2019
DOI: 10.1039/c9sc00169g
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Symmetry breaking and the turn-on fluorescence of small, highly strained carbon nanohoops

Abstract: By breaking the centrosymmetry of the structure, the most strained carbon nanohoops become fluorescent as predicted by optical selection rules.

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Cited by 119 publications
(241 citation statements)
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“…This value is higher than that observed in [4]C-diEt-F for which the angle is zero. [7] The mean torsion angle appearsherein as high as 40.68 (values comprised between 38.38 and 42.358,F igure S24), which is similar to that measured in [4]C-diEt-F (41.58 between two fluorene units) [30] and significantly higher than that of [8]CPP (24.38 between two phenyl units, Figure S29). Thus, the nitrogen bridge provides more structural flexibility than the carbon bridge in an anoringc onstituted of four units.…”
Section: Resultssupporting
confidence: 68%
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“…This value is higher than that observed in [4]C-diEt-F for which the angle is zero. [7] The mean torsion angle appearsherein as high as 40.68 (values comprised between 38.38 and 42.358,F igure S24), which is similar to that measured in [4]C-diEt-F (41.58 between two fluorene units) [30] and significantly higher than that of [8]CPP (24.38 between two phenyl units, Figure S29). Thus, the nitrogen bridge provides more structural flexibility than the carbon bridge in an anoringc onstituted of four units.…”
Section: Resultssupporting
confidence: 68%
“…[2][3][4][5][6] Compared to their linearc ounterparts, nanorings present singular electronic and structuralc haracteristics. [3][4][5][6][7] In addition, studies on the influence of the nanoring size and of the building units on the structural, electronic, physical, chiral and encapsulating properties have already shown the diversity of this field. [3][4][5][6][7][8] The growinginterestinnanorings chemistry and physics has led to recent applications such as imaging tools in biology [9] or complexation of single-walledc arbonn anotubes.…”
Section: Introductionmentioning
confidence: 99%
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“…Additionally, as a consequence of breaking molecular orbital symmetry, it should be noted that both 3 and 4 were fluorescent, with 3 emitting at λ max of 509 nm ( Φ =0.14) and 4 at λ max of 476 nm ( Φ =0.62). Of note, the all para ‐substituted nanohoop with a single embedded pyridine is non‐emissive; a detailed investigation of the result of symmetry breaking on nanohoop fluorescence is disclosed in a separate study …”
Section: Figurementioning
confidence: 99%
“…[27,28] Finally, most CPPs are brighter than similar emitting smallmolecule fluorophores, they retain their fluorescent properties in aqueous media, have minimal cytotoxicity and are cell permeable making them attractive as novel biological fluorophores. [7,18,29,30] However, bright CPPs with emissions beyond 500 nm have yet to be realized. CPP fluorescence red-shifts as the size of the nanohoop decreases, however, decreasing size leads to a dramatic decrease in quantum yield due to strain and orbital-symmetry rules.…”
mentioning
confidence: 99%