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人工晶体学报 ›› 2017, Vol. 46 ›› Issue (9): 1803-1808.

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Mn掺杂半金属铁磁体Fe2Si电磁特性的第一性原理计算

李瑞杰;杨吟野;岑伟富;吕林;谢泉   

  1. 贵州大学大数据与信息工程学院,贵阳550025;贵州民族大学,贵州省光电信息分析与处理特色重点实验室,贵阳550025;贵州民族大学,贵州省光电信息分析与处理特色重点实验室,贵阳550025;贵州民族大学材料科学与工程学院,贵阳550025;贵州大学大数据与信息工程学院,贵阳,550025
  • 出版日期:2017-09-15 发布日期:2021-01-20
  • 基金资助:
    贵州省科技厅联合基金项目([2016]7077);贵州省教育厅青年科技人才成长项目([2016]166);贵州大学研究生创新基金项目(研理工2017011)

Electromagnetic Properties of Mn-doped Half-metallic Ferromagnet Fe2 Si Calculated by First-principles

LI Rui-jie;YANG Yin-ye;CEN Wei-fu;LYU Lin;XIE Quan   

  • Online:2017-09-15 Published:2021-01-20

摘要: 采用基于密度泛函理论第一性原理的贋势平面波方法,计算了不同比例Mn掺杂Fe2-xMnxSi体系的电子结构和磁学特性,分析了不同比例Mn掺杂对Fe2-xMnxSi体系电磁特性的影响.计算结果表明:不同比例Mn掺杂Fe2-xMnxSi体系是铁磁体,自旋向上的能带结构穿过费米面表现金属特性,未掺杂Fe2Si的半金属隙为0.164eV;掺杂比例为8.3;时,自旋向下部分转变为L间的直接带隙半导体,Fe2-xMnxSi(x=0.17)体系呈现半金属特性;掺杂比例为12.5;时,自旋向下部分转变为A间的直接带隙半导体,Fe2-xMnxSi(x=0.25)体系呈现半金属特性;掺杂比例为25;时,自旋向下部分的带隙值接近于0,Fe2-xMnxSi(x=0.5)体系呈现金属特性.Mn掺杂使Fe2-xMnxSi体系的能带结构和电子态密度向低能方向移动,费米能级落入自旋向下的禁带之中,使得自旋极化率达到100;.Fe2-xMnxSi体系的半金属性和磁性主要来源于Fe-3d电子与Mn-3d电子之间的d-d交换,Si-3p电子与Fe-3d电子之间的p-d杂化.这些结果为半金属铁磁体Fe2Si的电磁调控提供了有效的理论指导.

关键词: Mn掺杂;电子结构;磁学特性;第一性原理

Abstract: The electronic structure and magnetic properties of Mn-doped Fe2-x Mnx Si systems have been calculated by the first-principles pseudo-potential method based on density functional theory ( DFT) .The results show that the Mn-doped Fe2-x Mnx Si system is a ferromagnet with different ratios of Mn , the half-metallic gap of undoped Fe2Si is 0.164 eV.When the doping ratio is 8.3;, the spin-down part is transformed into the direct bandgap semiconductors of L .The Fe2-x MnxSi (x=0.17) system exhibits half-metallic properties .When the doping ratio is 12 .5;, the spin-down part is transformed into the direct bandgap semiconductor of A, and the Fe2-x MnxSi (x =0.25) system exhibits half-metallic properties .The system is transformed into metal when the doping ratio is 25;.Mn-doped makes the band structure and electron density of Fe 2-x Mnx Si systems move in the low energy direction , and the Fermi level falls into the spin-down band gap , which makes the spin polarization rate reach 100;.The half-metallic and magnetic properties of Fe 2-x Mn x Si systems are mainly derived from the d-d exchange between Fe-3d and Mn-3d electrons, p-d hybridization between Si-3p and Fe-3d electrons.The results provide effective theoretical guidance for the electromagnetic control of half-metallic ferromagnet Fe 2 Si.

Key words: The electronic structure and magnetic properties of Mn-doped Fe2-x Mnx Si systems have been calculated by the first-principles pseudo-potential method based on density functional theory ( DFT) .The results show that the Mn-doped Fe2-x Mnx Si system is a ferromagnet with different ratios of Mn , the half-metallic gap of undoped Fe2Si is 0.164 eV.When the doping ratio is 8.3;, the spin-down part is transformed into the direct bandgap semiconductors of L .The Fe2-x MnxSi (x=0.17) system exhibits half-metallic properties .When the doping ratio is 12 .5;, the spin-down part is transformed into the direct bandgap semiconductor of A, and the Fe2-x MnxSi (x =0.25) system exhibits half-metallic properties .The system is transformed into metal when the doping ratio is 25;.Mn-doped makes the band structure and electron density of Fe 2-x Mnx Si systems move in the low energy direction , and the Fermi level falls into the spin-down band gap , which makes the spin polarization rate reach 100;.The half-metallic and magnetic properties of Fe 2-x Mn x Si systems are mainly derived from the d-d exchange between Fe-3d and Mn-3d electrons, p-d hybridization between Si-3p and Fe-3d electrons.The results provide effective theoretical guidance for the electromagnetic control of half-metallic ferromagnet Fe 2 Si.

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