The tribovoltaic effect is a type of
triboelectric current where a direct-current (DC) current is generated by sliding a
P-type semiconductor on top of a
N-type semiconductor or a metal surface without the illumination of photons, which was firstly proposed by Wang et al.[1] in 2019 and later observed experimentally in 2020. When a
P-type semiconductor slides over a
N-type semiconductor,
electron-hole pairs can be produced at the interface, which separate in the built-in electric field (
contact potential difference) at the semiconductor interface, generating a DC current. Research has shown that the tribovoltaic effect can occur at various interfaces, such as metal-semiconductor interface,[2] P-N semiconductors interface,[3] metal-insulator-semiconductor interface,[4] metal-insulator-metal interface,[5] and liquid-semiconductor interface.[6][7] The tribovoltaic effect may find applications in the fields of energy harvesting and smart sensing.[3]
Nomenclature
It has been suggested that the generation of tribo-current at the sliding
PN junction or
Schottky junction is analogous to the generation of
photo-current in the
photovoltaic effect, and the only difference is that the energy for exciting the
electron-hole pairs is different, so it was named “tribovoltaic effect” by Wang et al.[1]
Energy band diagram of the tribovoltaic effect
Experimental evidence
The tribovoltaic effect was observed at both macro- and nano-scale. It was found that a direct current can be generated by sliding the
N-type diamond coated tip over the
P-typeSi samples, and the direction of the tribo-current depends on the direction of the built-in electric field at the
PN and
Schottky junctions.
Tribovoltaic experiment
Tribovoltaic effect at different interfaces
Metal-semiconductor interface. When a Pt-coated silicon atomic force microscopy (AFM) tip rubs on molybdenum disulfide (MoS2) surface, a DC current with a maximum density of 106 A/m2 is generated.[2] Similarly using a pure Pt tip to rub both p-type and
N-type silicon samples, the current follows the contact potential.[3]
P-N semiconductors interface. When using a
N-type silicon to rub with a
P-typeSi, a DC current from the
P-typeSi to the
N-type silicon is produced, with the same direction as the built-in electric field at the
PN junction.[8] Furthermore, when a
N-type diamond-coated silicon tip is used to rub with the surfaces of
N-type silicon and
P-typeSi, tribocurrent can be generated at the interfaces of
N-type tip and
P-typeSi.[3]
Metal-insulator-semiconductor interface. When a conducting tip rubs with a silicon, the tribovoltaic effect can induce water molecules to form an oxide layer on the silicon surface, and the tribo-current decreases gradually with increasing the thickness of oxide layer.[4]
Metal-insulator-metal interface. The studies of DC output characteristics of Al-TiO2-Ti heterojunctions show that the open-circuit voltage increases with increasing the thickness of TiO2, while the short-circuit current first increases and then decreases. The experiments have revealed that the tribo-current is contributed by quantum tunneling, thermionic emission and trap-assisted transport.[5]
Liquid-semiconductor interface. The tribovoltaic effect can also occur at
aqueous solution and solid semiconductor interface, in which the aqueous solution is considered as a liquid semiconductor.[9][10][11][12] The tribovoltaic effect at liquid-solid interface was also observed by Wang et al.[7][13]