L.K. Gupta, S. Chandra / Spectrochimica Acta Part A 65 (2006) 792–796
795
Table 5
EPR spectral data of the complexes
Complexes
Temperature
g||
g⊥
giso
g3
g2
g1
R
G
[
[
[
[
[
[
[
[
[
[
Cr(L)Cl2]Cl
Cr(L)(NO3)2]NO3
Mn(L)Cl2]
RT
RT
RT
LNT
LNT
LNT
LNT
RT
–
–
–
–
–
–
1.982
1.984
1.982
4.002
2.854
2.715
2.731
2.131
2.177
2.231
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
–
4.45
4.13
–
Co(L)Cl2]
5.871
4.254
3.902
4.232
2.271
2.308
–
5.871
4.254
3.902
4.232
2.061
2.075
–
Co(L)(NCS)2]
Co(L)](NO3)2
Co(L)SO4]
Cu(L)Cl2]
Cu(L)(NO3)2]
Cu(L)SO4]
RT
RT
–
–
–
–
4.424
2.177
2.092
0.344
RT, room temperature; LNT, liquid nitrogen temperature.
3
3
3
3
3
.5. Co(L)Cl2 and Co(L)(NCS)2
ration transitions: A2g(F) → T2g(F), A2g(F) → T1g(F) and
3
3
A2g(F) → T1g(P), respectively.
The electronic spectra of complexes prepared from CoCl2
and Co(NCS)2 are characteristic of octahedral cobalt(II)
9–10]. They show three peaks (Table 3), corresponding
The Naphelauxetic parameter β is calculated by using the
relation: β = B(Complex)/B(Free ion), where B is the Racah inter-
electronic repulsion parameter. The values of B, lowered than
the free Ni(II) ion, i.e. 1041 cm , suggesting 24–37% covalent
character in the M N linkage. Other ligand field parameter are
also calculated and are listed in Table 4.
[
4
4
4
4
4
4
4
4
−
1
to T1g( F) → T2g( F), ν1; T1g( F) → A2g( F), ν2 and
4
4
4
4
T1g( F) → T1g( P), ν3 transitions, respectively. The EPR
spectra of the complexes under study were recorded at liq-
uid nitrogen temperature because we found that the rapid
relaxation of Co(II) broadened the lines at higher temperature
3
.9. Copper(II) complexes
(
g|| = 4.254–5.871 and g⊥ = 2.154–3.067). The large deviations
of the g-values from the spin only value (g = 2.0023) is due to
The room temperature magnetic moment values of the Cu(II)
the large angular momentum contribution.
complexes (1.90–2.02 B.M.) indicates the monomeric nature of
the complexes. The values correspond to one unpaired electron
and the complexes may be considered as tetragonal geometry,
except the sulphato complex whish possess five coordinated
square pyramidal geometry and Cu2 ion and anions occupies
the axial position. The chloro and nitrato complexes of the Cu(II)
3
.6. Co(L)(NO3)2
+
The electronic spectra of the tetrahedral and octahedral
cobalt(II) complexes are almost similar. The remarkable differ-
−
1
2
2
ence is the presence of a band at ∼5000 cm , in the tetrahedral
givestwoelectronicpeaks(Table3)assignedtothe B → A
1
g
1g
2
2
complexes, which is absent in the octahedrals. In the present
and B1g → E transitions, characteristic for tetragonal geom-
g
−
1
case the presence of the band at 5400 cm , suggests tetrahe-
dral geometry of this complex [11].
etry. The copper(II) sulphato complex gives the electronic peaks
comparable with five coordinate square pyramidal geometry.
The complexes have anisotropic EPR spectra, characteristic
to tetragonal geometry [14]. The g-values have been calculated
by the method published earlier [15–16], and are summarized in
Table 5. The value of G = (g − 2)/(g − 2) which measure the
3
.7. Co(L)SO4
The electronic spectra of the sulphate complex display three
||
⊥
−
1
−1
−1
bands at ∼12,400 cm , ν1; ∼15,504 cm , ν2; ∼21,368 cm
,
exchange interaction between the copper centers in polycrys-
talline samples. If the value of G > 4, the exchange interaction is
negligible but the G < 4 value suggest considerable interaction
between the solid complex. The value of G in the complexes
reported here is G > 4, suggesting that there is no interaction
between the copper centers.
ν3, corresponding to the square pyramidal geometry [9]. Ligand
field parameters for the complex have been calculated and are
in the tune of the results published earlier [12].
3
.8. Nickel(II) complexes
Five coordinated copper(II) complex may possess two
geometries, i.e. trigonal bi-pyramidal and square pyramidal [17],
All complexes are of high spin type and show room temper-
ature magnetic moments in the range 3.04–3.20 B.M. (Table 3),
correspond to two unpaired electrons. High spin Ni(II) com-
plexes may be four coordinated tetrahedral and six coordi-
nated octahedral. The observed μeff values are low for tetra-
hedral Ni(II) complexes, which is known to show magnetic
moments in the range 3.40–4.12 B.M. The electronic spec-
tra are in favor of octahedral geometry [13]. It shows three
bands (Table 3) which are assignable to octahedral configu-
which are characterized by ground states d
2
2
or dz , respec-
2
x −y
tively [18]. The EPR spectra provides an excellent basis for
distinguishing between these two ground states. For system with
g3 > g2 > g1 the ratio (g2 − g1)/(g3 − g2) called the parameter
‘R’, is very useful for this purpose. If the ground state predom-
inantly, dz
2
, the value of R is greater than 1, and the value of R
less than 1 is in the case of d
g1, g2, g3 and R (Table 5) for the complex under study suggest
2
2
ground state. The value of
x −y