2014
DOI: 10.1007/s10812-014-9885-x
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Absorption and Luminescence Properties of [2.2]Paracyclophane due to Strong Transannular Interaction

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Cited by 12 publications
(8 citation statements)
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“…The observed CD spectra, however, are not simply explained by the conventional excitonic coupling between the two substituted benzene chromophores. , Due to the effective σ–π interaction with the bridging linker, the relevant orbitals are degenerated to afford a more complex mixture of states . The cyclophane band is described by exciton and charge resonance interactions between the two facing phenes. , Thus, the apparent difference in the CD shapes of 1 and p - 2 and of m ′- 2 and o ′- 2 pairs is ascribable to the altered energy splitting of relevant orbitals due to the different interplanar interaction between the phenes. It is reasonable that the strengths of CEs in dibromocyclophanes are always comparable, as the number of bromine atoms or the steric hindrance derived therefrom is a decisive factor for the cyclophane structure (i.e., dihedral angle Φ) rather than the electronic factor.…”
Section: Resultsmentioning
confidence: 98%
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“…The observed CD spectra, however, are not simply explained by the conventional excitonic coupling between the two substituted benzene chromophores. , Due to the effective σ–π interaction with the bridging linker, the relevant orbitals are degenerated to afford a more complex mixture of states . The cyclophane band is described by exciton and charge resonance interactions between the two facing phenes. , Thus, the apparent difference in the CD shapes of 1 and p - 2 and of m ′- 2 and o ′- 2 pairs is ascribable to the altered energy splitting of relevant orbitals due to the different interplanar interaction between the phenes. It is reasonable that the strengths of CEs in dibromocyclophanes are always comparable, as the number of bromine atoms or the steric hindrance derived therefrom is a decisive factor for the cyclophane structure (i.e., dihedral angle Φ) rather than the electronic factor.…”
Section: Resultsmentioning
confidence: 98%
“…The characteristic spectral features based on the distinctive electronic structure of [2.2]­paracyclophane are apparent in their UV–vis spectra, exhibiting absorption peaks at around 270, 230, and 200 nm, which are assignable to the 1 L a , 1 L b , and 1 B bands, respectively. Additionally, weak absorption assignable to the cyclophane band was observed as a tail at around 310 nm, which is known as the specific transition observable only for [2. n ]­cyclophanes. ,, In parent [2.2]­paracyclophane, the lowest transition of B 2 u symmetry appears at 329 nm in single crystals at 20 K and at ≈305 nm in liquid media. , The corresponding CD peaks were observed for all of the brominated cyclophanes 1 – 2 . Accordingly, the band A with positive CE is assignable to the cyclophane band.…”
Section: Resultsmentioning
confidence: 98%
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“…The Stokes shift values of K4C , K3C , K2C ‐1, K2C ‐2, K2C ‐3, K2C ‐4 and K2M in toluene, defined by the difference in peak frequency between emission and absorption, were approximately 3938, 2813, 1512, 5210, 3991, 3465, and 1812 cm −1 , respectively. The Stokes shift values of the aforementioned PCP derivatives with rigid structures were similar to that of the pristine PCP (4500 cm −1 ) [14] . The relatively small Stokes shift value of K2C ‐1 arises from the localized transition in the IFO‐based chromophore, as presented by K2M [4] …”
Section: Methodsmentioning
confidence: 58%