Transition Met Chem (2013) 38:199–206
Results and discussion
203
the three bands from the azomethine ligand (p–p*), charge
transfer (MLCT), and d–d transitions are observed at 373
and 378, 419 and 425 and 500 and 520 nm, for [CoL] and
[MnLCl], respectively.
Structural description of H2L
An ORTEP view of the unsymmetrical Schiff base mole-
cule, which crystallized in orthorhombic P bca space
group, is shown in Fig. 1. The crystal data and selected
bond lengths and angles are listed in Tables 1 and S1,
respectively. The packing diagram is also shown in Fig. S1.
The aromatic ring systems are in almost planar confor-
mation, with endocyclic torsion angles of 1.9 (3)ꢁ, -0.9
(2)ꢁ, and -0.6 (2)ꢁ. The mean plane between the rings
(C9–C10–C11–C16–C17 and C2–C3–C4–C14–C15) is
55.19ꢁ. All the bond lengths are comparable to those
observed in similar compounds [1–4]. The bond lengths of
In the FTIR spectrum of the free ligand H2L, a broad
band at 3428 cm-1 might be attributed to O–H vibration
(Fig. S4a). On the other hand, in the FTIR spectra of [CoL]
and [MnLCl], the bands due to the O–H modes are no
longer observed, suggesting that the hydroxyl protons are
displaced by the metal atoms leading to M–O bonding (Fig.
S4b, S4c). In addition, the band due to the CH=N groups of
H2L was shifted from 1613 to 1606 and 1605 cm-1 for
[CoL] and [MnLCl], respectively, consistent with involve-
ment of the azomethine nitrogen atoms in the coordination
[28].
˚
˚
C8=N2 [1.285(2) A] and C5=N1 [1.284 (2) A] conform to
the values for double bonds and are comparable to those in
other Schiff bases [23, 24]. In addition, the bond lengths
The bands assigned to the intramolecular H-bonding
vibration (O–HÁÁÁN) (2650–2700 cm-1) of H2L are absent
from the spectra of complexes, as a result of deprotonation
and coordination of the oxygen atoms [29]. The bonding of
the Co(II) and Mn(III) atoms to the ligand through the
nitrogen and oxygen atoms is further supported by the
presence of new bands at 520 (Co) and 541 (Mn) cm-1 and
450 (Co) and 445 (Mn) cm-1 assigned to the M–O and
M–N stretching, respectively [30].
˚
˚
(C6—N1) = 1.410(2) A and (C7—N2) = 1.408(2) A are
typical for the single bonds. Three torsion angles, C8–N2–
C7–C18 [43.4 (2)ꢁ], C21–N1–C6–C5 [-10.3 (2)ꢁ], N2–C7
–C6–N1 [6.7 (2)ꢁ], are responsible for mutual orientation
of both aromatic ring systems. In the crystal structure, the
˚
NÁÁÁN distance is equal to 2.732 (2) A.
The hydrogens attached to O2 and O3 form asymmetric
weak intramolecular hydrogen bonds to N2 and N1,
Immobilization of [CoL] and [MnLCl] onto
SiO2–APTS
˚
respectively: O2–H2ÁÁÁN2 1.875(1), O2ÁÁÁN2 2.608(2) A,
˚
145.1(8)ꢁ; O3–H3ÁÁÁN1 1.871(1), O3ÁÁÁN1 2.610(1) A,
146.0(7)ꢁ. There are columns of molecules arranged in a
2D network connected by intermolecular hydrogen bonds
along the crystallographic c direction (Fig. S2): C8–H8…
Modification of the silica support through surface func-
tionalization with APTS and immobilization of [CoL] and
[MnLCl] onto the modified silica was carried out by using
the procedure shown in Schemes 2 and 3. On the basis of
nitrogen elemental analysis, the amount of APTS anchored
to the silica was determined as 2.42 mmol g-1. The
amounts of [CoL] and [MnLCl] immobilized onto SiO2–
APTS were 0.51 and 0.46 mmol g-1, respectively, deter-
mined from metal analyses by AAS.
˚
O3, 2.716 (2) A, 142.3ꢁ (3), x, ?y, ?z?1; C12–H12ÁÁÁO1,
˚
2.405 (1) A, 161.3ꢁ (1), -x?/2, -y?1, ?z-1/2). These are
reinforced by C–HÁÁÁp interactions formed between rings.
Moreover, there is a weak face-to-face stacking interaction
˚
[3.632 (2) A] between the rings C2–C3–C4–C13–C14–C15
and C6–C7–C18–C19–C20–C21.
The DR–UV–vis spectra of SiO2–APTS, CoL@SiO2–
APTS, and MnL@SiO2–APTS are given in Fig. S5. There
are important differences between the spectrum of SiO2–
APTS and the spectra of CoL@SiO2–APTS and MnL@
SiO2–APTS. In the spectrum of SiO2–APTS, no peaks are
observed in the range from 300 to 500 nm. In contrast,
there are two intense peaks in this range at the spectra of
both CoL@SiO2–APTS and MnL@SiO2–APTS,consistent
with the presence of the metal complexes on the surface of
SiO2–APTS.
Characterization of the complexes
The results of elemental analysis are in good agreement
with the suggested compositions of the metal complexes.
The effective room temperature magnetic moments of
[CoL] and [MnLCl] were calculated as 4.31 BM and 4.46
BM, respectively, indicating distorted tetrahedral [25] and
square pyramidal [26] geometries, respectively.
The solution conductivities of [CoL] and [MnLCl] in
DMSO were measured as 0.5 and 0.8 X-1 cm2 mol-1
respectively, showing that the complexes are non-electro-
,
The FTIR spectra of SiO2, APTS functionalized silica
(SiO2–APTS), CoL@SiO2–APTS, and MnL@SiO2–APTS
are shown in Fig. S6. The spectrum of SiO2 shows a broad
band in the range 3430–3080 cm-1, attributed to the sila-
nol (–OH) groups, and a broad absorption at 1089 cm-1
assigned to the Si–O–Si bonds. After functionalization of
lyte as expected [27].
The electronic spectra of H2L, [CoL] and [MnLCl] were
measured in chloroform. The UV–vis spectra of H2L and
[CoL] are given in Fig. S3. In the spectra of the complexes,
123