Further analysis of the quantum critical point of CeLaRuSi
arXiv:cond-mat/0611503 · doi:10.1007/s10909-007-9315-z
Abstract
New data on the spin dynamics and the magnetic order of CeLaRuSi are presented. The importance of the Kondo effect at the quantum critical point of this system is emphasized from the behaviour of the relaxation rate at high temperature and from the variation of the ordered moment with respect to the one of the Néel temperature for various .
Contribution for the Festschrift on the occasion of Hilbert von Loehneysen 60 th birthday. To be published as a special issue in the Journal of Low Temperature Physics
References in corpus (13)
- Quantum phase transitions
- How do Fermi liquids get heavy and die?
- Rare region effects at classical, quantum, and non-equilibrium phase transitions
- Local Defect in Metallic Quantum Critical Systems
- Anomalous scaling behavior of the dynamical spin susceptibility of CeLaRuSi
- Quantum Critical Point of Itinerant Antiferromagnet in Heavy Fermion
- Spin Fluctuation in Heavy Fermion CeRu_2Si_2
- Quantum Critical Scaling and origin of Non-Fermi-Liquid behavior in ScUPd
- Novel dynamic scaling regime in hole-doped La2CuO4
- Pressure dependence of the spin dynamics around a quantum critical point : An inelastic neutron scattering study of Ce0.87La0.13Ru2Si2
- Non-Fermi-liquid behavior in Ce(RuFe)Ge: cause and effect
- Artificial scaling laws of the dynamical magnetic susceptibility in heavy-fermion systems
- Low energy spin fluctuations in the heavy fermion compound CeLaRuSi
Cited by in corpus (6)
- Heavy fermions in high magnetic field
- High-field metamagnetism in the antiferromagnet CeRhSi
- Interplay of magnetism, Fermi surface reconstructions, and hidden-order in the heavy-fermion material URuSi
- Convergence of the enhancement of the effective mass under pressure and magnetic field in heavy-fermion compounds: CeRu2Si2, CeRh2Si2, and CeIn3
- Magnetic field-induced instability of the cooperative paramagnetic state in ZnCo(OD)Cl
- Quantum criticality of CeLaRuSi : the magnetically ordered phase