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Charge-Transfer Plasmon Polaritons at Graphene/α-RuCl3 Interfaces
Daniel J Rizzo1, Bjarke S Jessen1,2, Zhiyuan Sun1
1Department of Physics, Columbia University, New York, New York 10027, United States.
Nano Letters
|November 9, 2020
Summary
Researchers visualized massive charge transfer at graphene/α-RuCl3 interfaces using charge-transfer plasmon polaritons (CPPs). This method enables nanoscale charge control for 2D materials without external doping or contacts.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Nanotechnology
Background:
- Nanoscale charge control is crucial for plasmonics, band structure engineering, and topological properties of 2D materials.
- Exploiting material properties for intrinsic charge control is an ongoing research area.
Purpose of the Study:
- To visualize and quantify charge transfer at graphene/α-RuCl3 interfaces.
- To develop a novel method for nanoscale plasmonic interface generation without external doping or contacts.
Main Methods:
- Nanoimaging experiments on graphene/α-RuCl3 at ambient and cryogenic temperatures.
- Utilizing the electron affinity of α-RuCl3 to generate charge-transfer plasmon polaritons (CPPs).
- First-principles calculations to correlate plasmonic response with work function differences.
Main Results:
- Discovered robust plasmonic features in ungated and undoped graphene/α-RuCl3 structures.
- Quantified massive charge transfer via CPPs, enabling accurate Fermi energy measurement of graphene (EF = 0.6 eV).
- Linked the observed plasmonic response to the work function difference between graphene and α-RuCl3.
Conclusions:
- Charge-transfer plasmon polaritons (CPPs) provide a high-fidelity measure of graphene's Fermi energy.
- The work function difference between graphene and α-RuCl3 drives the formation of CPPs.
- This study presents a general strategy for creating nanometer-scale plasmonic interfaces intrinsically.
Keywords:
Mott insulatorsgrapheneplasmon polaritonsscanning near-field optical microscopy (SNOM)two-dimensional (2D) materialsα-RuCl3
