I. Nath et al. / Journal of Catalysis 377 (2019) 183–189
185
networks, a trend in decreased microporosity is usually observed
39,40]. Owing to an efficient cross-coupling between randomly
claim of ionic Pd species comprehended from FT-IR analysis. A
1.0 eV negative shift of the Pd(II)3d5/2 peak compared to free Pd
[
oriented tetra-connected azo-monomer and tris-connected alkynyl
co-monomer in the highly concentrated nonpolar organic phase,
B -Azo was also anticipated to show supressed microporosity.
3 4
Though, substantial mesoporosity was expected due to the col-
loidal synthetic approach.
2
(OAc) (338.4 eV) suggested an increased electron density over
Pd possibly arising from the azo-N atoms of the polymeric back-
bone, inferring a more stable coordination environment provided
by the organic network [44]. A comparison of the N1s spectrum
3 4
of Pd-B -Azo and that of pristine polymer demonstrated almost
Following our assumption, the non-local density functional
theory (NLDFT) revealed completely mesoporous distribution of
500 unit decrease in the N-C peak area and 0.3 eV positive shift
after Pd loading (Fig. 2c). These observations are further indicative
of the strong coordination between Pd(II) and azo-N-atoms present
in the network. Such coordination of Pd ions with azo-N are pre-
vailing in literature [37,38]. Moreover, apart from the usual C@C
and CAN peaks appearing at 284.7 and 286.3 eV respectively,
another shakeup peak was observed at 288.5 eV in the C1s region
as well (Fig. 2b). This is attributed to the OACAO units arising from
the acetate counter anions of Pd(II).
2
ꢀ1
B
3
-Azo
mmett–Teller (BET) surface area and 0.14 cm g pore volume of
the polymer. Corresponding Type-V N -sorption plot also supports
this porosity distribution pattern (Fig. 1a) [41]. Adsorption of N in
4
(Fig. 1b) resulting in relatively low 31 m g Brunauer–E
3
ꢀ1
2
2
the micropores is accounted as a major contributing factor to
attain high BET value. However, the micropores present in the
polymers obtained by colloidal technique often remain too small
for the gas molecules to access due to highly interwoven network
3 4 3 4
The FESEM images of B -Azo and Pd-B -Azo showed identical
[
39,40]. Therefore, no identifiable gaseous monolayer can form
during adsorption, lowering the overall surface area. A similar
explanation can be drawn for B -Azo as well. Despite apparently
morphology of both materials (Figs. S2 and S3), while TEM images
confirmed relatively homogeneous distribution of Pd in amor-
phous polymeric nano-sheets (Figs. S4 and S5). Gaining a control
over polymeric particle size in the nano-scale range, typically
within 200–500 nm, has been ascribed to the colloidal synthesis
approach of organic networks. Such methods have previously been
proven as a promising route for attaining desirable particle sizes
[30,43]. Average size of Pd particles were found to be 3.8 nm. The
3
4
low BET surface area, good mesoporosity is generally desirable
for catalytic applications as it allows efficient reactant and product
mass-transport without imposing any steric constrain.
3 4
Successful synthesis of B -Azo network was confirmed by solid
1
3
state C CP/MAS NMR spectroscopy. Appearance of peaks at
d = 151.8 and 90.1 ppm proved the respective presence of CAN
and C„C bonds in the polymer (Fig. S1), while the absence of
any residual signals for unreacted alkynes, which typically appear
at ꢁ80–82 ppm, inferred a high degree of polymerization. Forma-
tion of C„C can also be seen from the weak stretching peaks at
3 4 3 4 2
TGA profile of both B -Azo and Pd-B -Azo obtained under N
atmosphere confirmed their excellent thermal stability till 350 °C
with high residual mass even at 1000 °C (Fig. S6).
2.2. Photophysical and electrochemical properties
ꢀ
ꢀ
1
1
ꢁ
2200 cm
3 4
in the FT-IR spectra of B -Azo , whereas peaks at
ꢁ
3000 cm can be ascribed to typical aromatic C-H stretching
EPR analysis displayed an increase in the Lorentzian signal
intensity upon visible light illumination on both materials, reveal-
ing their substantial photo-responsive character (Figs. S7 and S8).
(
Fig. 1d). Pd was loaded onto this organic network (Pd-B
3
-Azo
4
)
using acetone-water dual solvent technique. ICP analysis showed
ꢀ1
0
.293 mmol g
Pd-B -Azo demonstrated the immergence of new peaks at
1670 and 1080 cm (Fig. 1d). These peaks were postulated to
loading of Pd in Pd-B
3
-Azo
4
. FTIR spectrum of
Accordingly, the steady-state UV–vis absorption spectra of B
3
-
3
4
Azo and Pd-B -Azo also showed high visible light absorption
4
3
4
ꢀ1
ꢁ
cross-sections (Fig. 3a). A significant absorbance tail is attributed
to efficient coupling of monomer and co-monomer leading to
originate from C@O and CAO stretches inferring the possible pres-
ence of acetate moieties in the network. This, in turn, suggests that
Pd might be present in ionic states in the polymer where acetates
remained as counter anions. Disappearance of C„C peaks com-
increased
p–conjugation. Certain decrease in absorption maxima
after Pd-incorporation occurred, inferring possible existence of a
polymer to metal energy transfer process [19]. Interestingly,
despite their well-accounted photo-responsive nature, no fluores-
cence were observed for pristine as well as Pd-loaded networks
after repeated trials with variable excitation wavelengths. The
3 4
pared to parent B -Azo also supports this idea of ionic Pd species,
as these metals ions are well known for their coordination ability
with alkynes [42,43]. The otherwise identical FTIR patterns of both
materials demonstrated the retention of structural integrity of the
polymeric skeleton after metal incorporation.
Oxidation state of Pd was confirmed by XPS analysis where
peaks for Pd(II)3d3/2 and Pd(II)3d5/2 were appeared at 342.7 and
3 4
absence of any fluorescence for B -Azo suggest a feasible inter
system crossing of the excited electron to available low-energy tri-
plet states possessing relatively extended life-span, which would
further ease the chances of polymer to metal energy transfer in
3
37.4 eV respectively (Fig. 2a). This observation supports our initial
3 4
Pd-B -Azo upon photo-illumination [45,48].
Fig. 2. (a) Pd3d and (b) C1s XPS peaks of Pd-B
3 4
-Azo showing the position of each peaks; (c) comparative XPS pattern of N1s peak before (top) and after (bottom) Pd-loading
demonstrating slight shift and decrease in peak area after metal incorporation inferring N-Pd coordination.