Full Papers
doi.org/10.1002/cctc.202101016
ChemCatChem
[
18]
providing hydrogen source and sacrificing hole at the same
time, (iii) a highly reducing and stable photocatalyst, and (iv)
normal pressure and temperature.
structure for Zn Cd S. With the increase of the Cd content,
0.7 0.3
the X-ray diffraction (XRD) peaks of Zn Cd S solid solution
becomes broader, which is due to the larger particle size from
x
1À x
Zn Cd S solid solution is an extensively studied semi-
conductor material due to its adjustable bandgap and band
edge position with the change of Zn/Cd ratio. It shows excellent
60 nm of TÀ Zn Cd S to 80 nm of TÀ Zn Cd S (Figure S1). In
x
1À x
0.1
0.9
0.9
0.1
addition, the XRD peaks continuously shifts to the lower angle
+
2
(Figure 1e), which is due to the larger radius of Cd (0.97 Å)
[19]
photocatalytic H evolution performance with visible light
incorporated into crystal lattice. At the same time, the crystal
phase of Zn Cd S gradually changes from the cubic phase to
2
[14]
excitation.
Among various Zn Cd S structures, nano-twin
x 1À x
x
1À x
crystal Zn Cd S (TÀ Zn Cd S) solid solution, composed of two
the hexagonal phase. The composition of as-prepared
x
1À x
x
1À x
(
zinc-blende (ZB) and wurtzite (WZ)) crystal phases, has inner
TÀ Zn Cd S was determined by inductively coupled plasma
x
1À x
homo-junction, which promoted charge separation, and then
atomic emission spectrometry (ICP-AES) experiments. The result
in Table S1 shows that the practical atomic ratios of Cd to Zn
are very close to the stoichiometric atomic ratio for all
TÀ Zn Cd S materials, which indicates the composition accu-
[
16]
excellent catalytic activity. Moreover, TÀ Zn Cd S are more
x
1À x
stable and more efficient proton reduction ability in comparison
with CdS. Previous work has reported that the apparent
x
1À x
quantum yield (AQY) for photocatalytic H evolution can reach
racy. With the increase of atomic ratio of Cd/Zn, the specific
2
[17]
to 62% at 425 nm without the presence of any co-catalysts.
Therefore, we use Zn Cd S with nano-twin crystal structure as
surface area of TÀ Zn Cd S notably increases and the max-
x
1À x
2
À 1
imum value reached to 14.20 m g for Zn Cd S (Table S1 and
x
1À x
0.5
0.5
catalyst for the photocatalytic reduction of DNDPE to ODA in
water-ethanol solution under normal pressure, room temper-
ature and visible light irradiation. Without any noble metal
cocatalysts or additional hydrogen source, DNDPE shows the
conversion of more than 95% in 10 min and complete
conversion within 40 min, which greatly exceeds traditional
catalysis method. The yield of corresponding ODA product over
TÀ Zn Cd S achieved >99% under acidic condition. The
Figure S4). In addition, X-ray photoelectron spectra (XPS) was
measured to investigate the surface chemical states of
TÀ Zn Cd S photocatalysts. As shown in Figure S5a, the bind-
x
1À x
ing energies of Cd 3d upon TÀ Zn Cd S are found at 404.87
0
.7
0.3
and 411.60 eV, which is negatively shifted in comparison with
CdS. Similarly, the XPS peaks of Zn 2p1/2 and 2p3/2 observed for
TÀ Zn Cd S sample shifted to lower binding energies at
0
.7
0.3
1021.85 and 1044.87 eV (Figure S5b), compared with those of
pure ZnS. Due to the hybridization of Cd and Zn composing the
0.7
0.3
catalyst performed excellent stability under the reaction
conditions. This is the first report of the photocatalytic
reduction of DNDPE to ODA under visible light excitation in
water-ethanol system. According to HPLC-MS analysis and
theoretical calculation, the reduction of the two nitro groups of
DNDPE are reduced separately, following the order of:
DNDPE!NO À RÀ NO!NO À RÀ NHOH!NO À RÀ NH !
[
20]
conduction band (CB) of TÀ Zn Cd S, above negative energy
0
.7
0.3
shifts of Cd 3d and Zn 2p for TÀ Zn Cd S sample indicate that
0
.7
0.3
the hybridization facilitates the increase of electron density,
which could enhance the photocatalytic reduction activity.
The photocatalytic reduction of DNDPE was carried out in
an ethanol-water suspension of TÀ Zn Cd S under visible light
2
2
2
2
x
1À x
NOÀ RÀ NH !NH À RÀ NHOH!ODA. The isotope label experi-
irradiation. The photoreactor was sealed and purged with N for
2
2
2
ment result demonstrates that hydrogen protons of water,
instead of ethanol, provide the hydrogen source for the
photocatalytic reduction of DNDPE to ODA.
30 minutes to remove air before light irradiation. High-perform-
ance liquid chromatography (HPLC) was used to determine the
amount of DNDPE, ODA and other products. External standard
method was carried out to quantify the amount of DNDPE, ODA
and 4-(4-Nitrophenoxy) aniline. The standard curves of DNDPE,
ODA and 4-(4-Nitrophenoxy) aniline in Figure S6 show favorable
linear relationship between response area and standard con-
Results and Discussion
9
9
7
A series of TÀ Zn Cd S photocatalysts with various Zn/Cd
centration, with the slope of 1.08×10 , 1.12×10 , and 6.30×10 ,
respectively. A series of blank experiments (Table S2) reveal that
the photocatalyst and photoirradiation are indispensable for
the reduction of DNDPE. Then we investigated and compared
the catalytic performance under different solvent composition
in ethanol-water mixture using TÀ Zn Cd S as photocatalyst.
x
1À x
molar ratio were prepared via a NaOH-assisted hydrothermal
[5f]
method according to our previous work. Detailed procedures
were described in Experimental Section and various character-
izations were employed to figure out the morphology and twin
crystal structure of Zn Cd S. As shown in the representative
x
1À x
0.7
0.3
scanning electron microscope (SEM) and transmission electron
microscopy (TEM) images (Figure 1 and S1-S3), the average
diameter of particles upon pure CdS, Zn Cd S, Zn Cd S,
As shown in Table 1, the conversion of DNDPE to ODA is hardly
detected in both pure water or ethanol. When photocatalytic
reaction is carried out in pure water, the separation efficiency of
photogenerated charges is poor and most photogenerated
electrons recombined with holes. PL emission spectra in
Figure S7 shows that the emission intensity in pure water is
much stronger than that in ethanol-water system. Therefore,
the amount of photogenerated electrons reacted with DNDPE is
significantly reduced and the conversion is low. At the same
0
.1
0.9
0.3
0.7
Zn Cd S, and Zn Cd S samples is 65�5.0 nm. However,
0.5
0.5
0.7
0.3
Zn Cd S and pure ZnS show obviously large particle size with
0.9
0.1
about 80 and 115 nm. High-resolution TEM image in Figure 1c
exhibits obvious boundary of twin crystal structure, which is
zinc-blende (ZB) and wurtzite (WZ) segments, respectively. The
lattice spacing of 0.320 nm belongs to the (100) diffraction
plane of Zn Cd S and the corresponding fast Fourier trans-
time, pure ethanol possesses much smaller ionization equili-
0.7
0.3
À 15.9
form (FFT) image further suggests the presence of twin crystal
brium constant (1×10
) than water, which indicates that the
ChemCatChem 2021, 13, 1–12
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