Facile one-pot synthesis of flower-like AgCl microstructures and enhancing of visible light photocatalysis
© Li et al.; licensee Springer. 2013
Received: 26 June 2013
Accepted: 13 October 2013
Published: 24 October 2013
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© Li et al.; licensee Springer. 2013
Received: 26 June 2013
Accepted: 13 October 2013
Published: 24 October 2013
Flower-like AgCl microstructures with enhanced visible light-driven photocatalysis are synthesized by a facile one-pot hydrothermal process for the first time. The evolution process of AgCl from dendritic structures to flower-like octagonal microstructures is investigated quantitatively. Furthermore, the flower-like AgCl microstructures exhibit enhanced ability of visible light-assisted photocatalytic degradation of methyl orange. The enhanced photocatalytic activity of the flower-like AgCl microstructure is attributed to its three-dimensional hierarchical structure exposing with  facets. This work provides a fresh view into the insight of electrochemical process and the application area of visible light photocatalysts.
The semiconductor-mediated photocatalytic decomposition of organic pollutions in the environment has attracted much attention  because of the abundant available solar resources and the minimum requirements of carbon footprint generated. Among the various semiconductor photocatalysts, TiO2 is the most extensively employed photocatalyst, owing to its high photocatalytic activity, good chemical stability, non-toxicity, and low cost. However, TiO2 absorbs only ultraviolet light, which accounts for only 4% of the total sunlight. Since about 48% of sunlight is visible light, it is strongly important to develop the photocatalysts which are active and effective under visible light.
As a well-known material used for photographic film, AgCl has shown its valuable applications as visible light photocatalysts [2–8]. AgCl is a stable photosensitive semiconductor material with a direct band gap of 5.15 eV and an indirect band gap of 3.25 eV. Although the intrinsic light response of AgCl is located in the ultraviolet region as well, once AgCl absorbs a photon, an electron-hole pair will be generated and subsequently, the photogenerated electron combines with an Ag+ ion to form an Ag atom . Finally, a lot of silver atoms are formed on the surface of the AgCl, which could extend the light response of AgCl into the visible light region [1, 6, 7].
Besides, the morphology of AgCl has significant influence on its photocatalytic activity, so it is important to develop facile methods to synthesize size- and shape-controlled AgCl materials. Recently, the facile hydrothermal method is employed to synthesize variable micro-/nano-AgCl structures, including AgCl nanocubes , cube-like Ag@AgCl , and even near-spherical AgCl crystal by an ionic liquid-assisted hydrothermal method . However, for AgCl microcrystals, this narrow morphology variation (simply varied from near-spherical to cubical [2–7]) inspired that more particular attention is deserved to pay on the novel AgCl morphologies, including the synthesis methods and their generation mechanisms, even the possible morphology evolution processes.
Herein, the novel flower-like AgCl microstructures similar to PbS crystals  are synthesized by a facile hydrothermal process without any catalysts or templates. Also, a series of AgCl morphology evolution processes are observed. Flower-like structures are recrystallized after the dendritic crystals are fragmentized, assembled, and dissolved. The detailed mechanism of these evolution processes has been further discussed systemically. Furthermore, flower-like AgCl microstructures exhibited enhanced photocatalytic degradation of methyl orange under visible light.
The AgCl dendritic and flower-like structure are synthesized via hydrothermal method by reacting silver nitrate (AgNO3, 99.8%) with ethylene glycol (EG, 99%) in the presence of poly(vinyl pyrrolidone) (PVP-K30, MW = 30,000). In a typical synthesis, all the solutions are under constant stirring. Firstly, a 10-ml EG solution with 0.2 g of PVP was prepared. Then using droppers, another 7 ml of EG which contained 10 mM of AgNO3 is added. Afterwards, 3 ml of undiluted hydrochloric acid (HCl, 36% ~ 38%) is added into this mixture. The mixed AgNO3/ PVP/HCl/EG solution is further stirred for several minutes until it becomes uniform. This solution is then transferred into a 25-ml Teflon-lined autoclave tube and dried in the drying tunnel at 160°C for different times. The final products are collected by centrifugation (6,000 rpm, 10 min) and washed several times with deionized water.
The electron scanning microscopy (SEM) measurements are obtained on FEI Quanta 200F microscope (FEI Company, Hillsboro, OR, USA). The X-ray powder diffraction (XRD) patterns of samples are examined by Bruker D8 focus X-ray powder diffractometer (Bruker Corporation, Billerica, MA, USA) with Cu Kα radiation at λ = 1.5406 Å. Photocatalytic degradation of organic dye methyl orange (MO) is conducted under visible light at room temperature with a prepared solution of 100 mg/L AgCl powder and 20 mg/L MO dye in a 100-ml beaker. The concentration of MO in the solution is tested with a UV-vis spectrophotometer (UNICO UV-2450; UNICO, Dayton, NJ, USA).
At the first stage, the dendritic AgCl crystal structures are composed when the reagent concentration is very high. As we know, according to the crystal growth theory, under a certain concentration, the fastest growth face would fade away earliest while the crystal was growing. Besides, AgCl crystals have preferential overgrowth along <111> and then <110> direction based on the previous work . Hence for AgCl crystal, when the reactants’ concentration are below a certain value, the  face would finally disappear and leave  face presented, thus forming cubic-faceted crystals; however, if the concentration were above the critical value, crystals would grow along  face, therefore forming dendritic crystals. This is the reason that dendritic structures are more likely to be generated during the early period while cubic structures are preferred in the subsequent period. As described in Figure 1a, we obtained dendritic crystals with the reaction time of 3 h.
Meanwhile, in Figure 1a, it can be seen that the initial dendrites are so large that their lengths expand to several hundred micrometers. However, the small branches would separate from the trunk, as many sub-branch arms showed in Figure 1b. These small branches own the same size and morphology with the sub-branch in Figure 1a. We can also observe from Figure 1a that shorter sub-dendrites are more robust and ordered than longer sub-dendrites when attached alongside the main truck. So longer side branches are more easily to fragmentize. Similar branch-breaking phenomenon has been observed in Ag dendrites . Actually, several reasons can contribute to these results. First, not only large-size dendrites create greater stress in the connections between sub-branches and the trunk, but also a larger branch distance decreases the interactions among each sub-branch. Additionally, a high growth speed is inclined to compound-multiply twinned dendrites which are more active and impressionable to be modified. As a whole, all of these are immersed in heat convection surroundings that create a flowing condition for branch fragment.
After the first stage, the crystal growth model of AgCl changes due to the reduction of reagent concentration to a certain value. Then cubic-faceted crystals are easier to synthesize than dendritic crystals. The new growing cubic and original dendritic crystals would integrate into assembled dendrites in Figure 1c. In the process, we find that all the dendrites are well organized with three faces of sub-branches, owing to the specific AgCl crystal structure as shown in Figure 2a,b. From the insert images in Figure 2c, we can see that the sub-branch dendritic root is plane, the surface is the  face. Thus, during the formation of a cubic structure, there is a period that the eight  faces are exposed outside, just as shown in Figure 2c and the scheme image in Figure 2d. Because of the co-existing of two similar crystallographic orientation faces, the two faces would attach together thermodynamically in order to eliminate the pairs of high-energy surface. This is exactly the so-called oriented attachment mechanism . After the assembling of the sub-branch dendrites, ions in the solution continue to aggregate around the assembled sites to form robust AgCl-assembled dendrites (Figure 2e,f). As a result, assembled dendrites with eight branches are created, which we call octagonal dendrites, as shown in Figure 1c.
As we know, nucleating and dissolving simultaneously take place throughout the whole reaction process, and their rates changed constantly. The reagent concentration decreases as the reaction time prolonged, so the rate of nucleating becomes slow and reaches equilibrium with the dissolving rate. Basically, no extra amount of AgCl crystal is generated under this circumstance.
However, due to the extremely high concentration of HCl, a third round of instability referring to Equation 2 is underlying. So the octagonal dendrite dissolves into eight dendrites and their surface becomes smoother. Therefore, smaller smooth dendrites (20 to 30 μm compared with 50 to 60 μm before) are generated as showed in Figure 1d.
Apart from the detailed analyzing of the growth mechanism of the flower-like AgCl microstructures, the photocatalytic performance of the AgCl microstructures also has been evaluated with the decomposition of MO, under the illumination of the visible light. In fact, the decomposition of organic contaminant happened because the light-induced oxidative holes are generated around the MO molecules when the AgCl microstructures are exposed to sunlight.
Figure 5b shows the linear relationship of lnC0/C vs. time. We can see that the photocatalytic degradation of MO follows pseudo-first-order kinetics, lnC0/C = kt, where C0/C is the normalized MO concentration, t is the reaction time, and k is the pseudo-first-rate constant. The apparent photochemical degradation rate constant for the flower-like AgCl microstructure is 3.38 × 10-2 min-1, which is almost two times that for the dendritic AgCl, 1.87 × 10-2 min-1. This further confirms that flower-like AgCl microstructures exhibit higher photocatalytic efficiency. Overall, the flower-like AgCl microstructures exhibit excellent photocatalytic activity under visible light irradiation.
The enhanced photocatalytic activity of the flower-like AgCl microstructure can be attributed to their three-dimensional hierarchical structure. As we know, the morphology can affect the photocatalytic activity of photocatalysts. Three-dimensional hierarchical structures are regarded to have a higher superficial area and a greater number of active sites than either one-dimensional or two-dimensional architectures. Furthermore, for the three-dimensional flower-like octagonal crystals as shown in Figure 3b,c, all the surfaces of the steps on the petals are , , or  direction facets. And it has been demonstrated that the  facets are more reactive toward dissociative adsorption of reactant molecules compared with  facets, and crystals of exposed  facets exhibit much higher photocatalytic activity than the exposed  [13–17]. In addition, for flower-like AgCl samples, the faces mainly exposed on the petals are the  crystal facet system. Therefore, high photocatalytic efficiency is achieved for the flower-like AgCl microstructure with  facets.
In summary, flower-like octagonal AgCl microstructures with enhanced photocatalysis are synthesized by a facile one-pot hydrothermal process for the first time. We investigate the evolution process of flower-like AgCl microstructures, including dendritic crystals’ fragmentizing, assembling, dissolving, and recrystallizing. Furthermore, flower-like AgCl microstructures exhibit enhanced photocatalytic degradation of methyl orange under sunshine. It is believed that the flower-like AgCl microstructures has potential application in the degradation of organic contaminations and disinfection of water, as well as in photovoltaic cells and other optoelectronic devices.
We acknowledge the support partly from the National Natural Science Foundation of China (grant nos. 51372082, 51172069, 50972032, 61204064, and 51202067), the Ph.D. Programs Foundation of Ministry of Education of China (grant no. 20110036110006), and the Fundamental Research Funds for the Central Universities (key project 11ZG02).
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