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重费米子半金属PrOsGe具有良好的热电性能。

Promising thermoelectric properties of heavy-fermion semimetal PrOsGe.

作者信息

Ogunbunmi Michael O, Strydom André M

机构信息

Highly Correlated Matter Research Group, Physics Department, University of Johannesburg, P.O. Box 524, Auckland Park 2006, South Africa.

出版信息

J Phys Condens Matter. 2020 Jul 6;32(40). doi: 10.1088/1361-648X/ab9da2.

DOI:10.1088/1361-648X/ab9da2
PMID:32644946
Abstract

Here we report the magnetic, electronic and thermal transport properties of the heavy-fermion semimetal PrOsGewith a cage-like structure by means of magnetic susceptibility,(), isothermal magnetization,(,), electrical resistivity,(,), Hall coefficient,(), specific heat,(), thermal conductivity,() and thermoelectric power,().() and() show semimetallic features in a manner that mimics a thermal activated behaviour with an activation energy, Δ/= 6.5 K indicating the opening of a small energy gap in the material. At low temperatures, a Sommerfeld coefficient,= 128 mJ (molK) observed indicates a mass enhancement of the quasiparticles at low temperatures which bears witness to a heavy fermion state in PrOsGe. A Wilson-Sommerfeld ratio,and the dimensionless ratio,/of 1.01 and 0.62 ± 0.018 observed, respectively, are in good agreement with the Fermi liquid scenario.() and() reveal hole dominated transport (p-type material) with a relatively large room temperature value of() = 32.85 ± 0.98V K. A room temperature low value of() = 1.61 W K mleads to a thermoelectric figure of merit,= 0.03 ± 0.001 which is comparable to values achieved in several clathrates around the same temperature. Features from() and() favour the realization of a highervalue at elevated temperatures.

摘要

在此,我们通过磁化率(χ)、等温磁化强度(M,H)、电阻率(ρ,T)、霍尔系数(RH)、比热(C,T)、热导率(κ,T)和热电功率(S,T),报道了具有笼状结构的重费米子半金属PrOsGe的磁性、电子和热输运性质。ρ(T)和C(T)呈现出半金属特征,其方式类似于具有激活能Δ/= 6.5 K的热激活行为,表明材料中存在一个小的能隙。在低温下,观察到的索末菲系数γ = 128 mJ(mol K²)表明低温下准粒子质量增强,这证明了PrOsGe中存在重费米子态。观察到的威尔逊 - 索末菲比γ/γ0和无量纲比γ/γH分别为1.01和0.62 ± 0.018,与费米液体模型吻合良好。RH(T)和S(T)揭示了空穴主导的输运(p型材料),室温下RH值相对较大,为(RH) = 32.85 ± 0.98 μV K。室温下κ值较低,为(κ) = 1.61 W K⁻¹ m⁻¹,导致热电优值ZT = 0.03 ± 0.001,这与在相同温度下几种笼合物所达到的值相当。κ(T)和S(T)的特征有利于在高温下实现更高的ZT值。

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