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避免 BaFe(2-x)Ni(x)As2 中的量子临界和磁弹耦合。

Avoided quantum criticality and magnetoelastic coupling in BaFe(2-x)Ni(x)As2.

机构信息

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.

出版信息

Phys Rev Lett. 2013 Jun 21;110(25):257001. doi: 10.1103/PhysRevLett.110.257001. Epub 2013 Jun 18.

DOI:10.1103/PhysRevLett.110.257001
PMID:23829752
Abstract

We study the structural and magnetic orders in electron-doped BaFe(2-x)Ni(x)As2 by high-resolution synchrotron x-ray and neutron scatterings. Upon Ni doping x, the nearly simultaneous tetragonal-to-orthorhombic structural (T(s)) and antiferromagnetic (T(N)) phase transitions in BaFe2As2 are gradually suppressed and separated, resulting in T(s)>T(N) with increasing x, as was previously observed. However, the temperature separation between T(s) and T(N) decreases with increasing x for x≥0.065, tending toward a quantum bicritical point near optimal superconductivity at x≈0.1. The zero-temperature transition is preempted by the formation of a secondary incommensurate magnetic phase in the region 0.088≲x≲0.104, resulting in a finite value of T(N)≈T(c) + 10  K above the superconducting dome around x≈0.1. Our results imply an avoided quantum critical point, which is expected to strongly influence the properties of both the normal and superconducting states.

摘要

我们通过高分辨率同步加速器 X 射线和中子散射研究了电子掺杂 BaFe(2-x)Ni(x)As2 中的结构和磁有序。随着 Ni 掺杂量 x 的增加,BaFe2As2 中近乎同时的四方-正交结构(T(s))和反铁磁(T(N))相变逐渐被抑制和分离,导致 T(s)>T(N),这与之前的观察结果一致。然而,对于 x≥0.065,T(s)和 T(N)之间的温度分离随着 x 的增加而减小,趋向于在最佳超导附近的量子双临界点 x≈0.1。在超导穹顶附近的 x≈0.1 左右,由于在 0.088≲x≲0.104 区域中形成了二次非共格磁相,零温转变被预先阻止,导致 T(N)≈T(c) + 10  K 的有限值,T(c)为超导转变温度。我们的结果表明存在一个避免量子临界点,这预计会强烈影响正常态和超导态的性质。

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