A.Z. El-Sonbati et al. / Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy 99 (2012) 211–217
217
and remained slightly changed for metal complexes. The absorp-
Conclusions
tion shift and intensity change in the spectra of the metal com-
plexes most likely originated from the metallation, increased the
conjugation and delocalization of the whole electronic system
and resulted in the energy change of the
tions of the conjugated chromophore [26].
Based on the above observations of the elemental analysis, mo-
lar conductivity, UV–vis, magnetic, IR, 1H NMR spectral data it is
possible to determine the type of coordination of the ligands in
their metal complexes. The spectral data show that all the Schiff
bases exist as neutral bidentate in mononuclear (NO)/Schiff base
complexes (NNꢀ) and monobasic tridentate (NNꢀO) in Schiff bases
complexes. The analytical data show the presence of one metal
ion per one/two ligand molecules and suggest a mononuclear
structure for the complexes. The correlation of the experimental
data allows assigning a square planar stereochemistry to all the
above synthesized complexes as shown in Scheme 1. The present
study shows the construction of a Pt(II)-based metallopyrazolone
on the skeleton of a simple tridentate Schiff base which provides
an electron rich cavity. The space provided by the cavity is found
to be suitable for comparatively stronger binding of an electron
acceptor molecule. This study also allows the difference in the
reactivity of Pd(II) and Pt(II) complexes with tridentate Schiff base
to be understood.
p ?
pꢀ and n ? pꢀ transi-
The electronic spectra of patinum(II) and palladium(II) com-
plexes are indicative of square planar geometry (Structure 1). The
absorption bands for the platinum(II) and palladium(II) complexes
may be assigned to the three d–d forbidden transition expected
from the three lower lying d levels to empty dx2–y2 orbitals. The
1
ground state is A1g and the excited states corresponding to the
1
above transitions are A2g
,
1B1g and 1Eg in order of increasing en-
ergy. By assuming a value of F2 = 10F4 = 600 cmꢄ1 for a Slater–Con-
don interactions repulsion parameters and subsequently the
equations suggested by Cray and Ballhausen [27], it is possible to
calculate the single electron parameter D1, D2 and D3 (Table 6).
The t2 t1 value lies in the 1.059–1.251 range, comparable with
/
the values reported earlier for square planar complexes [14,15].
The values of D1 for Pt(II) complexes are much higher than those
observed for palladium(II) complexes but are in accordance with
those required for platinum(II) square planar complexes. The
values of D1 lie in between those observed for cyanide
(ꢁ30,000 cmꢄ1) and chloride complexes (ꢁ19,000 cmꢄ1) and are
consistent with intermediate ligand field strength [28,29]. The
crystal field stabilization energies for Pd(II) and Pt(II) complexes
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4
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