G Model
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ARTICLE IN PRESS
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C.A. Mak et al. / Catalysis Today xxx (2017) xxx–xxx
Fig. 5. The UV–vis spectrum of (MNPs)- (BTSE) −(COOH-POPP) nanomaterial.
tion bond; the intense band at 1234 cm−1 is attributed to aromatic
C bonds; the band from1483 cm−1 is attributed to valence
C
O
vibrations of C N bonds; broadened 1587 cm−1 band is corre-
sponding to asymmetric stretching of entire porphyrin macrocycle
due to all vibrations of the methyn bridges and of the pyrrole rings
3032 cm−1 is assigned to asymmetric stretching of C H phenyl
vibrations and the band at 3311 cm−1 belongs to the stretching
vibration of N H bond [26–29].
Fig. 4. Superposed FT-IR spectra of 5-(4-carboxyphenyl)-10,15,20-tris(4-
phenoxyphenyl)-porphyrin (full line) and the nanocomposite c3 material
(dashed line).
The FT-IR spectrum (Fig. 4) of the c3 new nanocomposite
material shows a reduced number of bands that are differently posi-
of both magnetite and silica in the hybrid material. The formation
of this new material is also confirmed by the presence of the intense
cles is noticed. This fact can be due to the bulky presence of three
porphyrin unit associated with the presence of the bis-linker, that
facilitates both the linkage of the MNPs and the side by side (J
type) and sandwich (H-type) aggregates. (Fig. 3(c)). The aggrega-
tion behavior observed for material c3 is somewhat expected. As
mentioned in the experimental part, for the design of this hybrid
material we make use of a bis-triethoxysilane linker. The possible
phenomena that occurs is the iron oxide magnetic nanoparticles
get functionalized to one-another, due to the presence of this lig-
and. The ideal scenario would be that one of the triethoxysilane
units attaches to the surface of the nanoparticles and the other to
the porphyrin. However, it is well known, that the triethoxysilane
this reason, this tendency of aggregation takes place in the case of
material c3.
Besides, the weak forces, Van der Waals or hydrophobic, hydro-
gen bond and - stacking got rise to triangular type morphology
of porphyrin based hybrid materials (Fig. 7) with dimensions in the
range of 350–400 nm. Self- organization gave multi lamellar trian-
gles, uniformly in shape, dimensions and orientation, due to J–type
and H-type aggregation specific to functionalized porphyrins, that
balance side- by- side with sandwich- type aggregation. [30]
One very interesting fact, worth mentioning, was observed in
the case of material c1. When studying the TEM images at higher
magnification very small nanoparticles, besides the iron oxide ones,
were observed. (Fig. 3(d)). These nanoparticles are believed to be
porphyrin nanoparticles which are formed due to the presence
of the polysaccharide. This can be confirmed by the fact that the
same small nanoparticles, of an average diameter of 2 nm, were
also observed in the case of material c2 (Fig. 3(e)).
band attributed to stretching vibrations of the Si
also Si
Fe bridges at 900 cm−1 [31,32,33]. The bond formed
confirmed by the presence of the very intense band at 1058 cm−1
O Si bonds and
O
,
attributed to asymmetric stretching mode of Si
O
O
C bond [34]. The
C bond and/or ꢀ
weak band at 1457 cm−1 is attributed to the C
C
N bond and is due to porphyrin [27] The medium- intense signals
at 2871 cm−1 and 2973 cm−1, can be attributed to stretching C
H
vibrations in methylene groups from the linker. The large, medium
intensity band at 3424 cm−1 in the nanocomposite FT-IR spectrum
is related to O H stretching vibration due to the presence of H2O.
-(COOH-POPP) nanomaterial
The UV–vis spectrum of (MNPs)- (BTSE) -(COOH-POPP) nano-
material (Fig. 5) presents the characteristic bands of bare
porphyrin, namely: the intense Soret band at 419 nm assigned to
*
the transition from a1u () - eg () and the four Q bands of less
intensity with absorption maxima located at 514, 549, 591 and
*
647 nm, that are generated by a2u () - eg () transitions. The
spectrum belongs to etio pattern, meaning that the intensities of
Q bands are decreasing as follows: QIV > QIII > QII > QI.
Moreover, the presence of the combined hybrid materials could
be confirmed by EDX and elemental analysis. Even more, the results
from EDX match the ones obtained from elemental analysis in all
cases (see supporting information for details, Figs. S5–S7).
3.4. UV–vis response of the (MNPs)- (BTSE) -(COOH-POPP)
nanomaterial to CO2 exposure
erties of (MNPs)-(BTSE)-(COOH-POPP) nanomaterial in DMF was
monitored by UV–vis spectroscopy.
By increasing the CO2 gas concentration, the intensity of absorp-
concentration range of CO2, varying from 30 M to 200 M, the
dependence between absorption intensity measured at 419 nm and
the concentration of CO2 in solution was linear and characterized by
an excellent correlation coefficient (Fig. 6), meaning that the mate-
3.2. FT-IR characterization of the (MNPs)- (BTSE) -(COOH-POPP)
nanomaterial in comparison with bare porphyrin
The FT-IR spectrum (Fig. 4) of the bare porphyrin displayed
bands at 796 cm−1, attributed to the bending of C H pyrrole bond
and to out of plane ␥ N H deformation in free base porphyrin; the
1sharp band at 1161 cm−1 is assigned to in-plane N H deforma-
Please cite this article in press as: C.A. Mak, et al., Functionalization of A3B-type porphyrin with Fe3O4 MNPs. Supramolecular assemblies,