Q. Gu et al.
Molecular Catalysis 504 (2021) 111441
Fig. 6. Photocatalytic performance histogram of different photocatalysts.
can be observed that typical IV curve and a noticeable H3-type hyster-
esis loop at the relative pressure ranging from 0.45 to 1.0, the former
indicating the presence of mesopores and macropores in the materials
[56] and the latter suggesting the formation of slit-like pores. According
to the BET experimental parameters (Table S2, Supporting information)
and the pore size distributions curves (Fig. S1, Supporting information),
compared with CN, the increasing of specific surface area and pore
volume in the CN-Mo-2 indicates that it can provide more active sites.
All photocatalysts have an absorption edge at ~ 460 nm in the
UV–vis absorption spectra (Fig. 5a). Compared with CN, CN-Mo-X ex-
hibits a stronger absorption in ultraviolet wavelengths and a red shift of
the absorption edge, indicating the enlarged band gap. This phenome-
non may be caused by the doping of Mo element. The steady-state
fluorescence photoluminescence (PL) was applied to explore the
charge migration and separation of photocatalysts [57]. In the PL
spectra (Fig. 5b), the peak centre of CN-Mo-2 appears at the wavelength
of 486 nm, while the peak centre of CN appears at the lower wavelength
of 476 nm. It shows that the peak centre of CN-Mo-2 has a red shift,
2.004) is higher than that of CN (g = 2.003), implying the existence of
defects, which may be caused by the doping of Mo element into the
g-C3N4 skeleton.
The transient photocurrent spectrum and electrochemical imped-
ance spectroscopy (EIS) of photocatalysts were obtained using chro-
noamperometry, as shown in Fig S3 (Supporting information). It can be
seen that the photocurrent response density of CN-Mo-2 is higher than
that of CN (Fig S3 a.), indicating that the CN-Mo-2 has higher conduc-
tivity at the same voltage, which proves that the separation and
migration of charge carriers is enchanced. However, in the Nyquist di-
agram (Fig S3 b), the arc radius of CN-Mo-2 is smaller than that of CN,
inferring that CN-Mo-2 has lower resistance in the process of charge
carrier migration. Thus, the results of photocurrent and EIS also has
suggested that CN-Mo-2 can improve the capacity of carrier separation
and photocatalytic activities. Therefore, combined with the above
characterization results, it is inferred that the doping of Mo promote
separation capacity of photoinduced electron-hole pairs, improve car-
rier separation capability and enhance the range of light absorption. At
the same time, the doping of Mo element leads to a porous structure of g-
C3N4, which provides more active sites. Benefiting from these features,
the lamellar porous Mo-modified C3N4 shows better competence for
diverse photocatalytic application.
which is caused by the extended
π conjugated system. Additionally, the
PL intensity of CN-Mo-2 is lower than that of CN, which is beneficial to
restrain electron-hole recombination and promote the mobility of the
charge carriers [58]. The time-resolved fluorescence spectroscopy was
further used to validate the improvement of charge separation efficacy,
as shown in the Fig. 5c and Table S3 (Supporting information).
Compared with CN, CN-Mo-2 has a slower exponential decay with
average fluorescence lifetimes of 13.05 ns, which means the carrier
lifetime is extended. Increasing the carrier migration rate, inhibiting the
recombination of electron holes and prolonging the carrier lifetime are
beneficial for improving the photocatalytic performance.
3.2. Photocatalytic activities
To explore the optimized Mo content of CN-Mo-X, photocatalytic
epoxidation of styrene was carried out as model reaction (Scheme 1).
The composition of products was determined by gas phase spectrometry,
and the percentage of products was calculated by the peak area in the
spectrum. As shown in Fig. 6, CN-Mo-X displays the better photo-
catalytic performance for epoxidation of styrene under simulated sun-
light irradiation at the room temperature for 6 h with 50 wt. % H2O2 as
oxygen source. Detailed data are presented in Table S5 (supporting in-
formation), the lamellar CN is used as photocatalyst, the conversion rate
of styrene reaches 13.2 % and increase of 29.5 % over the bulk g-C3N4.
When Mo element is introduced into lamellar CN, the conversion rate of
styrene is more than 30 % and 3-fold enhancement over the CN. As the
increasing of Mo content, the conversion rate of styrene increased
slowly, but the selectivity of styrene oxide decreased. The main by-
products are benzyl alcohol and benzoic acid (Fig. S5, Supporting
Electron paramagnetic resonance (EPR) signals were used to explore
the charge effect on the photocatalysts, as illustrated in Fig. 5d. CN and
CN-Mo-2 produce an single Lorentz derived line which is derived from
the signals of the lone pair electrons in the heptazine ring carbon atoms
[59]. More electrons are excited when the sunlight irradiates photo-
catalysts, leading to photocatalysts exhibit an intensive EPR signal under
simulated sunlight illumination. Additionally, CN-Mo-2 exhibits an
obviously stronger signal than CN, indicating CN-Mo-2 has stronger
electron delocalization ability and is easier to generate lone pair elec-
tron. The g value was obtained and shown in Fig S2 (Supporting infor-
mation) by the analysis of EPR signals. The g value of CN-Mo-2 (g =
6