Abstract:Directing
single atoms (SAs) to occupy specific lattice sites in
support materials and correlating the resulting changes in atomic
coordination structures to catalytic activity are crucial for the
rational design of high-performance single-atom catalysts (SACs).
Herein, for the same copper (Cu) SAs, two coordination structures
on 1T-phase molybdenum disulfide (MoS2) are identified.
In the adsorption model, Cu SAs are coordinated onto the outermost
sulfur (S) plane in a trigonal pyramidal geometry (Cuads@MoS2),… Show more
“…As expected, the Tafel slope of CS‐2 (201 mV dec −1 ) was smaller than SnO 2 (229 mV dec −1 ) and g‐C 3 N 4 (211 mV dec −1 ), revealing that the sluggish hydrogen evolution kinetics had been significantly accelerated after the heterojunction formed (Figure S14c , Supporting Information). [ 52 , 53 , 54 ] The photoelectrochemical performances of other composite samples were also compared to illustrate the effect of g‐C 3 N 4 content. The CS‐2 showed the highest current density among three composites.…”
The identity of charge transfer process at the heterogeneous interface plays an important role in improving the stability, activity, and selectivity of heterojunction catalysts. And, in situ irradiation X-ray photoelectron spectroscopy (XPS) coupled with UV light optical fiber measurement setup is developed to monitor and observe the photoelectron transfer process between heterojunction. However, the in-depth relationship of binding energy and irradiation light wavelength is missing based on the fact that the incident light is formed by coupling light with different wavelengths. Furthermore, a quantitative understanding of the charge transfer numbers and binding energy remains elusive. Herein, based on the g-C 3 N 4 /SnO 2 model catalyst, a wavelength-dependent Boltzmann function to describe the changes of binding energy and wavelength through utilizing a continuously adjustable monochromatic light irradiation XPS technique is established. Using this method, this study further reveals that the electrons transfer number can be readily calculated forming an asymptotic model. This methodology provides a blueprint for deep understanding of the charge-transfer rules in heterojunction and facilitates the future development of highly active advanced catalysts.
“…As expected, the Tafel slope of CS‐2 (201 mV dec −1 ) was smaller than SnO 2 (229 mV dec −1 ) and g‐C 3 N 4 (211 mV dec −1 ), revealing that the sluggish hydrogen evolution kinetics had been significantly accelerated after the heterojunction formed (Figure S14c , Supporting Information). [ 52 , 53 , 54 ] The photoelectrochemical performances of other composite samples were also compared to illustrate the effect of g‐C 3 N 4 content. The CS‐2 showed the highest current density among three composites.…”
The identity of charge transfer process at the heterogeneous interface plays an important role in improving the stability, activity, and selectivity of heterojunction catalysts. And, in situ irradiation X-ray photoelectron spectroscopy (XPS) coupled with UV light optical fiber measurement setup is developed to monitor and observe the photoelectron transfer process between heterojunction. However, the in-depth relationship of binding energy and irradiation light wavelength is missing based on the fact that the incident light is formed by coupling light with different wavelengths. Furthermore, a quantitative understanding of the charge transfer numbers and binding energy remains elusive. Herein, based on the g-C 3 N 4 /SnO 2 model catalyst, a wavelength-dependent Boltzmann function to describe the changes of binding energy and wavelength through utilizing a continuously adjustable monochromatic light irradiation XPS technique is established. Using this method, this study further reveals that the electrons transfer number can be readily calculated forming an asymptotic model. This methodology provides a blueprint for deep understanding of the charge-transfer rules in heterojunction and facilitates the future development of highly active advanced catalysts.
“… 37 Li et al reported the ability to enhance the HER performance of 1T-MoS 2 by either substituting lattice sites with copper (Cu) SAs or adsorbing Cu SAs along the 1T-MoS 2 basal plane. 38 Each of these methods of stabilizing Cu SAs was achieved by employing syringe injection and hydrothermal synthetic methods, respectively. Meanwhile, in a volcano plot reported by Deng et al, Zn demonstrated a Δ G H* value near 0 eV, indicating that it is one of the few nonprecious metals that may be able to modify the HER activity of MoS 2 .…”
Section: Introductionmentioning
confidence: 99%
“…Huang et al discovered that hydrothermally synthesizing 1T-MoS 2 with Fe, Co, and Ni enhances HER activity in alkaline media by doping the guest metals into the 1T-MoS 2 lattice in a 1:6 X:Mo ratio (X = Fe, Co, or Ni) . Li et al reported the ability to enhance the HER performance of 1T-MoS 2 by either substituting lattice sites with copper (Cu) SAs or adsorbing Cu SAs along the 1T-MoS 2 basal plane . Each of these methods of stabilizing Cu SAs was achieved by employing syringe injection and hydrothermal synthetic methods, respectively.…”
Active sites are atomic sites within catalysts that drive
reactions
and are essential for catalysis. Spatially confining guest metals
within active site microenvironments has been predicted to improve
catalytic activity by altering the electronic states of active sites.
Using the hydrogen evolution reaction (HER) as a model reaction, we
show that intercalating zinc single atoms between layers of 1T-MoS2 (Zn SAs/1T-MoS2) enhances HER performance by decreasing
the overpotential, charge transfer resistance, and kinetic barrier.
The confined Zn atoms tetrahedrally coordinate to basal sulfur (S)
atoms and expand the interlayer spacing of 1T-MoS2 by ∼3.4%.
Under confinement, the Zn SAs donate electrons to coordinated S atoms,
which lowers the free energy barrier of H* adsorption–desorption
and enhances HER kinetics. In this work, which is applicable to all
types of catalytic reactions and layered materials, HER performance
is enhanced by controlling the coordination geometry and electronic
states of transition metals confined within active-site microenvironments.
“…However, since the catalytically active sites of MoS 2 are usually located in a few edge positions, resulting in catalytic inertness at most of the exposed sites, which also leads to its low catalytic activity. 15 Besides, severe aggregation and unsatisfactory electrical conductivity further hinder the enhancement of HER activity. 16 Therefore, there is an urgent need to find out how the activity of the base surface can avoid aggregation and enhance conductivity.…”
Section: Introductionmentioning
confidence: 99%
“…(2) Many 2D materials themselves are good electrocatalysts for HER, such as molybdenum disulfide (MoS 2 ). However, since the catalytically active sites of MoS 2 are usually located in a few edge positions, resulting in catalytic inertness at most of the exposed sites, which also leads to its low catalytic activity . Besides, severe aggregation and unsatisfactory electrical conductivity further hinder the enhancement of HER activity .…”
A green process to produce an efficient and inexpensive
electrocatalyst
toward hydrogen evolution reaction (HER) is of importance for hydrogen
energy. Here, an efficient HER electrocatalyst is made by electrochemically
depositing Co2P quantum dots (QDs) on MoS2-carbon
cloth (Co2P QDs/MoS2-CC). Due to the MoS2 porous structure, ∼3 nm Co2P QDs uniformly
deposit on MoS2. The produced unique 3D-structured Co2P QDs/MoS2-CC not only prevents an agglomeration
of the active material and improves the diffusion rate of H2 but also renders large accessible surface area and hierarchical
pores for high-density reaction sites and enhanced mass transport
rate. Experimental results and theoretical analysis of this unique
heterostructure indicate that the evolution process of hydrogen is
dominated by proton adsorption, and the introduction of sufficient
edge active sites can significantly promote the HER. As a consequence,
the hierarchical Co2P QDs/MoS2-CC electrocatalyst
affords an ultra-low overpotential (41 mV at a current density of
10 mA cm–2) that ranks the best among all reported
MoS2 HER catalysts and exhibits excellent durability in
1 M KOH solutions, thus holding great promise for the practical application
while shedding on fundamentals to nanoengineering an efficient electrocatalyst.
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