Collapse of the Kondo state and ferromagnetic quantum phase transition in YbFe2Zn20

Kaluarachchi, Udhara S.; Xiang, Li; Ying, Jianjun; Kong, Tai; Struzhkin, Viktor; Gavriliuk, Alexander; Bud'ko, Sergey L.; Canfield, Paul C.

doi:10.1103/physrevb.98.174405

Title: Collapse of the Kondo state and ferromagnetic quantum phase transition in YbFe₂Zn₂₀

Journal Article · 04 November 2018 · Physical Review. B

DOI: https://doi.org/10.1103/physrevb.98.174405 · OSTI ID:1481867

Kaluarachchi, Udhara S. ^[1]; Xiang, Li ^[1]; Ying, Jianjun ^[2]; Kong, Tai ^[1]; Struzhkin, Viktor ^[3]; Gavriliuk, Alexander ^[4]; Bud'ko, Sergey L. ^[1]; Canfield, Paul C. ^[1]

Ames Lab. and Iowa State Univ., Ames, IA (United States)
Carnegie Inst. of Washington, Washington, DC (United States); Carnegie Inst. of Washington, Argonne, IL (United States)
Carnegie Inst. of Washington, Washington, DC (United States)
FSRC Crystallography and Photonics of Russian Academy of Sciences, Moscow (Russia); Russian Academy of Sciences, Troitsk (Russia); Immanuel Kant Baltic Federal Univ., Kaliningrad (Russia)

Here, we present the electrical resistivity data under application of pressures up to ~26 GPa and down to 50 mK on YbFe₂Zn₂₀. We find a pressure induced magnetic phase transition with an onset at p_c = 18.2±0.8 GPa. At ambient pressure, YbFe₂Zn₂₀ manifests a heavy fermion, nonmagnetic ground state and the Fermi liquid behavior at low temperatures. As pressure is increased, the power law exponent in resistivity, n, deviates significantly from Fermi liquid behavior and tends to saturate with n = 1 near p_c. A pronounced resistivity maximum T_max, which scales with the Kondo temperature, is observed. T_max decreases with increasing pressure and flattened out near pc indicating the suppression of Kondo exchange interaction. For p > p_c,T_max shows a sudden upward shift, most likely becoming associated with crystal electric field scattering. Application of magnetic field for p > p_c broadens the transition and shifts it toward the higher temperature, which is a typical behavior of a transition towards a ferromagnetic state, or a state with a significant ferromagnetic component. The magnetic transition appears to abruptly develop above pc, suggesting probable first-order (with changing pressure) nature of the transition; once stabilized, the ordering temperature does not depend on pressure up to ~26 GPa. Taken as a whole, these data suggest that YbFe₂Zn₂₀ has a quantum phase transition at p_c = 18.2 GPa associated with the avoided quantum criticality in metallic ferromagnets.

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Research Organization:: Ames Laboratory (AMES), Ames, IA (United States)

Sponsoring Organization:: USDOE Office of Science (SC), Basic Energy Sciences (BES); USDOE Office of Science (SC), Basic Energy Sciences (BES) (SC-22)

Grant/Contract Number:: AC02-07CH11358; FG02-99ER45775

OSTI ID:: 1481867

Report Number(s):: IS-J-9797

Journal Information:: Physical Review. B, Journal Name: Physical Review. B Journal Issue: 17 Vol. 98; ISSN 2469-9950; ISSN PRBMDO

Publisher:: American Physical Society (APS)Copyright Statement

Country of Publication:: United States

Language:: English

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