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The primary photoprocesses of chromium (III) complexes

Energy transfer between Reineckate ion (donor) and
hexacyanochromate(III) ion (acceptor) has been studied through
quenching of donor phosphorescence (lifetime and intensity)
and sensitization of acceptor phosphorescence. Results from
all measurements fit the expected Stern-Volmer relationship
with a quenching constant kQH = 7.2 x 10⁵ M⁻¹ sec⁻¹ at -65°C.
The pre-exponential factor and activation energy of kQH are
6.6 x 10¹º M⁻¹ sec⁻¹ and 4.8 Kcal/mol respectively. The
constant, kQH’ is attributed entirely to an energy transfer
rather than a quenching process. The electronic states directly involved are the ²Eg (and/or² T₁g) states of both donor and acceptor. Energy transfer is a diffusion-controlled
(collisional) process. Hexacyanochromate(III) ion is itself
quenched in the presence of Reineckate ion. The quenching
constant, k'QH, which may be attributed to back energy transfer from acceptor to donor, has a pre-exponential factor of 2 x 10¹² M⁻¹ sec⁻¹ and an activation energy of 7.6 Kcal/mol.
In the same system, quenching of photoaquation has also
been studied at -65°C. The photoaquation quantum yield of
Reineckate ion is 1.02 x 10⁻². It is reduced in the presence
of hexacyanochromate(III) ion, but not as much as the phosphorescence
of Reineckate ion is reduced. The limiting unquenchable part, ϕ∞chem, occurs via the ⁴T₂g state, while
the quenchable part must occur through the ²Eg state as an
intermediate. The actual path for the quenchable part proposed is back intersystem crossing from the ²Eg to the ⁴T₂g state, which then undergoes aquation.

The primary processes of ²Eg state molecules have been
investigated through the temperature dependence of phosphorescence lifetimes of some Cr(III) complexes. All the available evidence supports the idea of the thermally activated back
intersystem crossing. According to this mechanism, the origins of the ⁴T₂g states of Cr (III)complexes reached by crossing are
far lower in energy than has been expected.
Assuming the occurrence of back intersystem crossing, the application of energy transfer to the determination of intersystem crossing quantum yield, ϕisc’ has been demonstrated. The values of ϕisc for Reineckate and hexacyanochromate (III) ions are estimated to be 0.52 and 0.35, respectively. The variation of ϕisc with temperature for these Cr(III) complexes has also been measured, which suggests that in general, internal conversion has a strong temperature dependence.
From the rise of phosphorescence with time after pulse excitation, a new parameter, Tx, has been obtained which represents population of the phosphorescing state and is believed to be the lifetime of the ⁴T₂g (or less likely ²T₁g)
state. Efforts have been made to confirm and identify this
parameter. Studies of ϒx have been carried out as a function of temperature. Mechanisms based on different tentative assignments of ϒx are proposed and their implications examined. All primary processes, except the intrinsic radiative transitions, seem to consist of at least two components, which take different pathways and are different functions of temperature. / Science, Faculty of / Chemistry, Department of / Graduate

Identiferoai:union.ndltd.org:UBC/oai:circle.library.ubc.ca:2429/35225
Date January 1970
CreatorsChen, Schoen-Nan
PublisherUniversity of British Columbia
Source SetsUniversity of British Columbia
LanguageEnglish
Detected LanguageEnglish
TypeText, Thesis/Dissertation
RightsFor non-commercial purposes only, such as research, private study and education. Additional conditions apply, see Terms of Use https://open.library.ubc.ca/terms_of_use.

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