Unconventional Strong Spin-Fluctuation Effects around the Critical Pressure of the Itinerant Ising-Type Ferromagnet URhAl
arXiv:1501.06701 · doi:10.1103/PhysRevB.91.125115
Abstract
Resistivity measurements were performed for the itinerant Ising-type ferromagnet URhAl at temperatures down to 40 mK under high pressure up to 7.5 GPa, using single crystals. We found that the critical pressure of the Curie temperature exists at around ~ 5.2 GPa. Near , the -coefficient of the Fermi-liquid resistivity term below is largely enhanced with a maximum around 5.2-5.5 GPa. Above , the exponent of the resistivity deviates from 2. At , it is close to , which is expected by the theory of three-dimensional ferromagnetic spin fluctuations for a 2nd-order quantum-critical point (QCP). However, disappears as a 1st-order phase transition, and the critical behavior of resistivity in URhAl cannot be explained by the theory of a 2nd-order QCP. The 1st-order nature of the phase transition is weak, and the critical behavior is still dominated by the spin fluctuation at low temperature. With increasing pressure, the non-Fermi-liquid behavior is observed in higher fields. Magnetic field studies point out a ferromagnetic wing structure with a tri-critical point (TCP) at ~ 4.8-4.9 GPa in URhAl. One open possibility is that the switch from the ferromagnetic to the paramagnetic states does not occur simply but an intermediate state arises below the TCP as suggested theoretically recently. Quite generally, if a drastic Fermi-surface change occurs through , the nature of the interaction itself may change and lead to the observed unconventional behavior.
9 pages, 9 figures
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- Pressure induced multicriticality and electronic instability in quasi-kagome ferromagnet URhSn
- Ferromagnetic quantum critical point in a locally noncentrosymmetric and nonsymmorphic Kondo metal
- Localization of 5f-electrons and pressure effects on magnetism in U intermetallics in the light of spin-fluctuation theory
- Spatially modulated, orbital selective ferromagnetism in LaCoGe
- Avoided ferromagnetic quantum critical point in CeZn