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Published on: June 14, 2024
Two-Orbital Kondo Screening in a Self-Assembled Metal-Organic Complex
Giulia E Pacchioni1, Marina Pivetta1, Luca Gragnaniello1
1Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL) , CH-1015 Lausanne, Switzerland.
Iron atoms on a copper surface show spatially anisotropic Kondo features, with directionally dependent temperatures and shapes. This arises from polarized iron orbitals enabling Kondo screening, forming a honeycomb superlattice.
Area of Science:
- Surface science
- Condensed matter physics
- Quantum phenomena
Background:
- Kondo effect describes the interaction between localized magnetic moments and conduction electrons.
- Surface science studies phenomena occurring at the interface of materials.
- Polyphenyl dicarbonitrile molecules can form protective layers on metal surfaces.
Purpose of the Study:
- Investigate the spatial anisotropy of Kondo features in iron atoms on a Cu(111) surface.
- Understand the role of electronic orbital polarization in Kondo screening.
- Characterize the arrangement of iron atoms under a molecular layer.
Main Methods:
- Scanning tunneling spectroscopy (STS) to probe electronic features.
- First-principles calculations to model electronic structure and orbital polarization.
- X-ray absorption spectroscopy (XAS) and X-ray magnetic circular dichroism (XMCD) for spin state confirmation.
Main Results:
- Observed strongly spatial anisotropic Kondo features with directionally dependent Kondo temperatures and line shapes.
- Calculations revealed nearly full polarization of Fe 3dxz and 3dyz orbitals.
- XAS and XMCD confirmed effective Kondo screening of the spin in both orbital channels.
- Identified a self-assembled honeycomb superlattice of iron impurities at ideal coverage.
Conclusions:
- The observed Kondo anisotropy is attributed to polarized Fe orbitals, leading to directional Kondo screening.
- The molecular layer effectively isolates and organizes the magnetic impurities.
- This system serves as a model for studying multi-orbital Kondo physics in a tunable 2D lattice.
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