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Singlet Exciton Fission and Tri plet-Tri plet Exciton Fusion in Crystalline Tet racene
99
Citations
17
References
1969
Year
EngineeringNuclear PhysicsSolid-state ChemistryExcitation Energy TransferChemistryElectronic Excited StatePhosphorescence ImagingCrystalline TetraceneQuantum MaterialsPhotophysical PropertyPhysicsPhotochemistryQuantum ChemistrySinglet Exciton FissionNuclear AstrophysicsExperimental Nuclear PhysicsNatural SciencesApplied PhysicsCondensed Matter PhysicsCrystalline Tet RaceneMagnetic FieldRate Constants
AbstractThe dominant radiationles decay channel in crystalline tetracene at 300 °K is a fission of an excited singlet into two triplet excitons with a rate constant γS = 1.5 × 10−12 ± 5% cm3 -sec−1. The efficiency of this process at room temperature is estimated as 95%and constitutesan efficient intersystem crossing mechanism. At light intensities I ⩾ 1015 quanta-cm−2 sec−1 (366 μm excitation), the triplet densities at 300 °K are sufficiently high to produce radiative triplet-triplet annihilation or fusion. As the light intensity is increased the quantum efficiency of fluorescence φ increases, and eventually reaches a constant value (about twice its value in the low intensity region, where fusion is not important). It is assumed that triplet-triplet fusion gives rise to either an excited singlet (rate constant γTS = (4.8 ± 1.2) × 10−10 cm3-sec−1), or excited triplet (rate constant γTT = (11 ± 5) × 10−10 cm3-sec−1). The effect of a magnetic field H = 4000 gauss on the rate constants is determined. The radiative triplet-triplet fusion constant and γS both decrease in approximately the same manner when a magnetic field is applied. γTT is shown to be at most slightly dependent on H.
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