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high-resolution N1s spectrum of NPS-HCS can be fit well
with four kinds of N species. Peaks at about 398.8, 400.0,
401.0, and 404.9 eV were corresponding to pyridinic nitrogen,
pyrrolic nitrogen, graphitic nitrogen, and pyridinic N+-OÀ,
respectively.[16] Besides above four peaks, another peak at
N+-OÀ, while there were four nitrogen species (pyridinic
nitrogen, pyrrolic nitrogen, graphitic nitrogen, and pyridinic
N+-OÀ) in NPS-HCS. Finally, the existence of a ZIF-67 core
during the calcination improved the wettability of the NPS-
HCS in water. Contact angle (CA) measurement (Figure S8)
showed that the sample produced after calcinations of pure
ZIF-67 under the same conditions displayed superhydrophi-
licity with a CA close to 08, while the sample produced after
calcinations of pure PZS displayed hydrophobicity with a CA
of about 1358. And the NPS-HCS also showed superhydro-
philicity with a CA of about 08. A digital photo showed that
NPS-HCS was well-dispersed in water (Figure S9). This is also
beneficial for catalytic processes in water.
398.6 eV can also be seen, which may be ascribed to the
[17]
=
À
pyridinic nitrogen or P N/P N bonds. A similar peak was
also found in the pure PZS (Figure S4). The P2p spectrum
showed two peaks at 132.7 and 133.9 eV, corresponding to P-
C and P-O, respectively (Figure 3c).[18] The S2p spectrum
displayed three peaks at 164.0, 165.2, and 168.3 eV, which
were ascribed to 2p3/2, 2p1/2 splitting of the S2p spin orbital
(-C-S-C-) and oxidized S, respectively (Figure 3d).[19] These
data adequately confirmed that N, P and S atoms have been
successfully incorporated into the hollow carbon shells.
The porous structure of NPS-HCS was determined by the
N2 adsorption–desorption method. As shown in Figure 4a,
a typical type-IV isotherms with a distinct hysteresis loop was
observed, indicating a mesoporous structure of hollow carbon
shells.[20] The pore size distribution calculated by the Barrett–
Joyner–Halenda (BJH) method showed a peak centered at
around 4.3 nm (Figure 4b). The NPS-HCS had a Brunauer–
Emmett–Teller (BET) surface area of 1020 m2 gÀ1 with a total
pore volume of 1.31 cm3 gÀ1. The high surface area and porous
structure are very beneficial for catalysis.
To study the performance of this NPS-HCS carbocatalyst
À
for the selective oxidation of C H bonds, ethylbenzene was
first chosen as a substrate to explore the efficiency (Table 1).
Table 1: Optimization for the selective oxidation of ethylbenzene.[a]
[a] Reaction conditions: catalyst (0.010 g), TBHP (1.0 mL, 70 wt% in
water), ethylbenzene (1.0 mmol), H2O (2.0 mL), 808C.
For comparison, control samples (including pure PZS, ZIF-
67, and PZS-HCS after calcination at 9008C for 2 h in Ar
atmosphere) were also tested. The NPS-HCS catalyst showed
high activity and excellent selectivity during 6 h (entry 5),
much better than those of the test samples (entries 2–4) and
nitrogen-doped graphene reported in the literature.[11] When
the reaction time was prolonged to 12 h, conversion of 99%
with a selectivity 99.5% for acetophenone was achieved
(entry 6). The NPS-HCS catalyst could be easily separated
from the solution by centrifugation and was reused five times
without obvious loss of activity and selectivity (Figure S10).
The morphology, structure, and chemical states of the NPS-
HCS after five runs were nearly the same relative to that of
the fresh catalyst (Figures S11–S13). A little decrease of
activity can be ascribed to the unavoidable sample loss during
the recycle process and partial oxidation of carbon active sites
under the oxidative conditions (Table S2).
Various benzyl aromatic hydrocarbons could also be
oxidized with high yields (Table 2), indicating the superior
efficiency of the NPS-HCS catalyst. The electron-donating
group-substituent (MeOÀ) showed a higher reactivity relative
to those of the electron-withdrawing groups (NO2À; Table 2,
entries 2–3). A high reaction activity could also be obtained
for bulky and sterically hindered molecules, such as 2-
ethylnaphthalene, cumene, fluorine, and diphenylmethane
Figure 4. a) N2 adsorption–desorption isotherms and b) mesopore
size distribution curve of NPS-HCS.
The ZIF-67 core template plays a very important role in
the formation of the final NPS-HCS. First, ZIF-67 was the
structural template for PZS coating. ZIF-67 also helped to
maintain the structural integrity of the hollow carbon shells
during the calcination process. Some broken hollow carbon
shells can be clearly seen in the TEM images of pure PZS
hollow shells after calcination (denoted as PZS-HCS; Fig-
ure S5). Second, ZIF-67 helped to generate a mesoporous
structure and to increase the surface area of NPS-HCS by the
released gases after the decomposition of ZIF-67. For
comparison, PZS-HCS showed no mesopores and a signifi-
cantly lower surface area of 667 m2 gÀ1 (Figure S6). Third,
nitrogen atoms in the ZIF-67 core were also doped into the
hollow carbon shells during thermal calcination, increasing
the total amount of N doping and optimizing the distribution
of nitrogen species in the final NPS-HCS. According to the
XPS result, the N atomic ratio increased from 1.98% in PZS-
HCS to 3.15% in NPS-HCS (Table S1). Furthermore, the N1s
spectrum of PZS-HCS (Figure S7) can be divided into three
peaks of pyridinic nitrogen, graphitic nitrogen, and pyridinic
ꢀ 2016 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2016, 55, 4016 –4020