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Products
the tertiary N atoms in the center of the tri-s-triazine ring NC3
and to partially hydrogenated N atoms of ÀNH (x=1, 2)
x
During further heating of the 3:1 complex to 5508C, denitrifi-
groups arising from incomplete condensation, respectively.
These results are in full agreement with the literature data re-
cation of [Al(NO ) ] and condensation of melamine to polymer-
3
3
[
2d]
ic carbon nitride occur. The resulting C N products are denot-
ported for the graphitic carbon nitride
and thus indicate
3
4
ed in the following as MAxy-S-C N , in which x and y represent
that the chemical structure of the synthesized products is built
of tri-s-triazine units. The O1s signal shown in the Supporting
Information (Figure S6D) reveals two contributions assigned to
the surface-absorbed water (533.1 eV) and surface hydroxyl
groups (531.7 eV) originating from rather oxidative synthesis
path as well as aqueous work up of the products. As it was
mentioned above, there is no residual aluminium in the prod-
ucts (see Al 2p binding energy region in the Supporting Infor-
mation, Figure S6E), demonstrating that the template was suc-
cessfully removed after the synthesis.
3
4
the taken ratio between melamine and [Al(NO ) ]·9H O, and S
3
3
2
indicates the solvent. PXRD patterns and FTIR spectra of the
final products are similar to those of the reference bulk carbon
nitride prepared from melamine, indicating the successful for-
mation of polymeric carbon nitride network. In the case of
bulk g-C N , typical reflections at 27.3 (002) and 12.88 (100) in
3
4
the PXRD pattern correspond to graphite-like interlayer stack-
[
2d]
ing and in-plane structural repeating motifs, respectively
the Supporting Information, Figure S4A and B). In MAxy-C N4
(
3
products, both peaks are much broader and weaker than in
the reference material, which suggests a decreased structural
order, smaller crystallite size, and more distorted graphite-like
All products are characterized by a particle-like morphology
(the Supporting Information, Figure S7), particles having rather
small grain size, random shapes and size distribution, and
being perforated as the result of gas evolution during the de-
composition of [Al(NO ) ]·9H O, condensation of melamine,
[
14]
packing. The weakening of layer stacking motif in products,
which was well-pronounced in intermediates (Figure 3), is
probably caused by rapid and violent denitrification of
3
3
2
and etching of the remaining aluminium species that provides
macroporosity to most of prepared materials. The study of the
nitrogen sorption properties of MAxy-C N (N adsorption–de-
[
Al(NO ) ]. The FTIR spectra of MAxy-C N , displayed in the Sup-
3 3 3 4
porting Information (Figure S4C and D) are identical to those
3
4
2
À1
of g-C N . The vibrations between 1200 and 1650 cm are as-
sorption isotherms are shown in the Supporting Information,
Figure S8) shows that all the products possess higher specific
surface areas than the reference, ground g-C N (13–90 vs.
3
4
sociated with the stretching vibrations of aromatic CN hetero-
À1
cycles, and the strong band at 808 cm is attributed to the
3
4
2
À1
deformation vibrations of the tri-s-triazine ring. We did not ob-
serve significant differences between water and ethanol-de-
rived products, except for a slightly better structural order in
water-derived carbon nitrides, which is due to the lower initial
content of the template, leading to less distortion caused by
template decomposition.
9.5 m g , see the Supporting Information, Table S2). This is ac-
companied by the development of some micro-, meso- and
macroporosity and a 26-fold increase of the total pore volume,
which is expected to be beneficial for the photocatalytic activi-
ty of the prepared materials. Typically, ethanol-derived prod-
ucts have slightly higher surface areas than water-derived ones
(see the Supporting Information, Table S2, entries 11, 12, and
14 vs. entries 3 and 4), which are due to the higher initial tem-
plate content. These values can be further improved by either
increasing template content in the starting complex (the Sup-
porting Information, Table S2, entries 8 and 9) or directly heat-
ing the obtained gel to 5508C (Table S2, entry 10 and Fig-
Elemental analysis and EDX spectroscopy were employed to
determine the composition of the resulting products. Both
methods showed C/N molar ratio similar to the one of bulk
C N , indicating the formation of polymeric carbon nitride
3
4
structure from the complexes (the Supporting Information,
Table S1 and Figure S5). The absence of the aluminium species
in nanoporous MAxy-C N was confirmed by a missing Al 2p
2
À1
ure S9). Expectedly, the highest surface areas (50–90 m g ,
the Supporting Information, Table S2, entries 17–19) are ob-
served for the smallest complex particles collected from top of
suspensions. The porous character of the products is demon-
strated in Figure 4 by representative TEM images.
3
4
peak in the high-resolution X-ray photoelectron spectrum (the
Supporting Information, Figure S6E).
X-ray photoelectron spectroscopy (XPS) provided more infor-
mation about the chemical composition and the valence states
in the products (the Supporting Information, Figure S6). Fig-
Compared with surface areas (s.a.) of carbon nitrides pre-
pared by using SiO2 templates (e.g., mpg-C N , s.a.
ure S6A, showing the survey spectrum of the MA23-C N4
3
3
4
2
À1
sample, indicates that C, N, and some O atoms are present in
the material. The C1s spectrum (the Supporting Information,
ꢀ200 m g ), the surface areas obtained by using
Figure S6B) reveals two main contributions at 288.2 and
2
2
84.8 eV, which correspond to sp -carbon atoms in tri-s-triazine
rings (CN ) and the adventitious carbon, respectively. The small
3
contribution at 286.2 eV is assigned to the hydroxylated sur-
face carbon atoms as corroborated by O 1s signal at 531.7 eV
(
see below). The N 1s signal (the Supporting Information, Fig-
ure S6C) is deconvoluted into three peaks having binding en-
ergies of 398.6, 399.7, and 400.8 eV. The strongest peak at
2
3
98.6 eV is assigned to sp -nitrogen atoms in tri-s-triazine ring
3 4
Figure 4. TEM images of a) MA21-EtOH-top-C N , and of a directly heated
(
CÀN=C), whereas the peaks at 399.7 and 400.8 originate from
gel b) MA31-H O-C
2
3 4
N .
Chem. Eur. J. 2015, 21, 10805 – 10811
10808
ꢀ 2015 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim