First-principles study of superconducting in LiFeAs: FM, AFM, and NM states via DFT and DFT+U techniques

The interplay between magnetism and superconductivity in Fe-based superconductors remains a topic of significant interest. This study investigates the electronic structure and superconducting properties of LiFeAs in ferromagnetic (FM), antiferromagnetic (AFM), and non-magnetic states using Density F...

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Main Authors: Manza Zityab Kasiab, Kumneger Tadele, Mesfin Asfaw Afrassa, Omololu Akin-Ojo
Format: Article
Language:English
Published: AIP Publishing LLC 2025-05-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/5.0269638
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author Manza Zityab Kasiab
Kumneger Tadele
Mesfin Asfaw Afrassa
Omololu Akin-Ojo
author_facet Manza Zityab Kasiab
Kumneger Tadele
Mesfin Asfaw Afrassa
Omololu Akin-Ojo
author_sort Manza Zityab Kasiab
collection DOAJ
description The interplay between magnetism and superconductivity in Fe-based superconductors remains a topic of significant interest. This study investigates the electronic structure and superconducting properties of LiFeAs in ferromagnetic (FM), antiferromagnetic (AFM), and non-magnetic states using Density Functional Theory (DFT) and DFT+U approximations. Notably, the DFT approximation favors AFM coupling, but DFT+U stabilizes an FM configuration in spin-polarized simulations. The DFT approximation predicts a lattice parameter of 3.651 Å, a mean-field AFM/FM transition temperature [Tc(MFA)] of 38.7 K, and a magnetic moment of 1.47 μB per Fe atom. In contrast, DFT+U yields a lattice parameter of 3.768 Å, closely matching the experimental value of 3.771 Å. It also predicts a significantly enhanced Tc(MFA) of 464.2 K and a magnetic moment of 3.13 μB per Fe atom. The significance of these findings lies in the ability of DFT+U to capture electron correlation effects better, leading to structural and magnetic properties that align more closely with an experimental observation of 3.42 μB. Finally, the DFT+U approximation structure increases bond length and angle by 0.1995 Å and 1.424°, respectively, compared to the DFT approximation. The non-magnetic state appears most favorable for superconductivity, whereas FM and AFM states suppress superconducting behavior because of spin polarization effects. This analysis provides valuable insights into the delicate balance between magnetism and superconductivity in Fe-based materials, contributing to the theoretical understanding of their electronic properties.
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spelling doaj-art-1750a8356dfd44d88d1aa4fe188f25292025-08-20T03:20:34ZengAIP Publishing LLCAIP Advances2158-32262025-05-01155055110055110-1010.1063/5.0269638First-principles study of superconducting in LiFeAs: FM, AFM, and NM states via DFT and DFT+U techniquesManza Zityab Kasiab0Kumneger Tadele1Mesfin Asfaw Afrassa2Omololu Akin-Ojo3Department of Physics, School Applied Natural Science, Adama Science and Technology University, Adama, EthiopiaDepartment of Physics, School Applied Natural Science, Adama Science and Technology University, Adama, EthiopiaDepartment of Physics, School Applied Natural Science, Adama Science and Technology University, Adama, EthiopiaDepartment of Physics, University of Ibadan, Oyo, NigeriaThe interplay between magnetism and superconductivity in Fe-based superconductors remains a topic of significant interest. This study investigates the electronic structure and superconducting properties of LiFeAs in ferromagnetic (FM), antiferromagnetic (AFM), and non-magnetic states using Density Functional Theory (DFT) and DFT+U approximations. Notably, the DFT approximation favors AFM coupling, but DFT+U stabilizes an FM configuration in spin-polarized simulations. The DFT approximation predicts a lattice parameter of 3.651 Å, a mean-field AFM/FM transition temperature [Tc(MFA)] of 38.7 K, and a magnetic moment of 1.47 μB per Fe atom. In contrast, DFT+U yields a lattice parameter of 3.768 Å, closely matching the experimental value of 3.771 Å. It also predicts a significantly enhanced Tc(MFA) of 464.2 K and a magnetic moment of 3.13 μB per Fe atom. The significance of these findings lies in the ability of DFT+U to capture electron correlation effects better, leading to structural and magnetic properties that align more closely with an experimental observation of 3.42 μB. Finally, the DFT+U approximation structure increases bond length and angle by 0.1995 Å and 1.424°, respectively, compared to the DFT approximation. The non-magnetic state appears most favorable for superconductivity, whereas FM and AFM states suppress superconducting behavior because of spin polarization effects. This analysis provides valuable insights into the delicate balance between magnetism and superconductivity in Fe-based materials, contributing to the theoretical understanding of their electronic properties.http://dx.doi.org/10.1063/5.0269638
spellingShingle Manza Zityab Kasiab
Kumneger Tadele
Mesfin Asfaw Afrassa
Omololu Akin-Ojo
First-principles study of superconducting in LiFeAs: FM, AFM, and NM states via DFT and DFT+U techniques
AIP Advances
title First-principles study of superconducting in LiFeAs: FM, AFM, and NM states via DFT and DFT+U techniques
title_full First-principles study of superconducting in LiFeAs: FM, AFM, and NM states via DFT and DFT+U techniques
title_fullStr First-principles study of superconducting in LiFeAs: FM, AFM, and NM states via DFT and DFT+U techniques
title_full_unstemmed First-principles study of superconducting in LiFeAs: FM, AFM, and NM states via DFT and DFT+U techniques
title_short First-principles study of superconducting in LiFeAs: FM, AFM, and NM states via DFT and DFT+U techniques
title_sort first principles study of superconducting in lifeas fm afm and nm states via dft and dft u techniques
url http://dx.doi.org/10.1063/5.0269638
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