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Non-Fermi-liquid behavior in the periodic anderson model
A Amaricci1, G Sordi, M J Rozenberg
1Laboratoire de Physique des Solides, CNRS-UMR8502, Université de Paris-Sud, Orsay 91405, France.
Physical Review Letters
|October 15, 2008
Summary
Researchers studied the Mott metal-insulator transition, finding a non-Fermi-liquid metallic state caused by magnetic scattering. This state is tunable via doping or magnetic fields, challenging prior assumptions about heavy fermion systems.
Area of Science:
- Condensed Matter Physics
- Quantum Materials Science
Background:
- The Mott metal-insulator transition is a key phenomenon in condensed matter physics.
- Understanding non-Fermi-liquid behavior in correlated electron systems is crucial for materials science.
Purpose of the Study:
- Investigate the Mott metal-insulator transition in the periodic Anderson model.
- Characterize the electronic state near the quantum critical point.
- Identify the microscopic origins of non-Fermi-liquid behavior.
Main Methods:
- Utilized dynamical mean field theory (DMFT) to model the periodic Anderson model.
- Analyzed the system's behavior near the quantum transition.
- Examined the influence of doping and magnetic fields.
Main Results:
- Observed a non-Fermi-liquid metallic state persisting to low temperatures near the quantum transition.
- Attributed the non-Fermi-liquid behavior to magnetic scattering of charge carriers by localized magnetic moments.
- Demonstrated that this state is controllable through doping and external magnetic fields.
Conclusions:
- Magnetic scattering, not spatial magnetic fluctuations, drives non-Fermi-liquid behavior in this model.
- Dynamical mean field theory is sufficient to capture essential non-Fermi-liquid physics in heavy fermion systems.
- The findings offer new insights into the complex physics of correlated electron systems and metal-insulator transitions.
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