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J. Lin et al. / Journal of Catalysis 385 (2020) 338–344
Miniflex 600 diffractometer with Cu K
a
radiation (40 kV, 15 mA,
Fig. S1a and S1b. The XPS signal of C1s certified the chemical states
of carbon included CAC/C@C/CAH (284.8 eV) and CAN/C@N
(286.7 eV). The XPS signal of N1s showed the charts of TPBP con-
tained -N= (398.7 eV) and -N- (399.9 eV). ICP-MS result showed
that there is negligible palladium existing in TPBP. The 13C solid
state NMR spectrum was also used to study the local structures
of TPBP. As depicted in Fig. 1b, the peak at dc = 170 ppm belonged
to the carbon of triazine rings and other peak located at
105 ~ 150 ppm is ascribed to the carbon atoms of the benzene
groups. The resonance peak at 142 ppm was assigned to the carbon
atoms of CAN between triazine ring and phenazine. All of the
above characterizations clearly suggested that the obtained solid
is the target product.
The porosity properties of TPBP were analyzed by nitrogen
adsorption/desorption isotherms at 77 K. In order to remove the
residual compounds within the porous framework, TPBP was
washed thoroughly with low boiling point solvents, and then
degassed under high vacuum at 100 °C for 10 h. As shown in
Fig. 2a, TPBP exhibited a combination of type I and type IV nitrogen
isotherms according to the IUPAC classification. The nitrogen iso-
therm curves shown a steep rise of N2 uptake at a low relative
pressure P/P0, indicated the existence of abundant micropores.
The gradual rising of N2 uptake in the P/P0 ranging from 0.1 to
0.99 in the isotherm indicated the existence of a few mesopores
and macropores. The Brunauer-Emmett-Teller (BET) surface areas
of TPBP were calculated to be 359 m2 gꢀ1 and the total volume
(P/P0 = 0.99) was 0.313 cm3 gꢀ1, respectively. The pore size distri-
bution (PSD) of TPBP was calculated by the nonlocal density func-
tional theory (NLDFT) approach. As shown in Fig. 2b, 1.4 and
1.8 nm pores are dominant in polymer TPBP, which clearly indi-
cates its microporous nature.
k = 0.1541 nm). Fourier transform infrared (FT-IR) Spectra were
collected on a Thermo Nicolet 5700 spectrometer with the KBr pel-
let technique. Thermo-gravimetric analyses (TGA) were obtained
using a Netzsch STA449-F5 analyzer under N2 atmosphere at the
heating rate of 10 °C minꢀ1 within a temperature range of 30–
900 °C. Electron paramagnetic resonance (EPR) measurements
were carried out on a Bruker model A300 spectrometer. X-ray pho-
toelectron spectroscopy (XPS) measurements were performed on a
Thermo ESCALAB 250 spectrometer, using non-monochromatic Al
Ka X-rays as the excitation source and choosing C 1 s (284.6 eV)
as the reference line. UV-visible (UV-vis) spectra were recorded
at room temperature on an Agilent Cary 7000 in the wavelength
range of 200–1500 nm. Transmission Electron Microscope (TEM)
images were collected on a Tecnai G2 F20. Scanning electron micro-
scope (SEM) images were obtained on a FEI Nova NanoSEM 230. 1H
NMR spectra were recorded on a Bruker AVANCE III NMR spec-
trometer at 400 MHz, respectively, using tetramethylsilane (TMS)
as an internal standard. Solid-state 13C CP/MAS NMR was per-
formed on a Bruker SB AVANCE III 500 MHz spectrometer with a
4-mm double-resonance MAS probe. GC-MS determinations were
performed using an Agilent Technologies 7890B GC system with
5977B MSD and a column of Agilent 19091S-433UI HP-5MS. The
oven temperature program of GC measurements was 30 °C
(3 min), 30–300 °C (20 °C/min), 300 °C (3 min). Palladium content
in TPBP was determined using inductively coupled plasma-mass
spectrometry (ICP-MS, XSERIES 2).
3. Results and discussion
3.1. Structural characterization
The powder- X-ray- diffraction (PXRD) patterns showed no
characteristic peak, indicating the amorphous nature of this poly-
mer (Fig. 3a). Thermogravimetric analysis (TGA) measurement
was carried out to study the thermal stability of TPBP. As shown
in Fig. 3b, TPBP exhibits comparative good thermal stability. Under
the N2 atmosphere, it showed no more than 5% weight loss under
420 °C. Scanning-electron microscopy (SEM) images of the pre-
pared polymer networks are shown in Fig. 3c and 3d. The low mag-
nifications images demonstrated the irregular morphology
resulted from aggregation of small particles. Further magnification
showed the existence of clustered particles, which was common
among polymers with the size range between 50 and 600 nm.
Transmission electron microscopy (TEM) was used to investigate
the microstructure of the formed TPBP materials. The high-
resolution TEM images illustrated the amorphous structure of TPBP
and the existence of homogenous pore constituted an extended
As shown in Scheme 1, phenazine and TBT were successfully
coupled to afford TPBP as a brown powder, which was insoluble
in common organic solvents, such as acetone, ethanol and N, N’-
dimethylformamide. TPBP was further detailed characterized by
Fourier transform infrared spectroscopy (FTIR), X-ray photoelec-
tron spectroscopy (XPS), and 13C cross-polarization magic-angle
spinning (CP/MAS) NMR spectrum. The FTIR spectra of the polymer
and its building monomers are shown in Fig. 1a. The peaks at
1593 cmꢀ1, 1506 cmꢀ1 and 1307 cmꢀ1 are assigned to the triazine
rings. The new vibration band at 1330 cmꢀ1 is corresponding to the
C-N stretching vibrations in the polymer TPBP, while the disap-
pearance vibration band at 495 cmꢀ1 is C-Br stretching vibration
of the monomer TBT. These FTIR profiles together suggest the suc-
cessful coupling reaction between TBT and phenazine. The results
of the XPS verified the two characteristic elements C and N in
Fig. 1. (a) IR spectra of TBT (black line), phenazine (red line) and TPBP (blue line). (b) Solid-state 13C CP-MAS NMR spectrum of TPBP.