Strongly correlated Fermi-systems: non-Fermi liquid behavior, quasiparticle effective mass and their interplay
arXiv:0904.1799 · doi:10.1016/j.physleta.2009.04.046
Abstract
Basing on the density functional theory of fermion condensation, we analyze the non-Fermi liquid behavior of strongly correlated Fermi-systems such as heavy-fermion metals. When deriving equations for the effective mass of quasiparticles, we consider solids with a lattice and homogeneous systems. We show that the low-temperature thermodynamic and transport properties are formed by quasiparticles, while the dependence of the effective mass on temperature, number density, magnetic fields, etc gives rise to the non-Fermi liquid behavior. Our theoretical study of the heat capacity, magnetization, energy scales, the longitudinal magnetoresistance and magnetic entropy are in good agreement with the remarkable recent facts collected on the heavy-fermion metal YbRh2Si2.
7 pages, 5 figures
References in corpus (9)
- Quantum Criticality in Heavy Fermion Metals
- Quantum criticality
- Weak magnetism and non-Fermi liquids near heavy-fermion critical points
- Quantum magnetism and criticality
- Divergence of the Magnetic Grüneisen Ratio at the Field-Induced Quantum Critical Point in YbRhSi
- Curie law, entropy excess, and superconductivity in heavy fermion metals and other strongly interacting Fermi liquids
- Universal Behavior of Two-Dimensional 3He at Low Temperatures
- Universal low-temperature behavior of the CePd_{1-x}Rh_x ferromagnet
- Energy scales and magnetoresistance at a quantum critical point