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Ferromagnetic Quantum Critical Point in the Heavy-Fermion Metal YbNi <sub>4</sub> (P <sub>1−</sub> <i> <sub>x</sub> </i> As <i> <sub>x</sub> </i> ) <sub>2</sub>
167
Citations
37
References
2013
Year
Superconducting MaterialMagnetic PropertiesEngineeringMagnetic MaterialsCritical CurrentsMagnetismSuperconductivityQuantum MaterialsHigh Tc SuperconductorsQuantum MatterSuperconducting DevicesContinuous Phase ChangeLow-temperature SuperconductivityMaterials ScienceQuantum ScienceHigh-tc SuperconductivityPhysicsCondensed Matter TheoryQuantum MagnetismSpintronicsAbsolute ZeroHigh-temperature SuperconductivityNatural SciencesApplied PhysicsCondensed Matter PhysicsUnconventional Superconductivity
Unconventional superconductivity and other previously unknown phases of matter exist in the vicinity of a quantum critical point (QCP): a continuous phase change of matter at absolute zero. Intensive theoretical and experimental investigations on itinerant systems have shown that metallic ferromagnets tend to develop via either a first-order phase transition or through the formation of intermediate superconducting or inhomogeneous magnetic phases. Here, through precision low-temperature measurements, we show that the Grüneisen ratio of the heavy fermion metallic ferromagnet YbNi(4)(P(0.92)As(0.08))(2) diverges upon cooling to T = 0, indicating a ferromagnetic QCP. Our observation that this kind of instability, which is forbidden in d-electron metals, occurs in a heavy fermion system will have a large impact on the studies of quantum critical materials.
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