Origin of Visible Light Photocatalytic Activity of Ag3AsO4 from First-Principles Calculation
Hindawi Publishing Corporation
International Journal of Photoenergy
Volume 2014, Article ID 639509, 5 pages
http://dx.doi.org/10.1155/2014/639509
Research Article
Origin of Visible Light Photocatalytic Activity of
Ag3AsO4 from First-Principles Calculation
Yan Gong, Hongtao Yu, and Xie Quan
Key Laboratory of Industrial Ecology and Environmental Engineering of Ministry of Education, School of
Environmental Science and Technology, Dalian University of Technology, Dalian 116024, China
Correspondence should be addressed to Xie Quan;
Received 12 December 2013; Revised 18 February 2014; Accepted 4 March 2014; Published 21 May 2014
Academic Editor: Yuexiang Li
Copyright © 2014 Yan Gong et al. This is an open access article distributed under the Creative Commons Attribution License, which
permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
Recently a novel sliver oxide Ag3 AsO4 has been found to be an excellent photocatalyst with strong oxidation capability for pollutant
degradation under visible light. But the origin of its high visible light photocatalytic activity was unclear which hindered further
research of Ag3 AsO4 . For clarifying that, the electronic structure and optical properties of Ag3 AsO4 have been analyzed by the
hybrid density functional method. The results reveal that the Ag3 AsO4 presents a narrow band gap with strong oxidation ability of
the valence bands maximum edge and the highly delocalized charge distribution of the conduction bands minimum is beneficial for
the carriers transfer to surface to participate in the photocatalytic reaction. These results provide clear explanations of the excellent
visible light photocatalytic performance of the Ag3 AsO4 from microscopic aspect. And it is significant to design novel materials
with high photocatalytic performance.
1. Introduction
Semiconductor photocatalysts are finding increasing applications in high-efficiency solar cells [1], water/air purification
[2], and water splitting [3, 4]. For the purpose of effectively
utilizing solar energy, ideal semiconductor photocatalysts
should at least have the two characteristics. One important
aspect is a narrow band gap for utilizing the visible light
which dominates 43% of the solar light and almost 100% of
indoor light. The other one is a suitable band edge position for
water splitting and environment pollutants decomposition
or other target reactions. In the past decades, overwhelming
attention has focused on designing visible-light response
photocatalysts, such as BiVO4 [5], CdS [6], and WO3 [7].
However, their low visible-light photocatalytic activity is
of course a great inhibition to use as a highly efficient
photocatalysts.
Since Yi’s group has reported the strong oxidation power
of Ag3 PO4 under visible light [8], a series of sliver based
oxides has aroused wide attention on account of their excellent photocatalytic abilities under visible light region, such as
Ag3 VO4 [9], AgSbO3 [10], and Ag2 O [11]. Among them, as a
novel sliver oxide photocatalyst, Ag3 AsO4 , has been found to
be an excellent photocatalyst with powerful oxidation ability
under visible light by Tang’s group recently [12]. It has a band
gap of 1.6 eV which can fulfill the high absorption capacity
of visible light. And the potential of valence band edge
is about 2.22 eV that the photogenerated holes own strong
oxidation to decompose the pollutants efficiently. Despite
important insight being achieved, the mechanisms involved
in photocatalysis are not yet clear. Fulfilling this goal requires
the assistance of theoretical investigations such as electronic
structure calculations. Therefore, a systemic investigation
about microscopic mechanism of photocatalysis is vitally
important for understanding the excellent photocatalytic
performance of Ag3 AsO4 .
To understand the superior photocatalytic activity of
Ag3 AsO4 from its intrinsic properties, the first-principles
calculations on its electronic structure and optical properties
were carried out in our work. As a common problem, the
band gaps of the semiconductors are usually underestimated by the conventional DFT methods due to the selfinteraction error as well as the missing discontinuity in the
exchange-correlation potential. For instance, the band gap
error exceeds 2 eV for ZnO [13, 14] and Ag3 PO4 [15]. This is
adverse to analysis of the redox ability of the semiconductor.
2
The hybrid-DFT with PBE0 formalism has been successfully
used as an available method to calculate the band gap
accurately, such as Ag3 PO4 [16]. So in our work, the hybridDFT method PBE0 was applied to calculate the electronic
structures and optical properties. The results revealed that
the hybrid-DFT method is more precise for the calculation of
the electronic and band structures of Ag3 AsO4 . Furthermore,
we analyzed the relations of these microscopic factors to
photocatalytic activities of Ag3 AsO4 .
International Journal of Photoenergy
while the interaction between silver and oxygen is formed
mainly by ionic bond. Previous study showed that the short
Ag–Ag distance results in the formation of the metallic Ag–
Ag bond, which contributes to the dispersive conduction
bands and a small effective mass of electron [20]. The length
of Ag–Ag bond is 3.112 Å which is much smaller than that
in Ag2 O (3.30 Å) and AgNbO3 (3.90 Å), but a little larger
than AgPO3 (2.95 Å). So the shorter Ag–Ag distance in
the Ag3 AsO4 indicates the metallic Ag–Ag bond which has
remarkable influence of the band structure of the Ag3 AsO4 .
2. Computational Methods
In this paper, our first-principles calculations were performed using the plane-wave pseudopotential method based
on hybrid-DFT with PBE0 formalism, which was implemented in the CASTEP code [17]. Three-dimensional periodic boundary conditions were employed to simulate an
infinite solid. The generalized gradient approximation (GGA)
in the PBE0 hybrid functional formalism was applied combined with norm-conserving pseudopotentials. To achieve
the accurate density of the electronic states, a 4 × 4 ×
4 Monkhorst-Pack grid [18] was used for Brillouin-zone
sampling. A plane-wave basis set with a cutoff of 400 eV
was used. Geometric optimization was achieved and the
convergence criterion for the force between atoms was 3 ×
10−2 eV/Å, the maximum displacement was 1 × 10−3 Å, and the
total energy and the maximal stress were 1 × 10−5 eV/atom and
5 × 10−2 GPa, respectively. The self-consistent convergence
accuracy was set at 1.0 × 10−6 eV/atom, and the valence
configurations of the pseudopotentials are 4d10 5s1 for Ag,
4s2 4p3 for As, and 2s2 2p4 for O, respectively.
3. Results and Discussion
3.1. Geometry Structure and Bonding Character. The geometry optimization crystal structure of Ag3 AsO4 is a cubic
structure with P4-3n symmetry which is shown in Figures
1(a) and 1(b). Figure 1(b) presents the polyhedron configurations of the Ag3 AsO4 . It clearly shows that both the (...truncated)