nitrogen-containing acceptor groups in both neutral (pyridine) and charged forms (pyridinium and methylpyridinium) to provide insights into how this functionalization affects the structural, electronic, and optical properties of these systems. We focus also on the singlet-trip… Show more

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Cited by 15 publications
(33 citation statements)
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References 93 publications
(103 reference statements)
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“…In addition and as for the two other nanorings, [8]CPP [28] and [4]C-diEt-F, [30] [4]C-Et-Cbz dis-play ab and tail at around 400 nm, which is due, according to TD-DFT (time-dependent density functional theory) calculations, to asymmetry forbidden( f = 0) HOMO!LUMO transition ( Figure 3B). The H-1, H-2, H-5 and H-6 orbitals are all delocalized all over the nanoring, including the nitrogen atoms, and are thus specific of chromophore [4]C-Et-Cbz.H owever,t he HOMO density resembles that of [8]CPP, [38,39] with no participation of the nitrogen atoms, whereas the LUMO density resembles the one of the molecule of carbazole Cbz itself, with no participation of the carbon atom in para positiono ft he nitrogen atom. LUMO and H-6!LUMO (l th = 340 nm).…”
Section: Resultsmentioning
confidence: 94%
“…In addition and as for the two other nanorings, [8]CPP [28] and [4]C-diEt-F, [30] [4]C-Et-Cbz dis-play ab and tail at around 400 nm, which is due, according to TD-DFT (time-dependent density functional theory) calculations, to asymmetry forbidden( f = 0) HOMO!LUMO transition ( Figure 3B). The H-1, H-2, H-5 and H-6 orbitals are all delocalized all over the nanoring, including the nitrogen atoms, and are thus specific of chromophore [4]C-Et-Cbz.H owever,t he HOMO density resembles that of [8]CPP, [38,39] with no participation of the nitrogen atoms, whereas the LUMO density resembles the one of the molecule of carbazole Cbz itself, with no participation of the carbon atom in para positiono ft he nitrogen atom. LUMO and H-6!LUMO (l th = 340 nm).…”
Section: Resultsmentioning
confidence: 94%
“…The experimental synthesis of donor–acceptor (D–A) compounds [ 288–290 ] has propelled the study of the photophysical and semiconducting properties of this set of materials. [ 112,125,291 ] Figure 7 shows some functionalization strategies of CPPs leading to N‐doped systems. An inmediate consequence of the D–A fragments introduced is the localization of the HOMO and LUMO on different parts of the molecule, thus poorly overlapping and consequently reducing the HOMO‐LUMO energy gap with respect to the undoped CPP systems.…”
Section: Optical and Photophysical Propertiesmentioning
confidence: 99%
“…An inmediate consequence of the D–A fragments introduced is the localization of the HOMO and LUMO on different parts of the molecule, thus poorly overlapping and consequently reducing the HOMO‐LUMO energy gap with respect to the undoped CPP systems. This has important consequences on the lowest singlet‐ and triplet‐excited states of these compounds, [ 125,291 ] and also leads to a relatively low singlet‐triplet energy gap ΔEST, allowing thus to theoretically explore the use of these molecules as thermally activated delayed fluorescence (TADF) emitters [ 292,293 ] : The full harvesting of both singlet and triplet excitons can facilitate light‐emission mechanisms beyond the spin statistical limit [ 294–297 ] for sufficiently small ΔEST values (around 0.1–0.2 eV). Whereas the 8CPP system has a singlet‐triplet gap of 0.5 eV and a forbidden (for symmetry reasons) S1S0 transition, thus precluding its use for any intended TADF application, the D–A strategy roughly halves the singlet‐triplet gap while keeping non‐vanishing oscillator strength values.…”
Section: Optical and Photophysical Propertiesmentioning
confidence: 99%
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“…[30] Several computational investigations have contributed to get insight on the unique properties of CPPs, covering structural, energetic, electronic, magnetic properties [9,10,17,31,32,33] along with their potential application in optoelectronics [34], for instance as thermally activated delayed fluorescence emitters. [35] In addition, charge transport properties of [n]CPPs were initially explored through the estimate of intramolecular reorganization energies and electronic couplings. [36] Prompted by the availability of the crystal structure of N,Ndimethylaza [8]CPP (hereafter labelled DMA [8]CPP, see also Fig.1 and Fig.…”
Section: Introductionmentioning
confidence: 99%