三元硫化物Rb2Mn3S4的电子和磁性能

G. B. Acharya, Madhav Prasad Ghimire
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引用次数: 0

摘要

半导体材料,特别是具有直接带隙的半导体材料,对现代光伏和光电子器件的制造有很大的帮助。本文基于密度泛函理论计算,利用全势局域轨道码预测了Rb2Mn3S4的电子和磁性能。考虑非磁性、铁磁性、亚铁磁性和反铁磁性的不同构型,发现磁性基态是总能量最低的亚铁磁性。计算得到Rb2Mn3S4中Mn (I)和Mn (II)原子自旋相互作用产生的有效磁矩为10μBunit cell(2个公式单位)。通过计算,发现Rb2Mn3S4是一种直接能带隙为0.75 eV的半导体。随着库仑相互作用(即GGA+U)的加入,当U = 4 eV时,带隙增大到2.34 eV。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Electronic and magnetic properties of ternary sulfide Rb2Mn3S4
Semiconducting materials, especially with a direct band gap, are helpful for modern photovoltaic and optoelectronic device fabrication. Here, based on density functional theory calculations, we predict the electronic and magnetic properties of Rb2Mn3S4 by using the full potential local orbital code. Considering different configurations such as nonmagnetic, ferromagnetic, ferrimagnetic, and antiferromagnetic, the magnetic ground state was found to be ferrimagnetic with the lowest total energy. The calculated effective magnetic moment is 10μBunit cell (two formula units) resulting from the opposite spin interaction between Mn (I) and Mn (II) atoms in Rb2Mn3S4. From our calculations, Rb2Mn3S4 is found to be a semiconductor with a direct energy band gap of 0.75 eV. With the inclusion of the Coulomb interaction (i.e., GGA+U), the band gap is found to rise to 2.34 eV for U = 4 eV.
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