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Effect of the Structure of Ti Species on the Photoepoxi-
dation Activity. As shown in Table 1, the T-S(4.1) sample
showed lower selectivity to PO (21.5%) than the T-S(0.34)
sample (57.5%). The lower selectivity over the T-S(4.1) sample
-
related to a lower ratio of O3-/O2 (Figure 5), which should
correspond to species III/(species III + species V) in Scheme
1. Thus, route B is mainly promoted, or route A is less promoted
over the aggregated titanium oxide species because of the
-
smaller amount of O3
.
In the stoichiometric reactions over the T-S(4.1) sample,
-
when propene was contacted with O3 and O2-, PO was not
obtained, but ethanal, acrolein, and propanal were formed (Table
2, run 6). The products distribution is essentially identical to
that obtained in method C (run 8). The O3- over the T-S(4.1)
-
sample in method A (run 6) would decompose to OL and O2
before it reacts with propene during warming the sample from
-
77 K to room temperature. This result indicates that the O3
over the aggregated titanium oxide species would be unstable
and more likely to decompose to OL- and O2 than that over the
isolated tetrahedral Ti species. This difference in stability of
-
the O3 would be the major reason the isolated tetrahedral Ti
species is effective for PO production.
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In addition, the consecutive reaction of PO is little promoted
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Conclusion
The isolated tetrahedral Ti species on the TiO2-SiO2 samples
catalyze the photoepoxidation of propene with molecular
oxygen. [Ti4+-OL2-] is excited by UV light to form a [Ti3+
-
OL-]* radical pair. The Ti3+ moiety reacts with O2 to form O2
.
-
-
The OL moiety, a hole center on lattice oxygen, reacts with
O2 to form O3-, which reacts with propene to yield PO. The
O3- would be the electrophilic oxygen species effective for the
-
epoxidation of propene. When the OL moiety reacts with
propene, acrolein or ethanal is produced through H abstraction
or CC bond fission.
The isolated tetrahedral Ti species exhibit the higher stability
-
of the O3 and lower activity for the consecutive reactions of
PO in comparison with the case of the aggregated titanium oxide
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Acknowledgment. We thank Prof. Y. Okamoto, Dr. Y. Isobe
(Department of Applied Chemistry, Graduate School of Engi-
neering, Nagoya University), Mr. Y. Nagara, and Mr. M.
Kawahara (Japan Chemical Innovation Institute, Nagoya) for
their aid in ESR measurement. This work was supported by a
grant-in-aid from the Japanese Ministry of Education, Science,
Art, Sports and Culture, and by Nippon Sheet Glass Foundation
for Materials Science and Engineering.
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