TY - JOUR
T1 - A General Strategy to Achieve Colossal Permittivity and Low Dielectric Loss Through Constructing Insulator/Semiconductor/Insulator Multilayer Structures
AU - Liu, Kai
AU - Sun, Yalong
AU - Zheng, Fengang
AU - Tse, Mei Yan
AU - Sun, Qingbo
AU - Liu, Yun
AU - Hao, Jianhua
N1 - Publisher Copyright:
© 2018, Springer Science+Business Media, LLC, part of Springer Nature.
PY - 2018/9/1
Y1 - 2018/9/1
N2 - In this work, we propose a route to realize high-performance colossal permittivity (CP) by creating multilayer structures of insulator/semiconductor/insulator. To prove the new concept, we made heavily reduced rutile TiO2 via annealing route in Ar/H2 atmosphere. Dielectric studies show that the maximum dielectric permittivity (~ 3.0 × 104) of our prepared samples is about 100 times higher than that (~ 300) of conventional TiO2. The minimum dielectric loss is 0.03 (at 104–105 Hz). Furthermore, CP is almost independent of the frequency (100–106 Hz) and the temperature (20–350 K). We suggest that the colossal permittivity is attributed to the high carrier concentration of the inner TiO2 semiconductor, while the low dielectric loss is due to the presentation of the insulator layer on the surface of TiO2. The method proposed here can be expanded to other material systems, such as semiconductor Si sandwiched by top and bottom insulator layers of Ga2O3.
AB - In this work, we propose a route to realize high-performance colossal permittivity (CP) by creating multilayer structures of insulator/semiconductor/insulator. To prove the new concept, we made heavily reduced rutile TiO2 via annealing route in Ar/H2 atmosphere. Dielectric studies show that the maximum dielectric permittivity (~ 3.0 × 104) of our prepared samples is about 100 times higher than that (~ 300) of conventional TiO2. The minimum dielectric loss is 0.03 (at 104–105 Hz). Furthermore, CP is almost independent of the frequency (100–106 Hz) and the temperature (20–350 K). We suggest that the colossal permittivity is attributed to the high carrier concentration of the inner TiO2 semiconductor, while the low dielectric loss is due to the presentation of the insulator layer on the surface of TiO2. The method proposed here can be expanded to other material systems, such as semiconductor Si sandwiched by top and bottom insulator layers of Ga2O3.
KW - Colossal permittivity
KW - Multilayer structures
KW - Semiconductor
UR - http://www.scopus.com/inward/record.url?scp=85048362896&partnerID=8YFLogxK
U2 - 10.1007/s10909-018-1985-1
DO - 10.1007/s10909-018-1985-1
M3 - Article
SN - 0022-2291
VL - 192
SP - 346
EP - 358
JO - Journal of Low Temperature Physics
JF - Journal of Low Temperature Physics
IS - 5-6
ER -