Abstract

hbox {Sb}_2hbox {S}_3 and hbox {Sb}_2hbox {Se}_3 are well-known layered bulk structures with weak van der Waals interactions. In this work we explore the atomic lattice, dynamical stability, electronic and optical properties of hbox {Sb}_2hbox {S}_3, hbox {Sb}_2hbox {Se}_3 and hbox {Sb}_2hbox {Te}_3 monolayers using the density functional theory simulations. Molecular dynamics and phonon dispersion results show the desirable thermal and dynamical stability of studied nanosheets. On the basis of HSE06 and PBE/GGA functionals, we show that all the considered novel monolayers are semiconductors. Using the HSE06 functional the electronic bandgap of hbox {Sb}_2hbox {S}_3, hbox {Sb}_2hbox {Se}_3 and hbox {Sb}_2hbox {Te}_3 monolayers are predicted to be 2.15, 1.35 and 1.37 eV, respectively. Optical simulations show that the first absorption coefficient peak for hbox {Sb}_2hbox {S}_3, hbox {Sb}_2hbox {Se}_3 and hbox {Sb}_2hbox {Te}_3 monolayers along in-plane polarization is suitable for the absorption of the visible and IR range of light. Interestingly, optically anisotropic character along planar directions can be desirable for polarization-sensitive photodetectors. Furthermore, we systematically investigate the electrical transport properties with combined first-principles and Boltzmann transport theory calculations. At optimal doping concentration, we found the considerable larger power factor values of 2.69, 4.91, and 5.45 for hole-doped hbox {Sb}_{{2}}hbox {S}_{{3}}, hbox {Sb}_{{2}}hbox {Se}_{{3}}, and hbox {Sb}_{{2}}hbox {Te}_{{3}}, respectively. This study highlights the bright prospect for the application of hbox {Sb}_2hbox {S}_3, hbox {Sb}_2hbox {Se}_3 and hbox {Sb}_2hbox {Te}_3 nanosheets in novel electronic, optical and energy conversion systems.

Highlights

  • Sb2S3 and Sb2Se3 are well-known layered bulk structures with weak van der Waals interactions

  • There is a large number of monolayers that used in nanodevices, catalysis, field-effect transistors, batteries, hydrogen evolution, and supercapacitors are based on the exfoliated layered materials, for example but not limited to, Bi2Se3 and Bi2Te39, MoS210, WS2 and MoSe211, MoTe212, WSe213, ­CaGe14, MnPS3 and MnPSe315,16

  • We found that the valance band minimum (VBM) of Sb2Se3 and Sb2Te3 originates from Se/Te-px,y orbitals, while the conduction band maximum (CBM) consists of Se/Te-pz and Sb-pz orbital states

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Summary

Introduction

Sb2S3 and Sb2Se3 are well-known layered bulk structures with weak van der Waals interactions. The layered semiconductor chalcogenides belonging to the V-VI family has drawn significant attention due to its exceptional properties, such as earth-abundant constituents, low t­oxicity[21,22], optical, electronic and thermoelectric p­ roperties[23]. According to their semiconducting nature, these material allow overcoming the deficiencies of zero-bandgap in the graphene, showing gorgeous potential for building memory ­switching[24], microelectronics, and photovoltaic ­devices[25,26]. These experimental studies have demonstrated that Sb2X3(X= S, Se, Te) can be efficiently used as potential material for various applications

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