论文标题

各向同性普兰克散射率的线性温度电阻率

Linear-in temperature resistivity from an isotropic Planckian scattering rate

论文作者

Grissonnanche, G., Fang, Y., Legros, A., Verret, S., Laliberté, F., Collignon, C., Zhou, J., Graf, D., Goddard, P., Taillefer, L., Ramshaw, B. J.

论文摘要

各种“奇怪的金属”具有电阻率,与温度为$ t \ rightarrow 0 $线性降低,与传统的金属相比,电阻率降低为$ t^2 $。该$ t $ - 线性电阻率已归因于载体散射的速度为$ \ hbar/τ=αk_ {\ rm b} t $,其中$α$是订单统一的常数。在各种材料上观察到散射速率和温度之间的这种简单关系,这表明散射的基本上限 - “ Planckian极限” - 但对此极限的基本起源知之甚少。在这里,我们报告了ND-LSCO的角度依赖性磁倍率(ADMR)的测量---掺杂孔的库酸盐,显示出$ t $ - 线性电阻率,降至最低测量的温度。 ADR揭示了一个定义明确的费米表面,该表面与角度分辨的光发射光谱(ARPES)测量数量同意,并揭示了$ t $ - 线性散射速率,使Planckian限制饱和,即$ $ $α= 1.2 \ pm 0.4 $。值得注意的是,我们发现,与“热点”模型的期望相反,这种普朗克散射速率是各向同性的,即它独立于方向。我们的发现表明,奇怪金属中的$ t $线性电阻率是由于动量独立的非弹性散射率而出现的,该弹性散射速率达到了普兰克限制。

A variety of "strange metals" exhibit resistivity that decreases linearly with temperature as $T\rightarrow 0$, in contrast with conventional metals where resistivity decreases as $T^2$. This $T$-linear resistivity has been attributed to charge carriers scattering at a rate given by $\hbar/τ=αk_{\rm B} T$, where $α$ is a constant of order unity. This simple relationship between the scattering rate and temperature is observed across a wide variety of materials, suggesting a fundamental upper limit on scattering---the "Planckian limit"---but little is known about the underlying origins of this limit. Here we report a measurement of the angle-dependent magnetoresistance (ADMR) of Nd-LSCO---a hole-doped cuprate that displays $T$-linear resistivity down to the lowest measured temperatures. The ADMR unveils a well-defined Fermi surface that agrees quantitatively with angle-resolved photoemission spectroscopy (ARPES) measurements and reveals a $T$-linear scattering rate that saturates the Planckian limit, namely $α= 1.2 \pm 0.4$. Remarkably, we find that this Planckian scattering rate is isotropic, i.e. it is independent of direction, in contrast with expectations from "hot-spot" models. Our findings suggest that $T$-linear resistivity in strange metals emerges from a momentum-independent inelastic scattering rate that reaches the Planckian limit.

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