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arXiv 2002.08352cond-mat.str-el
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Ta $_2$ NiSe $_5$中由带心光学声子不稳定性引起的正交-单斜相变

Orthorhombic-to-monoclinic transition in Ta$_2$NiSe$_5$ due to a zone-center optical phonon instability

Alaska Subedi

摘要:

我研究的动力学不稳定性在Ta $_2$ NiSe $_5$使用密度泛函理论为基础的计算。计算的声子色散显示出两个不稳定的光学分支。所有的声学分支都是稳定的,这表明弹性不稳定性不是实验观察到的正交单斜结构转变的主要原因。光学分支的最大不稳定性发生在区域中心,与实验观察一致,即单位晶胞的大小在相变中不会倍增。不稳定模式有两个不稳定模式:$B_{1g}$和$B_{2g}$。充分的结构松弛最小化的力量和应力发现,单斜$C2/c$结构对应的$B_{2g}$不稳定性具有最低的能量。电子结构计算表明,这种低对称结构具有相当大的带隙。这表明$B_{2g}$的带心光学声子不稳定性是导致相变的主要原因。当从上面接近跃迁时,观察到$B_{2g}$区心声子模的软化将证实这里提出的机制。如果材料中存在的$B_{2g}$模式都没有软化,这意味着跃迁是由电子或弹性不稳定性引起的。

英文摘要:

I study dynamical instabilities in Ta$_2$NiSe$_5$ using density functional theory based calculations. The calculated phonon dispersions show two unstable optical branches. All the acoustic branches are stable, which shows that an elastic instability is not the primary cause of the experimentally observed orthorhombic-to-monoclinic structural transition in this material. The largest instability of the optical branches occurs at the zone center, consistent with the experimental observation that the size of the unit cell does not multiply across the phase transition. The unstable modes have the irreps $B_{1g}$ and $B_{2g}$. Full structural relaxations minimizing both the forces and stresses find that the monoclinic $C2/c$ structure corresponding to the $B_{2g}$ instability has the lowest energy. Electronic structure calculations show that this low-symmetry structure has a sizable band gap. This suggest that a $B_{2g}$ zone-center optical phonon instability is the primary cause of the phase transition. An observation of a softening of a $B_{2g}$ zone-center phonon mode as the transition is approached from above would confirm the mechanism proposed here. If none of the $B_{2g}$ modes present in the material soften, this would imply that the transition is caused by electronic or elastic instability.

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