A D Fauzi1, M A Majidi1 and A Rusydi2,3
1Department of Physics, Faculty of Mathematics and Natural Sciences Universitas
Indonesia, Kampus UI Depok, Depok 16424, Indonesia
2NUSNNI-NanoCore, Department of Physics, Faculty of Science, National University
of Singapore, Singapore 117576, Singapore
3Singapore Synchrotron Light Source, National University of Singapore, Singapore
117603, Singapore
Corresponding author’s email: aziz.majidi@sci.ui.ac.id
Abstract.
We propose a simple tight-binding based model for Fe3O4 that captures the
preference of ferrimagnetic over ferromagnetic spin configuration of the system. Our model is
consistent with previous theoretical and experimental studies suggesting that the system is half
metallic, in which spin polarized electrons hop only among the Fe B sites. To address the metal insulator
transition (MIT) we propose that the strong correlation among electrons, which may
also be influenced by the electron-phonon interactions, manifest as the temperature-dependence
of the O-p−Fe-d hybridization parameter, particularly Fe-d belonging to one of the Fe B sites
(denoted ast
(2)
FeB−O). By proposing that this parameter increases as the temperature decreases, our
density-of-states calculation successfully captures a gap opening at the Fermi level, transforming
the system from half metal to insulator. Within this model along with the corresponding choice
of parameters and a certain profile of the temperature dependence of t
(2)
FeB−O, we calculate the
resistivity of the system as a function of temperature. Our calculation result reveals the drastic
uprising trend of the resistivity profile as the temperature decreases, with the MIT transition
temperature located around 100 K, which is in agreement with experimental data.
To download the article click on the link below:
http://iopscience.iop.org/article/10.1088/1757-899X/188/1/012014/pdf
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