# Polymeric Graphitic Carbon Nitride Doped with CuO Dispersed on Dealuminated Clinoptilolite (CuO/HCP): Synthesis and Characterisation

Authors: Saheed Olalekan Sanni; Omoruyi Gold Idemudia
Journal: Journal of Nanomaterials
 (2015)

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## Abstract

CuO dispersed on dealuminated clinoptilolite (CuO/HCP) and further doped with polymeric graphitic carbon nitride (CuO/HCP-g-C3N4) was synthesized through 2 facile routes: precipitation method for CuO/HCP and impregnation through ultrasonication method for the hybrid composite material. The hybrid composite material crystalline phase, surface morphology, and structural and thermal properties were investigated by X-ray diffraction (XRD), scanning electron microscopy (SEM), energy-dispersive X-ray analysis (EDAX), Fourier transform infrared spectroscopy (FTIR), and thermal analysis. The formation of the hybrid composite material was confirmed by XRD showing crystalline phase of CuO and g-C3N4 present on the surface of dealuminated clinoptilolite (HCP). SEM images analysis depicts no aggregation of the mixed metal oxide semiconductor nanoparticles at the center of HCP. The hybrid composite material, CuO/HCP-g-C3N4, with a good homogeneously dispersed metal oxide conductor having excellent catalytic activities has been synthesized.


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## Body

## 1. Introduction

The development of efficient, sustainable, stable, and alternative novel titania based photocatalytic materials, with visible light absorption, has gained a lot of research interest. A host of new metal oxide semiconductor which found application in environmental remediation consisting of CaIn2O4 [1], NaTaO3 [2], BaTi4O9 [3], InTaO4 [4], BiVO4 [5–7], CdS [8], and Bi2WO6 [9] has been extensively studied as a new series of photocatalyst. Cupric oxide (CuO), a p-type metal oxide semiconductor with a narrow band gap of 1.36 eV, that is inexpensive and nontoxic in nature, is another alternative metal oxide semiconductor used as TiO2 based photocatalyst. CuO has found huge potential application in optical electronics, gas sensing [10], field emission emitters [11], lithium ion batteries [12], photovoltaic materials, and catalytic material [13, 14]. Studies revealed that the fabrication of CuO on mesoporous based material such as graphene [15], titania nanotubes [16], and clinoptilolite [17] results in strong interaction between CuO and these mesoporous materials. This interaction results in the efficient transfer of photogenerated electrons from CuO conduction band to the mesoporous material, which invariably suppress recombination rate of photogenerated electron-hole pairs. CuO presence on these mesoporous materials surface allows efficient charge separation and the mesoporous materials promote electron migration, which aids enhanced photocatalytic activities and water splitting effectively.Polymeric graphitic carbon nitride (g-C3N4), a “metal free” n-type metal oxide semiconductor with band gap of 2.8 eV, has shown immense properties for H2 or O2 evolution via water splitting and good chemical stability in photocatalysis [18, 19]. Several studies have employed polymeric carbon nitride alone in degradation of organic contaminant [20] under visible light irradiation. Though inefficient separation of photogenerated electron-hole pairs impairs the potential application of g-C3N4, several attempts have been carried out to improve overall performance of g-C3N4 for enhanced photocatalytic activities under visible light irradiation. The combination of g-C3N4 with other novel metal oxide semiconductors, mesoporous material, and polymer or as a nanocomposite has greatly enhanced organic contaminant removal and H2 evolution in water splitting, respectively [20–22]. Studies have also showed the combination of different metal oxide semiconductors with distinct energy levels and dispersion of these mixed photocatalysts on these mesoporous materials surface assist in charge separation of electron-hole pair under visible light irradiation which enhances photocatalytic activity effectively [23–26].Clinoptilolite (CP), a cheap and natural form of zeolite, has found wide application for the dispersion of nanoparticles due to its exceptional chemical composition [27, 28], ion exchange, and surface properties, and it is employed as our mesoporous material in this study. Dealuminated clinoptilolite (HCP) with large surface area acts as excellent support material to disperse metal oxide conductor [27, 28] which invariably facilitates movement of photogenerated electrons and efficient separation within the composite material. Presented here is the facile synthesis of g-C3N4-CuO/HCP composite material, and the structural, morphological, thermal, and optical properties of prepared composite were characterized using Fourier transform infrared (FTIR) spectroscopy, X-ray diffraction (XRD), scanning electron microscopy (SEM), energy dispersive spectroscopy (EDS), and thermal analysis. The photocatalytic reaction mechanism for the hybrid photocatalyst is also proposed, to throw some light on their potential application stability and photocatalytic activities on organic pollutants.


## 2. Experimental

### 2.1. Synthesis of Dealuminated Clinoptilolite (HCP), CuO/HCP, and CuO/HCP-g-C3N4

The preparation of dealuminated clinoptilolite (HCP) has been discussed and highlighted in our previous studies [27, 28]. For copper oxide dispersed on dealuminated clinoptilolite, stoichiometric amount of CuCl2 was added to ethanol solution and allowed to continue stirring; to this stirring solution HCP was later added. This was followed by the addition of an appropriate amount of oxalic acid solution (chelating agent) to precipitate CuO on the surface of HCP and the solution further subjected to heating at 80°C for 5 hr. The obtained homogenous solution was further filtered and washed well with ethanol and water mixture to remove any impurities present. The final product was air-dried in the oven overnight (60°C) and further calcined at 300°C for 2 hr. The same preparation route was applied for CuO synthesis without the addition of HCP.Metal free g-C3N4 were prepared by thermal calcination of thiourea placed inside cover alumina crucible in a muffle furnace, which was calcined to 550°C and the products were collected after the heated crucible was cooled to room temperature. Polymeric graphitic nitride doped with CuO/HCP was prepared via a facile impregnation via ultrasonication route, by adding CuO/HCP to g-C3N4 dissolved in ethanol solution and the mixture was further allowed to ultrasonicate for 30 minutes. The resulting solution was filtered and washed well with distilled water and ethanol to remove any impurities present in the hybrid composites. The material was dried in the oven at 80°C and stored in the dark before elucidation of physical and chemical properties.


### 2.2. Characterization of the Hybrid Composite Material

The surface morphology of the samples was examined using scanning electron microscopy equipped with an EDAX system for energy dispersive spectroscopic analysis, which was coated with a thin layer of gold film to avoid charging. Powder X-ray diffraction patterns were examined using Bruker diffractometer AXS with Cukα source. The bond vibrations were analyzed on Fourier transform infrared (FTIR) spectrophotometer (Perkin Elmer spectrum 400) and the FTIR spectra were in the range of 600–4000 cm−1. Thermogravimetric analysis (TGA) was carried out using Perkin Elmer STA 6000 thermal simultaneous analyzer at heating rate of 10°C/min from 30 to 900°C under 19.8 mL/mins in nitrogen purge stream.


## 2.1. Synthesis of Dealuminated Clinoptilolite (HCP), CuO/HCP, and CuO/HCP-g-C3N4

The preparation of dealuminated clinoptilolite (HCP) has been discussed and highlighted in our previous studies [27, 28]. For copper oxide dispersed on dealuminated clinoptilolite, stoichiometric amount of CuCl2 was added to ethanol solution and allowed to continue stirring; to this stirring solution HCP was later added. This was followed by the addition of an appropriate amount of oxalic acid solution (chelating agent) to precipitate CuO on the surface of HCP and the solution further subjected to heating at 80°C for 5 hr. The obtained homogenous solution was further filtered and washed well with ethanol and water mixture to remove any impurities present. The final product was air-dried in the oven overnight (60°C) and further calcined at 300°C for 2 hr. The same preparation route was applied for CuO synthesis without the addition of HCP.Metal free g-C3N4 were prepared by thermal calcination of thiourea placed inside cover alumina crucible in a muffle furnace, which was calcined to 550°C and the products were collected after the heated crucible was cooled to room temperature. Polymeric graphitic nitride doped with CuO/HCP was prepared via a facile impregnation via ultrasonication route, by adding CuO/HCP to g-C3N4 dissolved in ethanol solution and the mixture was further allowed to ultrasonicate for 30 minutes. The resulting solution was filtered and washed well with distilled water and ethanol to remove any impurities present in the hybrid composites. The material was dried in the oven at 80°C and stored in the dark before elucidation of physical and chemical properties.


## 2.2. Characterization of the Hybrid Composite Material

The surface morphology of the samples was examined using scanning electron microscopy equipped with an EDAX system for energy dispersive spectroscopic analysis, which was coated with a thin layer of gold film to avoid charging. Powder X-ray diffraction patterns were examined using Bruker diffractometer AXS with Cukα source. The bond vibrations were analyzed on Fourier transform infrared (FTIR) spectrophotometer (Perkin Elmer spectrum 400) and the FTIR spectra were in the range of 600–4000 cm−1. Thermogravimetric analysis (TGA) was carried out using Perkin Elmer STA 6000 thermal simultaneous analyzer at heating rate of 10°C/min from 30 to 900°C under 19.8 mL/mins in nitrogen purge stream.


## 3. Results and Discussion

### 3.1. Morphology and Elemental Properties

The surface morphology of CuO, CuO/HCP, and g-C3N4 and the hybrid composite material (CuO/HCP-g-C3N4) nanostructure were observed using scanning electron microscopy (SEM) at the same resolutions. The materials (CuO, g-C3N4, and CuO/HCP) show partial particle aggregation or agglomeration as depicted in Figure 1, with very good homogeneous particle size and shape distribution within the texture of the materials synthesized. Dealuminated clinoptilolite acts as capping agent or stabilizer, which hampers excessive growth of the metal oxide semiconductors within the hybrid composite material. However, upon doping of CuO/HCP on g-C3N4, the hybrid material displays partial agglomeration microstructure which is attributed to pure CuO/HCP sparsely covering the surface of g-C3N4 within the hybrid composite material.SEM images of (a) CuO; (b) CuO/HCP; (c) g-C3N4; and (d) CuO/HCP-g-C3N4.
(a)
(b)
(c)
(d)The different resolutions of CuO/HCP-g-C3N4 at alternative magnifications are also depicted in Figure 2(a), there exist partial agglomeration of the CuO/HCP particle in contact with g-C3N4 surface at the center at lower magnification (Figure 2(a)). There seems to be signs of small gaps in the CuO/HCP-g-C3N4 material which can facilitate its enhanced photocatalytic activity on organic contaminants, which is ascribed to an exceptional large surface area of HCP. The large surface area of HCP can facilitate mass transfer and also provides more activity sites for surface-dependent reactions that will aid photocatalytic process for organic contaminant breakdown. However, as the magnification increases as depicted in Figures 2(b) and 2(c), irregular morphology and agglomeration begins to appear within the hybrid composite material.((a)–(c)) SEM images of CuO/HCP-g-C3N4 of different magnifications.
(a)
(b)
(c)The EDAX analysis was employed to obtain the elemental composition of prepared photocatalyst material. From Figure3, the existence of doped CuO/HCP within the framework of CuO/HCP-g-C3N4 is revealed with the composite material made up of Cu, O, Si, Al, C, and N. The elements Si, Al, and O are attributed to dealuminated clinoptilolite (HCP), Cu originated from the CuO material and C, and N is attributed to polymeric graphitic carbon nitride present within the hybrid composite materials.Figure 3
SEM image and EDAX of CuO/HCP-g-C3N4.


### 3.2. XRD Analysis

The XRD pattern of CuO/HCP-g-C3N4 is shown in Figure 4 within the 2θ range of 5 to 60°. From the XRD data, characteristic peaks of CuO are observed at 2θ values of 32.50°, 35.60°, 38.80°, 48.89°, 56.50°, and 58.80° [29, 30] which are coherent with diffraction card peak (JCPDS 073-6234). The weak diffraction card peak of g-C3N4 (JCPDS 050-1250) is observed at 2θ value of 27.74° which is tuned to characteristic interlayer stacking peak of conjugated aromatic systems in agreement with previous report [31]. The characteristic peaks observed at 9.83°, 17.30°, 23.17°, 27.50°, and 30.5° are ascribed to the clinoptilolite (CP) diffraction card peak (JCPDS 025-1349) and depict that CP is the mesoporous material employed as our support layer for dispersion of our metal oxide semiconductors. From Figure 4, diffraction peaks of CuO are more pronounced than the peak of g-C3N4 in relation to SEM results in Figure 1. The result depicts the coexistence of CuO and g-C3N4 on the surface of dealuminated clinoptilolite; it is also worthy of note that the deposition of CuO and g-C3N4 on the surface of HCP did not destroy the clinoptilolite structure.Figure 4
XRD pattern at 2θ of (a) CuO/HCP-g-C3N4 and (b) CuO/HCP.


### 3.3. Structural Properties

The FTIR spectra of g-C3N4 in Figure 5 show consistent phase broad peak at 3195 and 3300 cm−1 due to stretching modes of amine unit and intermolecular hydrogen-bond interactions. Absorption peaks at 1638, 1437, 1376, and 1273 cm−1 are ascribed to stretching modes of CN heterocycles [32, 33], while the characteristic peak of triazines unit is found at 825 cm−1 [32]. However, the FTIR spectrum of CuO/HCP shows absorption peaks at 3487 to 3350 cm−1 ascribed to stretching vibrations of –OH units present in the zeolitic water. The OH units bending absorption peak of the zeolitic water are also pronounced at 1627 cm−1, while absorption bands at between 1100 and 916 cm−1 are ascribed to internal Si–O(Si) and Si–O(Al) stretch vibrations presented in the dealuminated clinoptilolite [34, 35]. The absorption peak at 701 cm−1 is due to pseudo-lattice vibrations of –OH deformation unit and weak peaks of CuO at 1431 and 1395 cm−1 are observed in CuO/HCP. However, in the hybrid composite material, the weak peaks of CuO become broader (1445 cm−1) upon the dispersion of CuO/HCP on g-C3N4. The stretching vibrations of –OH and amine units were reduced to 3470, 3000, and 3250 cm−1, respectively, while the bending –OH unit also reduces to 1620 cm−1 in the hybrid composite material. The absorption peak of stretching modes of CN heterocycles of g-C3N4 in the hybrid composite material is also increased to 1480 cm−1. However, the pseudo-lattice vibrations of –OH deformation unit in the hybrid composite increases to 798 cm−1 and a reduction in wavenumber for internal Si–O(Si) and Si–O(Al) stretch vibrations to 1081 cm−1.Figure 5
FTIR spectra of (a) g-C3N4 (b) CuO/HCP and (c) CuO/HCP-g-C3N4.


### 3.4. Thermal Properties

Thermal gravimetric analysis of CuO/HCP and the composite material was carried out to determine their thermal decomposition behaviour, which is depicted in Figures6(a) and 6(b), respectively. However, CuO/HCP-g-C3N4 depicts exceptional thermal stability compared to CuO/HCP in overall temperature from 30 to 900°C. The peak at 153.15°C for both materials as depicted in Figure 6(a) is ascribed to elimination of physically adsorbed water from the surface [36]. However, the weight loss peak at 258.01°C (CuO/HCP) and 393.18°C (hybrid composite material) are also ascribed to exchangeable cations present in the HCP cavities and also the oxidation of volatile organic species. The weight loss at 619.33 and 695.79°C in both materials is ascribed to phase transformation of metal oxide semiconductors on the surface of dealuminated clinoptilolite. The associated mass loss of the hybrid composite material was more pronounced than CuO/HCP (Figure 6(a)) depicting successful dispersion of CuO/HCP on g-C3N4 surface; this is coherent to similar observation in SEM image result of Figure 1.(a) TGA profile of (a) CuO/HCP and (b) CuO/HCP-g-C3N4. (b) DTA profile of (a) CuO/HCP and (b) CuO/HCP-g-C3N4.
(a)
(b)Similar weight loss is noticeable with an endothermic peak in differential thermal analysis (DTA) result at 183°C for both materials (Figure6(b)) that is due to loss of zeolitic water. The broad endothermic peak is prominent at 269.81°C for CuO/HCP, while the peaks at 321.03 and 400°C for the hybrid composite material are ascribed to elimination of residual zeolitic water and higher hydroxyls groups present on the surface of dealuminated clinoptilolite. The associated mass loss of hybrid composite material (21.65%) is more than CuO/HCP (7.88%) in the TGA (Figure 6(a)), with similar observations in the DTA result in Figure 6(b). Another broad endothermic peak for both materials at 583.78°C and 676.97°C is attributed to loss of residual coordinated water and the isolated OH groups. At this temperature, decomposition becomes steady and residual materials left are copper oxide and polymeric graphitic carbide. Mass weight loss of the hybrid composite material (42.53%) was more than CuO/HCP (35.18%).


### 3.5. Photocatalytic Reaction Mechanism

A possible photocatalytic reaction mechanism hereby proposed judging from the characterization analysis which in a long run will assist in understanding the photocatalytic efficiency of the hybrid composite material on organic contaminants. In the hybrid composite material, both CuO and C3N4 metal semiconductors are in close contact and also separated by HCP. Under a visible light, the hybrid composite is excited and the generation of electron-hole pairs occurs, respectively (in the conduction and valence band), within the two different metal semiconductors. In close contact (e−) from CuO conduction band (CB) is transferred directly to g-C3N4 CB (more negative Fermi), while transfer ofh+ from g-C3N4 valance band directly to CuO VB (more positive Fermi) and there is a facilitation of electron-hole pair separation.However, in terms of separated CuO and g-C3N4 dispersed on the surface of HCP, the pathway of e transfer between the two metal semiconductors is altered due to the presence of HCP as depicted in Scheme 1. HCP possesses intrinsic properties to act as electron acceptors from the excited molecule and also as electron donor [37] invariably within the system. Heree− from CuO (CB) is transferred to HCP, where the latter facilitates interfacial charge transfers along HCP surface to g-C3N4. The same transfer of holes from g-C3N4 to CuO occurs in the presence of HCP, which results in an efficient charge separation by HCP. Also, the g-C3N4 (e−) displays good reduction ability and the CuO (h+) shows oxidizing power. The high reduction electron on the g-C3N4 (CB) reacts with molecular O2 to form superoxide anions, which invariably oxidizes the organic pollutant. The hole in the VB of CuO reacts with water to generate hydroxyl radical which degrades the pollutant effectively. The hole in VB of CuO can also break down the organic pollutants directly due to high positive potential of CuO.Scheme 1
Proposed reaction mechanism of separated electron-hole pair in CuO/HCP-g-C3N4 under visible light.Overall, HCP provides exceptional high surface area, good adsorption, and catalytic sites which favours the reaction process. HCP within the hybrid composite will act as an electron transporter, due to its high electron mobility of zeolites framework and ability to act as an electron acceptor or donor [38]. HCP in real sense acceptse− from the metal semiconductor (lower band gap) in a rapid manner and transfers thee− to other metal semiconductors (narrow band gap) and vice versa for hole transfer. In this same manner photogenerated electron-hole pairs are kept away from the metal oxide semiconductors, which invariably also reduces the recombination rate of photogenerated electron-hole pairs and improves overall catalytic activity of the hybrid composite material. The photocatalytic reaction mechanism highlighted in this study is consistent with the reported literature on the dispersion of mixed metal oxide semiconductor on mesoporous materials [23–26, 39].


## 3.1. Morphology and Elemental Properties

The surface morphology of CuO, CuO/HCP, and g-C3N4 and the hybrid composite material (CuO/HCP-g-C3N4) nanostructure were observed using scanning electron microscopy (SEM) at the same resolutions. The materials (CuO, g-C3N4, and CuO/HCP) show partial particle aggregation or agglomeration as depicted in Figure 1, with very good homogeneous particle size and shape distribution within the texture of the materials synthesized. Dealuminated clinoptilolite acts as capping agent or stabilizer, which hampers excessive growth of the metal oxide semiconductors within the hybrid composite material. However, upon doping of CuO/HCP on g-C3N4, the hybrid material displays partial agglomeration microstructure which is attributed to pure CuO/HCP sparsely covering the surface of g-C3N4 within the hybrid composite material.SEM images of (a) CuO; (b) CuO/HCP; (c) g-C3N4; and (d) CuO/HCP-g-C3N4.
(a)
(b)
(c)
(d)The different resolutions of CuO/HCP-g-C3N4 at alternative magnifications are also depicted in Figure 2(a), there exist partial agglomeration of the CuO/HCP particle in contact with g-C3N4 surface at the center at lower magnification (Figure 2(a)). There seems to be signs of small gaps in the CuO/HCP-g-C3N4 material which can facilitate its enhanced photocatalytic activity on organic contaminants, which is ascribed to an exceptional large surface area of HCP. The large surface area of HCP can facilitate mass transfer and also provides more activity sites for surface-dependent reactions that will aid photocatalytic process for organic contaminant breakdown. However, as the magnification increases as depicted in Figures 2(b) and 2(c), irregular morphology and agglomeration begins to appear within the hybrid composite material.((a)–(c)) SEM images of CuO/HCP-g-C3N4 of different magnifications.
(a)
(b)
(c)The EDAX analysis was employed to obtain the elemental composition of prepared photocatalyst material. From Figure3, the existence of doped CuO/HCP within the framework of CuO/HCP-g-C3N4 is revealed with the composite material made up of Cu, O, Si, Al, C, and N. The elements Si, Al, and O are attributed to dealuminated clinoptilolite (HCP), Cu originated from the CuO material and C, and N is attributed to polymeric graphitic carbon nitride present within the hybrid composite materials.Figure 3
SEM image and EDAX of CuO/HCP-g-C3N4.


## 3.2. XRD Analysis

The XRD pattern of CuO/HCP-g-C3N4 is shown in Figure 4 within the 2θ range of 5 to 60°. From the XRD data, characteristic peaks of CuO are observed at 2θ values of 32.50°, 35.60°, 38.80°, 48.89°, 56.50°, and 58.80° [29, 30] which are coherent with diffraction card peak (JCPDS 073-6234). The weak diffraction card peak of g-C3N4 (JCPDS 050-1250) is observed at 2θ value of 27.74° which is tuned to characteristic interlayer stacking peak of conjugated aromatic systems in agreement with previous report [31]. The characteristic peaks observed at 9.83°, 17.30°, 23.17°, 27.50°, and 30.5° are ascribed to the clinoptilolite (CP) diffraction card peak (JCPDS 025-1349) and depict that CP is the mesoporous material employed as our support layer for dispersion of our metal oxide semiconductors. From Figure 4, diffraction peaks of CuO are more pronounced than the peak of g-C3N4 in relation to SEM results in Figure 1. The result depicts the coexistence of CuO and g-C3N4 on the surface of dealuminated clinoptilolite; it is also worthy of note that the deposition of CuO and g-C3N4 on the surface of HCP did not destroy the clinoptilolite structure.Figure 4
XRD pattern at 2θ of (a) CuO/HCP-g-C3N4 and (b) CuO/HCP.


## 3.3. Structural Properties

The FTIR spectra of g-C3N4 in Figure 5 show consistent phase broad peak at 3195 and 3300 cm−1 due to stretching modes of amine unit and intermolecular hydrogen-bond interactions. Absorption peaks at 1638, 1437, 1376, and 1273 cm−1 are ascribed to stretching modes of CN heterocycles [32, 33], while the characteristic peak of triazines unit is found at 825 cm−1 [32]. However, the FTIR spectrum of CuO/HCP shows absorption peaks at 3487 to 3350 cm−1 ascribed to stretching vibrations of –OH units present in the zeolitic water. The OH units bending absorption peak of the zeolitic water are also pronounced at 1627 cm−1, while absorption bands at between 1100 and 916 cm−1 are ascribed to internal Si–O(Si) and Si–O(Al) stretch vibrations presented in the dealuminated clinoptilolite [34, 35]. The absorption peak at 701 cm−1 is due to pseudo-lattice vibrations of –OH deformation unit and weak peaks of CuO at 1431 and 1395 cm−1 are observed in CuO/HCP. However, in the hybrid composite material, the weak peaks of CuO become broader (1445 cm−1) upon the dispersion of CuO/HCP on g-C3N4. The stretching vibrations of –OH and amine units were reduced to 3470, 3000, and 3250 cm−1, respectively, while the bending –OH unit also reduces to 1620 cm−1 in the hybrid composite material. The absorption peak of stretching modes of CN heterocycles of g-C3N4 in the hybrid composite material is also increased to 1480 cm−1. However, the pseudo-lattice vibrations of –OH deformation unit in the hybrid composite increases to 798 cm−1 and a reduction in wavenumber for internal Si–O(Si) and Si–O(Al) stretch vibrations to 1081 cm−1.Figure 5
FTIR spectra of (a) g-C3N4 (b) CuO/HCP and (c) CuO/HCP-g-C3N4.


## 3.4. Thermal Properties

Thermal gravimetric analysis of CuO/HCP and the composite material was carried out to determine their thermal decomposition behaviour, which is depicted in Figures6(a) and 6(b), respectively. However, CuO/HCP-g-C3N4 depicts exceptional thermal stability compared to CuO/HCP in overall temperature from 30 to 900°C. The peak at 153.15°C for both materials as depicted in Figure 6(a) is ascribed to elimination of physically adsorbed water from the surface [36]. However, the weight loss peak at 258.01°C (CuO/HCP) and 393.18°C (hybrid composite material) are also ascribed to exchangeable cations present in the HCP cavities and also the oxidation of volatile organic species. The weight loss at 619.33 and 695.79°C in both materials is ascribed to phase transformation of metal oxide semiconductors on the surface of dealuminated clinoptilolite. The associated mass loss of the hybrid composite material was more pronounced than CuO/HCP (Figure 6(a)) depicting successful dispersion of CuO/HCP on g-C3N4 surface; this is coherent to similar observation in SEM image result of Figure 1.(a) TGA profile of (a) CuO/HCP and (b) CuO/HCP-g-C3N4. (b) DTA profile of (a) CuO/HCP and (b) CuO/HCP-g-C3N4.
(a)
(b)Similar weight loss is noticeable with an endothermic peak in differential thermal analysis (DTA) result at 183°C for both materials (Figure6(b)) that is due to loss of zeolitic water. The broad endothermic peak is prominent at 269.81°C for CuO/HCP, while the peaks at 321.03 and 400°C for the hybrid composite material are ascribed to elimination of residual zeolitic water and higher hydroxyls groups present on the surface of dealuminated clinoptilolite. The associated mass loss of hybrid composite material (21.65%) is more than CuO/HCP (7.88%) in the TGA (Figure 6(a)), with similar observations in the DTA result in Figure 6(b). Another broad endothermic peak for both materials at 583.78°C and 676.97°C is attributed to loss of residual coordinated water and the isolated OH groups. At this temperature, decomposition becomes steady and residual materials left are copper oxide and polymeric graphitic carbide. Mass weight loss of the hybrid composite material (42.53%) was more than CuO/HCP (35.18%).


## 3.5. Photocatalytic Reaction Mechanism

A possible photocatalytic reaction mechanism hereby proposed judging from the characterization analysis which in a long run will assist in understanding the photocatalytic efficiency of the hybrid composite material on organic contaminants. In the hybrid composite material, both CuO and C3N4 metal semiconductors are in close contact and also separated by HCP. Under a visible light, the hybrid composite is excited and the generation of electron-hole pairs occurs, respectively (in the conduction and valence band), within the two different metal semiconductors. In close contact (e−) from CuO conduction band (CB) is transferred directly to g-C3N4 CB (more negative Fermi), while transfer ofh+ from g-C3N4 valance band directly to CuO VB (more positive Fermi) and there is a facilitation of electron-hole pair separation.However, in terms of separated CuO and g-C3N4 dispersed on the surface of HCP, the pathway of e transfer between the two metal semiconductors is altered due to the presence of HCP as depicted in Scheme 1. HCP possesses intrinsic properties to act as electron acceptors from the excited molecule and also as electron donor [37] invariably within the system. Heree− from CuO (CB) is transferred to HCP, where the latter facilitates interfacial charge transfers along HCP surface to g-C3N4. The same transfer of holes from g-C3N4 to CuO occurs in the presence of HCP, which results in an efficient charge separation by HCP. Also, the g-C3N4 (e−) displays good reduction ability and the CuO (h+) shows oxidizing power. The high reduction electron on the g-C3N4 (CB) reacts with molecular O2 to form superoxide anions, which invariably oxidizes the organic pollutant. The hole in the VB of CuO reacts with water to generate hydroxyl radical which degrades the pollutant effectively. The hole in VB of CuO can also break down the organic pollutants directly due to high positive potential of CuO.Scheme 1
Proposed reaction mechanism of separated electron-hole pair in CuO/HCP-g-C3N4 under visible light.Overall, HCP provides exceptional high surface area, good adsorption, and catalytic sites which favours the reaction process. HCP within the hybrid composite will act as an electron transporter, due to its high electron mobility of zeolites framework and ability to act as an electron acceptor or donor [38]. HCP in real sense acceptse− from the metal semiconductor (lower band gap) in a rapid manner and transfers thee− to other metal semiconductors (narrow band gap) and vice versa for hole transfer. In this same manner photogenerated electron-hole pairs are kept away from the metal oxide semiconductors, which invariably also reduces the recombination rate of photogenerated electron-hole pairs and improves overall catalytic activity of the hybrid composite material. The photocatalytic reaction mechanism highlighted in this study is consistent with the reported literature on the dispersion of mixed metal oxide semiconductor on mesoporous materials [23–26, 39].


## 4. Conclusion

CuO/HCP-g-C3N4 was synthesized through 2 facile routes, the precipitation method for CuO/HCP and impregnation via ultrasonication method for the hybrid composite material (CuO/HCP-g-C3N4). The surface morphology of the hybrid material revealed good homogenous dispersion of the metal oxide conductors within the textural of the dealuminated clinoptilolite. The thermal properties of the hybrid composite material depict excellent thermal stability more than CuO/HCP. The contribution of mixed metal oxide semiconductors within the hybrid composite assists to reduce the recombination rate of photogenerated electron-hole pairs, which invariably can facilitate enhanced photocatalytic activity. HCP in the hybrid composite material acts as electron transporter; it also reduces recombination rate and improves overall catalytic activity of the photocatalyst material. CuO/HCP-g-C3N4 is a promising hybrid composite material for environmental purification and also for generation of clean energy from water splitting application.



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*Source: 450526-2015-02-12.xml*