S. Singh et al. / Inorganica Chimica Acta 407 (2013) 31–36
35
similar to the thiocarboxylate complexes of Cd(II)/Ag(I) [15] and
Pb(II)/Ag(I) [17].
For unambiguous assignment of the absorption bands time
dependent density functional theory (TDDFT) calculations have
been performed at PBE1 level. The orbital transition plots of 1
are shown in Fig. 3. The calculated absorptions at 455 nm and
440 nm are due to electron transfers from lone pair of silver atom
to the p⁄ orbital of thiophene ring of the bridging thiocarboxylate.
This involves transitions (n ? p⁄) from HOMOÀ4 and HOMOÀ3 to
LUMO, LUMO+1 orbitals. Experimentally these transitions are
responsible for the broad absorption peak ranging from 400 to
450 nm (with an absorption maximum at 426 nm). Other absorp-
tion peaks at 372 and 345 nm are due to admixing of metal to li-
gand, intra-ligand and inter-ligand charge transfer transitions.
These peaks are observed experimentally at 368 and 342 nm
respectively.
3.4. Emission spectra
Fig. 4. Emission spectrum of 2 in solid state.
To the best of our knowledge there is no literature available on
the photoluminescence properties of Zn(II)/Ag(I) heterobimetallic
compounds. Emission spectra of complexes 1 and 2 have been re-
corded in solid state. When exited at 426 nm complex 1 showed
two weak emission bands at 469 and 522 nm (broad) (Fig. S9,
Supporting information). Complex 2 showed a strong and broad
emission band at 490 nm (Fig. 4) when it was exited at 400 nm.
In both the cases, no significant changes were observed in the
emission spectrum on changing the excitation wavelengths. The
emission bands observed are thus due to the excitation of electrons
by metal centered charge transfer transitions [17].
ven in Table 2. In this case all three thiophene rings and two phenyl
rings of triphenylphosphine are distorted.
The three thiocarboxylate ligands exhibit three different coordi-
nation modes. One of the ligands binds monodentately to Zn(II)
through the sulfur atom (S5) and the other two form bridges be-
tween Zn and Ag atoms. The bridging in one case is
is ( -O,S) in the other. The Zn(II) being harder as compared to
Ag(I) is bounded by O2 atom of the ( -O,S) bridging ligand. The
l-S while it
l
l
fourth coordination site of Zn is occupied by the oxygen atom of
a water molecule. A look at the various angles subtended at Zn1
by the donor atoms also reveals a distorted tetrahedral geometry
around it. However, the presence of S3 atom affects the geometry
to some extent by capping the S1, S5, O2 face of tetrahedron.
Geometry around Ag1 is also tetrahedral with significant distortion
which is possibly a consequence of large steric demands of the two
triphenylphosphine ligands.
Evidently, there is no Zn–Ag bonding in this complex as the two
atoms are separated by 3.723 Å which is even larger than the sum
of the van der Waals’ radii of these two atoms.
The structure of complex 2 revealed an unusual co-crystalliza-
tion of two different molecules in the same lattice (Fig. 2). Molec-
ular core in one of these (containing Zn1 and Ag1) is isostructural
to that of 1. In the second molecule, the two metals Zn2 and Ag2
4. Conclusions
Two new heterobimetallic complexes, [(PPh3)2Ag(
Zn(SCOth)(H2O)] (1) and {[(PPh3)2Ag( -SCOPh)2Zn(SCOPh)(H2-
O)][(PPh3)2Ag( -SCOPh)Zn(SCOPh)2]} (2) have been synthesized
l-SCOth)2-
l
l
and characterized by spectral and X-ray diffraction studies.
Structure of 2 is unique as two different molecules, [(PPh3)2Ag
(l-SCOPh)2Zn(SCOPh)] and [(PPh3)2Ag(l-SCOPh)2Zn(SCOPh)H2O]
co-crystallize in the same lattice. Electronic spectral behavior of
the complex 1 has been explained by TDDFT calculations. The
two complexes may further be explored for their application as
single source precursors for Ag/Zn sulfide nanoparticles.
are held together by the sulfur (l2-S) atom of a thiobenzoate
ligand. The Zn2 atom is coordinated by O7 besides the three S
atoms. The Ag2 is tricoordinated having bonded to one sulfur
and two phosphorus atoms. Notably, the Ag2 atom is tipped above
the P2S plane by 0.317 Å which is possibly a consequence of
Ag2Á Á ÁO6 interaction. [The Ag2–O6 distance is 2.757 Å which is
substantially shorter than the sum of the van der Waals’ radii of
the Ag and O atoms (3.24 Å).]
Acknowledgements
The authors are grateful to Professor R.J. Butcher, Howard Uni-
versity, USA for his help in refining the structures (particularly of
compound 1). Financial supports in the form of a research project
to S.B. by the university grants commission, India, SRF to S.S. and
J.C. by the Council of Scientific and Industrial Research, India are
gratefully acknowledged.
3.3. Electronic absorption spectra
Appendix A. Supplementary material
Absorption spectrum of 1 showed absorptions at 234, 239, 255
and 312 nm. In solid state the peaks at higher frequencies appeared
at 272 and 288 nm, while the lower energy absorptions were
observed at 321, 342, 368 nm and a broad peak at 426 nm. Simi-
larly, the complex 2 showed absorption peaks at 225, 234, 239,
246 and 314 nm in solution state whereas in solid state peaks were
observed at 252, 305, 326, 342 and 412 (broad) nm (Figs. S5–S8,
Supporting information). In general, lower energy peaks appear be-
cause of the metal to ligand (or ligand to metal) charge transfers
while peaks below 300 nm are due to the inter- or intra-ligand
charge transfers. Spectral behavior of both the complexes are very
CCDC 772371 and 772370 contains the supplementary crystal-
lographic data for 1 and 2. These data can be obtained free of
charge from The Cambridge Crystallographic Data Centre via
ated with this article can be found, in the online version, at http://
References