6533b7cefe1ef96bd12571ff
RESEARCH PRODUCT
Computational determination of the dominant triplet population mechanism in photoexcited benzophenone
Daniel Roca-sanjuánRia BroerRémi MauriceRémi MauriceDumitru-claudiu SergentuDumitru-claudiu SergentuRemco W. A. HavenithRemco W. A. Havenithsubject
STATE DIPOLE-MOMENTSPopulationMechanistic organic photochemistryEXCITED BENZOPHENONEGeneral Physics and AstronomyGAS-PHASEABSORPTION-SPECTROSCOPYchemistry.chemical_compoundORGANIC-PHOTOCHEMISTRYMOLECULAR WAVE-FUNCTIONSBenzophenonePhysical and Theoretical ChemistryeducationWave functioneducation.field_of_studyROW ATOMSChemistryCONICAL INTERSECTIONSPhotoexcitation[CHIM.THEO]Chemical Sciences/Theoretical and/or physical chemistryIntersystem crossingExcited state2ND-ORDER PERTURBATION-THEORYANO BASIS-SETSAtomic physicsPhosphorescencedescription
In benzophenone, intersystem crossing occurs efficiently between the S-1(n pi(star)) state and the T-1 state of dominant n pi(star) character, leading to excited triplet states after photoexcitation. The transition mechanism between S-1(n pi(star)) and T-1 is still a matter of debate, despite several experimental studies. Quantum mechanical calculations have been performed in order to assess the relative efficiencies of previously proposed mechanisms, in particular, the direct S-1 -> T-1 and indirect S-1 -> T-2(pi pi(star)) -> T-1 ones. Multiconfigurational wave function based methods are used to discuss the nature of the relevant states and also to determine minimum energy paths and conical intersections. It is found that the T-1 state has a mixed n pi(star)/pi pi(star) character and that the T-2(pi pi(star)) state acts as an intermediate state between the S-1 and T-1 states. This result is in line with recent experiments, which suggested a two-step kinetic model to populate the phosphorescent state after photoexcitation [Aloise et al., J. Phys. Chem. A, 2008, 112, 224-231].
year | journal | country | edition | language |
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2014-09-30 |