Investigation on prospective thermoelectrics — cubic Nd-doped LMO and rhombohedral Cu4Mn2Te4 materials — first principles approach

IF 2.6 4区 物理与天体物理 Q2 PHYSICS, APPLIED
S. Priyadharshini, M. Sundareswari
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引用次数: 0

Abstract

Structural, electronic, magnetic and optical properties of Cu 4 Mn 2 Te 4 have been reported earlier by the authors, and here, the transport properties of the same are discussed along with the band structure investigation of the neodymium-doped cubic material LMO (LiMn 2 O 4 ), namely LiMn[Formula: see text]Nd[Formula: see text]O 4 compound, under spin polarized schemes through the First Principles calculations. The Full Potential-Linearized Augumented Plane Wave Method (FP-LAPW) method is adopted to investigate the electronic structures based on the framework of Density Functional Theory (DFT). Exchange potentials are treated using the Generalized Gradient Approximations (GGA). Cohesive energy calculations reveal that the ferromagnetic phase of LiMn[Formula: see text]Nd[Formula: see text]O 4 and the antiferromagnetic phase of Cu 4 Mn 2 Te 4 exhibits a stable phase. Of these, FM-LiMn[Formula: see text]Nd[Formula: see text]O 4 shows a semi-metallic-like behavior in spin-up channel and metallic behavior in spin-down channel whereas antiferromagnetic Cu 4 Mn 2 Te 4 exhibits a band gap in both spin-up and spin-down channels. Dirac points are identified at −0.0625[Formula: see text]eV in the band structure plot of FM-LiMn[Formula: see text]Nd[Formula: see text]O 4 at its high symmetry points [Formula: see text] and W which is an indication of high electron mobility at ambient condition. The presence of flat and dispersive bands around the Fermi energy level is an indication of high thermopower, and it is present in both the compounds FM-LiMn[Formula: see text]Nd[Formula: see text]O 4 and AFM-Cu 4 Mn 2 Te 4 . From the present computations, at 300[Formula: see text]K, a power factor range of ([Formula: see text] scaled by relaxation time in [Formula: see text]W/msK 2 ) [Formula: see text] and [Formula: see text] is obtained for ferromagnetic LiMn[Formula: see text]Nd[Formula: see text]O 4 compounds at up and down spins, respectively. A typical power factor ([Formula: see text]Wm[Formula: see text]s[Formula: see text]K[Formula: see text]) of [Formula: see text] and [Formula: see text] is obtained for antiferromagnetic Cu 4 Mn 2 Te 4 at 325[Formula: see text]K required for good thermoelectric performance.
前景热电材料的研究-立方掺nd LMO和菱面体Cu4Mn2Te4材料-第一性原理方法
本文讨论了Cu 4 Mn 2 Te 4的结构、电子、磁性和光学性质,并通过第一原理计算研究了自旋极化方案下掺钕立方材料LMO (limn2o4),即LiMn[公式:见文]Nd[公式:见文]2o4化合物的能带结构。采用基于密度泛函理论(DFT)框架的全势线性化增强平面波方法(FP-LAPW)对电子结构进行了研究。交换势用广义梯度近似(GGA)处理。内聚能计算表明,LiMn[公式:见文]Nd[公式:见文]o4的铁磁相和cu4 Mn 2 Te 4的反铁磁相表现为稳定相。其中,FM-LiMn[公式:见文]Nd[公式:见文]o4在自旋向上的通道中表现出半金属的行为,在自旋向下的通道中表现出金属的行为,而反铁磁性cu4mn2te 4在自旋向上和自旋向下的通道中都表现出带隙。在FM-LiMn[公式:见文]的能带结构图中,Dirac点在−0.0625[公式:见文]eV[公式:见文]Nd[公式:见文]O 4在其高对称点[公式:见文]和W,这是环境条件下高电子迁移率的指示。在费米能级附近存在平坦和色散带是高热能的标志,它存在于两种化合物中:FM-LiMn[公式:见文]Nd[公式:见文]O 4和AFM-Cu 4 Mn 2 Te 4。从目前的计算中,在300[公式:见文]K下,对于铁磁性的LiMn[公式:见文]Nd[公式:见文]o4化合物,分别得到了([公式:见文])[公式:见文]和[公式:见文]的功率因数范围([公式:见文]在[公式:见文]W/msK 2中按弛豫时间缩放)[公式:见文]和[公式:见文]。得到了反铁磁cu4 Mn 2 Te 4在325[公式:见文]K为良好热电性能所需的[公式:见文]和[公式:见文]的典型功率因数([公式:见文]Wm[公式:见文]s[公式:见文]K[公式:见文])。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
International Journal of Modern Physics B
International Journal of Modern Physics B 物理-物理:凝聚态物理
CiteScore
3.70
自引率
11.80%
发文量
417
审稿时长
3.1 months
期刊介绍: Launched in 1987, the International Journal of Modern Physics B covers the most important aspects and the latest developments in Condensed Matter Physics, Statistical Physics, as well as Atomic, Molecular and Optical Physics. A strong emphasis is placed on topics of current interest, such as cold atoms and molecules, new topological materials and phases, and novel low dimensional materials. One unique feature of this journal is its review section which contains articles with permanent research value besides the state-of-the-art research work in the relevant subject areas.
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