Effect of intrinsic vacancy defects on the electronic properties of monoclinic Ag2S

https://doi.org/10.1016/j.matchemphys.2020.122961Get rights and content

Highlights

  • Formation energy of VAg defect is lower than that of VS defect.

  • VAg defect is intrinsic defect in Ag2S crystal.

  • Non-zero N(EF) leads to higher conductivity for VAg defects.

  • Effect masses of holes are lighter than those of electrons.

  • Ag2S with VAg defect is a p-type conductive material.

Abstract

The formation energy and electronic properties of intrinsic defects in Ag2S are studied using first-principle calculations. Three possible intrinsic defect configurations are considered, including VAg_I, VAg_II and VS. The calculation results show that VAg defects are more energetic favorable than VS defects. It is found that electrical neutral VAg_I is energetically favorable over the negative charged VAg_I below EF = 0.335eV. We find electronic conductivity could be enhanced by introducing intrinsic VAg defects into crystalline Ag2S. Our electronic band structures show that the curvatures of conduction band minimum of Ag2S are much flatter than the curvatures of valence band maximum, suggesting that the effect masses of holes are much lighter than those of electrons. Compared to pristine Ag2S, the effective masses of holes get larger by introducing vacancy into crystal. Fermi level is passing through the valence band, suggesting Ag2S with VAg defect would be a better conductivity. Non-vanishing N(EF) as well as light effect masses of holes make Ag2S suitable for construction of highly conductive p-type materials.

Introduction

Point defects are traditionally considered to play a major role in influencing on the properties of semiconductors. It is well known that lattice defects, especially for intrinsic point defects are inevitable at finite temperature. These intrinsic point defects could influence the geometric, mechanical, optical and electronic properties of the semiconductors. In recent years, considerable theoretical and experimental efforts are devoted to the fundamental understanding of the role of point defects on the electronic and optical properties of semiconductors. The conductive properties of semiconductors such as SnSe [1], MoSe2 [2] and Ag2S [3] could be significantly affected by intrinsic point defects.

The monoclinic Ag2S (α-Ag2S) is a narrow band gap semiconductor with the band gap values of 1.1 eV [[4], [5], [6], [7], [8]]. Extensive researches showed that Ag2S would be potential candidate materials in photo conducting cells [9], IR detectors [10], solar selective coating [11], photovoltaic [12], and photochemical cells [13]. It is found that the electronic and ionic conductivity of Ag2S increases three and two orders of magnitude, respectively, during structural phase transition from monoclinic structure to the disordered cubic structure [[14], [15], [16]]. Due to its superior ionic characteristics, Ag2S is considered potential materials for solid electrolytes. The existence of intrinsic point vacancy defects in monoclinic Ag2S would reduce the hopping barrier between lattices and improve the ionic conductivity. Point vacancy defects not only modify the geometry of Ag2S but also alter its electronic properties. Alekberov et al. [3] reported that cationic vacancy defects in Ag2S are acceptor-like defects.

Nanoparticles, quantum dots and core-shell nanostructures of non-stoichiometric Ag1.93-1.98S as well as nanoheterostructures Ag2S/Ag were synthesized through hydrochemical bath deposition [[17], [18], [19], [20], [21], [22], [23]]. Various structures, including hexagonal structure, quantum dots, Ag2S/Ag composite were prepared by template synthesis, thermal decomposition, etc. [[24], [25], [26], [27], [28], [29], [30]] Mixed nanostructures of Ag2-δS/Ag were shown to exhibit better photocatalytic performance. By changing the composition of non-stoichiometric Ag2-δS (δ > 0), Ag vacancy also become an active site of charge recombination, which can control the optical properties of the composite and improve its photocatalytic activity under irradiation conditions [19]. Different non-stoichiometric Ag2-δS, include Ag1.1S, Ag1.7S, Ag1.93S, Ag1.95S, Ag1.98S were reported by experiments. It was found that the occupancy of the metal sublattice by Ag atoms is smaller than 1, suggesting Ag2S nanoparticles are non-stoichiometric and contain vacant sites in the metal sublattice [31]. However, the electronic properties of monoclinic Ag2-δS at low temperature are still unknown. A systematic theoretical study on the effect of the intrinsic vacancy defects on the electronic properties, correlation between defect concentration and electronic conductivity, and formation energy of these vacancy defects is highly desirable. In this paper, we aim to elucidate the effects of Ag vacancy defects on the electronic properties of Ag2S by using different compositions near the stoichiometric composition.

Formation energy and electronic properties of monoclinic Ag2S with intrinsic vacancy defects are investigated by first-principles calculations. We find VAg defects are intrinsic defects. VAg_I defects with electrical neutral states are stable below EF = 0.335 eV and VAg_I defects negative charged are energetic favorable above EF = 0.335 eV. The density-of-state at Fermi level gradually increases along with the concentration of the VAg defects increases. The valence band holes are much lighter than those of conductive band electrons, indicating Ag2S with VAg defects is a p-type conductive material.

Section snippets

Computational methods

Ab initio density functional theory (DFT) calculations are performed by using the VASP [[32], [33], [34]] code, and the projector augmented wave (PAW) [35,36] method is applied to describe for electron-ion interaction. The generalized gradient approximation (GGA) of Perdew-Burke-Ernzerhof (PBE) functional [37] is adopted for electron exchange-correlation. 4d10 and 5s1 electrons of Ag as well as 3s2 and 3p4 electrons of S are treated as valence electrons in the calculations. The wave functions

Structure and bond length

First, we examine the geometry structures of Ag2S with intrinsic vacancy defects compared to that of defect free Ag2S. Local structures of pristine Ag2S, Ag2S with VAg_I, VAg_II and VS are shown in Fig. 2. The dashed circles represent the location of the intrinsic Ag or S vacancy defects in Fig. 2(b)~(d). The bond lengths between Ag_I and S atoms as well as Ag_II and S atoms are 2.53 Å and 2.42 Å, respectively in pure Ag2S as we can see from Fig. 2(a). The results show that the bond length

Conclusions

We have performed first-principles calculations to study formation energy and electronic properties of Ag2S with intrinsic vacancy defects. The geometry of our non-stoichiometric Ag2S is similar to the case of the experimental studies. We find the formation energy of VAg is lower than that of VS, suggesting that VAg defects are intrinsic defects. The transition energy level of VAg0/VAg1 occurs at EF = 0.335 for VAg_I defects. VAg defects are shallow acceptor-like defects. Electronic

CRediT authorship contribution statement

Chunyan Du: Software, Investigation, Writing - original draft, Formal analysis, Visualization, Validation, Visualization, Data curation, Writing - review & editing. Jiayuan Tian: Formal analysis, Software. Xiaojie Liu: Resources, Writing - review & editing, Supervision.

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.

Acknowledgements

The authors acknowledge the support by the National Natural Science Foundation of China under Grant Nos. 11574044, 11774048 and Open Project of Key Laboratory for UV-Emitting Materials and Technology of Ministry of Education (No. 130028608).

References (49)

  • K. Akamatsu et al.

    Thin Solid Films

    (2000)
  • P. Jiang et al.

    Biomaterials

    (2012)
  • T.B. Nasrallah et al.

    Synthetic Met.

    (2005)
  • D. Karashanova et al.

    Solid State Ionics

    (2004)
  • M.M. El-Nahass et al.

    Vacuum

    (2004)
  • H. Meherzi-Maghraoui et al.

    Thin Solid Films

    (1996)
  • S. Kashida et al.

    Solid State Ionics

    (2003)
  • S.I. Sadovnikov et al.

    Superlattice. Microst.

    (2015)
  • S.I. Sadovnikov et al.

    Chem. Phys. Lett.

    (2015)
  • S.I. Sadovnikov et al.

    Int. J. Hydrogen Energy

    (2017)
  • C.L. Zhang et al.

    Mater. Lett.

    (2012)
  • Y. Zhao et al.

    Mater. Lett.

    (2007)
  • S. Yan et al.

    Synth. Met.

    (2011)
  • C. Siva et al.

    Mater. Lett.

    (2014)
  • G. Kresse et al.

    Comput. Mater. Sci.

    (1996)
  • S.-H. Wei

    Comput. Mater. Sci.

    (2004)
  • T. Ohachi et al.

    Solid State Ionics

    (1988)
  • Y. Huang et al.

    RSC Adv.

    (2017)
  • A. Shafqat et al.

    AIP Adv.

    (2017)
  • O. Alekberov et al.

    Phys. Status Solidi C

    (2015)
  • W. Jiang et al.

    RSC Adv.

    (2015)
  • H.-Y. Yang et al.

    Nanotechnology

    (2013)
  • Y. Du et al.

    J. Am. Chem. Soc.

    (2010)
  • C.D. Lokhande et al.

    Bull. Electrochem.

    (1990)
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