Journal of Renewable Materials

DOI: 10.32604/jrm.2022.018556

REVIEW

g-C3N4 Derived Materials for Photocatalytic Hydrogen Production: A Mini Review on Design Strategies

Kai Su1,*, Shaoqi Deng1, Linxiao Li1, Qirui Qin1, Jingyu Yang1, Yan Chen2,3, Shengli Zhang1 and Junming Chen1

1Faculty of Geosciences and Environmental Engineering, Southwest Jiaotong University, Chengdu, 611756, China
2Analysis and Testing Center, South China Normal University, Guangzhou, 510006, China
3MOE Key Laboratory of Theoretical Chemistry of the Environment, School of Chemistry, South China Normal University, Guangzhou, 510006, China
*Corresponding Author: Kai Su. Email: ksu@swjtu.edu.cn
Received: 02 August 2021; Accepted: 20 August 2021

1  Introduction

The rapid economic growth has encouraged researchers to find new forms of energy, along with the global goals for low/zero carbon dioxide emissions. The adoption of renewable energy is one of the most important pathways [1]. As renewable energy, hydrogen energy has high calorific value and clean properties [2]. Massive studies have adopted photocatalytic process to decompose pure water or waste water to relieve environmental pollutants and to obtain hydrogen energy, simultaneously [3,4]. Among the numerous materials, inorganic semiconductor materials are of low cost compared with rare metal catalysts [5]. The g-C3N4 polymer can induce visible light and its unique electronic structure and adaptive capacity to adjust the band structure has attracted wide interest [6,7]. Moreover, the easy acquaintance from nature, no toxicity and strong stability of the C and N elements make them stand out.

In this regard, some preparation methods for g-C3N4, including the thermal condensation, solvothermal synthesis, microwave assisted synthesis, ionic liquids, and molten salt methods have been widely reported [8–10]. Meanwhile, the utilization of the precursor such as urea, melamine, thiourea and the preparation with other materials are crucial [11,12]. At present, the structure of the g-C3N4 models has been widely recognized, as shown in Fig. 1. Abundant modification pathways are taken to reduce the g-C3N4 interchange material used in catalytic hydrogen production defects, including metal or nonmetal doping, while the micro structure is modified to address the issues of generally low specific surface area, the raw carrier transfer, light electronic-hole, forbidden band width and other problems. In this review, relevant modifications of g-C3N4 were summarized, and the enhancement mechanisms in a hydrogen production scenario and future application challenges of the design strategies g-C3N4 materials were presented.

Figure 1: Structural model of g-C3N4: (a) S-triazine ring structure (blue shadow unit); (b) 3-s-triazine ring structure (red shadow unit)

2  Mechanism of g-C3N4 Photocatalysis for Hydrogen Production

As one of the most important application scenarios of g-C3N4 photocatalysis, hydrogen production has received a lot of attention. Based on the Gibbs free energy change (H2O → H2 + 1/2O2, ΔG = 238 kj/mol) and thermodynamics, the splitting should meet the energy source [12]. Therefore, extra photon energy is needed to break an energy barrier of 1.23 eV. Thus, the band-energy gap of the g-C3N4 or the derivatives should be in the range of 1.23–3.0 eV to maintain effective splitting of water [13]. Valence band (VB) and empty conduction band (CB) can be separated by forming finite band energy gap [14]. When irradiation of incidence light is developed during the generation of photo-excited charge carrier, the exciting electrons from VB to CB can separate the e− and h+ pair involved in reduction and oxidation [15]. In this regard, the photocatalytic process generally includes several processes [16] (Fig. 2): (a) photon absorption; (b) exciton separation; (c) carrier diffusion, in which the low charge recombination rate decreases the charge separation rate and leads to a poor transmittance; (d) carrier transport; (e) catalysis efficiency, which decides the apparent quantum efficiency; (f) the light-generated e−/h+ pairs are adsorbed, followed by the movement of e− to CB with the holes in VB, which enhances the h+ and e−. Through these steps, appropriate modification strategy to enhance the overall water splitting efficiency can be predicted.

Figure 2: Mechanism of photocatalytic reaction for g-C3N4

There have been extensive studies on the mechanism of photocatalysis. g-C3N4 is very active under visible light due to the wide band gap. Considering the wide band gap of g-C3N4 and over-potentials, the band-energy gap ranges from 2.0 eV to 3.1 eV is higher than that of the endothermic driving forces which is about 1.23 eV but lower than visible light absorption scope [17]. The CB is higher than the potentials of H2 production in the negative position. It is known that the sp2 hybridization in 2D can form layered construction due to the poor van-der Waal’s forces between C and N in g-C3N4, and the thermal conversion process can help the condensation of feedstock with a molar ratio of 0.75 [18]. The photo-generated holes of g-C3N4 facilitate oxygen generation from H2O oxidation and avert the CO2 mineralization by strong •OH. But the low efficiency aroused by high e−/h+ recombination rate of smooth g-C3N4 has been noticed and a lot of downstream technologies focus on the enhancement of active sites, grain boundary defects and kinematics [16,17]. Additionally, researchers have widely followed the first principle based on density functional theory in the field of photocatalysis as a clear research method for effective and quick exploration to improve the g-C3N4 photocatalytic performance [19,20]. With the incomparable advantage of semi-empirical method like Grimme, first principle based on density functional theory has become an important basis for calculation and simulation [21]. Thus, the lattice constant, density, cell volume, relative energy, electron structure, and absorption spectra based on g-C3N4 can be obtained. With the calculation of band structure, density of states, and etc., it will provide more theoretical guidance for the properties and modification of g-C3N4. As described above, typical normal potentials of redox reaction with g-C3N4 band-energy gap under pH of 7 are presented in Fig. 3 [22].

Figure 3: Typical band structures of various type of semiconductor photocatalysts compared with g-C3N4

3  Modification Pathways for g-C3N4

To modify the energy band structure of g-C3N4, doping metallic or nonmetallic elements by physical or chemical pathways has been proved to be effective. The light absorption, charge density, charge dispersion and mobility, as well as the crystallinity can be changed by introducing external doping elements into the semiconductor lattice. Generally speaking, nonmetals doping is realized by embedding in the body structure of g-C3N4, including B, O, S, P, Cl, Br, I, and F [23–25]. It is critical to determine the location and defects of the introduced element in the skeleton structure of g-C3N4. For example, P element can exist in the structure matrix of g-C3N4 in the form of P-N bond, which makes the band gap narrow and promotes exciton separation, and some studies have found that P doping delayed the rapid recombination of electron hole pairs [25]. As for B and N, the introduction defects can broaden the visible light absorption range of g-C3N4, and abundant unsaturated sites can enhance the interaction of the interlayer C-N, and further promote the separation of excitons and charge transmission [26].

Generally, Mn, Zn, Cu, Ni, Fe, Co etc. are the main metal doping elements in present works [27]. Since g-C3N4 is a hepazine ring composed of three triazine rings along with a cavity structure formed by six unsaturated N-coordination structures, it is easy to facilitate metal elements to form metal coordination electronic structure. For example, Mn can be embedded in g-C3N4 as Mn-N-C group, which can adjust the positron and energy band structure, and further promote the charge transfer [27]. On this basis, researchers also try to study the influence of metal doping on g-C3N4 in order to optimize the strength of the metal-C-N bond or to adjust the spin state of metal ions. However, the amount of element doping is also a crucial factor. For instance, Fe doped g-C3N4 nanosheet structure will be cracked beyond certain Fe mass ratio. Until now, various characterization techniques including nuclear magnetic resonance, XPS, FTIR, NMR, XANES, etc., have showed that the doping elements were not only related to the size of the atomic radius of the element, but also related to the pathways and forms of the embedding. The typical doping sites of nonmatals and metals in g-C3N4 are shown in Figs. 4 and 5. In addition to element doping, modification of the morphology of g-C3N4 is another strategy, which can also modify the electronic structure, optical properties, and desirable surface characteristics. Different dimensions of g-C3N4 structures like carbon dots, nanorods/wires/bands/tubes/sheets/spheres/gels, etc., are defined as 0D-3D materials and show obvious differences in preparation conditions, specific surface area, exposure degree of active site, and lifetime of photogenerated carriers [28,29]. With this, secondary modification of materials with different dimensions of g-C3N4 and doping elements will have great potential. Nevertheless, the preparation of materials cannot be perfect due to the absence of N, C and cyanogroup, which is also called defect engineering, but this will provide opportunities for the improvement of optical properties of g-C3N4 [30,31].

Additionally, after the light excitation process, the electron-hole pair has a high repetition rate, which can affect the photocatalytic performance of the material. Numerous studies have proved that the formation of heterojunction structure with composite of semiconductor materials such as TiO2, ZnO, NiS, Ni2P, etc., and even metal organic framework (MOF) was an effective strategy to improve the photocatalytic performance of bulk g-C3N4 [32,33]. The heterojunction structure can be formed by seamless combination of g-C3N4 with carbon materials through π conjugated bonds [33]. Through the formation of heterojunction, the surface or cross linked to the crystal lattice interface inside the semiconductor can be tightly bonded and can induce the formation of internal electric field. The typical heterojunction of Type II and Z-scheme charge transfer for g-C3N4 are shown in Fig. 6 [34]. Specifically, the electrons in the excited state can be firstly transferred to the conduction band under the light condition, and the semiconductor with more negative conduction band position then moves forward as more positive semiconductor, while the photogenerated hole is on the opposite and accelerates the effective separation of the photogenerated electron hole pair, which is very favorable in the field of photocatalytic hydrogen production [35,36]. In a nutshell, the purpose of modification of g-C3N4 materials is to enhance the utilization of light and to increase the active sites and reduce the recombination of photogenerated electron-hole pairs, which will be the basis for further breakthroughs in g-C3N4 material innovation in the future.

Figure 4: Potentials substituted sites of non-metals doping in a single g-C3N4 layer

Figure 5: Typical diagram of metal ion (Ma+) incorporation in g-C3N4 framework

Figure 6: Typical heterojunction of Type II and Z-scheme charge transfer for g-C3N4

4  Design Strategies of g-C3N4 for H2 Generation

The significant progress of g-C3N4 nanostructures tailoring techniques for catalytic H2 generation has got a great deal of attention during the past ten years. In this section, the myriads of applications for H2 production via water splitting were reviewed with various design strategies of g-C3N4 materials. For solo inorganic element doped g-C3N4, the H2 generation rate can be increased by 10–20 times and more. For instance, the H2 generation rate derived from sulfur-doped polymeric g-C3N4 photocatalysts reached 12.16 μmol h−1 [36], while the value was 57 μmol h−1 for P-doped g-C3N4 tubes [37], and 70.05 μmol h−1 for B doped g-C3N4 quantum dots [26], respectively. A lot of studies have also proved that g-C3N4 simultaneously doped with various species of inorganic elements or metals could also ameliorate visible-light photocatalytic H2 generation [38,39]. For example, in Yang et al. [24]’s study, a higher surface area with optimized sp2 conjugated heterocyclic structure was obtained for g-C3N4 prepared with C-I, and the hydrogen evolution rate reached 168.2 μmol/h. Generally, researchers prepared catalyst by using porous g-C3N4 to further modify and obtain higher efficiency of hydrogen production. Wu et al. [40] fabricated porous g-C3N4 nanobelts by using method of C, O binary-doped hierarchical, and the replacement of N atoms narrowed the bandgap and favored the harvest of visible-light for high H2 evolution. In Deng et al. [41]’s work, the low electron-hole recombination rate and rapid electron transfer were found to account for the high hydrogen evolution reaction of Ni/porous g-C3N4. Unlike that, several works found that heterostructure could be fabricated by formation of crystal. For example, Jia et al. [42] found that FeSe2/g-C3N4 formed nanosheets and accelerated the decomposition of H2O2 generation on the nanosheet surface via a stepwise two-electron/two-step pathway. In conclusion, a number of enhanced hydrogen production pathways have been demonstrated by developing and designing a robust photocatalyst. Representative g-C3N4 material preparation and the superiority for H2 generation rate are summarized in Tab. 1. Meanwhile, based on the section discussed above, the design strategies of g-C3N4 for H2 generation are summarized in Fig. 7.

Figure 7: Design pathways and strategies of g-C3N4 for H2 generation

5  Conclusion and Future Challenges

In this review, the modification pathways of g-C3N4 related to the elemental doping, heterojunction development and other methods were elaborated. The enhancement mechanisms in a hydrogen production scenario and future application challenges of the design strategies g-C3N4 materials are presented. Despite that the g-C3N4 materials used for photocatalytic hydrogen production have been investigated by numerous scientific works for water splitting application, the preparation, optimization of raw materials, and the cost of hydrogen production, as well as related mechanisms of research require further extensive exploration. The detailed future challenges to overcome are as below:

(1)   The durability and stability of g-C3N4 should be taken into more consideration regarding the recycling and efficiency.

(2)   The choice of precursor feedstock for g-C3N4 is critical. It is essential to understand the thermal method and all other methods that can provide a better strategy for the g-C3N4 preparation.

(3)   More morphological research should be conducted on the new heterojunction and homojunction with surface or interface characteristics and narrow absorption range.

(4)   Carbonaceous semiconductors should be investigated on the metal and non-metal doping, defects, and interaction mechanisms of multiple functions, and can provide references of optimized hydrogen production rate and lower catalyst cost in the future.

Funding Statement: This work was supported by Sichuan Science and Technology Program (2021YFS0284, 2018SZDZX0026, 2021YFS0289), the Opening Project of Key Laboratory of Theoretical Chemistry of Environment (South China Normal University), Ministry of Education (20200103), the Fundamental Research Funds for the Central Universities of Southwest Jiaotong University (210824), and the Opening Project of Key Laboratory of Southwest Jiaotong University (ZD2021210001).

Conflicts of Interest: The authors declare that they have no conflicts of interest to report regarding the present study.

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