Thermal and Electrical Transport across a Magnetic Quantum Critical Point
H. Pfau, S. Hartmann, U. Stockert, P. Sun, S. Lausberg, M. Brando, S., Friedemann, C. Krellner, C. Geibel, S. Wirth, S. Kirchner, E. Abrahams, Q., Si, F. Steglich

TL;DR
This study investigates thermal and electrical transport near a magnetic quantum critical point in YbRh₂Si₂, revealing a breakdown of Landau quasiparticles and providing insights into non-Fermi-liquid behavior in correlated materials.
Contribution
It provides experimental evidence of quasiparticle breakdown at a magnetic QCP through thermal and electrical transport measurements, challenging the traditional Fermi liquid theory.
Findings
Wiedemann-Franz law holds above critical field Bc
Electrical conductivity exceeds thermal conductivity at Bc
Breakdown of quasiparticles at the quantum critical point
Abstract
A quantum critical point (QCP) arises at a continuous transition between competing phases at zero temperature. Collective excitations at magnetic QCPs give rise to metallic properties that strongly deviate from the expectations of Landau's Fermi liquid description, the standard theory of electron correlations in metals. Central to this theory is the notion of quasiparticles, electronic excitations which possess the quantum numbers of the bare electrons. Here we report measurements of thermal and electrical transport across the field-induced magnetic QCP in the heavy-fermion compound YbRhSi. We show that the ratio of the thermal to electrical conductivities at the zero-temperature limit obeys the Wiedemann-Franz (WF) law above the critical field, . This is also expected at , where weak antiferromagnetic order and a Fermi liquid phase form below 0.07 K ().…
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