1973
DOI: 10.1016/0375-9601(73)90565-3
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Magnetic field effect on delayed fluorescence from pyrene crystals

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Cited by 7 publications
(5 citation statements)
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“…Experimentally, 2 ao = 113 ± 20, hence and the acute bisector of the resonance directions (this should be the x axis) is at 30 ± 3° from the a direction (which was not determined with high accuracy). The experimental anisotropy in other planes, such as the (b, c') plane [6], is also compatible with the same D*/E*. It appears therefore that the mobile species responsible for T-T annihilation and delayed fluorescence at 300 K in pyrene is the triplet monomer exciton.…”
Section: Classificationsupporting
confidence: 66%
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“…Experimentally, 2 ao = 113 ± 20, hence and the acute bisector of the resonance directions (this should be the x axis) is at 30 ± 3° from the a direction (which was not determined with high accuracy). The experimental anisotropy in other planes, such as the (b, c') plane [6], is also compatible with the same D*/E*. It appears therefore that the mobile species responsible for T-T annihilation and delayed fluorescence at 300 K in pyrene is the triplet monomer exciton.…”
Section: Classificationsupporting
confidence: 66%
“…(5) is therefore also correct). Moreover, with the assumption of a Lorentzian shape, the anisotropy at high field is found to be, as in reference [2b] where w = AElk -, à is the resonance width and yoff and yon are given by (6) and (5).…”
Section: Classificationmentioning
confidence: 63%
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