Abstract
The variety of semiconductor materials has been extended in various directions, for example, to very wide bandgap materials such as oxide semiconductors as well as to amorphous semiconductors. Crystalline β-Ga2O3 is known as a transparent conducting oxide with an ultra-wide bandgap of ~4.9 eV, but amorphous (a-) Ga2Ox is just an electrical insulator because the combination of an ultra-wide bandgap and an amorphous structure has serious difficulties in attaining electronic conduction. This paper reports semiconducting a-Ga2Ox thin films deposited on glass at room temperature and their applications to thin-film transistors and Schottky diodes, accomplished by suppressing the formation of charge compensation defects. The film density is the most important parameter, and the film density is increased by enhancing the film growth rate by an order of magnitude. Additionally, as opposed to the cases of conventional oxide semiconductors, an appropriately high oxygen partial pressure must be chosen for a-Ga2Ox to reduce electron traps. These considerations produce semiconducting a-Ga2Ox thin films with an electron Hall mobility of ~8 cm2V−1 s−1, a carrier density Ne of ~2 × 1014 cm−3 and an ultra-wide bandgap of ~4.12 eV. An a-Ga2Ox thin-film transistor exhibited reasonable performance such as a saturation mobility of ~1.5 cm2 V−1 s−1 and an on/off ratio >107.
Highlights
Carrier doping and consequent control of carrier density are essential requirements for semiconductors
This paper reports semiconducting amorphous Ga2Ox (a-Ga2Ox) thin films deposited on glass at room temperature and their applications to thin-film transistors and Schottky diodes, accomplished by suppressing the formation of charge compensation defects
MATERIALS AND METHODS a-Ga2Ox films were fabricated by pulsed laser deposition (PLD) using a KrF excimer laser in an O2 gas flow on silica glass substrates at room temperature
Summary
Carrier doping and consequent control of carrier density are essential requirements for semiconductors. Carrier doping to a known insulating material has been a guiding principle in developing new semiconductors. It is difficult to dope carriers to a wide bandgap material, as explained, for example, by the intrinsic doping limit.[1] Developing new amorphous semiconductors is another area of interest because amorphous semiconductors can be fabricated even at room temperature on plastic and are applicable to flexible devices. Obtaining electron conduction in an amorphous material is much more difficult than obtaining electron conduction in a crystalline material. Hydrogenated amorphous silicon and amorphous oxide semiconductors (AOSs) have been utilized as active layers in practical semiconductor devices.[2]
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