Inorganic Chemistry
Communication
[NO]+, which displays a band at 924 cm−1 consistent with an
oxygen-bound sulfoxide.3 UV−vis spectroelectrochemical data
were also obtained for the oxidized forms of 1-L1, 1-L2, and 2-
L2: The visible spectra are dominated by a moderately intense
Cl(pπ) → Ru(dπ) LMCT transition in each case.
Various parameters were quantitatively determined for 2-L2
following earlier treatments of similar data: CVs with an initial
anodic scan direction were recorded at a variety of scan rates
(see the SI).10 The equilibrium constant, KIIIO→S, was calculated
Notes
The authors declare no competing financial interest.
ACKNOWLEDGMENTS
■
We thank both the Research Corporation for Science
Advancement (Cottrell College Science Award) and the NSF
(MRI 0923051) for support. We also thank the Jess and
Mildred Fisher College of Science and Mathematics at TU and
TU Faculty Development and Research Committee for
financial support. Dr. S. Stitzel is thanked for assistance in
obtaining the spectroelectrochemical data.
to be 1.33
0.06, indicating marginally greater stability of
Ru3+[S,S] versus Ru3+[S,O]. KIIO→S was then determined to be
1.91 × 109; i.e., the Ru2+[S,S] form is highly favored versus
Ru2+[S,O]. The rate constants kIII
and kIII
were also
S→O
REFERENCES
O→S
■
estimated as 2.8 and 2.1 s−1, respectively. Compared to related
DMSO complexes, the stability of the oxygen-bound form is
decreased, but there is a slight increase in the isomerization
kinetics (on Ru3+).9,10 Although difficulty in measuring accurate
peak currents in CVs of 2-L1 precluded similar analysis, the
forms of the CVs imply that both Ru3+[S,O] and Ru2+[S,O]
have greater stability than that in 2-L2.
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In our ruthenium complexes, RILI occurs only with the cis-β
isomers and within the strongest ligand-field environment,
consistent with certain earlier reports.7,10 Inspection of the
DFT-calculated highest occupied molecular orbitals (HOMOs)
of each isomer shows that all lie in the Cl−Ru−Cl plane (see
Figure 3) and are predominantly of Ru(d)−Cl(π) antibonding
(12) Butcher, D. P.; Rachford, A. A.; Petersen, J. L.; Rack, J. J. Inorg.
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(17) Additional metal complex stereoisomers are possible because of
the nitrogen stereocenters and, in the case of the cis-α and cis-β
isomers, a ruthenium stereocenter.
Figure 3. Calculated HOMOs of the three isomers.
(18) Hiroi, K.; Suzuki, Y.; Abe, I.; Hasegawa, Y.; Suzuki, K.
Tetrahedron: Asymm. 1998, 9, 3797−3817.
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(20) Henn, M.; Alessio, E.; Mestroni, G.; Calligaris, M.; Attia, W. M.
Inorg. Chim. Acta 1991, 187, 39−50.
(21) In CVs of 2-L1, another feature is seen approximately 0.5 V
cathodically shifted from the major couple; we attribute this to an, as
yet, unknown impurity.
character. Only in the cis-β isomer is the Ru−S bond also in this
plane. We propose that depopulation of this HOMO upon
oxidation leads to increased “hardness” in this plane, resulting
in the tendency of this sulfoxide to isomerize in the cis-β
isomer. Ongoing investigations will seek to further clarify the
electronic origin of RILI in these complexes and other
outstanding questions, including the relationship of the ligand
structure to the metal complex geometric isomer distribution.
ASSOCIATED CONTENT
* Supporting Information
■
S
X-ray crystallographic data in CIF format, complete exper-
imental details and characterization data for the synthesis of
ligands and ruthenium complexes, UV−vis and CD spectral
data, CV data and X-ray crystallographic data for solution and
refinement, and table of selected bond lengths and angles, and
details of DFT calculations. This material is available free of
AUTHOR INFORMATION
Corresponding Author
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dx.doi.org/10.1021/ic302188y | Inorg. Chem. 2013, 52, 1170−1172