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Thermal conductivity and thermal Hall effect in Bi- and Y-based high-T_c superconductors

机译:Bi和Y基高T_c超导体的导热率和霍尔效应

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Measurements of the thermal conductivity (k_(xx)) and the thermal Hall effect (k_(xy)) in high magnetic fields in Y- and Bi-based high-T_c superconductors are presented. We describe the experimental technique and test measurements on a simple metal (niobium). In the high-T_c superconductors k_(xx) and k_(xy) increase below T_c and show a maximum in their temperature dependence. k_(xx) has contributions from phonons and quasiparticle (QP) excitations, whereas k_(xy) is purely electronic. The strong increase of k_(xy) below T_c gives direct evidence for a strong enhancement of the QP contribution to the heat current and thus for a strong increase of the QP mean free path. Using k_(xy) and the magnetic field dependence of k_(xx) we separate the electronic thermal conductivity (K_(xx)~(el)) of the CuO_2-planes from the phononic thermal conductivity (k_(xx)~(ph)). In YBa_2Cu_3O_(7-δ) k_(xx)~(el) shows a pronounced maximum in the superconducting state. This maximum is much weaker in Bi_2Sr_2CaCu_2O_(8+δ), due to stronger impurity scattering. The maximum of k_(xx)~(el) is strongly suppressed by a magnetic field, which we attribute to the scattering of QPs on vortices. An additional magnetic field independent contribution to the maximum of k_(xx) occurs in YBa_2Cu_3O_(7-δ), reminiscent of the contribution of the CuO-chains, as determined from the anisotropy in untwined single crystals. Our data analysis reveals that below T_c as in the normal state a transport (τ) and a Hall (τ_H) relaxation time must be distinguished: The inelastic (i.e. temperature dependent) contribution to τ is strongly enhanced in the superconducting state, whereas τ_H displays the same temperature dependence as above T_c. We determine also the electronic thermal conductivity in the normal state from k_(xy) and the electrical Hall angle. It shows an unusual linear increase with temperature.
机译:提出了在基于Y和Bi的高T_c超导体中的高磁场中的热导率(k_(xx))和热霍尔效应(k_(xy))的测量方法。我们描述了一种简单的金属(铌)的实验技术和测试测量。在高T_c超导体中,k_(xx)和k_(xy)增加到T_c以下,并显示出它们的温度依赖性最大。 k_(xx)来自声子和准粒子(QP)激发,而k_(xy)是纯电子的。低于T_c的k_(xy)的强劲增加直接证明了QP对热流的贡献大大增强,从而大大提高了QP平均自由程。使用k_(xy)和k_(xx)的磁场依赖性,我们将CuO_2平面的电子热导率(K_(xx)〜(el))与声子热导率(k_(xx)〜(ph))分开。 )。在YBa_2Cu_3O_(7-δ)中,k_(xx)〜(el)在超导状态下显示出明显的最大值。由于杂质散射较强,Bi_2Sr_2CaCu_2O_(8 +δ)的最大值大大弱了。 k_(xx)〜(el)的最大值受到磁场的强烈抑制,这归因于QP在涡旋上的散射。由YBa_2Cu_3O_(7-δ)产生的最大k_(xx)的磁场无关的额外贡献,使人想起了CuO链的贡献,这是由未缠绕的单晶的各向异性确定的。我们的数据分析表明,在正常状态下低于T_c时,必须区分输运(τ)和霍尔(τ_H)弛豫时间:在超导状态下,对τ的非弹性(即与温度有关)的贡献会大大增强,而τ_H显示与以上T_c相同的温度依赖性。我们还根据k_(xy)和电霍尔角确定正常状态下的电子热导率。它显示出随温度的异常线性增加。

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