ynm

Physics, Semicondcutors, Materials Science

Graphitic Carbon Nitride (g-C₃N₄)/Al₂O₃ Heterostructure as Double Dielectric: A Comparative Study in MIS Based on a-IGZO


Journal article


P. Patra, Y. N. Mohapatra
IEEE Journal of the Electron Devices Society, 2021

Semantic Scholar DOI
Cite

Cite

APA   Click to copy
Patra, P., & Mohapatra, Y. N. (2021). Graphitic Carbon Nitride (g-C₃N₄)/Al₂O₃ Heterostructure as Double Dielectric: A Comparative Study in MIS Based on a-IGZO. IEEE Journal of the Electron Devices Society.


Chicago/Turabian   Click to copy
Patra, P., and Y. N. Mohapatra. “Graphitic Carbon Nitride (g-C₃N₄)/Al₂O₃ Heterostructure as Double Dielectric: A Comparative Study in MIS Based on a-IGZO.” IEEE Journal of the Electron Devices Society (2021).


MLA   Click to copy
Patra, P., and Y. N. Mohapatra. “Graphitic Carbon Nitride (g-C₃N₄)/Al₂O₃ Heterostructure as Double Dielectric: A Comparative Study in MIS Based on a-IGZO.” IEEE Journal of the Electron Devices Society, 2021.


BibTeX   Click to copy

@article{p2021a,
  title = {Graphitic Carbon Nitride (g-C₃N₄)/Al₂O₃ Heterostructure as Double Dielectric: A Comparative Study in MIS Based on a-IGZO},
  year = {2021},
  journal = {IEEE Journal of the Electron Devices Society},
  author = {Patra, P. and Mohapatra, Y. N.}
}

Abstract

We present a systematic study of how graphitic carbon nitride (g-C<sub>3</sub>N<sub>4</sub>) in combination with Al<sub>2</sub>O<sub>3</sub> can be used as a double dielectric to control threshold and flat band voltage in capacitance-voltage (C-V) characteristics of an a-IGZO metal-insulator-semiconductor (MIS) device fabricated on ITO substrate. We study temperature dependence of C-V characteristics for Al<sub>2</sub>O<sub>3</sub> based MIS structures with and without g-C<sub>3</sub>N<sub>4</sub> in the oxide. The effective dielectric constants are estimated in both cases. We show that g-C<sub>3</sub>N<sub>4</sub> in combination with Al<sub>2</sub>O<sub>3</sub> can be used as an effective dielectric with larger relative permittivity than either of them. It also leads to positive threshold shift without affecting the active interface at the semiconductor. The carrier density in the semiconductor is measured from the depletion region showing small variation with respect to frequency and temperature.