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Resonant Tunneling Spectroscopy to Probe the Giant Stark Effect in Atomically Thin Materials
Shoujun Zheng1, Sanghyun Jo2, Kyungrok Kang1
1Department of Energy Science, Sungkyunkwan University, Suwon, 16419, Korea.
Advanced Materials (Deerfield Beach, Fla.)
|February 7, 2020
Summary
This study introduces resonant tunneling spectroscopy to probe giant Stark effect band splits in 2D semiconductors, enabling novel device designs for atomically thin materials.
Area of Science:
- Condensed matter physics
- Materials science
- Device physics
Background:
- Van der Waals heterostructures offer tunable electronic band structures for advanced devices.
- Giant Stark effect-induced band splits in these materials are crucial but underexplored.
- Existing spectroscopy methods face limitations in probing these effects at the device scale.
Purpose of the Study:
- To develop and demonstrate a novel spectroscopy technique for analyzing electronic band structures in 2D semiconductors.
- To investigate and visualize the giant Stark effect band splits in atomically thin materials.
- To overcome limitations of conventional spectroscopy for device-scale characterization.
Main Methods:
- Utilized resonant tunneling spectroscopy in resonant tunneling transistors with 2D semiconductors.
- Leveraged the negligible quantum capacitance of 2D semiconductors for precise measurements.
- Applied the technique to probe bandgaps, sub-band structures, and giant Stark effect band splits.
Main Results:
- Successfully demonstrated a new conceptual spectroscopy for device-scale band structure analysis.
- Probed giant Stark effect band splits in channel materials, overcoming conventional spectroscopy limitations.
- Obtained essential information on band structures without relying on debatable quasiparticle effects.
Conclusions:
- Resonant tunneling spectroscopy is a powerful tool for characterizing 2D semiconductor devices.
- The technique enables the design of novel devices by exploiting the giant Stark effect.
- This method provides practical insights for harnessing the full potential of atomically thin materials.

