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The transport properties of iron-based superconductors

Li Miao-Cong Tao Qian Xu Zhu-An

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The transport properties of iron-based superconductors

Li Miao-Cong, Tao Qian, Xu Zhu-An
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  • There are a variety of order states in iron-based pnictides, such as electronic nematic phase, spin density wave, and so on, which leads to plenty of novel physical phenomena. The measurements of transport properties can provide extremely useful information for understanding of the low-energy excitations of iron-based superconductors. Due to the multi-band electronic structure in iron-based pnictides, the temperature dependence of resistivity and Hall coefficient varies with different systems, however, there are no evidence for the pseudo-gap opening in the normal state which is a common feature in underdoped high-$T_{\rm{c}}$ cuprates. In the hole-doped iron-based superconductors, the Hall coefficient changes its sign in low temperatures, and meanwhile the resistivity shows a broad hump in the same temperature range. Such a behavior is proposed as a crossover from incoherent to coherent transport. The Seebeck coefficients of iron-based superconductors also show remarkable differences from the cuprates. In iron-based superconductors, the absolute value of Seebeck coefficients in the normal state becomes the largest at the optimally doping point with highest $T_{\rm{c}}$, which is probably related to the strong inter-band scattering. The Nernst effect in the normal state of iron-based superconductors indicates that superconducting phase fluctuations is not obvious above $T_{\rm{c}}$, which is also significantly different from the cuprates. These unusual thermoelectric properties observed in iron-based superconductors have not been observed in the nickel-based pnictide superconductors with the analogous structure, i.e., LaNiAsO, and the nickel-based superconductors behave more like a usual metal. All these results above illustrate that these unusual transport properties of iron-based superconductors are inherently associated with their high temperature superconductivity, and these factors should be taken into account in the theory on its superconducting mechanism.
      Corresponding author: Xu Zhu-An, zhuan@zju.edu.cn
    • Funds: Project supported by the National Key Projects for Research & Development of China (Grant No. 2016YFA0300402), and the National Natural Science Foundation of China (Grant No.11774305)
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  • 图 1  各掺杂浓度下的面内电阻率随温度变化的曲线, 分别为以下样品: (a) Ba(Fe1–xCox)2As2, (b) BaFe2(As1–xPx)2, (c) Ba1–xKxFe2As2[19]

    Figure 1.  Doping evolution of the temperature dependence of the in-plane resistivity for (a) Ba(Fe1–xCox)2As2, (b) BaFe2(As1–xPx)2, and (c) Ba1–xKxFe2As2[19]

    图 2  空穴掺杂的“122”体系的霍尔系数随温度的变化[38]

    Figure 2.  The temperature dependence of Hall coefficients for hole-doping “122”-type iron-based superconductors[38]

    图 3  (a) 样品SmFe1–xCoxAsO随温度变化的热电势, (b) 热电势绝对值及超导转变温度随掺杂浓度的变化[45]

    Figure 3.  (a) The temperature dependence of Seebeck coefficients for SmFe1–xCoxAsO, (b) Doping dependence of thermopower, |S(300 K)|, |S'(300 K)| and superconducting transition temperature $T^{\rm{mid}}_{{\rm{c}}}$ for SmFe1–xCoxAsO samples[45]

    图 4  多个体系铁基超导体的热电势最大值与$T_{\rm{c}}$之间的关系. 图中未加引文的部分为本文作者尚未发表的数据

    Figure 4.  The relation between the maximum of thermopower and the $T_{\rm{c}}$ for various iron-based superconductors. The unreferenced portion of the figure is the unpublished data

    图 5  能斯特系数与温度之间的曲线, 分别为: (a) “1111”体系[49]; (b) “122”体系中. 图中BaFe2As2的结果与文献[60]一致

    Figure 5.  The temperature dependence of Nernst coefficients for (a) “1111”-type[49]; (b) “122”-type. The result of BaFe2As2 is consistent with the report in the Ref. [60]

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Metrics
  • Abstract views:  6820
  • PDF Downloads:  533
  • Cited By: 0
Publishing process
  • Received Date:  04 November 2020
  • Accepted Date:  25 December 2020
  • Available Online:  24 December 2020
  • Published Online:  05 January 2021

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