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首页> 外文期刊>Physics Letters, A >First principles study on the structural, magnetic, electronic and optical properties of un-doped and La-doped BiFe0.75Mn0.125Ti0.125O3
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First principles study on the structural, magnetic, electronic and optical properties of un-doped and La-doped BiFe0.75Mn0.125Ti0.125O3

机译:未掺杂和掺杂La的BiFe0.75Mn0.125Ti0.125O3的结构,磁性,电子和光学性质的基本原理研究

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Based on the generalized gradient approximation (GGA), the structural, magnetic, electronic and optical properties of BiFe0.75Ti0.125Mn0.125O3 (TM) and Bi1-yLayFe0.75Ti0.125Mn0.125O3 (y = 0.125, 0.25) (LTM) were researched by the first principles. Compared with the pure BiFeO3 (zero magnetic moment), the magnetic moment of TM gets improved greatly and the value computed here is similar to 3 mu(B), while La doping almost has no effect on that of TM. Ti and Mn co-doping converts the indirect band gap of BiFeO3 (2.20 eV) to a direct band gap of TM (0.95 eV). The bandwidth of TM is similar to that of LTM1 (1 La atom, y = 0.125) within the tolerance, but smaller than that of LTM2 (2 La atoms, y = 0.25). This is consistent with their gradually increased absorption edges to infrared region, and suggests that doping La into the B sites of TM makes it more potential application on photovoltaic. According to the results of reflectivity, (Ti, Mn)-codoped BiFeO3 is transparent, while LTM is nontransparent in the visible light region which indicates more potential valuable for visible-light-responsive devices. To gain some insight into the optical properties of the samples, three relationships have been discussed: (1) the reflectivity and energy loss function, (2) the extinction coefficient and the imaginary part of the dielectric function, and (3) the refractive index and the real part of the dielectric function. (C) 2016 Elsevier B.V. All rights reserved.
机译:基于广义梯度近似(GGA),BiFe0.75Ti0.125Mn0.125O3(TM)和Bi1-yLayFe0.75Ti0.125Mn0.125O3(y = 0.125,0.25)(LTM)的结构,磁性,电子和光学性质由第一原理研究。与纯BiFeO3(零磁矩)相比,TM的磁矩得到了很大的改善,此处计算的值与3 mu(B)相似,而La掺杂对TM的磁化几乎没有影响。 Ti和Mn共掺杂将BiFeO3的间接带隙(2.20 eV)转换为TM的直接带隙(0.95 eV)。在容差范围内,TM的带宽与LTM1的带宽(1 La原子,y = 0.125)相似,但小于LTM2的带宽(2 La原子,y = 0.25)。这与它们逐渐增加的对红外区的吸收边相吻合,并表明将La掺杂到TM的B位置使其在光伏领域具有更大的应用潜力。根据反射率的结果,掺有(Ti,Mn)的BiFeO3是透明的,而LTM在可见光区域是不透明的,这表明对可见光响应设备更有价值。为了深入了解样品的光学特性,已讨论了三个关系:(1)反射率和能量损失函数,(2)消光系数和介电函数的虚部,以及(3)折射率以及介电函数的实部(C)2016 Elsevier B.V.保留所有权利。

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