Chao Li
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Chao Li has a total of 24 co-authors. Here are the top co-authors by number of shared publications:
- Wei Ren
State Key Laboratory for Manufacturing Systems Engineering, Electronic Materials Research Laboratory, Key Laboratory of the Ministry of Education, School of Electronic Science and Engineering, Xi’an Jiaotong University, Xi’an 710049, China
2 shared publications - Yijun Zhang
School of Electronic Science and Engineering, Electronic Materials Research Laboratory, Key Laboratory of the Ministry of Education, State Key Laboratory for Manufacturing Systems Engineering Xi’an Jiaotong University, Xi’an 710049, China
2 shared publications - Chaoqiang Liu
State Key Laboratory of Powder Metallurgy, Central South University, Changsha, China
1 shared publication - Daogui Liao
School of Electronic Science and Engineering, Electronic Materials Research Laboratory, Key Laboratory of the Ministry of Education, State Key Laboratory for Manufacturing Systems Engineering Xi’an Jiaotong University, Xi’an 710049, China
1 shared publication - Gang Niu
RIKEN Center for Advanced Intelligence Project
1 shared publication - Guang Yang
University of Illinois at Chicago 1 Department of Physics Chicago, Illinois 60607, USA
1 shared publication
Latest Publications
- Open Access
- 1 July 2025
- Published by MDPI AG in Nanomaterials
- Vol. 15 (13) , 1020
Growth of Zn–N Co-Doped Ga2O3 Films by a New Scheme with Enhanced Optical Properties
Gallium oxide (Ga2O3), as a wide-bandgap semiconductor material, is highly expected to find extensive applications in optoelectronic devices, high-power electronics, gas sensors, etc. However, the photoelectric properties of Ga2O3 still need to be improved before its devices become commercially viable. As is well known, doping is an effective method to modulate the various properties of semiconductor materials. In this study, Zn–N co-doped Ga2O3 films with various doping concentrations were grown in situ on sapphire substrates by atomic layer deposition (ALD) at 250 °C, followed by post-annealing at 900 °C. The post-annealed undoped Ga2O3 film showed a highly preferential orientation, whereas with the increase in Zn doping concentration, the preferential orientation of Ga2O3 films was deteriorated, turning it into an amorphous state. The surface roughness of the Ga2O3 thin films is largely affected by doping. As a result of post-annealing, the bandgaps of the Ga2O3 films can be modulated from 4.69 eV to 5.41 eV by controlling the Zn–N co-doping concentrations. When deposited under optimum conditions, high-quality Zn–N co-doped Ga2O3 films showed higher transmittance, a larger bandgap, and fewer defects compared with undoped ones.
- 1 July 2025
- Published by MDPI AG in Nanomaterials
- Vol. 15 (13) , 1020
Open AccessGrowth of Zn–N Co-Doped Ga2O3 Films by a New Scheme with Enhanced Optical Properties
Gallium oxide (Ga2O3), as a wide-bandgap semiconductor material, is highly expected to find extensive applications in optoelectronic devices, high-power electronics, gas sensors, etc. However, the photoelectric properties of Ga2O3 still need to be improved before its devices become commercially viable. As is well known, doping is an effective method to modulate the various properties of semiconductor materials. In this study, Zn–N co-doped Ga2O3 films with various doping concentrations were grown in situ on sapphire substrates by atomic layer deposition (ALD) at 250 °C, followed by post-annealing at 900 °C. The post-annealed undoped Ga2O3 film showed a highly preferential orientation, whereas with the increase in Zn doping concentration, the preferential orientation of Ga2O3 films was deteriorated, turning it into an amorphous state. The surface roughness of the Ga2O3 thin films is largely affected by doping. As a result of post-annealing, the bandgaps of the Ga2O3 films can be modulated from 4.69 eV to 5.41 eV by controlling the Zn–N co-doping concentrations. When deposited under optimum conditions, high-quality Zn–N co-doped Ga2O3 films showed higher transmittance, a larger bandgap, and fewer defects compared with undoped ones.
- Open Access
- 20 May 2024
- Published by AIP Publishing in Applied Physics Letters
- Vol. 124 (21)
Strain-driven high energy storage in BaTiO3-based lead-free epitaxial thin films
In this work, the epitaxial 0.85BaTiO3-0.15Bi(Mg1/2Ti1/2)O3 (BT-BMT) films with large compressive strain were fabricated on SrTiO3 (001). The expansion of the unit cell volume and out-of-plane lattice parameter and the large built-in electric field (Ebi) in BT-BMT films indicate the existence of defect dipoles. It was found that the polarization and the breakdown strength can be optimized by the strain and the defects, respectively. Ultimately, a desirable energy density of 90.3 J/cm3 with efficiency of 62.3% was achieved. It suggests that strain can serve as a practical means to modulate the energy storage performance of ferroelectric epitaxial film capacitors.
- 20 May 2024
- Published by AIP Publishing in Applied Physics Letters
- Vol. 124 (21)
Open AccessStrain-driven high energy storage in BaTiO3-based lead-free epitaxial thin films
In this work, the epitaxial 0.85BaTiO3-0.15Bi(Mg1/2Ti1/2)O3 (BT-BMT) films with large compressive strain were fabricated on SrTiO3 (001). The expansion of the unit cell volume and out-of-plane lattice parameter and the large built-in electric field (Ebi) in BT-BMT films indicate the existence of defect dipoles. It was found that the polarization and the breakdown strength can be optimized by the strain and the defects, respectively. Ultimately, a desirable energy density of 90.3 J/cm3 with efficiency of 62.3% was achieved. It suggests that strain can serve as a practical means to modulate the energy storage performance of ferroelectric epitaxial film capacitors.
- Open Access
- 26 March 2024
- Published by World Scientific Pub Co Pte Ltd in Journal of Advanced Dielectrics
- Vol. 14 (06)
Atomic resolution microstructure study of Bi-doped SrTiO3
Intrinsic SrTiO3 is a quantum paraelectric, but moderately Bi-doped SrTiO3 exhibits dielectric frequency dispersion similar to relaxor ferroelectrics. In this paper, detailed electron microscopic studies of the microstructures of Bi-doped SrTiO3 samples were presented. It was found that the Sr sites were replaced by off-central Bi, resulting in tensile strain in the strontium titanate (STO) lattice. In the Bi-doped SrTiO3 samples, the valence of titanium mainly showed the Ti[ ] characteristic. According to the dielectric behavior and microstructure analysis, the polar nanoregions (PNRs) composed of strained SrTiO3 nanoclusters should be responsible for the ferroelectric relaxor behavior in samples with moderate Bi content.
- 26 March 2024
- Published by World Scientific Pub Co Pte Ltd in Journal of Advanced Dielectrics
- Vol. 14 (06)
Open AccessAtomic resolution microstructure study of Bi-doped SrTiO3
Intrinsic SrTiO3 is a quantum paraelectric, but moderately Bi-doped SrTiO3 exhibits dielectric frequency dispersion similar to relaxor ferroelectrics. In this paper, detailed electron microscopic studies of the microstructures of Bi-doped SrTiO3 samples were presented. It was found that the Sr sites were replaced by off-central Bi, resulting in tensile strain in the strontium titanate (STO) lattice. In the Bi-doped SrTiO3 samples, the valence of titanium mainly showed the Ti[ ] characteristic. According to the dielectric behavior and microstructure analysis, the polar nanoregions (PNRs) composed of strained SrTiO3 nanoclusters should be responsible for the ferroelectric relaxor behavior in samples with moderate Bi content.
- Open Access
The Vertically Heteroepitaxial Structure for Lead-Free Piezoelectric K0.5Na0.5NbO3 Films
The effect of epitaxial strain on the electrical properties of ferroelectric films has been widely investigated. However, this kind of strain is generally attributed to the substrate clamping constraints and is easily relaxed when the thickness of films is over 100 nm. In this work, a vertically epitaxial strain was introduced into lead-free piezoelectric K0.5Na0.5NbO3 films to improve the electrical properties of ferroelectric films. Two-phase, vertically epitaxial composite KNN-ZnO thin films were grown on the (001) STO substrate using a pulsed laser deposition (PLD) method. The highly (001) preferentially oriented KNN phase and (11 0)-oriented ZnO phase were orderly arranged. Two types of morphologies of “square-like” and “stripe-looking” grains were observed in the surface image. An asymmetric “square” out-of-plane phase hysteresis loop and a “butterfly” displacement loop were exhibited in the KNN phase, whereas the ZnO phase showed a closed phase hysteresis loop and a slim displacement-voltage loop. Two different kinds of polarization behaviors for domains were also observed under applied electric fields, in which the domain of the KNN phase is easily switched to the opposite state, whereas the ZnO phase keeps a stable domain state when applying a DC bias of ±50 V. the vertically epitaxial growth of the KNN-ZnO composited films in this work provides a new way to fabricate complex nanoscale materials.Open AccessThe Vertically Heteroepitaxial Structure for Lead-Free Piezoelectric K0.5Na0.5NbO3 Films
The effect of epitaxial strain on the electrical properties of ferroelectric films has been widely investigated. However, this kind of strain is generally attributed to the substrate clamping constraints and is easily relaxed when the thickness of films is over 100 nm. In this work, a vertically epitaxial strain was introduced into lead-free piezoelectric K0.5Na0.5NbO3 films to improve the electrical properties of ferroelectric films. Two-phase, vertically epitaxial composite KNN-ZnO thin films were grown on the (001) STO substrate using a pulsed laser deposition (PLD) method. The highly (001) preferentially oriented KNN phase and (11 0)-oriented ZnO phase were orderly arranged. Two types of morphologies of “square-like” and “stripe-looking” grains were observed in the surface image. An asymmetric “square” out-of-plane phase hysteresis loop and a “butterfly” displacement loop were exhibited in the KNN phase, whereas the ZnO phase showed a closed phase hysteresis loop and a slim displacement-voltage loop. Two different kinds of polarization behaviors for domains were also observed under applied electric fields, in which the domain of the KNN phase is easily switched to the opposite state, whereas the ZnO phase keeps a stable domain state when applying a DC bias of ±50 V. the vertically epitaxial growth of the KNN-ZnO composited films in this work provides a new way to fabricate complex nanoscale materials.