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Kondo resonance for orbitally degenerate systems
A K Zhuravlev1, V Yu Irkhin, M I Katsnelson
1Institute of Metal Physics, 620219 Ekaterinburg, Russia.
Physical Review Letters
|December 17, 2004
Summary
This study reveals asymmetric Kondo resonance in a two-band model, unlike the one-band case. Magnetic fields split and broaden this resonance, pinning the Kondo peak without suppression.
Area of Science:
- Condensed Matter Physics
- Quantum Many-Body Theory
Background:
- The Kondo effect describes the interaction between localized magnetic moments and conduction electrons.
- The standard Anderson model is a key theoretical framework for studying the Kondo state.
- Extending these models to multiple bands is crucial for understanding complex materials.
Purpose of the Study:
- Investigate the formation of the Kondo state in a general two-band Anderson model.
- Analyze the behavior of the Abrikosov-Suhl resonance under different conditions.
- Examine the impact of external magnetic fields on the Kondo state.
Main Methods:
- Numerical renormalization group (NRG) calculations were employed.
- The study focused on the quarter filling case (one electron per impurity).
- External magnetic (or pseudomagnetic) fields were applied to break degeneracy.
Main Results:
- The Abrikosov-Suhl resonance exhibits essential asymmetry in the two-band model, differing from the one-band case.
- An external field causes asymmetric splitting and significant broadening of the many-body resonance.
- The 'spin-up' Kondo peak remains pinned at the Fermi level and is not suppressed by the magnetic field.
Conclusions:
- The two-band Anderson model presents distinct Kondo physics compared to the single-band model.
- Magnetic fields significantly alter the resonance structure but do not suppress the pinned Kondo peak.
- These findings offer insights into the behavior of strongly correlated electron systems.