Materials Today: Proceedings
Available online 2 March 2023
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Effect of nickel impurity on structural, magnetic and electronic properties of WX2MLs (X = S, Se): An ab-initio study

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Abstract

We have studied the spin dependent structural, electronic and magnetic properties of pristine and Ni doped WX2 (X = S, Se) 2D monolayers by using density functional theory (DFT). The doping process improves and control the electronic and magnetic properties of TMDCs which is essential for application in electronics, optoelectronics and spintronics. WX2MLs with Ni impurity shows ferromagnetic behaviour. Spin resolved energy band gap have been observed. The Ni doped WSe2 exhibits the characteristics of half metal with 0.88 (D) and 0.02 (D) eV energy band gap for up and down spin respectively. The WS2ML with Nickel impurity shows 1.03 (I) and 0.17 (D) eV energy band gap for up and down spin respectively. The total magnetic moment of both Ni doped WX2MLs is found to be approximately 4µB which is due to local effect of the dopant. The exclusive combination of magnetic response and narrow bandgap which expedite the application of spintronics and yields magnetic semiconductors.

Introduction

The discovery of graphene drew the attention of scientists towards 2D materials [1]. This leads to excitement in the world of material science and researchers started discovering a new class of materials called Transition Metal Dichalcogenides (TMDCs). These TMDCs have the power to completely revolutionize industries like electronics and energy storage. TMDCs belongs to a novel class of two-dimensional materials that have garnered significant attention in recent years. These materials possess unique electronic, optical and mechanical properties that have the potential to transform the industries, from electronics and energy storage to biomedicine [2], [3], [4], [5], [6], [7], [8], [9], [10], [11], [12], [13]. TMDCs are also explored as a possible replacement for conventional semiconductors due to their wide energy bandgap. TMDC monolayers are MX2-type atomically thin semiconductors, where M is a transition metal and X is a chalcogen atom (S, Se, Te). The WX2MLs are one important category of TMDCs in which a W-atom is sandwiched between two layers of X-atoms (X = S, Se). The monolayers of WS2 and WSe2 exhibit metallic and semiconducting properties and have direct band gaps of 1.8 eV and 1.566 eV, respectively [14]. To enhance the significant potential of 2D materials for use in optoelectronics, energy storage devices, and catalysis impurity defects, one important technique is to modify the bandgap of 2D materials. There are several approaches for this purpose [15], [16], [17]. Generally, substitutional and doping methods are used to tune the energy bandgap of 2D materials. Theoretically, predictions proved the transition elements prefer to substitute at the M−site instead of the X-site. Several experimental and theoretical studies on the effect of defects and impurities on transition metal dichalcogenide monolayers (TMDMLs) have been conducted in recent years. It has been demonstrated that the electrical and magnetic characteristics of WX2 monolayers are significantly affected by the doping of magnetic impurities [16], [17], [18], [19]. Local magnetic moments created by magnetic impurities may interact with the magnetic moments of nearby WX2 atoms. This interaction can result in changes to the electronic structure of the WX2 monolayer, including modifications to the bandgap and magnetic ordering. According to studies, magnetic impurities can significantly change the magnetic characteristics of WX2 monolayers, causing the formation of novel magnetic phases and improving magnetic ordering [17]. Furthermore, it has been demonstrated that the creation of magnetic skyrmions, which are topologically protected spin structures, results from the doping of WX2 monolayers with magnetic impurities. This type of material shows possible applications in the fields of electronics and spintronics [18]. Recently, TMDC's 2D monolayer (ML) of WS2 doped with Fe has become paramagnetic in nature [19]. WSe2MLs are doped with Cr, Mn, Fe, and Co impurities [20] and Fe doped system a robust and stable half metallic materials due to the presence of three connected states peak spanning to the fermi level. Kyungnam Kang investigated the effect of Fe-doping in MoS2 and WS2 monolayers, concluding that Fe-doped MoS2 is ferromagnetic while Fe-doped WS2 monolayer is paramagnetic [21]. As researchers continue to unravel the mysteries of TMDCs, it is becoming increasingly clear that these materials have the potential to play a major role in shaping our future landscape of technology. In the present paper, we have investigated the density functional theory (DFT)-based structural, electronic, and magnetic properties of 2D TMDMLs of WX2 (X = S, Se) doped with Ni impurity and observed the effect of impurity on band structure, which leads to an induced magnetic moment and is helpful in spintronics.

Section snippets

Computational detail

We have used SIESTA (Spanish Initiative for Electronic Simulation with Thousands of Atoms) code [22] for doing all the calculations. We have used Troullier Martin, norm-conserving, relativistic pseudopotentials in this work. The exchange–correlation between electrons have been described using GGA-PBE functional [23]. The double zeta polarization (DZP) basis sets with confinement energy of 20 meV and 300Ry mesh cut off is used in all calculations. A vacuum of 15 Å along the Z-direction has been

Structural properties

A 6 ×6 supercell of WX2 has been constructed with 108 atoms (36 atoms of W and 72 atoms of X  = S, Se)) shown in Fig. 1(a). In this supercell, one metal atom is replaced with impurity of Ni as shown in Fig. 1(b). Firstly, lattice constants of optimized WS2 and WSe2 MLs are calculated and found to be 3.214 Å and 3.345 Å respectively which are in good agreement with previous studies [14]. There is no change in lattice constant of Ni doped WS2ML and WSe2ML. The optimized structures of WX2MLs

Conclusion

In this paper, we have presented the effect of Ni impurities on pristine monolayers of WS2 and WSe2 using first-principle calculations. The average bond length of Ni-X (S, Se) varies as compared to W-X bond length due to the smaller atomic radius of the Ni atom than the W atom. Ni-doped WSe2 shows the property of half metal with a bandgap of 0.02 eV for one spin orientation. The induced magnetic effect of Ni impurity on WX2ML is observed in the surrounding atoms of nickel impurity. The W0.972Ni

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.

Acknowledgment

Authors would like to acknowledge SIESTA team for providing the code. This research was supported in part through computational resources provided by the Kathmandu University Supercomputer Center, which was established with equipment donated by CERN.

*Lalita Devi; did her M.Sc. in Physics and project in condensed matter physics from Swami Vivekanand Govt. College Ghumarwin, Himachal Pradesh, India. Her current research interests are electronic magnetic properties of 2D materials using DFT.

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  • Cited by (0)

    *Lalita Devi; did her M.Sc. in Physics and project in condensed matter physics from Swami Vivekanand Govt. College Ghumarwin, Himachal Pradesh, India. Her current research interests are electronic magnetic properties of 2D materials using DFT.

    Dr. Arun Kumar; pursued his Ph.D. in Condensed Matter Physics from Himachal Pradesh University Shimla, Himachal Pradesh, India. Presently he is a faculty at Department of Physics, Swami Vivekanand Government College Ghumarwin, Himachal Pradesh, India. His current research interests are electronic, optical and transport properties of 0D, 1D and 2D nanomaterials using DFT.

    Mahesh Pathania; pursued his M.Sc Physics and project in Theoretical Condensed Matter Physics from Swami Vivekanand Govt. College Ghumarwin, Himachal Pradesh, India. Currently pursuing DFT based project in search of PhD position.

    Kuldeep Kumar; did his M.Sc Physics and project in Theoretical Condensed Matter Physics from Swami Vivekanand Govt. College Ghumarwin, Himachal Pradesh, India. Currently pursuing DFT based project in search of PhD position.

    Rishu Dhiman; did his M.Sc Physics and project in Theoretical Condensed Matter Physics from Swami Vivekanand Govt. College Ghumarwin, Himachal Pradesh, India. Currently pursuing DFT based project in search of PhD position.

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