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consistent with those obtained from the single crystal X-ray struc-
ac
1
ture determination of c-3 ꢂ2toluene. It is to be noted that the
experimental and calculated bond lengths of the picolinic acid
anion radical are significantly different from those of the picolinate
chelates (ESI,† Chart S1). The calculated C3–N1 (1.393 Å) distance
of the pyridine ring of the picolinic acid anion radical is longer than
that (exp., 1.339(10) Å; cal., 1.350 Å) in the picolinate chelate while
the C2–C3 (1.404 Å) length in the picolinic acid anion radical is
much shorter than that (exp., 1.487(12) Å; cal., 1.525 Å) in the
picolinate chelate. A similar trend has been established precisely by
Wieghardt et al. in one electron reduced iminopyridine complexes
of 3d elements.5 The C2–O2 length in the anion radical is also
comparatively shorter. The C2–O3 distance (1.363 Å) is remarkably
longer in the acid anion radical compared to that, 1.227(10) Å
(cal., 1.231 Å), in the acid chelate. The two alternate C–C bonds in the
picolinic acid anion radical (C3–C4 and C5–C6, 1.426 and 1.421 Å)
are longer than the average C–C length in a pyridine ring.
Fig. 2 ORTEP plot (30% probability level) of c-3acꢂ2toluene (H atoms and
1
solvents are excluded for clarity).
t-2rad and c-2rad. The spectrum of Arad is consistent with the presence
of two equivalent PPh3 ligands. The hyperfine couplings due to four
equivalent pyridine H atoms correlate excellently with the existence
of the picolinic acid anion radical in t-2rad and c-2rad complexes.
Similar spectral features of the bipyridine anion radicals have been
documented in the literature.4
The moderately strong absorption bands of t-2rad and c-2rad above
600 nm which are absent in picolinate complexes, t-3ac and c-3ac, as
shown in Fig. S5 (ESI†), are characteristics of a picolinic acid anion
radical complex. The lower energy absorption maxima of t-2rad and
c-2rad of LMCT origins disappear during proton induced electron
transfer reaction reducing H+ to H2 slowly in solution as shown in Fig.
S13 (ESI†). Origins of the lower energy absorptions of t-2rad and c-2rad
have been investigated by TD DFT calculations on t-2rMade and c-2Mrade in
CH2Cl2 solvent using the CPCM model. The responsible photoactive
orbitals are illustrated in Fig. S14 (ESI†). Calculations have predicted
three lower energy absorption bands at 744.5, 709.9 and 617.6 nm
due to LMCT i.e., SOMO (a-HOMO) to LUMO (dz2) or LUMO +
1(dx2ꢀy2) orbitals as summarized in Table S6 (ESI†). The transition
Single crystal X-ray structure determinations have confirmed
the C–C bond cleavage forming the picolinic acid from the (PyCO)2
ac
and trans and cis geometries of the t-3ac and c-3 ꢂ2toluene com-
1
plexes. However, t-3ac poorly diffracts and the crystallographic data
ac
1
%
are not reported here. c-3 ꢂ2toluene crystallizes in the P1 space
group. The molecular geometry with the atom labelling scheme is
illustrated in Fig. 2 (also Fig. S15, ESI†). The crystallographic data
and the bond parameters of c-3 ꢂ2toluene are summarized in
Tables S2 and S3 (ESI†) (CCDC 833917).
ac
1
The spin density distributions of Arad, t-2rad and c-2rad were
elucidateꢀd by the unrestricted DFT calculations on [Ru(PMe3)2-
((PyCO)2 ꢁ)(CO)Cl] (AMrade), trans-[Ru(PMe3)2(PyCOOHꢀꢁ)(CO)(Cl)]
(t-2rMade) and c-2rad with a doublet spin state. The gas-phase geometry
of cis-[Ru(PMe3)2(PyCOOHꢀꢁ)(CO)(Cl)] (c-2Mrade) was also optimized.
The optimized geometries are shown in Fig. S12 (ESI†). The calcu-
lated bond parameters of all these radical complexes are summar-
features of picolinate complexes have also been elucidated by TD DFT
ac
Me
calculation on c-3 in dichloromethane using the CPCM model.
In this case, no lower energy excitations have been predicted. The
ac
Me
calculated lower energy excitations of c-3 are 329.01 and 324.58 nm
rad
Me
rad
Me
ized in Table S4 (ESI†). c-2 and t-2 have comparable energies
with oscillator strengths (f) of 0.015 and 0.042 respectively.
In conclusion, formation of a 2,20-pyridil anion radical and its
asymmetric cleavage by water affording unprecedented picolinic
acid anion radical complexes with a transition metal ion, which
produce hydrogen gas and picolinate complexes, is reported.
Financial support received from DST (SR/S1/IC/0026/2012) and
CSIR (3231/NS-EMRII), New Delhi, India, is gratefully acknowl-
edged. M. K. B. is thankful to CSIR for the fellowship (8/531(007)/
2012-EMR-I). We are thankful to Prof. J. K. Bera, IIT, Kanpur,
India, for providing us the facility to record hydrogen evolution.
and both the isomers are isolable experimentally. Mulliken spin
population analyses authenticated that the spin densities are pri-
marily localized on the 2,20-pyridil ligand in AMrade and PyCOOH
chelate of t-2Mrade and c-2rad. The spin density plots of AMrade, t-2Mrade and
c-2rad are shown in Fig. 3. In ArMade, spin density is mainly localized on
rad
the trans-CO–CO-fragment while in t-2 and c-2rad complexes it is
Me
mainly localized on the pyridine chelate forming a picolinic acid
anion radical, PyCOOHꢀꢁ. The spin density distribution features
correlate well with the fluid solution EPR spectra of Arad and pyridine
H hyperfine couplings of t-2rad and c-2rad complexes at 298 K (Fig. 1).
The gas phase geometry of cis-[Ru(PMe3)2(PyCOOꢀ)(CO)(Cl)] Notes and references
(c-3aMce) has also been optimized with the singlet spin state for
1 (a) G. H. Spikes, E. Bill, T. Weyhermu¨ller and K. Wieghardt, Angew.
ac
Me
comparison. The calculated bond parameters of c-3
are
Chem., Int. Ed., 2008, 47, 2973; (b) G. H. Spikes, S. Sproules, E. Bill,
T. Weyhermu¨ller and K. Wieghardt, Inorg. Chem., 2008, 47, 10935.
2 M. K. Biswas, S. C. Patra, A. N. Maity, S.-C. Ke, N. D. Adhikary and
P. Ghosh, Inorg. Chem., 2012, 51, 6687.
3 (a) W. T. Eckenhoff and R. Eisenberg, Dalton Trans., 2012, 41, 13004;
(b) T. Lazarides, T. McCormick, P. Du, G. Luo, B. Lindley and
R. Eisenberg, J. Am. Chem. Soc., 2009, 131, 9192.
4 E. Gore-Randall, M. Irwin, M. S. Denning and J. M. Goicoechea, Inorg.
Chem., 2009, 48, 8304.
5 (a) C. C. Lu, E. Bill, T. Weyhermu¨ller, E. Bothe and K. Wieghardt,
J. Am. Chem. Soc., 2008, 130, 3181; (b) A. C. Bowman, C. Milsmann,
C. C. H. Atienza, E. Lobkovsky, K. Wieghardt and P. J. Chirik, J. Am.
Chem. Soc., 2010, 132, 1676.
rad
Fig. 3 Mulliken spin population analyses of ArMade, t-2 and c-2rad
.
Me
c
4524 Chem. Commun., 2013, 49, 4522--4524
This journal is The Royal Society of Chemistry 2013