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[论文解读] EuCd$_2$As$_2$: a magnetic semiconductor

David Santos‐Cottin, Ivan Mohelský|PubMed|Jan 19, 2023
Topological Materials and Phenomena参考文献 39被引用 7
一句话总结

本研究将 EuCd₂As₂ 重新定义为具有 0.77 eV 带隙的磁性半导体,而非拓扑半金属。通过结合输运、光学和超快光电子能谱测量,研究发现外加磁场通过局域 Eu 4f 自旋与能带态之间的强交换耦合,使带隙减少 125 meV,且在整个温度和磁场范围内均保持半导体特性。

ABSTRACT

EuCd_{2}As_{2} is now widely accepted as a topological semimetal in which a Weyl phase is induced by an external magnetic field. We challenge this view through firm experimental evidence using a combination of electronic transport, optical spectroscopy, and excited-state photoemission spectroscopy. We show that the EuCd_{2}As_{2} is in fact a semiconductor with a gap of 0.77 eV. We show that the externally applied magnetic field has a profound impact on the electronic band structure of this system. This is manifested by a huge decrease of the observed band gap, as large as 125 meV at 2 T, and, consequently, by a giant redshift of the interband absorption edge. However, the semiconductor nature of the material remains preserved. EuCd_{2}As_{2} is therefore a magnetic semiconductor rather than a Dirac or Weyl semimetal, as suggested by ab initio computations carried out within the local spin-density approximation.

研究动机与目标

  • 重新评估 EuCd₂As₂ 的电子特性,挑战其被广泛接受为磁性外尔半金属的分类。
  • 确定在外加磁场下观测到的电子响应是否源于拓扑能带交叉,还是真实的带隙。
  • 研究局域 Eu 4f 自旋在调控 EuCd₂As₂ 中大范围、可调谐的能带结构变化中的作用。
  • 评估基于局域自旋密度近似(LSDA)的从头算计算在描述该强关联体系电子性质时的有效性。
  • 确定磁质诱导的带隙减小是否为本征且在顺磁相中持久存在。

提出的方法

  • 在超净单晶上进行电子输运测量,以确定载流子浓度并确认绝缘行为。
  • 采用红外反射率和透射测量等光学光谱技术,提取光学电导率的实部,并检测无 Drude 响应。
  • 利用泵浦-探测角分辨光电子能谱(ARPES),在皮秒时间尺度上直接探测带隙和载流子动力学。
  • 在高达 16 T 和 140 K 的条件下进行磁光反射率和透射率测量,以绘制带边和带隙随磁场与温度的变化关系。
  • 对多层光学响应进行建模,从反射率和透射率数据中提取光学电导率实部 σ₁。
  • 采用有效交换耦合模型 ΔE_g = -½ J_eff S M(T,H)/M_S,量化磁场依赖的带隙减小,并提取 J_eff ≈ 80 meV。
Figure 1: (a) Resistivity as a function of temperature for an insulating and a metallic sample. Inset shows the structure of EuCd 2 As 2 , with Eu atoms shown in green, Cd atoms in yellow, and As atoms in purple. Magnetic properties, (b) dc susceptibility, and (c) magnetization at 4 K, are shown for
Figure 1: (a) Resistivity as a function of temperature for an insulating and a metallic sample. Inset shows the structure of EuCd 2 As 2 , with Eu atoms shown in green, Cd atoms in yellow, and As atoms in purple. Magnetic properties, (b) dc susceptibility, and (c) magnetization at 4 K, are shown for

实验结果

研究问题

  • RQ1EuCd₂As₂ 真的是拓扑半金属,还是具有一个在先前研究中被误解的根本带隙?
  • RQ2外加磁场在多大程度上改变 EuCd₂As₂ 的电子能带结构?该效应是否可逆或持久?
  • RQ3磁场诱导的带隙减小是否源于拓扑相变,还是源于与局域 Eu 4f 自旋的自旋依赖交换相互作用?
  • RQ4在顺磁相中观测到的带隙调制是否具有鲁棒性,表明存在长程磁序或强局域交换耦合?
  • RQ5观测到的磁场依赖带隙变化能否通过涉及 Eu 4f 自旋与能带态的等效交换耦合模型进行定量解释?

主要发现

  • EuCd₂As₂ 是一种具有 0.77 eV 基本带隙的半导体,泵浦-探测 ARPES 和光学电导率测量结果证实无 Drude 响应。
  • 在 2 T 磁场下,带隙最多减少 125 meV,且带隙减小量与 Eu 4f 自旋的磁化强度成正比。
  • 带载流子与 Eu 4f 自旋之间的有效交换耦合强度 J_eff 估算约为 80 meV,表明存在强烈的局域交换相互作用。
  • 带隙减小效应持续至 140 K,即使在顺磁相中也保持不变,表明该效应不限于反铁磁基态。
  • 磁场依赖的带边位移与磁化曲线高度吻合,证实能带结构由 Eu 磁性亚晶格通过交换耦合所调控。
  • 无 Drude 成分且存在强 Reststrahlen 振子模式,证实材料的绝缘特性,排除了金属或半金属行为。
Figure 2: (a) Near infrared transmission showing the interband absorption edge at low fields, $B<1$ T. (b) Color plot of relative magneto-transmission, $T_{B}/T_{\text{AVR}}$ , in a broad energy range, and up to 2 T. (c) Magneto-transmission $T_{B}/T_{0}$ and (d) its first energy-derivative, $d/dE[T
Figure 2: (a) Near infrared transmission showing the interband absorption edge at low fields, $B<1$ T. (b) Color plot of relative magneto-transmission, $T_{B}/T_{\text{AVR}}$ , in a broad energy range, and up to 2 T. (c) Magneto-transmission $T_{B}/T_{0}$ and (d) its first energy-derivative, $d/dE[T

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