TY - JOUR
T1 - Quantum critical behavior in the heavy Fermion single crystal Ce(Ni 0.935Pd0.065)2Ge2
AU - Wang, C. H.
AU - Lawrence, J. M.
AU - Christianson, A. D.
AU - Chang, S.
AU - Gofryk, K.
AU - Bauer, E. D.
AU - Ronning, F.
AU - Thompson, J. D.
AU - McClellan, K. J.
AU - Rodriguez-Rivera, J. A.
AU - Lynn, J. W.
PY - 2011
Y1 - 2011
N2 - We have performed magnetic susceptibility, specific heat, resistivity, and inelastic neutron scattering measurements on a single crystal of the heavy Fermion compound Ce(Ni0.93BPd0.06B)2Ge 2, which is believed to be close to a quantum critical point (QCP) at T = 0. At lowest temperature(1.8-3.5 K), the magnetic susceptibility behaves as χ(T) - χ(0) T-1/6 with χ(0) = 0.032 × 10-6 m3/mole (0.0025 emu/mole). For T < 1 K, the specific heat can be fit to the formula ΔC/T = γ0 - T1/2 with γ0 of order 700 mJ/mole-K2. The resistivity behaves as ρ = ρ0 + AT3/2 for temperatures below 2 K. This low temperature behavior for γ(T) and ρ(T) is in accord with the SCR theory of Moriya and Takimoto[1]. The inelastic neutron scattering spectra show a broad peak near 1.5 meV that appears to be independent of Q; we interpret this as Kondo scattering with T K = 17 K. In addition, the scattering is enhanced near Q=(1/2, 1/2, 0) with maximum scattering at ΔE = 0.45 meV; we interpret this as scattering from antiferromagnetic fluctuations near the antiferromagnetic QCP.
AB - We have performed magnetic susceptibility, specific heat, resistivity, and inelastic neutron scattering measurements on a single crystal of the heavy Fermion compound Ce(Ni0.93BPd0.06B)2Ge 2, which is believed to be close to a quantum critical point (QCP) at T = 0. At lowest temperature(1.8-3.5 K), the magnetic susceptibility behaves as χ(T) - χ(0) T-1/6 with χ(0) = 0.032 × 10-6 m3/mole (0.0025 emu/mole). For T < 1 K, the specific heat can be fit to the formula ΔC/T = γ0 - T1/2 with γ0 of order 700 mJ/mole-K2. The resistivity behaves as ρ = ρ0 + AT3/2 for temperatures below 2 K. This low temperature behavior for γ(T) and ρ(T) is in accord with the SCR theory of Moriya and Takimoto[1]. The inelastic neutron scattering spectra show a broad peak near 1.5 meV that appears to be independent of Q; we interpret this as Kondo scattering with T K = 17 K. In addition, the scattering is enhanced near Q=(1/2, 1/2, 0) with maximum scattering at ΔE = 0.45 meV; we interpret this as scattering from antiferromagnetic fluctuations near the antiferromagnetic QCP.
UR - http://www.scopus.com/inward/record.url?scp=79960743498&partnerID=8YFLogxK
U2 - 10.1088/1742-6596/273/1/012018
DO - 10.1088/1742-6596/273/1/012018
M3 - Article
AN - SCOPUS:79960743498
SN - 1742-6588
VL - 273
JO - Journal of Physics: Conference Series
JF - Journal of Physics: Conference Series
IS - 1
M1 - 012018
ER -