A.A. El-Asmy, G.A.A. Al-Hazmi / Spectrochimica Acta Part A 71 (2009) 1885–1890
1889
Fig. 5. The ESR spectrum of [Cu(HBPPip-2H)].
3.2. Magnetic and spectral studies
the Ni(II)-ligand bonds. The values of 10Dq decrease by increasing
the percentage of square-planar participation (Table 4). The spec-
trum of [Ni(HBP4M-H)(OAc)] is different where the strong band at
20,675 cm−1 is attributed to the d–d transition in a square-planar
geometry. In DMF, this band appeared at 24,290 cm−1 indicating a
solvent effect. Fig. 4 presents the structure of [Cu(HBP4Ph-H)(OAc)]
and [Cu(HMBP4Ph-H)(OAc)].
The magnetic moments and the electronic spectral bands of the
studied Ni(II) and Cu(II) complexes are given in Table 4. The ligands
have spectral bands similar in solid and DMF solution and exist at
36,500–25,000 cm−1 corresponding to the → and n→ tran-
*
*
sitions [22].
Most of the Ni(II) complexes have subnormal magnetic val-
ues (0.85–2.02 BM) due to mixed stereochemistry of square-planar
and tetrahedral structure. The decrease in the moment values may
be attributed to the presence of square-planar with high percent.
The following complexes are ordered according to the percentage
of square-planar: [Ni(HBPPip-2H)] (75%) > [Ni(HMBP4Ph-2H)]H2O
(64%) > [Ni(HBP4Ph-H)(OAc)] (55%) > [Ni(HMBPPip-H)(OAc)] (41%)
which is calculated by relating the measured values to 3.4 BM (the
tetrahedral Ni(II) complexes have 3.4–3.8 BM range). On the other
hand, [Ni(HBP4M-H)(OAc)] measured zero moment indicative of
totally square-planar structure.
Also, all Cu(II) complexes measured subnormal values
(0.81–1.55 BM) indicating interaction between the copper centers;
the interaction becomes strong in [Cu(HMBP4Ph-H)(OAc)]H2O and
less in [Cu(HBP4Ph-H)(OAc)]; this may be related to the bulky of
HMBP4Ph rather than HBPP4Ph.
3.3. ESR spectra
To obtain further information about the stereochemistry of the
parameters were calculated (Table 5). The room temperature solid
state have ESR spectra (Fig. 3) quite similar and exhibit g-tensor
parameters with g > g > 2.0023 indicating that the copper site
||
⊥
2
has a dx2 − dy ground state [25] characteristic for a square-planar
geometry [26].
In axial symmetry, G = (g –2)/(g –2) where G is the exchange
||
⊥
interactions [27]. The band corresponding to the forbidden mag-
netic dipolar transition is not observed at half-field (ca. 1600G,
g = 4.0) indicating mononuclear complexes [28]. The ESR spectrum
of [Cu(HBPpip-2H)] is shown in Fig. 5.
The solution and solid electronic spectra of the complexes are
approximately the same; changes are recorded with the spectra of
their ligands. The band at 22,000–26,000 cm−1 in the spectra of
Cu(II) complexes may be due to LMCT [23].
References
The electronic spectra of the Cu(II) complexes showed one
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[9] R.M. El-Shazly, G.A.A. Al-Hazmi, S.E. Ghazy, M.S. El-Shahawi, A.A. EI-Asmy,
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band at 17,650–18,965 cm−1, in solid state, corresponding to the
2
2B1g→ Eg transition in a square-planar geometry [24]. In DMF
solution, this band is shifted to higher energy suggesting a weak
interaction with the solvent.
The spectra of Ni(II) complexes, in Nujol, showed three bands at
23,515–24,530, 17,650–18,180 and 70,000–10,500 cm−1 assignable
to the d–d transitions. The first band may be due to the transi-
structure (in DMF solution, the first band is observed at high energy
indicating strong interaction with the solvent). The ligand field
parameters (B, ˇ and 10Dq) calculated for the complexes in Nujol
and DMF solutions are presented in Table 4 according to the tetra-
hedral Ni(II) equations and found lower than those reported for the
suggested structure. The values of ˇ indicate an ionic character for
3
3
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Spectrochim. Acta A 61 (2005) 243.
[11] P. Bindu, M.R.P. Kurup, Ind. J. Chem. 38A (1999) 388.