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Mass Inversion at the Lifshitz Transition in Monolayer Graphene by Diffusive, High-Density, On-Chip Doping
Ayse Melis Aygar1, Oliver Durnan2, Bahar Molavi1
1Department of Electrical and Computer Engineering, McGill University, Québec, Montréal H3A-0E9, Canada.
We developed a new flip-chip method for doping graphene with alkali vapor, enabling ultrahigh charge carrier densities for transport measurements. This technique allows for detailed studies of electronic phase transitions in graphene under standard cryogenic conditions.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Nanotechnology
Background:
- Traditional charge transport measurements are limited by incompatibility with ultrahigh vacuum (UHV) chemical doping conditions.
- Existing field-effect methods (dielectric and ionic liquid gating) achieve insufficient carrier densities to study electronic phase transitions.
Purpose of the Study:
- To develop a method enabling charge transport measurements at ultrahigh charge carrier densities in graphene.
- To bridge the gap between UHV chemical doping and standard transport measurement setups.
Main Methods:
- An integrated flip-chip method using cesium vapor diffusion for doping monolayer graphene.
- Operando Hall measurements to monitor doping levels up to 4.7 × 1014 cm-2.
- Transport measurements (temperature and magnetic field dependence) within a sealed, oxidation-stable assembly.
Main Results:
- Achieved ultrahigh charge carrier densities in graphene via cesium diffusion doping.
- Observed cyclotron mass inversion, indicating a Lifshitz transition at the hyperbolic M point.
- Demonstrated stability against oxidation and compatibility with standard cryogenic measurement environments.
Conclusions:
- Chemical doping of graphene is feasible in a diffusive regime at ambient pressure using alkali vapor in an inert gas environment.
- This method facilitates charge transport studies at unprecedented carrier densities in standard experimental setups.
- Enables investigation of electronic phase transitions previously inaccessible by field-effect methods.
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