Two dimensional B2CX (X=O, S, Se) monolayer semiconductors for water splitting application

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Highlights

  • A new stable B2CX (X = O, S, Se) monolayers are predicted.

  • The thermodynamic, kinetic, and thermal stabilities of the predicted monolayers are proved by simulation.

  • 2D B2CO, B2CS, B2CSe monolayers are semiconductors with bandgaps of about 2.81, 2.63, 1.57 eV respectively.

  • 2D B2CX (X = O, S, Se) monolayers are promising photocatalysts materials for water splitting applications.

Abstract

The structural and electronic stabilities as well as photocatalytic properties of two-dimensional (2D) Janus B2CX (X = O, S, Se) monolayers are theoretically assessed. First, with the help of cohesive energy computations and phonon dispersion simulations, the energetically and kinetically stabilities of the proposed 2D B2CX (X = O, S, Se) monolayers are confirmed. Next, electronic properties computations using hybrid density functional (HSE06) indicates that 2D B2CO, B2CS, B2CSe monolayers show semiconducting properties with moderate bandgaps of about 2.81, 2.63, 1.57 eV respectively. Finally, comparing the positions of band edge of the proposed monolayers with the redox potentials of water shows that 2D B2CX (X = O, S, Se) monolayers are promising photocatalysts materials for water splitting applications.

Introduction

Increasing global energy demand coupled with climate change and environmental degradation regarding the growing use of fossil fuels can be considered as the greatest challenges facing the human societies for the time being, therefore, to find alternative clean and sustainable energy sources is an important task related to the issue. Solar and hydrogen energy are most common clean energy sources, have been gradually increasingly interested many efforts to be used as replacement of traditional resources [[1], [2], [3], [4], [5]].

Hydrogen in its pure form, is a good energy carrier, has been employed as one of the most useful substitute energy sources can be used in several different ways. In recent decades, different forms of hydrogen are employed in many practical applications, as examples, liquid hydrogen is used as rocket fuel, and hydrogen fuel cells are widely used in power electric cars. Unfortunately, hydrogen rarely exists on its pure form and it must be obtained from hydrogen containing compounds such as water [6]. Regarding this task, to find an efficient photocatalyst material which can utilize solar energy to produce pure hydrogen by water splitting procedure is the main challenge [7,8]. In principle, in a photocatalytic water splitting process based on a semiconductor, by absorbing a photon from sunlight by the surface of the semiconducting photocatalyst an electron–hole pairs is generated via an electron excitation from the valence band to the conduction band, and at last, the redox reaction splits water molecules into hydrogen and oxygen. For the aim of semiconducting photocatalyst based water splitting technology, to find an efficient photocatalyst is the root problem. To be used in practical applications, for overall water splitting, a promising efficient photocatalyst must have three characteristics: (a) a good photocatalyst semiconductor needs to have a bandgap of 1.2–3.0 eV to absorb a significant portion of solar energy; (b) the photo generated charge carriers need to promptly transfer as well as they need to separate to prevent their recombination; (c) The valence band maximum (VBM) must be lower than −5.67 eV, and the conduction band minimum (CBM) should be higher than (−4.44 eV) to further produce hydrogen. These two values are the oxidation potential of O2/H2O and the reduction potential of H/H2. A schematic representation of photocatalyst water splitting is shown in Fig. 1.

In recent years many efforts have been done to introduce new photocatalyst semiconductor materials to be used in water splitting and a large number of bulk and nanostructured photocatalyst semiconductors have been proposed [[9], [10], [11], [12], [13], [14], [15]], however, that most of the proposed bulk photocatalyst semiconductors exhibits low efficiencies. It is well known that due to their special properties, generally two dimensional (2D) materials may have promising applications in water splitting technology. Therefore, a huge number of research activities have been conducted to design promising two dimensional (2D) photo-catalyst semiconductors. Since now, the water splitting photocatalytic properties of phosphorene, 2D group III-VI monochalcogenides [16,17], 2D IV−VI compounds [18,19], 2D IV-IV compounds [20], 2D transition-metal dichalcogenides [21,22] have been investigated. Very recently, the water splitting application of 2D Ga2XY and In2XY (X = S, Se, Te; Y = S, Se, Te) Janus monolayers (MLs) have been investigated by Da Silva et al. [23], it has been shown that the proposed Janus monolayers Janus monolayers exhibit required conditions to be used in water splitting applications.

In this work, First Principles Calculations based on Density Functional Theory (DFT) were preformed to investigate, the structural stability, electronic and photocatalytic properties of two-dimensional (2D) Janus B2CX (X = O, S, Se) monolayers. In these calculations, once the stability of the proposed monolayers was confirmed, the electronic properties of the designed 2D monolayers was evaluated and it was found that all of the proposed monolayers shows semiconductor nature with strain tunable moderate bandgaps. Moreover, by analyzing the band edge positions of the proposed monolayers with the redox potentials of water shows that 2D B2CX (X = O, S, Se) monolayers are promising photocatalysts for using in water splitting technologies.

Section snippets

Computational methods

In this investigation, to find the most stable unit cell of the B2CX (X = O, S, Se) monolayers, the atomic force minimization and lattice parameter optimization were firstly performed. Once the optimized unit cell of the structures obtained, the stability of the designed 2D monolayer materials was evaluated. For the aim of confirming the stability of the proposed monolayers, their energetically and kinetically stabilities were examined. All the atomic force relaxation, lattice parameters

Structural model construction and stability

Fig. 1(a) and (b) display ball stick models of 2D B2CX (X = O, S, Se) crystal structures from top and side views. Our designed structures were initially inspired by 2D group IV-V monolayer semiconductors. To be more precise, in a unit cell of 2D group IV-V monolayer, there are two group-IV elements and two group-V elements, the proposed 2D B2CX (X = O, S, Se) monolayers can be simply obtained by replacement of the group-V elements in a unit cell of 2D group IV-V monolayer with carbon and X

Conclusions

In summary, by using computational simulation based on the Density Functional Theory (DFT), we systematically investigated the structural stability and promising electronic and photocatalytic properties of two-dimensional (2D) B2CX (X = O, S, Se) monolayers. It is confirmed that 2D B2CX (X = O, S, Se) monolayers are energetically and kinetically stable. Our calculation on their electronic characters indicates that 2D B2CO, B2CS, B2CSe monolayers show semiconducting properties with moderate

Authorship statement

All the theory and computations were performed by M.M. Abutalib.

Declaration of competing interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

References (39)

  • X.L. Zhang et al.

    Appl. Catal., B

    (2018)
  • A.H. Reshak

    Appl. Catal., B

    (2018)
  • C. Peng et al.

    Nanomater. Energy

    (2018)
  • R.S. Meng et al.

    Appl. Mater. Today

    (2018)
  • R. Kumar et al.

    J. Catal.

    (2018)
  • R. Abt et al.

    Physica B

    (1994)
  • J.Y. Zhang et al.

    Nat. Commun.

    (2017)
  • U.H. Bakhtiar et al.

    Mater. Sci. Semicond. Process.

    (2013)
  • A.J. Esswein et al.

    Chem. Rev.

    (2007)
  • A. Kudo et al.

    Chem. Soc. Rev.

    (2009)
  • K. Maeda et al.

    J. Phys. Chem. Lett.

    (2010)
  • C.F. Fu et al.

    Adv. Mater.

    (2018)
  • C.F. Fu et al.

    Adv. Mater.

    (2018)
  • W.H. Saputera et al.

    ACS Catal.

    (2019)
  • A.A. Dorothy et al.

    Mater. Res. Express

    (2019)
  • R. Peng et al.

    J. Mater. Chem.

    (2019)
  • K. Ren et al.

    RSC Adv.

    (2019)
  • Houlong L. Zhuang et al.

    Chem. Mater.

    (2013)
  • Yunguo Li et al.

    Catal. Sci. Technol.

    (2017)
  • Cited by (5)

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