TCAD model of amorphous gallium oxide calibrated on experimental data for TFT FET and FeFET TCAD simulations
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DATASET on TCAD model for amorphous gallium oxide calibrated on experimental data (for TCAD simulations of transistor employng amorphous gallium oxide as semiconductor)
- Experimental data: current-voltage characteristics plotted in in figures "IV_GaOxFET_al2o3.pdf" and "IV_GaOxFET_hfo2.pdf". The raw data can be found in the files "IV_GaOxFET.csv" and "IV_GaOxFET_hfo2.csv" in the columns “Vg_exp,Id_exp,Ig_exp” (respectively, gate voltage [V], drain current [A/um], gate voltage [A/um])- Simulated structures: 3-terminal bottom-gate FET shown in figures "struct_GaOx_FET_al2o3.pdf" and "struct_GaOx_FET_hfo2.pdf"- Simulator: Synopsys Sentaurus TCAD- TCAD model setup for amorphous gallium oxide: A bandgap of 5 eV, relative permittivity of 10 [1] and electron affinity of 4.07 eV [2] are used for the amorphous a–GaOx material. A constant n–type doping is considered. In addition, similarly to [3], a sub-gap density of states (DOS) is included for a–GaOx, consisting in exponential band tails decaying into the energy-gap from the conduction and valence band edges and Gaussian-distributed acceptor-like trap states. Calibrated parameters of acceptor-like traps are reported in "GaOx_bulk_traps_parameters.csv". Parameters used for band tails are reported in "GaOx_band_tail_parameters.csv". A constant mobility model is used (mobility equal to 10 cm2 V-1 s-1). The tungsten source and drain contacts to a–GaOx are modeled as Schottky contacts (Schottky barrier height of 0.55 eV, electron tunneling mass=0.2m0, hole tunneling mass=0.6m0). Fixed charges at the interface between a–GaOx and HfO2 or Al2 O3 are also considered, as well as uniformly distributed acceptor-type traps in the HfO2 and Al2 O3 dielectric layers [4], [5]. Trap parameters for HfO2 are reported in "HfO2_traps.csv". Trap parameters for Al2O3 are reported in "Al2O3_traps.csv"- The simulated current versus applied voltage is plotted against experiments in figures "IV_GaOxFET_al2o3.pdf" and "IV_GaOxFET_hfo2.pdf". The corresponding raw simulated data are reported in the files "IV_GaOxFET.csv" and "IV_GaOxFET_hfo2.csv", where V_down_TCAD(V) and V_up_TCAD(V) are the simulated applied gate voltages (up and down voltage sweep) and Id_up_TCAD(A/um) and Id_down_TCAD(A/um) are the corresponding simulated drain currents.
[1] H.Kröncke, F.Maudet, S.Banerjee, J.Albert, S.Wiesner, V.Deshpande, and C. Dubourdieu, “Effect of o2 plasma exposure time during atomic layer deposition of amorphous gallium oxide,” Journal of Vacuum Science and Technology A, vol. 39, p. 052408, 2021.[2] J. Kim, T. Sekiya, N. Miyokawa, N. Watanabe, K. Kimoto, K. Ide, Y. Toda, S. Ueda, N. Ohashi, H. Hiramatsu, H. Hosono, and T. Kamiya, “Conversion of an ultra-wide bandgap amorphous oxide insulator to a semiconductor,” NPG Asia Materials, vol. 9, no. e359, 2017.[3] Y. Zhang, C.-H. Huang, and K. Nomura, “High-mobility wide bandgap amorphous gallium oxide thin-film transistors for nmos inverters,” Applied Physics Reviews, vol. 11, no. 1, p. 011418, 03 2024.[4] S. Cimino, A. Padovani, L. Larcher, V. Afanas’ev, H. Hwang, Y. Lee, M. Jurczac, D. Wouters, B. Lee, H. Hwang, and L. Pantisano, “A study of the leakage current in TiN/HfO2/TiN capacitors,” Microelectronic Engineering, vol. 95, pp. 71–73, 2012.[5] A. Padovani, L. Larcher, V. Della Marca, P. Pavan, H. Park, and G. Bersuker, “Charge trapping in alumina and its impact on the operation of metal-alumina-nitride-oxide-silicon memories: Experiments and simulations,” Journal of Applied Physics, vol. 110, no. 1, p. 014505, 07 2011. [Online]. Available: https://doi.org/10.1063/1.3602999
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2026-06-04



