Study of local structure in amorphous indium oxide using first-principles calculations
Zheng-Hong Li1*, Minamitani Emi2, Chun-Liang Lin1, Chi-Cheng Lee3, Chien-Te Wu1
11Department of Electrophysics, National Yang Ming Chiao Tung University, Hsinchu, Taiwan
2SANKEN, Osaka University, Osaka, Japan
3Department of Physics, Tamkang University, Tamkang, Taiwan
* Presenter:Zheng-Hong Li, email:zhenghongli.sc11@nycu.edu.tw
Amorphous indium oxide (a-In2O3) has gained popularity in recent years as a transparent oxide semiconductor (a-TOS). Unlike crystalline transparent oxide semiconductors (c-TOS), the amorphous structure offers several advantages, such as high carrier mobility and smooth surfaces [1-2]. The presence of oxygen vacancies in a-In2O3 plays an important role in controlling the carrier concentration. Therefore, we investigated the characteristics of defects in a-In2O3 based on the density functional theory.
Amorphous structures were created from melt-quench simulations using ab initio molecular dynamics simulations implemented in VASP [3]. We employed the GGA-PBE functional and set the energy cutoff to 400 eV. We set the bixbyite In2O3 unit cell as the initial structure, which has 80 atoms, and we created oxygen vacancies in the systems. We investigated the influence of the quench rate in the simulation. In particular, we employed three different quench rates previously reported to create a-In2O3 [1, 4-6]. In these three types of models, following the liquid-quench process to 3000 K, the cooling behavior varies significantly. One model undergoes a rapid cool down to 100 K. Another model cools slowly to the melting point at 2000 K and then continues to cool down to 100 K. The final model follows an exponential decay pattern during cooling.
It is widely known that amorphous systems easily give rise to tail states, and we are particularly interested in the formation of these states in a-In2O3. To understand the origin of the tail states, we analyzed the partial charge density within a specific energy range. Our results indicate that the tail states in a-In2O3 arise from two different scenarios. The first scenario involves the O-O bond and is closely related to the unoccupied state of the oxygen atoms [7]. The second scenario is primarily caused by the In-In bond. We then organized the contributions of the local structures to the tail states, which helps us better understand the composition of a-In2O3.
Keywords: first-principles calculations, transparent oxide semiconductor, Amorphous structures