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High mobility Cu2O epitaxial films and the application to p-channel thin film transistor |
Kosuke Matsuzaki 1, Kenji Nomura 2, Hiroshi Yanagi 1, Toshio Kamiya 1,2, Masahiro Hirano 2,3, Hideo Hosono 1,2,3 |
1. Materials and Structures Laboratory, Tokyo Institute of Technology, Mailbox R3-1, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan |
Abstract |
Cuprous oxide (Cu2O) is a p-type oxide semiconductor expected as active layers of optoelectronic devices such as solar cells and thin film transistors (TFTs) because it has a large hole mobility ~100 cm2 V-1s-1 for single crystal [1]. However, it is in general difficult to grow high quality Cu2O thin films exhibiting large mobility because the chemical stoichiometry is easily changed by growth conditions. Here, we report the epitaxial film growth of high mobility Cu2O films on MgO (110) single crystal substrates. We also succeeded in p-channel operation of Cu2O channel TFTs.
The Cu2O films were prepared by a pulsed laser deposition technique using a Cu metal target. The substrate temperature (Tsub= 650 – 800 oC) and the oxygen partial pressure (Po2= 10-3 – 100 Pa) were varied. Hole mobility (mh) and carrier concentration (Nh) were measured by Hall effect using the van der Paw configuration. TFTs with amorphous Al2O3 gate insulators were fabricated by a standard photolithography and lift-off process.
It was found that pure semiconducting Cu2O films were obtained in growth conditions of Tsub= 650 – 700 oC and Po2= 0.30 – 1.0 Pa, while Cu impurity was observed at Po2 <0.30 Pa and Cu2O films were polycrystalline insulating at Tsub≥ 730 oC. The high-resolution X-ray diffraction measurements revealed that the pure semiconducting Cu2O films were grown epitaxially with the relationship of [110] Cu2O // [110] MgO in out-of-plane and [1-10] Cu2O // [1-10] MgO in in-plane. The tilting and twisting angles of the crystallites were 0.25 and 0.20 degrees, respectively, indicating that the films have high crystalline quality. 650-nm-thick Cu2O films showed large hole mobilities up to mh ~ 90 cm2 V-1s-1 (Nh ~ 1.6×1014 cm-3), which is comparable to that of a single crystal. The TFTs using Cu2O channels exhibited typical p-channel behavior in a depilation mode. The field-effect mobility was estimated to be ~0.25 cm2 V-1s-1.
[1] E. Fortin et al.,Can. J. Phys., 44, 1551 (1966). |
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Presentation: Oral at E-MRS Fall Meeting 2008, Symposium B, by Kosuke Matsuzaki Submitted: 2008-05-10 13:42 Revised: 2009-06-07 00:48 |