Theoretical and experimental investigation of highly photocatalytic performance of CuInZnS nanoporous structure for removing the NO gas
Graphical abstract
Introduction
Environmental issues caused by organic contaminants and noxious gases have attracted increasing attention, and, particularly, the removing of the NO poisonous gas is currently an intensively studied topic. Among various technologies to solve this problem, photocatalytic degradation of NO under visible-light irradiation is considered to be a very promising one [1], [2], [3], [4]. A central issue for this approach is to find suitable photocatalysts, which should be highly efficient, environment-friendly, and of low fabrication cost.
Roughly speaking, three major categories of photocatalysts have been widely studied for degrading air pollutants. First, TiO2 in the form of nanoparticles is the most intensively studied system so far [5]. The efficiency of these materials is, however, largely restricted by their bandgap (Eg = 3.2 eV), which is too wide for an effective utilization of visible-light [6]. In addition, TiO2 nanoparticles tend to aggregate, resulting in a reduction of surface area and thereby a degradation of photocatalytic efficiency [6]. Second, binary CdS, CdSe, and PbS also have high photocatalytic performances. Their practical applications are, however, strongly limited because of the toxic constituent elements such as Hg, Cd, and Pb [7]. Finally, noble metal doping, copolymerization, and semiconductor coupling have been proposed as alternative efficient approaches with, however, some restrictions for their practical applications [8], [9], [10], [11], [12], [13], [14], [15]. For example, although MoS2-g-C3N4 nanocomposites have a good photocatalytic performance, its wide usage is hindered by the high cost associated with its fabrication process (i.e., constructing of a heterostructure with MoS2) [16].
Recently, I–III–VI2 (I = Cu, Ag; III = Al, Ga, In; VI = S, Se, Te) ternary chalcopyrites (e.g., AgInS2 [17], [18], [19], [20], [21], [22], [23] and CuInS2 [24], [25], [26], [27]) are widely investigated for their possibilities as alternative candidates. One great advantage of those materials is that their electronic and optical properties can be readily optimized or tuned due to their structural complexity and flexibility [28], [29]. Furthermore, those materials can be mixed with binary zincblendes (e.g., ZnS and ZnSe), leading to ternary-binary solid solutions with an even greater space for materials designing and they often have improved performances. For example, the fundamental property of optical band gap, which is relevant to various optoelectronic applications including the photocatalytic, is adjustable between 1.02 eV and 3.49 eV for the Ag(Cu)InS2-ZnS solid solution [30]. For the photocatalytic properties, the CuInS2-ZnS (CIZS hereafter) compounds were found to have a high activity for water splitting under visible-light irradiation [31], [32], [33], [34]. Another advantage of those systems is that all their constituent elements can be non-toxic, earth-abundant, and very cheap.
Considering the great advantages of the ternary-binary compounds for water splitting, they are very promising to be advanced photocatalysts for degrading poisonous gases as well. Related reports are, however, unavailable so far. In this paper, we combine theoretical and experimental approaches to study the photocatalytic performance of CIZS for degrading NO poisonous gas under visible-light irradiation. Since the performance of a photocatalyst material is closely related to its fundamental electronic and optical properties, we first carry out corresponding theoretical predictions using first-principle approaches. The photocatalytic performance of a real sample is also strongly influenced by the morphology. Therefore, we synthesize CIZS nanospheres with nanoporous structures in order to generate large reaction surfaces, enhance the transport ability of photon-excited carriers, and avoid particle polymerization. Our CIZS samples have a high ratio of 47.71% for degrading NO, indicating a great potential for industrial applications.
Section snippets
Computational details
Because Cu+ (0.74 Å), In3+ (0.76 Å), and Zn2+ (0.74 Å) have similar radii, the occupation sites of these ions can be random in a real sample. Therefore, we use the special quasirandom structure (SQS) [35] to theoretically simulate the random occupation of Cu+, In3+, and Zn2+ (0.74 Å) ions in CIZS solid solutions. Four supercells with 64 atoms (i.e., Cu2In2Zn28S32, Cu4In4Zn24S32, Cu6In6Zn20S32, and Cu8In8Zn16S32) are constructed with increasing Cu concentrations. X-ray diffraction (XRD) patterns
Material properties of the CIZS compounds for photocatalytic application
Crystallization quality of a photocatalyst can influence its photocatalytic performance since high crystalline structures are required for a fast separation of photon-excited carriers. We select CuInS2 and ZnS for the formation of CIZS solid solutions because (1) the two constituting compounds are built with MS4 (M = Cu, In, Zn) tetrahedron blocks and (2) the Cu+ (r = 0.74 Å), In3+ (0.76 Å), and Zn2+ (0.74 Å) ions have very similar radii. Therefore, a strong random occupation of the cation
Conclusions
In this work, CuInS2-ZnS (CIZS) solid solutions in the form of nanosphere with nanoporous structures are used as a photocatalyst for degrading NO poisonous gas. Both theoretical and experimental investigations found that CIZS can form high-quality crystalline structures, which is beneficial to the transport of photon-excited carriers. In our experiments, we effectively tune the optical absorption ability and the band gap of CIZS compounds, which are primarily determined by Cu-3d valence states
Acknowledgment
This work is financially supported by Fundamental & Advanced Research Key Project of Chongqing (cstc2017jcyjBX0054), Fundamental & Advanced Research Key Project of Chongqing (cstc2015jcyjB0628), and National Natural Science Foundation of China-Emergency Treatment Project (21642013).
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