Related Experiment Video
Updated: Feb 28, 2026

Fabrication of Gate-tunable Graphene Devices for Scanning Tunneling Microscopy Studies with Coulomb Impurities
Published on: July 24, 2015
Abrupt p-n junction using ionic gating at zero-bias in bilayer graphene
Sameer Grover1, Anupama Joshi1,2, Ashwin Tulapurkar2
1Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai, 400005, India.
Researchers created an abrupt graphene p-n junction using dual gating for optoelectronics. This device exhibits a unique photovoltage pattern at low temperatures, driven by the photothermoelectric effect and supercollision scattering.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Nanotechnology
Background:
- Graphene's unique electronic properties make it suitable for optoelectronic devices.
- Fabricating controlled p-n junctions in graphene is crucial for advanced electronic applications.
- Previous methods often resulted in graded junctions, limiting device performance.
Purpose of the Study:
- To develop a novel method for creating abrupt p-n junctions in bilayer graphene FETs.
- To investigate the photovoltage characteristics of these junctions at low temperatures.
- To explore the underlying physical mechanisms responsible for the observed photovoltage.
Main Methods:
- Fabrication of a double gated bilayer graphene field-effect transistor (FET).
- Utilized a combination of electrostatic and electrolytic gating to form an abrupt p-n junction.
- Measured photovoltage at low temperatures with a frozen electrolyte.
Main Results:
- Confirmed the formation of an abrupt p-n junction via two Dirac peaks in the gating curve.
- Observed a six-fold pattern in photovoltage at low temperatures, indicating the photothermoelectric effect.
- Photovoltage increased with decreasing temperature, suggesting dominant supercollision scattering.
Conclusions:
- The developed dual-gating technique successfully creates abrupt graphene p-n junctions.
- The photothermoelectric effect and supercollision scattering play significant roles in the device's photoresponse.
- This technique is extendable to other 2D materials for large-area superlattice p-n junctions with enhanced photoresponse.
Related Concept Videos
Biasing of P-N Junction
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
P-N junction
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Biasing of FET
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the...
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Characteristics of MOSFET
Various vital parameters influence their functionality, which is crucial for theory and electronics applications. First, channel dimensions, precisely length, and width, are pivotal. The size of these channels affects the transistor's ability to carry current and switching speeds; shorter channels typically enable...

