分析化学(期刊)
X射线光电子能谱
无定形固体
电导率
原子层沉积
材料科学
电子顺磁共振
薄膜
异质结
钛
光谱学
化学
核磁共振
纳米技术
光电子学
结晶学
物理化学
冶金
色谱法
量子力学
物理
作者
Paul Nunez,Matthias H. Richter,Brandon D. Piercy,Christopher W. Roske,Miguel Cabán‐Acevedo,Mark D. Losego,Steven J. Konezny,David J. Fermı́n,Shu Hu,Bruce S. Brunschwig,Nathan S. Lewis
标识
DOI:10.1021/acs.jpcc.9b04434
摘要
Electrical transport in amorphous titanium dioxide (a-TiO2) thin films, deposited by atomic layer deposition (ALD), and across heterojunctions of p+-Si|a-TiO2|metal substrates that had various top metal contacts has been characterized by ac conductivity, temperature-dependent dc conductivity, space-charge-limited current spectroscopy, electron paramagnetic resonance (EPR) spectroscopy, X-ray photoelectron spectroscopy, and current density versus voltage (J–V) characteristics. Amorphous TiO2 films were fabricated using either tetrakis(dimethylamido)-titanium with a substrate temperature of 150 °C or TiCl4 with a substrate temperature of 50, 100, or 150 °C. EPR spectroscopy of the films showed that the Ti3+ concentration varied with the deposition conditions and increases in the concentration of Ti3+ in the films correlated with increases in film conductivity. Valence band spectra for the a-TiO2 films exhibited a defect-state peak below the conduction band minimum (CBM) and increases in the intensity of this peak correlated with increases in the Ti3+ concentration measured by EPR as well as with increases in film conductivity. The temperature-dependent conduction data showed Arrhenius behavior at room temperature with an activation energy that decreased with decreasing temperature, suggesting that conduction did not occur primarily through either the valence or conduction bands. The data from all of the measurements are consistent with a Ti3+ defect-mediated transport mode involving a hopping mechanism with a defect density of 1019 cm–3, a 0.83 wide defect band centered 1.47 eV below the CBM, and a free-electron concentration of 1016 cm–3. The data are consistent with substantial room-temperature anodic conductivity resulting from the introduction of defect states during the ALD fabrication process as opposed to charge transport intrinsically associated with the conduction band of TiO2.
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