Department of Materials Science & Engineering, and Inter-University Semiconductor Research Center, Seoul National University , Seoul 151-744, Republic of Korea.
IPIT & Department of Physics, Chonbuk National University , Jeonju 54896, Republic of Korea.
ACS Appl Mater Interfaces. 2018 Jan 31;10(4):3810-3821. doi: 10.1021/acsami.7b17906. Epub 2018 Jan 22.
p-Type SnO thin films were deposited on a Si substrate by a cosputtering process using ceramic SnO and metal Sn targets at room temperature without adding oxygen. By varying the dc sputtering power applied to the Sn target while maintaining a constant radio frequency power to the SnO target, the Sn/O ratio varied from 56:44 to 74:26 at the as-deposited state. After thermal annealing at 180 °C for 25 min under air atmosphere using a microwave annealing system, the films were crystallized into tetragonal SnO when the Sn/O ratio increased from 44:56 to 57:43. Notably, the metallic Sn remained when the Sn/O ratio was higher than 55:45 at an annealed state. When the ratio was lower than 55:45 at the annealed state, the incorporated Sn fully oxidized to SnO, making the films useful p-type semiconductors, whereas the films became metallic conductors at higher Sn/O ratios. At the Sn/O ratio of 55:45 at the annealed state, the film showed the highest Hall mobility of 8.8 cm V s and a hole concentration of 5.4 × 10 cm. Interestingly, the electrical conduction behavior showed trap-mediated hopping when the Sn metal was cosputtered, whereas the single SnO film showed regular band conduction behavior. The residual stress effect could interpret such property variation originated from the sputtering power and postoxidation-induced volumetric effects. This report makes a critical contribution to the in-depth understanding of the composition-structure-property relationship of this technically important thin film material.
p 型 SnO 薄膜通过室温下使用陶瓷 SnO 和金属 Sn 靶材的共溅射工艺沉积在 Si 衬底上,不添加氧气。通过改变施加到 Sn 靶材的直流溅射功率,同时保持 SnO 靶材的恒定射频功率,在沉积状态下 Sn/O 比从 56:44 变化到 74:26。在空气气氛下使用微波退火系统于 180°C 退火 25 min 后,当 Sn/O 比从 44:56 增加到 57:43 时,薄膜结晶为四方 SnO。值得注意的是,当 Sn/O 比在退火状态下高于 55:45 时,金属 Sn 仍然存在。当 Sn/O 比在退火状态下低于 55:45 时,掺入的 Sn 完全氧化为 SnO,使薄膜成为有用的 p 型半导体,而在较高的 Sn/O 比下,薄膜变为金属导体。在退火状态下 Sn/O 比为 55:45 时,薄膜表现出最高的霍尔迁移率 8.8 cm V s 和载流子浓度 5.4×10 cm。有趣的是,当 Sn 金属共溅射时,电传导行为表现出陷阱介导的跳跃,而单 SnO 薄膜表现出规则的能带传导行为。残余应力效应可以解释这种源于溅射功率和后氧化引起的体积效应的性能变化。本报告对深入了解这种具有重要技术意义的薄膜材料的组成-结构-性能关系做出了重要贡献。