本論文嘗試使用氧電漿處理法(oxygen plasma treatment)製程鈍化p型氮化鎵的效果來製作高電子遷移率電晶體(High Electron Mobility Transistor, HEMT)以及發光高電子遷移率電晶體(Light Emitting High Electron Mobility Transistor, LE-HEMT),並且同時進行p型氮化鎵乾蝕刻的元件作為對照組,藉此比較氧電漿處理法製程對元件所帶來的影響。 從實驗結果來看,我們展示了閾值電壓(threshold voltage, Vth)為0.5 V的常關型氮化鋁鎵/氮化鎵高電子遷移率電晶體,其閾值電壓與對照組相比十分接近,而其片電阻(sheet resistance, Rsh)為2590 Ω/□,在閘極電壓為4 V時,特徵導通電阻(specific on-state resistance, Ron,sp)為2.48 mΩ-cm2,閘極6 V時的飽和電流(saturation current, Isat)為183.81 mA/mm。此外,經過氧電漿處理的發光高電子遷移率電晶體的閾值電壓則為 -2.7 V,閘極4 V的特徵導通電阻為2.76 mΩ-cm2,閘極6 V時的飽和電流為279.91 mA/mm。 至於發光高電子遷移率電晶體的電致發光,本實驗發現氧電漿處理法與p型氮化鎵乾蝕刻法相比,並不會改變發光波長,並且在原本的磊晶層新增了高濃度n型電流擴散層之後,成功使發光區域變均勻,不過電晶體的閘極控制力也因此消失。
In this thesis, oxygen plasma treatment process to passivate p-GaN is used to fabricate HEMT(High Electron Mobility Transistor) and LE-HEMT(Light Emitting High Electron Mobility Transistor). At the same time, these transistors fabricated by p-GaN dry etch process are compared as the control group. From the experiment, normally off AlGaN/GaN HEMTs with a Vth(thresholdvoltage)=0.5 V are demonstrated. Vth is roughly the same compared with the control group. Rsh(sheet resistance) is 2590 Ω/□. When the gate voltage is 4 V, Ron,sp(specific on-state resistance) is 2.48 mΩ-cm2. When the gate voltage is 6 V, Isat(saturation current) is 183.81 mA/mm. On the other hand, the Vth of the oxygen plasma treated LE-HEMT is -2.7 V, and when the gate voltage is 4 V, the differential Ron,sp is 2.76 mΩ-cm2. When the gate voltage is 6 V, Isat is 279.91 mA/mm. As for the eletroluminescence of the LE-HEMT, we discover that oxygen plasma treatment will not change the wavelength of the emitted light compared with the control group. When an n+ current spreading layer is inserted in the epi, the light emitting region is more uniform, but the gate control of the channel in the transistor will be lost.