JOURNAL OF CHEMICAL RESEARCH 2009 773
The spectral results together with elemental analyses indicated that
the hydrazone can behave as a neutral bidentate (H2L), monobasic
bidentate (HL-), monobasic tridentate (HL-) or dibasic tridentate (L2-)
ligand towards the metal ions, and also, the ligand is coordinated to
the metal ion by the carbonyl oxygen of the hydrazide moiety and
carbonyl oxygen of the dibenzoylmethane moiety in the enolic or
ketonic form, as well as by azomethine nitrogen atoms.
and having an axial symmetry type of a d(x2-y2) ground state, which
is the most common for copper(II) complexes.33,42 The g-values
suggest a square planar or octahedral geometry23 and the complexes
show g||>g┴>2.0023, indicating a distortion around the copper(II)
ion43,44 The ESR parameters for the complexes are shown in Table 4
(deposited in the ESI). The g-values are related by the expression,43,44
G = (g||-2)/(g┴-2). If G > 4.0, then local tetragonal axes are aligand
parallel or only slightly misaligand and if G < 4.0, significant
exchange coupling is present. Complex (8) shows a value of 3.33,
indicating spin-exchange interaction takes place between copper(II)
ions, which is compatible with the magnetic moment value. However,
complexes (9) and (10) show G > 4.0 (Table 4, deposited in the ESI),
indicating tetragonal axes are present in these complexes. Also, the
g||/A|| values are considered as diagnostic of stereochemistry.43,44
The g||/A|| value for the complexes (Table 6, deposited in the ESI) lie
just within the range of expected structures. The g| -values reported
here are 2.2, 2.26 and 2.27 respectively, indicating considerable
covalent bonding character in these complexes.23,42,43 The isotropic
value of the hyperfine coupling constant Aiso is related to the σ-
bonding parameter (a2).44,46 If a2 = 1, the bond would be completely
ionic and if a2 = 0.5, the bond would be completely covalent.
The calculated values of a2 for complexes (8), (9) and (10) are 0.73,
0.64 and 0.63 respectively, suggesting covalent bonding.42,44 The
orbital reduction factor (K)45 can be used to measure the covalent
character of the metal-ligand band. For an ionic environmental,
K = 1 and for a covalent environmental K < 1; the lower the
value of K, the greater is the covalent character. The K-values for
the complexes (Table 4, deposited in the ESI) are indicative of a
covalent nature.23,42,43 Also, the in-plane and out-of plane π-bonding
Magnetic moments
Room temperature magnetic moments of the complexes (2–20) are
shown in Table 3 (deposited in the ESI). Nickel(II) complexes (3) and
(4) show diamagnetic values confirming a square planar geometry
around the nickel(II) ion. However, complex (2) shows 2.74 B.M.,
indicating octahedral geometry around the nickel(II) ion.24,28
Cobalt(II) complexes (5), (6) and (7) show values 3.4 and 4.2 and
3.2 B.M. (Table 1), which could indicate high spin square planar or
octahedral cobalt(II) complexes.8,29 However, the low values of (5)
and (7) indicate spin-exchange interactions take place between the
cobalt(II) ions in a square planner geometry. The magnetic moments
for the copper(II) complexes (8), (9) and (10) are 1.5, 1.81 and 1.72
B.M respectively. The value of complex (8) is well below the spin-
only value (1.73 B.M.), indicating spin-exchange interactions take
place between the copper(II) ions in a square planar environmental.30
However, the values of complexes (9) and (10) correspond to one
unpaired electron in an octahedral structure.8 The magnetic moment
value for manganese(II) complex (11) is 4.92 B.M., suggesting a high
spin octahedral geometry around the manganese(II) ion.17 The low
value is due to the presence of spin-exchange interactions between
the Mn(II) ions. Iron(III) complex (12) shows a value 5.66 B.M,
indicating a high spin iron(III) octahedral geometry.8 Ruthenium(III)
complex (13) shows a magnetic value 1.6 B.M indicating an
octahedral structure.31 Zirconium(IV) (14), hafnium(IV) (15),
zinc(II) complexes (16–18), lanthanum(III) (19) and uranyl(II) (20)
complexes are diamagnetic.
coefficients (b1 and B2) can be calculated.23,42,43 The complexes
2
show b2 and b2 values (Table 6, deposited in the ESI) that indicate
ionic character1in the in-plane π and covalent character in out-of
plane π-bonding.46 It is possible to calculate approximate orbital
populations for p or d orbitals using the following equations,47 where
Ao and 2B0 are the calculated dipolar couplings for unit occupancy of
s and d orbitals respectively.
Electronic spectra
The electronic spectral data of the ligand and its complexes in
DMF solution are presented in Table 3 (deposited in the ESI).
The ligand exhibits bands at 310 and 220 nm, assigned to n→π*
and π→π*transitions.17 The nickel(II) complex (2) shows bands at
345, 480 and 650 nm; the bands are attributable to 3A2g(F)→3T1g(P)
A11 = Aiso-2B[1± (7/4) ∆g11]
(1)
(2)
a2p, d = 2B/2B0
3
3
(υ3), A2g(F)→3T1g(F) (υ2) and A2g(F)→3T2g(F) (υ1) transitions
respectively of an octahedral nickel(II) complex.32 The υ2/υ1 ratio
is 1.37 indicating a distorted octahedral nickel(II) complex.33
However, complexes (3) and (4), show bands at 460 and 510 and
450 and 520 nm respectively. The bands are assigned to 3T1→3T2
When the data are analysed using the Cu63 hyperfine coupling and
considering all the sign combinations, for complexes (8), (9) and
(10) the only physically meaningful results are found when A11 and
A┴ are negative. The resulting isotropic coupling constant and the
parallel component of the dipolar coupling) are negative. The orbital
3
and T1(F)→3T2(P) transitions, of a square planar nickel(II) ion.27,34
2
population (ad %) for the complexes (Table 4, deposited in the ESI)
indicate that the main orbital is the d(x2-y2) ground state.44 However,
the ESR spectra of manganese(II) and ruthenium(III) complexes are
of the isotropic type with giso = 2.024 and 2.11 respectively, typical
of octahedral structure. The iron(III) complex (12) shows gav = 4.38
arising from very large zero field splitting effect. This g- value indicates
a high spin (5/2) octahedral geometry around the iron(III) ion.
The cobalt(II) complexes (5) and (7) show bands in the 460, 545 and
620 nm and 475, 555 and 610 nm respectively are which assigned to
a square planar geometry.35 However, complex (6) shows bands at
4
455, 550 and 650 nm; these bands are assigned to T1g(F)→4T2g(F),
4T1g(F)→4A2g and 4T1g(F)→4T1g(P) transitions respectively of a high
spin cobalt(II) octahedral complex.36 The copper(II) complexes (8),
(9) and (10) show different bands (Table 3, deposited in the ESI).
Complex (8) shows bands at 395, 480 and 590 nm, corresponding
Thermal analyses
2
2
to B1g→2B2g, 2B1g→2Eg and B1g→2A1g transitions respectively of
a square planar geometry.37 However, complexes (9) and (10) show
bands at 390, 475 and 640 nm and 395, 480, 650 nm respectively.
The bands are assigned to ligand→copper charge transfer, 2B1→2E
and 2B1→2B2 transitions, in a distorted octahedral structure.38
Manganese(II) complex (11) shows bands at 485, 550 and 650 nm,
The results of TG and DTAanalyses of complexes are shown in Table 5
(deposited in the ESI). The results show that complexes (2), (4), (13–
15) and (18) lose hydrated water molecules in the temperature range
60–100°C; this process is accompanied by an endothermic peak.
The coordinated water molecules were eliminated from complexes
(2), (6), (11) and (13) at relatively higher temperature than those
of the hydrated water molecules (110–170°C) (Table 5, deposited
in the ESI). The removal of an HCl molecule (accompanied by an
endothermic peak) was observed for (4), (11), (13–15) and (18)
complexes in the temperature 240–310°C range, compatible with
the TG result. For complex (6), the removal of an HNO3 molecule,
also accompanied by an endothermic peak, was observed in the
280–295°C range, compatible with the TG result. The removal of
a CH3COOH molecule, (accompanied by an endothermic peak), for
complex (12) occurs at 320°C, compatible with the TG result. The
complexes decompose through degradation of the hydrazone ligand
at a temperature above 400°C leaving metal oxides (490–660°C)
(Table 5, deposited in the ESI).
6
6
6
corresponding to A1g→4Eg, A1g→4T2g and A1g→4T1g transitions
which are compatible to an octahedral geometry around the
manganese(II) ion.39 Iron(III) complex (12) shows bands at 475, 550
and 640 nm. The first two bands are due to charge transfer transitions
while the last band is considered to arise from the 6A1→4T1 transition;
these bands suggest a distorted octahedral geometry around the
iron(III).35,37 Ruthenium(III) complex (13), shows bands at 475, 575
and 620 nm. The first bands are due to LMCT transitions and the
other band is assigned to a 2T2g → 2A2g transition. The band positions
are similar to those observed for other octahedral ruthenium(III)
complexes.31,40 Zirconium(IV) complex (14), hafnium(IV) (15),
zinc(II) (16-18), lanthanum(III) (19) and uranyl(VI) (20) complexes
show bands (Table 3, deposited in the ESI) indicating intraligand
transitions.37,41
Antibacterial and antifungal screening
The ligand and its complexes have been screened for their
antibacterial and antifungal activities and the results obtained are
presented in Table 6 (deposited in the ESI). It is observed that the
activity of the complexes increases with increase in the concentration
Electron spin resonance
The ESR spectra of solid copper(II) complexes (8), (9) and (10) at
room temperature are characteristic of a specie with a d9 configuration
PAPER: JC090772
JCR_12_2009 Book.indb 773
11/12/2009 15:37