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Signature of frustrated moments in quantum critical CePd1xNixAl

Akito Sakai, Stefan Lucas, Philipp Gegenwart, Oliver Stockert, Hilbert v. Löhneysen, and Veronika Fritsch
Phys. Rev. B 94, 220405(R) – Published 27 December 2016
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Abstract

CePdAl with Ce 4f moments forming a distorted kagome network is one of the scarce materials exhibiting Kondo physics and magnetic frustration simultaneously. As a result, antiferromagnetic (AF) order setting in at TN=2.7 K encompasses only two-thirds of the Ce moments. We report measurements of the specific heat, C, and the magnetic Grüneisen parameter, Γmag, on single crystals of CePd1xNixAl with x0.16 at temperatures down to 0.05 K and magnetic fields B up to 8T. Field-induced quantum criticality for various concentrations is observed with the critical field decreasing to zero at xc0.15. Remarkably, two-dimensional AF quantum criticality of Hertz-Millis-Moriya type arises for x=0.05 and x=0.1 at the suppression of three-dimensional magnetic order. Furthermore, Γmag(B) shows an additional contribution near 2.5T for all concentrations, which is ascribed to correlations of the frustrated one-third of Ce moments.

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  • Received 22 August 2016
  • Revised 7 December 2016

DOI:https://doi.org/10.1103/PhysRevB.94.220405

©2016 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Akito Sakai1, Stefan Lucas2, Philipp Gegenwart1, Oliver Stockert2, Hilbert v. Löhneysen3, and Veronika Fritsch1

  • 1Experimental Physics VI, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, 86135 Augsburg, Germany
  • 2Max Planck Institute for Chemical Physics of Solids, 01187 Dresden, Germany
  • 3Karlsruhe Institute of Technology, Institute for Solid State Physics and Physics Institute, 76131 Karlsruhe, Germany

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Issue

Vol. 94, Iss. 22 — 1 December 2016

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Images

  • Figure 1
    Figure 1

    4f-electron part of the specific heat plotted as C4f/T vs T (on logarithmic scale) for CePd1xNixAl single crystals at zero magnetic field. C4f is obtained after subtracting the nuclear and phonon contributions (see text for details).

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  • Figure 2
    Figure 2

    (a)–(d): Field dependence (Bc) of C4f/T of CePd1xNixAl for x=0.05, 0.10, 0.14, and 0.16 at the lowest temperatures. The black solid and gray dashed lines represent fits of the data according to the prediction for AF quantum criticality in 2D and 3D, respectively, using the parameters listed in Table 1. (e)–(h): Field dependence of the magnetic Grüneisen parameter, Γmag, at T=0.2 and 0.8K of CePd1xNixAl for x=0.05, 0.10, 0.14, and 0.16. The blue solid line in panel (e) indicates a fit of the magnetic Grüneisen parameter according to Γmag=Gr(BBc)1 with Bc=3.02±0.02T and Gr=0.81±0.01. The black dotted line in panel (e) has been obtained by assuming point inversion symmetry of the fit near the critical field. The arrows in panels (f)–(h) indicate the positions of broad maxima.

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  • Figure 3
    Figure 3

    4f contribution to the entropy of CePd1xNixAl (see text) vs magnetic field B at T=0.2K for Bc. The colored arrows indicate the positions of anomalies in the magnetic Grüneisen parameter (cf. Fig. 2).

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  • Figure 4
    Figure 4

    (a) T dependence of Γmag for CePd1xNixAl (x=0.05) at various fields along the c axis on semilogarithmic scale. (b) Quantum critical scaling ΓmagBBc vs T/(BBc)1.2 using Bc=3T. The solid and dashed lines represent Γmag1T and Γmag=Gr.

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