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Co-Activated Amorphous MoSx Nanodots Grown In Situ on Natural Attapulgite Nanofibers for Efficient Visible-Light-Driven Dye-Sensitized H2 Evolution Xiangyu Liu, Yuan Xue, Yonggang Lei, Fang Wang, and Shixiong Min ACS Appl. Nano Mater., Just Accepted Manuscript • DOI: 10.1021/acsanm.8b01785 • Publication Date (Web): 12 Oct 2018 Downloaded from http://pubs.acs.org on October 21, 2018
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Co-Activated Amorphous MoSx Nanodots Grown In
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Situ on Natural Attapulgite Nanofibers for Efficient
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Visible-Light-Driven Dye-Sensitized H2 Evolution
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Xiangyu Liu‡, Yuan Xue‡, Yonggang Lei, Fang Wang* and Shixiong Min*
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School of Chemistry and Chemical Engineering, Key Laboratory of Electrochemical Energy
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Conversion Technology and Application, North Minzu University, Yinchuan, 750021, P. R.
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China.
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KEYWORDS. amorphous MoSx, attapulgite (ATP) nanofibers, Co doping, dye-sensitization, H2
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evolution, visible light
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ABSTRACT. In-situ grown amorphous MoSx catalysts in an organic dye-sensitized system have
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shown promising performance for catalyzing H2 evolution; however, the inevitable aggregations
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and the low intrinsic activity of active sites of thus-obtained MoSx catalysts should be addressed
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to further enhance their activity. Herein, we report an exceptionally active catalyst of in situ grown
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Co-activated amorphous MoSx nanodots (15 MΩ) obtained by an YL-100B-
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D water-purification system. (NH4)2MoS4 was synthesized from (NH4)6Mo7O24 (15 g) and
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(NH4)2S solution (21%) (200 mL) according to the reported procedure.46 Raw attapulgite (ATP)
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were obtained from Linze County of Gansu Province in China and purified by a suspension-
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sedimentation method using SHMP as an dispersing agent. In a typical procedure, 100 g of raw
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ATP was dispersed into 2.0 L of water containing 3.0 g of SHMP under vigorously stirring for 2
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h to obtain a homogenous ATP suspension. Then, the thus-obtained ATP suspension was tip-
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ultrasonicated for 1 h and allowed statically settled overnight. The purified ATP was collected
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from the suspension by high-speed centrifugation and freezing-dried. After purification, the
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associated minerals such as calcite and dolomite in raw ATP was completely removed only a trace
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amount of quartz could be observed in purified ATP (Figure S1).
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2.2 Synthesis of ATP/Co(OH)2 hybrid and Co(OH)2. In a typical synthesis of ATP/Co(OH)2
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hybrid, 500 mg of purified ATP was dispersed into 500 mL of water by ultrasonication, to which
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a calculated amount of CoCl2·6H2O (1.25 mmol) as the Co source and HMT (22.5 mmol) as the
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hydroxide ions (OH-) source were added under magnetic stirring. The nominal loading amount of
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Co(OH)2 on ATP is ca. 18.9 wt.%. Afterwards, the obtained suspension was refluxed at 95 oC for
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5 h under stirring with a N2 atmosphere protection, during which the HMT will gradually hydrolyze
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to release OH- that subsequently reacted with Co2+ to exclusively form Co(OH)2 nanosheets by
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avoiding the oxidation under inert atmosphere. The obtained products were filtered, washed with
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water and ethanol, and dried at a vacuum oven at 80 oC overnight. In addition, ATP/Co(OH)2
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hybrids with different contents of Co(OH)2 (4.5 and 31.7 wt.%) were also synthesized using above
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procedures by changing the adding amount of CoCl2·6H2O at a fixed molar ratio of 18 for
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CoCl2·6H2O to HMT. For a comparison, Co(OH)2 was synthesized by the exact same procedures
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for the preparation of ATP/Co(OH)2 hybrid except the addition of ATP.
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2.3. In Situ Photochemical Synthesis of Catalysts. Free amorphous MoSx catalysts were
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prepared by in situ photoreduction of (NH4)2MoS4 during the ErB-sensitized photocatalytic H2
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evolution reaction (see below in Section 2.5). After 5 h irradiation, the produced products were
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filtered, washed with distilled water and anhydrous ethanol, and freezing-dried. For comparison,
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Co-MoSx, ATP/MoSx, and ATP/Co-MoSx catalysts were also synthesized by the exact same
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procedures for preparation of MoSx catalysts in the presence of Co(OH)2, ATP, and ATP/Co(OH)2,
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respectively.
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2.4 Characterization. Transmission electron microscopy (TEM) and high-resolution TEM
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(HRTEM) images were taken with a FEI Talos F200s field emission transmission electron
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microscope. X-ray diffraction (XRD) patterns were obtained with a Rigaku Smartlab
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diffractometer with a nickel filtrated Cu Kβ radiation. X-ray photoelectron spectroscopy (XPS)
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was performed on an X-ray photoelectron spectrometer (Thermo Scientific Escalab-250Xi, a
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monochromatic Al KR X-ray source). The zeta potential (ζ potential) was measured using a
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Zetasizer Nano-ZS90 (Malvern Instruments, UK). UV–vis absorption spectra were taken with a
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Thermo Scientific–Evolution 220 spectrophotometer.
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2.5 Dye-sensitized Photocatalytic H2 Evolution Experiments. Dye-sensitized photocatalytic
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H2 evolution experiments were performed in a sealed quartz reaction cell with a top flat window
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for light irradiation and a silicone rubber septum was fixed on its side for sampling. A 30-W white-
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light LED lamp was used as the light source with a cut-off filter of 450 nm. In a typical experiment,
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a certain amount of the catalyst precursor (NH4)2MoS4 was dissolved in 100 mL of 10% (v/v)
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aqueous TEOA solution (pH 8) containing 0.2 mM ErB and Co(OH)2 (1.9 mg), ATP (8.1 mg), or
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ATP/Co(OH)2 (10 mg) if needed. After removing the dissolved oxygen by repeated evacuation-
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N2 filling process, the reaction suspension was irradiated under stirring for photocatalytic H2
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evolution. The amount of evolved H2 was determined using an gas chromatograph (GC) (Tech
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comp, GC-7900) with a thermal conductivity detector (TCD), a 5 Å molecular sieve column (4
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mm×5 m), and N2 as carrier gas. In the stability test of catalysts, in-situ grown catalysts were
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separated by centrifugation every 5 h irradiation and redispersed into the fresh TEOA solution
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containing fresh ErB, and all the reaction conditions were the same as the above photocatalytic
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reaction.
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The monochromatic quantum yields for the H2 evolution were measured under the condition
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similar to the above photocatalytic reaction except the light source was equipped with various
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band-pass filters (450, 475, 500, 520, 550, and 600 nm). The photon flux of incident light was
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determined using a Ray virtual radiation actinometer (Apogee MQ-500, silicon ray detector, light
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spectrum, 389-692 nm; measurement range, 0~4000 μmol m-2 s-1). The apparent quantum yields
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(AQY) was calculated from the ratio of the number of reacted electrons during H2 evolution to the
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number of incident photons according to the following equation (1):
AQY (%) 8
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2 number of evolved H 2 molecules 100 number of incident photons
(1)
3. RESULTS AND DISCUSSION
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X-ray diffraction (XRD) characterizations were first performed to reveal the growth of Co(OH)2
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on ATP (ATP/Co(OH)2). Figure 1a shows the XRD patterns of the purified ATP, pristine
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Co(OH)2, and as-synthesized ATP/Co(OH)2 hybrid. The XRD pattern of purified ATP show four
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typical diffraction peaks belonging to (110), (200), (040), and (400) planes at 8.6°, 14.2°, 19.9°,
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and 26.8°, respectively, without significant XRD peaks of quartz impurities, showing that the ATP
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is highly pure.53 As to the pristine Co(OH)2, six characteristic peaks at 19.1°, 32.6°, 38.3°, 51.5°,
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58.1°, and 61.7°, which can be indexed to (001), (100), (101), (102), (110), and (111) crystalline
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planes of the β-Co(OH)2 (JCPDS No. 30-0443), respectively.55 In the XRD pattern of as-
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synthesized ATP/Co(OH)2 hybrid, the diffraction peaks ascribed to (001), (101), and (102) planes
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of the β-Co(OH)2 could be observed, whereas the main diffraction peak of ATP weakened
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remarkably, which might be due to the structural modification of ATP nanosheets by Co(OH)2
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through chemical coupling. The growth of Co(OH)2 on ATP was further identified by TEM
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analysis. As shown in Figure 1b, the purified ATP is the closed parallel aggregations of nanofibers
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with a length up to several micrometers and a width of 30~50 nm with no observable impurities.
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In the TEM image of ATP/Co(OH)2 hybrid (Figure 1c), a large number of Co(OH)2 nanosheets
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(lateral size: ca. 300~500 nm) were found to interconnect with the one-dimensional ATP
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nanofibers, which is further confirmed by its corresponding selected area electron diffraction
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(SAED) pattern (Figure 1d), where obvious diffraction rings originated from (002), (100), and
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(110) planes could be clearly observed. Therefore, these results firmly demonstrated the successful
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growth of Co(OH)2 on ATP leading to ATP/Co(OH)2 hybrid.
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Afterwards, the H2 evolution catalysts, free MoSx, ATP/MoSx, and ATP/Co-MoSx, were
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synthesized by an in situ photosensitization method from a ErB-TEOA system under visible light,
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as schematically illustrated in Figure 1e. It was observed that accompanying with the formation
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of catalysts, the evolution of H2 could be confirmed by gas chromatography, indicating that the in
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situ generated catalysts then acted as the active catalysts for catalyzing the subsequent H2 evolution
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reaction from the same sensitization system.46-49 Control experiments showed that the absence of
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any of the ErB, light, and TEOA leds to no or trace H2 evolution. Figure 2a displays the H2
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evolution activity catalyzed by free MoSx, ATP/MoSx, and ATP/Co-MoSx catalysts from the ErB-
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TEOA system. With free MoSx alone, only 13.5 μmol of H2 can be produced after a 5 h irradiation
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reaction. However, the loading of MoSx on ATP support (ATP/MoSx) drastically enhances the H2
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evolution activity. Total amount of 93.3 μmol of H2 could be produced over ATP/MoSx catalyst
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in 5 h reaction, which is about 7 times higher than that of over free MoSx catalyst. Significantly,
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when MoSx was loaded on ATP/Co(OH)2 hybrid to form ATP/Co-MoSx catalyst, the H2 evolution
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amount can be remarkably increased to 907.5 μmol after a 5 h reaction, which is 67.2 and 9.7 times
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that of free MoSx and ATP/MoSx catalysts, respectively.
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Several comparison experiments were also carried out to highlight the important roles of ATP
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and the Co species in enhancing the catalytic activity of MoSx catalyst. As shown in Figure 2b,
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without the loading of MoSx, pristine ATP and in situ sulfurized ATP show no activity toward H2
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evolution, indicating that the MoSx catalyst is the active component for H2 evolution reaction, and
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the possibility of trace metal species within ATP after sulfurization as H2 evolution catalysts can
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be excluded. With ATP/Co(OH)2 hybrid being used as the catalyst, the ErB-sensitized system
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shows an average H2 evolution rate of 17.8 μmol h-1, indicating that the Co(OH)2 could act as an
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active catalyst for H2 evolution, consistent with previous observations in the literature.56 After the
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ATP/Co(OH)2 hybrid was sulfurized with (NH4)2S, the resulted hybrid shows much higher H2
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evolution rate of 44.4 μmol h-1, probably due to the formation of active Co-S species. In addition,
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when Co(OH)2 was used as the support for MoSx catalyst, the resulted Co-MoSx hybrid catalyst
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exhibits a much higher H2 evolution rate of 70.5 μmol h-1 compared to free MoSx (2.7 μmol h-1)
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and ATP/MoSx (18.7 μmol h-1) catalysts. Moreover, the physical mixture of Co(OH)2/MoSx
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prepared by mixing in situ formed MoSx (centrifugated and washed with water and ethanol) with
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Co(OH)2 at a similar Co(OH)2:MoSx mass ratio shows much inferior activity (10.6 μmol h-1) to in
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situ formed Co-MoSx hybrid catalyst, suggesting that certain highly active species generated in
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situ during the photochemical reduction of the precursor (MoS42-) of MoSx in the presence of
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Co(OH)2 (see detailed discussion below) is important to achieve a high H2 evolution activity.
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These results demonstrate that both ATP and Co(OH)2 are absolutely necessary and can
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synergistically improve the catalytic H2 evolution activity of in-situ generated MoSx catalysts. In
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addition, the performance of ATP/Co-MoSx catalyst for H2 evolution was compared with various
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ATP/M-MoSx (M=Ni, Fe, Cu, Zn) catalysts prepared using exact same procedure as ATP/Co-
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MoSx catalyst from corresponding ATP/metal hydroxide supports and (NH4)2MoS4. As shown in
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Figure S2, the ATP/Co-MoSx catalyst outperforms other ATP/M-MoSx catalysts for H2 evolution.
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The Co, Ni, Fe, and Cu can obviously promote the H2 evolution activity of MoSx on ATP and
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follows the order of Co>Ni>Fe>Cu, while the Zn will deteriorate the activity of MoSx catalysts,
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consistent with the activity trend observed for transition metal-promoted MoSx catalyst for
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electrocatalytic and photocatalytic H2 evolution.57 DFT calculations demonstrated that these metal
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dopants, especially Co doing can efficiently decrease the hydrogen bonding energy (∆GH) of S-
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edges by forming active Co-S-Mo coordination,57,58 thus an enhanced HER activity could be
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achieved.
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Furthermore, the variations in activity for H2 evolution catalyzed by different concentrations of
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MoSx for both free MoSx and ATP/Co-MoSx catalysts were investigated and compared, as shown
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in Figure 2c. Overall, the average H2 evolution rates increase rapidly with increasing MoSx
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concentration for both type of catalysts and slow down when the concentration of MoSx is larger
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than 0.05 mM. The ATP/Co-MoSx catalysts at each MoSx concentration show much higher activity
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than free MoSx catalysts and an enhancement factor of as high as 67 is obtained at 0.05 mM MoSx.
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At higher MoSx concentrations, the enhancement factor was decreased, probably due to the
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aggregations of excess Co-MoSx on ATP, which will largely block the active sites for H2 evolution
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(Figure S3). Moreover, at higher MoSx concentrations, even though a larger amount of H2 is
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evolved, the turnover number (TON) decreases because of the limited lifetime of the system
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(Figure S4). The highest TON of 346 is achieved at 0.01 mM MoSx, which is much higher than
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the previously reported values.46-49 In contrast to ATP/Co-MoSx catalyst, the TONs of H2 evolution
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over free MoSx catalyst are low and increases with the MoSx concentration and reaches a plateau
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at MoSx concentrations higher than 0.1 mM, indicating that the H2 evolution activity of free MoSx
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catalyst is limited by the limited number of exposed active sties at higher MoSx concentrations. In
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addition, the effect of mass ratio of Co(OH)2 to ATP in ATP/Co(OH)2 hybrids on the catalytic H2
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evolution activity of resulted ATP/Co-MoSx catalysts were also investigated. With increasing
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Co(OH)2 content on ATP support, the diffraction peaks of ATP reduced while the diffraction peaks
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corresponding to Co(OH)2 become evident as confirmed by the XRD analysis in Figure S5,
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indicating the gradual covering of ATP by Co(OH)2. As shown in Figure S6, the optimum loading
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amount of Co(OH)2 of ATP/Co(OH)2 hybrids is found to be 18.9 wt.%, at which the obtained
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ATP/Co-MoSx catalyst exhibits an optimum H2 evolution activity at a fixed concentration of
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MoSx. At low Co(OH)2 content, there is no enough Co source that can be provided to form
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effective Co-MoSx catalyst on ATP, leading to a low activity, while at high Co(OH)2 content, the
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active sites of formed Co-MoSx catalyst may be blocked, showing activity deterioration. Figure
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2d shows the apparent quantum yield of H2 evolution catalyzed by ATP/Co-MoSx catalyst from
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ErB-TEOA. The highest AQY value was estimated to be 47.7% at 500 nm, which is in good
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agreement with the maximum absorption wavelength of ErB during the H2 evolution (Figure S7),
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indicating that the light absorption of ErB governs the H2 evolution from this system.
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In order to gain insight into the superior photocatalytic H2 evolution activity of ATP/Co-MoSx
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catalyst from ErB-TEOA system under visible light, the microstructural analyses were first
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performed on resulted catalysts. The XRD patterns in Figure 3a reveal that the in-situ generated
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free MoSx catalyst is amorphous, while the XRD pattern of ATP/Co-MoSx catalyst is identical to
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the purified ATP without the preservation of Co(OH)2 structures on ATP. Considering that the
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preparation of ATP/Co-MoSx catalyst was started from the ATP/Co(OH)2 hybrid and (NH4)2MoS4
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precursors, this result indicates that the formation of ATP/Co-MoSx catalyst proceeds via the in
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situ photoreduction of [MoS4]2- to amorphous MoSx with the Co doping from Co(OH)2 forming
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amorphous Co-doped MoSx on ATP. The transmission electron microscopy (TEM) and high-
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resolution TEM (HRTEM) images in Figure 3b present the typical aggregated structure and
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amorphous nature of free MoSx catalyst. The sizes of free MoSx catalyst are in the range of 150 to
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300 nm. When ATP was used as the support, the in situ grown MoSx particles show no significant
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change on size but the their dispersion is improved due to the presence of ATP (Figure 3c). By
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strong contrast, as shown in the TEM image of ATP/Co-MoSx catalyst in Figure 3d, a large
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number of tiny Co-MoSx nanodots with a size smaller than 5 nm are observed on the surfaces of
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ATP nanofibers. From its HRTEM image in Figure 3e, the Co-MoSx nanodots are found to be
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amorphous and highly dispersed on the surface of ATP nanofibers, implying the presence of Co-
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MoSx as abundant surface active sites.49 In addition, the high angle annular dark field-scanning
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transmission electron microscopy (HAADF-STEM) image of ATP/Co-MoSx catalyst in Figure 3f
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and corresponding element mappings demonstrate the uniform distribution of the Mo, Co, and S
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elements on the surface of ATP nanofibers, indicating the uniform doping of MoSx with Co and
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the high distribution of Co-MoSx nanodots on ATP nanofibers. The drastic differences in both size
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and dispersion of Co-MoSx nanodots on ATP as compared to free MoSx and MoSx on ATP
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(ATP/MoSx) highlights the important roles of ATP/Co(OH)2 support for mediating the growth of
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MoSx, where the Co(OH)2 nanosheets would act as the sacrificial Co sources to react with MoS42-
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during photoreduction process while ATP could act as the large surface area support to anchor the
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in situ formed Co-MoSx catalyst, as a result, the large size Co(OH)2 nanosheets (ca. 300~500 nm)
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on ATP vanished and eventually Co-MoSx nanodots were loaded on the surfaces of ATP
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nanofibers. In order to further clarify this important role of Co(OH)2 nanosheets, the formation
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behaviors of MoSx on free Co(OH)2 nanosheets in the absence of ATP was also investigated by
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TEM analysis, as shown in Figure S8. It is found that the two-dimensional hexagonal structures
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of Co(OH)2 nanosheets is severely destroyed during the photoreduction of [MoS4]2-and a number
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of aggregated nanoparticles (ca.100~300 nm) formed on the surfaces of broken Co(OH)2
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fragments. This result indicates that the ultrathin Co(OH)2 nanosheets with abundant exposed Co
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sites indeed act as an sacrificial Co source to react with MoS42- during photoreduction process,
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leading to the formation of Co-MoSx nanoparticles. Therefore, it can be safely inferred that a
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Co(OH)2/MoS42- assembly with the microstructure similar to its molecular analogue
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[CoII(MoVIS4)2]2- might form upon mixing of Co(OH)2 and MoS42-,44,49 which will then be reduced
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to Co-MoSx nanoparticles by the electrons of excited dye. It should also be noted that the size of
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Co-MoSx catalyst on ATP is much smaller than free Co-MoSx nanoparticles, which can be
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explained by the fact that the smaller size Co(OH)2 nanosheets on ATP as compared to free
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Co(OH)2 nanosheets should be more active to react with MoS42-, thus leading to a rapid nucleation
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of in situ formed Co-MoSx, consequently, Co-MoSx nanodots were grown on ATP. Moreover, zeta
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potential (ξ) measurements were also performed to get insight into the formation of MoSx in the
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presence of different supports, as shown in Table S1. It could be observed that the negatively
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charged surfaces of purified ATP could be changed to be positively charged after growth of
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Co(OH)2 nanosheets, which will greatly facilitate the adsorption of negatively charged [MoS4]2-
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and ErB anions during the in situ photochemical synthesis, thus a highly dispersed Co-MoSx with
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reduced size could be confinedly grown on the high surface area ATP nanofibers. As to the
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synthesis of ATP/MoSx catalyst, the electrostatic repulsion between ATP and [MoS4]2- is
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unfavorable to the adsorption of [MoS4]2- and nucleation of in-situ formed MoSx, finally leading
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to the formation of large-size MoSx particles on ATP, while the absence of ATP will further result
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in a severe aggregation during the growth of free MoSx.
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The surface chemical states of ATP/Co-MoSx catalyst were investigated by X-ray photoelectron
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spectroscopy (XPS), as shown in Figure 4 and Table 1. The Co 2p spectrum of ATP/Co(OH)2
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(Figure 4a) shows that the Co 2p3/2 (Co 2p1/2) peak occurs at 781.12 eV (797.26 eV), indicating
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the existence of a Co with an oxidation state of +2.59 It is worth noting that apart from the two
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spin-orbit doublets characteristic of Co2+ (781.99 and 797.34 eV), a new Co 2p3/2 (Co 2p1/2) peak
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ascribed to the complex heterobimetallic sulfide is found at 779.29 eV (794.69 eV) in the Co 2p
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spectrum of ATP/Co-MoSx catalyst, showing the in situ formation of “CoMoS” phase, consistent
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with that reported in the literature.43,47,49 In addition, it is found that the Co-MoSx catalyst on ATP
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contains 41.5% of sulfided Co species and 58.5% of Co oxide/hydroxide. This result indicates that
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the Co(OH)2 nanosheets on ATP could release Co ions as an dopant to react with MoS42-, which
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cannot only can activate the unsaturated S atoms of MoSx by forming CoMoS sites but also ensure
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the firm deposition of in situ formed Co-MoSx on ATP nanofibers. It should be also mentioned
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that Co species exist in the form of oxide/hydroxide or Co-S could contribute to the H2 evolution
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but their activities are relatively low, as shown in Figure 2b. This result indicates that the enhanced
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performance of ATP/Co-MoSx catalyst might be account for the formation of active “CoMoS”
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phase. In addition, as shown in Figure 4b, the fitting of the Mo 3d region reveals that there exist
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three Mo species for both free MoSx and ATP/Co-MoSx catalysts, indicating the presence of MoSx
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species on ATP in ATP/Co-MoSx catalyst. For free MoSx catalyst, the Mo 3d5/2 (3d3/2) peak
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ascribed to MoIVSx species (62.4%) occurs at binding energy of 228.53 eV (231.63 eV), while the
18
Mo 3d5/2 peaks at higher binding energies of 229.83 eV (231.63 eV) and 232.33 eV (235.43 eV)
19
are assigned to molybdenum oxysulfide type MoVOSx (20.1%) and a small amount of MoVIO3
20
(17.5%), respectively.34-36 By contrast, ATP/Co-MoSx catalyst presents an increased MoVOSx
21
(29.4%) and MoVIO3 (28.2%) species and decreased MoIVSx (42.4%) species, which can be
22
attributable to the oxidation occurring during the photocatalytic H2 production process, consistent
23
with the observations on amorphous CoMoSx catalysts. In addition, the binding energies of MoIVSx
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and MoVOSx species for ATP/Co-MoSx catalyst are shifted toward high energy region compared
2
to that of free MoSx catalyst, probably due to the incorporation of Co dopant. Analysis of the S 2p
3
XPS spectra in Figure 4c of free MoSx and ATP/Co-MoSx catalysts reveals the presence of both
4
monosulfide S2- and disulfide (S2)2- ligands, with minor sulfates at higher binding energies.34-36
5
Compared to free MoSx catalyst, the content of S2- ligand increases while the (S2)2- ligand decrease
6
accordingly, indicating that the Co dopant may attack the bridging (S2)2- to form “Co-S-Mo”
7
coordination. According to the fitting results of XPS, the S/Mo ratio is determined to be 2.97:1 for
8
both free MoSx and ATP/Co-MoSx catalysts and the stoichiometry for Co-MoSx catalyst is
9
calculated to be Co0.88Mo1.25S3.71. Similar to ATP/Co-MoSx catalyst, the XPS analysis (Figure S9)
10
of free Co-MoSx catalyst also shows the formation of “CoMoS” phase during the photochemical
11
synthesis of MoSx particles in the presence Co(OH)2, further confirming the role of Co(OH)2 as
12
an sacrificial Co source for the reaction with MoS42- precursor to lead to the formation of Co-MoSx
13
catalyst during photochemical reduction.
14
All of the aforementioned results thus demonstrate that the high performance of the ATP/Co-
15
MoSx catalyst in catalyzing photocatalytic H2 evolution can be ascribed to the presence of
16
ATP/Co(OH)2 serving as an active matrix, which can provide a large surface area and Co dopant
17
for effectively growing amorphous Co-activated MoSx. The large surface area of ATP nanofibers
18
confines the growth of small Co-MoSx nanodots with high dispersion, affording an abundance of
19
active sites for H2 evolution reaction. On the other hand, the accessible Co dopant released from
20
Co(OH)2 lead to the in situ formation of highly active “CoMoS” sites featuring low overpotential
21
for H2 evolution, thus rendering the ATP/Co-MoSx catalyst with high H2 evolution activity.
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Furthermore, the stability of catalytic H2 evolution over ATP/Co-MoSx catalyst was
2
investigated, including free MoSx catalyst for comparison, as shown in Figure 5. In the first run
3
reaction, the initial H2 evolution rate catalyzed by in situ generated ATP/Co-MoSx catalyst from
4
ErB-TEOA system is high and the activity of sensitization system decreases gradually with the
5
reaction time, which is probably due to the degradation of ErB during the reaction (Figure S7).
6
After completion of the first run reaction, the ATP/Co-MoSx catalyst was collected by high-speed
7
centrifugation and washed, and the fresh EY and TEOA were added. It is found that although the
8
H2 evolution activity of ATP/Co-MoSx catalyst decrease gradually with reaction run, the ATP/Co-
9
MoSx catalyst still shows reasonable H2 evolution activity in the third run reaction, whereas the
10
free MoSx catalyst totally deactivates after the first run reaction. The TEM analysis (Figure S10)
11
of ATP/Co-MoSx catalyst after recycling stability testing reveals that the density of loaded Co-
12
MoSx is remarkably reduced as compared to the fresh catalyst. XPS analysis (Figure S11) of used
13
ATP/Co-MoSx catalyst also indicates that the contents of Mo and S decrease significantly as
14
compared to fresh catalyst, while only trace signal corresponding to Co could be observed. These
15
results clearly indicate that the loss in activity for ATP/Co-MoSx catalyst is due to the leaching of
16
Co-MoSx from the surfaces of ATP. Our ongoing efforts are now being devoted to enhancing the
17
H2 evolution stability of ATP/Co-MoSx catalyst by improving the synthetic procedures.
18
4. CONCLUSIONS
19
In summary, we have developed an exceptionally active H2 evolution catalyst by confinedly
20
growing amorphous MoSx nanodots in situ on Co(OH)2 modified ATP (ATP/Co(OH)2) nanofibers
21
during photocatalytic H2 evolution in a ErB-TEOA system under visible light irradiation. The
22
Co(OH)2 on ATP could act as a sacrificial Co source to induce the formation of highly active
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“CoMoS” sites during the in situ growth of amorphous MoSx and the ATP nanofibers provides a
2
large area confinement surface to greatly reduce the size of in situ loaded Co-MoSx, as a result,
3
Co-MoSx nanodots with size smaller than 5 nm was uniformly grown on the surface of ATP.
4
Therefore, the thus-obtained ATP/Co-MoSx catalyst exhibits remarkably improved catalytic
5
activity for H2 evolution compared to free MoSx catalyst (67.2 times enhancement) and a AQY as
6
high as 47.7% at 500 nm owing to the abundance of exposed active sites and the presence of
7
additional “CoMoS” active sites. Moreover, ATP/Co-MoSx catalyst shows improved stability over
8
free MoSx catalyst during recycling H2 evolution reactions. Accordingly, this work is expected to
9
promote the development of high performance H2 evolution catalysts based on MoSx-based
10
hybrids.
11
ASSOCIATED CONTENT
12
Supporting Information.
13
XRD patterns of raw and purified ATP, activity comparison of different ATP/M-MoSx (M=Co,
14
Ni, Fe, Cu, Zn) catalysts, calculated enhancement factor, calculated turnover numbers of H2
15
evolution, zeta potentials, UV-vis absorption spectra of ErB during H2 evolution reactions, XRD
16
patterns of ATP/Co(OH)2 hybrids with different Co(OH)2 content, the H2 evolution acidity of
17
ATP/Co-MoSx prepared from different ATP/Co(OH)2 hybrids, TEM images and XPS spectra of
18
Co-MoSx catalyst, and TEM image and XPS spectra of ATP/Co-MoSx after recycling reactions.
19
AUTHOR INFORMATION
20
Corresponding Author
21
*E-mail:
[email protected];
[email protected] ACS Paragon Plus Environment
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ACS Applied Nano Materials
1
Author Contributions
2
‡These authors contributed equally.
3
Notes
4
The authors declare no competing financial interest.
5
ACKNOWLEDGMENT
6
This work is supported by the National Natural Science Foundation of China (Grant No.
7
21763001, 21463001), the Natural Science Foundation of Ningxia Hui Autonomous Region
8
(2018AAC02011), the Foundation of State Key Laboratory of High-Efficiency Utilization of
9
Coal and Green Chemical Engineering (Grant No. 2017-K26), the Key Scientific Research
10
Projects in 2017 at North Minzu University (Grant No. 2017KJ20), the Key Scientific Research
11
Projects of the Higher Education Institutions of Ningxia Hui Autonomous Region (Grant No.
12
NCX2017143), the Foundation of Key Laboratory of Electrochemical Energy Conversion
13
Technology and Application.
14
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Sci. 2012, 3, 2515-2525.
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Bonde, J.; Moses, P. G.; Jaramillo, T. F.; Nørskov, J. K.; Chorkendorff, I. Hydrogen
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Evolution on Nano-particulate Transition Metal Sulfides. Faraday Discuss. 2009, 140, 219-
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231.
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(59)
Biesinger, M. C.; Payne, B. P.; Grosvenor, A. P.; Lau, L. W. M.; Gerson, A. R. Smart, R.
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S. C. Resolving Surface Chemical States in XPS Analysis of First Row Transition Metals,
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Oxides and Hydroxides: Cr, Mn, Fe, Co and Ni. App. Surf. Sci. 2011, 257, 2717-2730.
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TABLE AND FIGURE CAPTION:
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Table 1 The fitting results of XPS spectra of Co 2p, Mo 3d, and S 2p core levels for ATP/Co(OH)2
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hybrid, free MoSx catalyst, and ATP/Co-MoSx catalyst.
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Figure 1. (a) XRD patterns of ATP, Co(OH)2, and ATP/Co(OH)2 hybrid. (b-d) TEM images of
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(b) ATP, (c) ATP/Co(OH)2 hybrid, and (d) the corresponding SAED pattern of ATP/Co(OH)2
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hybrid. (e) Schematic illustration of the in-situ photochemical fabrication of amorphous MoSx,
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ATP/MoSx, and ATP/Co-MoSx catalysts and the subsequent photocatalytic H2 evolution from
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ErB-TEOA system under visible light irradiation.
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Figure 2. (a) Time course of H2 evolution over different catalysts sensitized by ErB from TEOA
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solution, 0.05 mM MoSx. (b) Comparison of average H2 evolution rate over different catalysts
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from ErB-TEOA system, 0.05 mM MoSx. (c) Variations of H evolution rate from ErB sensitized
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free MoSx and ATP/Co-MoSx catalysts at different MoSx concentrations. (d) The dependence of
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AQY for H2 evolution over ErB sensitized ATP/Co-MoSx catalyst on the wavelength of incident
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light, 0.05 mM MoSx. Reaction conditions: 100 mL TEOA solution, 10%, pH 8; ErB, 0.2 mM; 30-
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W LED lamp, λ≥450 nm.
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Figure 3. (a) XRD pattern of free MoSx and ATP/Co-MoSx catalysts. (b-d) TEM and HRTEM
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images of (b) free MoSx (c) ATP/MoSx, and (d, e) ATP/Co-MoSx catalysts. The inset in panel (c)
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is the corresponding SAED pattern. (f) HADDF-STEM image and corresponding Co, Mo, and S
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element mappings of ATP/Co-MoSx catalyst.
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Figure 4. High-resolution XPS spectra of (a) Co 2p core level for ATP/Co-MoSx catalyst and
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ATP/Co(OH)2 hybrid. (b) Mo 3d and (c) S 2p core levels for ATP/Co-MoSx and free MoSx
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catalysts.
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Figure 5. The stability of photocatalytic H2 evolution over ATP/Co-MoSx and free MoSx catalysts
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from ErB-TEOA system. Reaction conditions: 100 mL TEOA solution, 10%, pH 8; ErB, 0.2 mM;
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30-W LED lamp, λ≥450 nm.
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Table 1 The fitting results of XPS spectra of Co 2p, Mo 3d, and S 2p core levels for
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ATP/Co(OH)2 hybrid, free MoSx catalyst, and ATP/Co-MoSx catalyst. Sample MoIVSx 3d5/2 (3d3/2) (eV) MoVOSx 3d5/2 (3d3/2) (eV) MoVIO3 3d5/2 (3d3/2) (eV) Co2+ 2p3/2 (2p1/2) (eV) “CoMoS” 2p3/2 (2p1/2) (eV) (S2)22p3/2 (2p1/2) (eV) S22p3/2 (2p1/2) (eV) Sulfate 2p3/2 (2p1/2) (eV) S/Mo ratio Co/Mo ratio
ATP/Co(OH)2 -
781.12 (797.26)
Free MoSx 228.53 (231.63) 62.4% 229.83 (232.93) 20.1% 232.33 (235.43) 17.5% -
-
-
-
162.89 (164.09) 48.7% 161.29 (162.49) 47.6% 167.65 (168.85) 3.7% 2.97 -
-
-
ATP/Co-MoSx 228.71 (231.81) 42.4% 229.90 (233.00) 29.4% 232.09 (235.19) 28.2% 781.99 (797.34) 58.5% 779.29 (794.69) 41.5% 163.10 (164.30) 32.8% 161.61 (162.81) 56.9% 167.78 (168.97) 10.3% 2.97 0.70
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Figure 1.
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200 0
0
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0
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ATP/Co-MoSx
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Co-MoSx
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Co(OH)2/MoSx mixture
ATP/Co-MoSx
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ATP/Co(OH)2/(NH4)2S
ATP/MoSx
ATP/Co(OH)2
Free MoSx
400
150
ATP/MoSx
600
(b)
Free MoSx
H2 evolution (mol )
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ATP+(NH4)2S
(a)
ATP
-1
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Average H2 evolution rate (mol h )
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time (min)
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300 250
(c)
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Free MoSx ATP/Co-MoSx
(d)
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AQE (%)
-1
Average H2 evolution rate (mol h )
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30 20
12 10
8 4 0
0.01
0.05
0.1 [MoSx] (mM)
0.3
0.5
0
450
475
500
520
550
600
Wavelength (nm)
Figure 2.
5 6 7 8 9 10 11
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Figure 3.
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(a)
ATP/Co-MoSx-Co2p
"CoMoS" Co 2p3/2
"CoMoS" Co 2p1/2 "CoMoS" Sat.
(b)
(c)
(2-)
S 2s (2-) S2 2s
ATP/Co-MoSx-Mo3d
ATP/Co-MoSx-S2p
(2-)
S 2p (2-) S2 2p Sulfate
4+
Mo 3d 5+ Mo 3d 6+ Mo 3d
"CoMoS" Sat.
2+
Co Sat. Co2+ 2p 1/2 2+
Co Sat. 2+
Co 2p3/2 MoSx-S2p
MoSx-Mo3d
2+
ATP/Co(OH)2-Co2p
Co 2p3/2
2+
Co 2p1/2
2+
Co Sat.
2+
Co Sat.
815 810 805 800 795 790 785 780 775 770 240
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Binding energy (eV)
236
232
228
224
220170
Binding energy (eV)
168
166
164
162
160
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Binding energy (eV)
Figure 4.
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1000 ATP/Co-MoSx Free MoSx
800
H2 evolution (mol )
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nd
rd
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th
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400 200 0
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st
1
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time(h)
Figure 5.
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