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Origin of the charge density wave state inBaFe2Al9
Physical Review B ( IF 3.2 ) Pub Date : 2024-11-06 , DOI: 10.1103/physrevb.110.195118 Yuping Li, Mingfeng Liu, Jiangxu Li, Jiantao Wang, Junwen Lai, Dongchang He, Ruizhi Qiu, Yan Sun, Xing-Qiu Chen, Peitao Liu
Physical Review B ( IF 3.2 ) Pub Date : 2024-11-06 , DOI: 10.1103/physrevb.110.195118 Yuping Li, Mingfeng Liu, Jiangxu Li, Jiantao Wang, Junwen Lai, Dongchang He, Ruizhi Qiu, Yan Sun, Xing-Qiu Chen, Peitao Liu
Recently, a first-order phase transition associated with charge density wave (CDW) has been observed at low temperatures in intermetallic compound B a F e 2 A l 9 . However, this transition is absent in its isostructural sister compound B a C o 2 A l 9 . Consequently, an intriguing question arises as to the underlying factors that differentiate B a F e 2 A l 9 from B a C o 2 A l 9 and drive the CDW transition in B a F e 2 A l 9 . Here, we set out to address this question by conducting a comparative ab initio study of the electronic structures, lattice dynamics, and electron-phonon interactions of their high-temperature phases. We find that both compounds are dynamically stable with similar phonon dispersions. The electronic structure calculations reveal that both compounds are nonmagnetic metals; however, they exhibit distinct band structures around the Fermi level. In particular, B a F e 2 A l 9 exhibits a higher density of states at the Fermi level with dominant partially filled Fe-3 𝑑 states and a more intricate Fermi surface. This leads to an electronic instability of B a F e 2 A l 9 toward the CDW transition, which is manifested by the diverged electronic susceptibility at the CDW wave vector 𝐪 C D W = ( 0 . 5 , 0 , 0 . 3 ) , observable in both the real and imaginary parts. Conversely, B a C o 2 A l 9 does not display such behavior, aligning well with experimental observations. Although the electron-phonon interactions in B a F e 2 A l 9 surpass those in B a C o 2 A l 9 by two orders of magnitude, the strength is relatively weak at the CDW wave vector, suggesting that the CDW in B a F e 2 A l 9 is primarily driven by electronic factors.
中文翻译:
BaFe2Al9 中电荷密度波态的由来
最近,在低温下在金属间化合物BaFe2Al9 中观察到与电荷密度波 (CDW) 相关的一阶相变。然而,这种转变在其同构姐妹化合物 BaCo2Al9 中不存在。因此,出现了一个有趣的问题,即区分 BaFe2Al9 和 BaCo2Al9 并驱动 BaFe2Al9 中 CDW 转变的潜在因素。在这里,我们通过对高温相的电子结构、晶格动力学和电子-声子相互作用进行从头开始的比较研究来解决这个问题。我们发现这两种化合物在相似的声子分散体中都是动态稳定的。电子结构计算表明,这两种化合物都是非磁性金属;然而,它们在费米能级周围表现出不同的能带结构。特别是,BaFe2Al9 在费米能级上表现出更高的态密度,具有占主导地位的部分填充 Fe-3d 态和更复杂的费米表面。这导致 BaFe2Al9 向 CDW 跃迁产生电子不稳定性,这表现为 CDW 波矢量 qCDW=(0.5,0,0.3) 处的发散电子磁化率,在实部和虚部都可以观察到。相反,BaCo2Al9 没有表现出这种行为,与实验观察结果非常一致。 尽管 BaFe2Al9 中的电子-声子相互作用比 BaCo2Al9 中的电子-声子相互作用高出两个数量级,但在 CDW 波矢量处的强度相对较弱,这表明 BaFe2Al9 中的 CDW 主要由电子因素驱动。
更新日期:2024-11-06
中文翻译:
BaFe2Al9 中电荷密度波态的由来
最近,在低温下在金属间化合物