The thermopower as a fingerprint of the Kondo breakdown quantum critical point
arXiv:1005.3354 · doi:10.1103/PhysRevB.83.073104
Abstract
We propose that the thermoelectric power distinguishes two competing scenarios for quantum phase transitions in heavy fermions : the spin-density-wave (SDW) theory and breakdown of the Kondo effect. In the Kondo breakdown scenario, the Seebeck coefficient turns out to collapse from the temperature scale , associated with quantum fluctuations of the Fermi surface reconfiguration. This feature differs radically from the physics of the SDW theory, where no reconstruction of the Fermi surface occurs, and can be considered as the hallmark of the Kondo breakdown theory. We test these ideas, upon experimental results for YbRhSi.
References in corpus (12)
- Fermi-liquid instabilities at magnetic quantum phase transitions
- Quantum Criticality in Heavy Fermion Metals
- Weak magnetism and non-Fermi liquids near heavy-fermion critical points
- Fractionalized Fermi liquids
- On the thermoelectricity of correlated electrons in the zero-temperature limit
- Fermi-surface collapse and dynamical scaling near a quantum critical point
- Kondo Breakdown as a Selective Mott Transition in the Anderson Lattice
- Thermoelectric response near a quantum critical point: the case of CeCoIn5
- Selective Mott transition and heavy fermions
- Multi-scale fluctuations near a Kondo Breakdown Quantum Critical Point
- Grüneisen ratio at the Kondo breakdown quantum critical point
- Enhancement of thermal transport in the degenerate periodic Anderson model
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- Magnetic Polarization and Fermi Surface Instability: Case of YbRh2Si2
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- Strongly correlated Fermi systems as a new state of matter
- Nambu-Eliashberg theory for multi-scale quantum criticality : Application to ferromagnetic quantum criticality in the surface of three dimensional topological insulators
- Thermodynamic signatures of a fractionalized Fermi liquid