Researchers uncover the mechanism of electric field detection in microscale graphene sensors
The ability to sense the magnitude and polarity of an electric field is of great scientific interest. Applications include early prediction of lightning and detection of supersonic aircraft. Presently, field mills are widely used electric field sensors. While they can detect electric fields of either polarity and field of magnitude as low as 1 V/m, the large size (>1m) hinders their wide use for real-life applications. Also, the motor inside the field mill, which enables the detection of the electric field, is prone to failure. Some efforts have been made to miniaturize the electric field sensor by introducing MEMS-based sensors. While they are small and do not involve any moving parts, the complex fabrication process makes these sensors less cost-effective.
Researchers at Japan Advanced Institute of Science and Technology (JAIST) and Otowa Electric Co., Ltd., a leading lightning protection equipment manufacturer, began looking for a better alternative. Their investigation led to graphene, a two-dimensional material of one atom thickness. "It is well known that the carrier density in graphene is highly sensitive to external perturbations. Such change in carrier density is reflected in the drain current. Although there was some attempt and proposal to use graphene as an electric field sensor, none of the previous works established the underlying mechanism of electric field sensing in graphene. We realized that it is vital to establish the mechanism first to make any improvement in the sensor, which became our primary goal," says Senior Lecturer Manoharan Muruganathan.
Through a series of experiments, the team finally established the mechanism of electric field sensing in graphene. They found that the transfer of charges between graphene and the traps at the SiO2/graphene interface under the application of an electric field is a crucial phenomenon in the sensing mechanism. Such a transfer of charges and the resultant change in carrier density are reflected as the drain current change. The direction of charge transfer depends on the polarity of the electric field. The electrons are transferred from traps to graphene under a positive electric field, whereas they are transferred from graphene to traps under a negative electric field. Thus, the change in drain current under an electric field is opposite for positive and negative electric fields, making it easier to detect the field's polarity. In addition, the number of charge carriers transferred between graphene and the trapsdepends on the magnitude of the electric field. The higher the electric field, the larger the electrons moved between graphene and the traps. The difference in the amount of charge transferred is also reflected in the drain current. Thus, the drain current variation under the application of an electric field can be equated to the magnitude of the electric field.