1974
DOI: 10.1016/0301-0104(74)85030-5
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Theoretical evaluation of potential surfaces, equilibrium geometries and vibronic transition intensities of excimers: the pyrene crystal excimer

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Cited by 83 publications
(67 citation statements)
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“…The formation of highly emissive excimers in the mesostructured organosilica films can be explained by considering the steric effects of the chromophores. The excimer state of pyrene is theoretically described as an exciton‐resonance state, which is responsible for the parallel arrangement of the molecular axes of the pyrenes . The excimer of pyrenes in a solid state has also been reported to form a sandwich geometry with a distance of ≈3.3 Å and a slight displacement .…”
Section: Resultsmentioning
confidence: 99%
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“…The formation of highly emissive excimers in the mesostructured organosilica films can be explained by considering the steric effects of the chromophores. The excimer state of pyrene is theoretically described as an exciton‐resonance state, which is responsible for the parallel arrangement of the molecular axes of the pyrenes . The excimer of pyrenes in a solid state has also been reported to form a sandwich geometry with a distance of ≈3.3 Å and a slight displacement .…”
Section: Resultsmentioning
confidence: 99%
“…[34,35] The excimer of pyrenes in a solid state has also been reported to form a sandwich geometry with a distance of ≈3.3 Å and a slight displacement. [35] The DPPy chromophore with two phenyl substituents on the 1,6positions of pyrene can form an excimer with a parallel arranged sandwich geom etry due to the small steric hindrance in its lateral direction (Figure 1b). On the other hand, the TPPy chromophore cannot form such a parallel arranged and closely stacked sandwich geometry, owing to its bulkiness due to the four phenyl sub stituents.…”
Section: Resultsmentioning
confidence: 99%
“…, (4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17) where k rad E and k rad M are the rate constants for the radiative decay of the excimer and the excited monomer. In practice, an upper integration limit t ∞ ≈ 10/(k S ) min will be virtually equivalent to infinity.…”
Section: Evolution Of the 1 M * · · · 1 M Pair Distribution Functionmentioning
confidence: 99%
“…First, for each discrete time t the corresponding mean radii R E (t) and R M (t) are calculated, (4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18) with an analogous expression for R M (t). First, for each discrete time t the corresponding mean radii R E (t) and R M (t) are calculated, (4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18) with an analogous expression for R M (t).…”
Section: Evolution Of the 1 M * · · · 1 M Pair Distribution Functionmentioning
confidence: 99%
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