V.T. Kasumo6 / Spectrochimica Acta Part A 57 (2001) 451–460
457
nitrogen (AN=2.22 G) and two sets of three
protons [(AHm=1.11 G (2H) and ANHH=2.22 G
(1H)] assuming that AN=ANHH=2AHm. It is inter-
esting to note that in the oxidation of parent
bis(salicylaidiminato)VO(II) chelates, only for
X=H complex the formation of low intensity
radical was observed. At the same time, our at-
tempts to oxidize X=Cl, Br, NO2 bearing bis(sal-
icylaldiminato)VO(II) complexes in various
solvents were unsuccessful [4c]. Thus, the hydro-
this signal is similar to that of the oxidized
NI(L%) sample. Note that essentially similar ESR
2 2
spectra were also observed in the oxidation of
Cu(II) [15] complexes with the same ligands.
These experimental observations allow us to con-
clude that, the observed ESR spectra originated
from secondary radical species.
9. Bis chelates of Pd(II)
genated VO(L% ) complexes, unlike their salicy-
x 2
laldimine precursors, are readily oxidized with
PbO2 with the formation of the stable phenoxyl
radicals.
All the Pd(Lx)2 complexes are diamagnetic, sug-
gesting a square planar geometry for these com-
pounds. The electronic spectra of these
compounds are different from those of the parent
salicylaldimine Pd(II) chelates. In the electronic
8. Bis chelates of Ni(II)
spectra of the Pd(L% ) complexes together intrali-
x 2
gand absorptions in the UV region, the new
bands at 378–385, 434–485 and 515–526 nm
were also observed. The bands in the regions of
434–485 and 515–526 nm may be assigned to the
All Ni(L% ) complexes are paramagnetic in the
x 2
solid state with magnetic moments in the range
3.32–3.38 B.M. (Table 1), which are close to
those found for tetrahedral Ni(II) complexes [14].
1
1Ag1A2g and Ag1B1g transitions, respectively
Electronic spectra of NI(L% ) in CHCl3 in the
[16]. The other intense band observed in the UV
region at 378–385 nm, probably has metal to
ligand charge transfer character.
x 2
visible region show absorption bands in the range
458–590 and 685–790 nm and according to the
values of coefficient extinction (m=320–450) can
Upon treatment of Pd(L%) and Pd(L%) com-
1 2
3 2
3
3
be assigned to T13A2 and T13T(P) in tetra-
hedral symmetry [14]. The bands appeared at
364–385 nm, and can be attributed to the ligand-
to-metal charge-transfer transitions.
plexes with PbO2 in CHCl3 solution under the
above mentioned conditions, well resolved ESR
spectral patterns having quite close magnetic reso-
nance parameters were observed. In all cases dur-
ing oxidation the gradually precipitation of the
These complexes, unlike their salicylaldimine
analogous, rather readily oxidized with PbO2 in
CHCl3 at room temperature giving corresponding
metallic Pd occurred. Upon oxidation of Pd(L%)
1 2
and Pd(L%) complexes, relatively stable radical
3 2
radical species. In the oxidation of Ni(L% ) low
species exhibiting nine line hyperfine splitting
spectral features with an intensity distribution of
1:4:7:8:8:8:7:4:1 and ESR parameters such as g=
2.0062, AH=1.25 G and g=2.0045, AH=l.223
G, respectively, were observed (Fig. 2(e)). In the
x 2
intensity unresolved signal centered at g=2.0038
was observed. However, under the same condi-
tions, oxidation of Ni(L%) and Ni(L%) results in
2 2
3 2
an ESR spectra which consist of equidistant nine-
and ten-line patterns (Fig. 1(d) and (e)) with the
parameters such as g=2.0041, AH=1.013 G and
g=2.0038, AH=1.127 G, respectively. The nine-
line spectrum, according to line shapes, number of
lines, intensity ratios and the values of g-factors
and hfsc (within experimental error) are very sim-
ilar to those of the oxidized VO(Lx)2 and Pd(II)
samples spectra. The highest field component of
the spectrum in Fig. 1(e) most probably has an-
other origin and equal spacing nine-line part of
case of oxidized Pd(L%) sample in CHCl3, at 300
2 2
K, the unusual spectrum having unresolved low
field wing and a well resolved nine-line pattern on
the high field side (g=2.0053, AH=1.166 G) was
detected (Fig. 2(g)). This spectral pattern remains
unchanged on varying in concentration of com-
plex over range of 10−4–10−3 M as well as with
changes in gain and modulation amplitude from
0.05 to 2 G. The unusual broadness and the
asymmetry of the overall pattern was probably