完整後設資料紀錄
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dc.contributor.author黃瑞乾en_US
dc.contributor.authorHuang, Jui-Chienen_US
dc.contributor.author張翼en_US
dc.contributor.authorChang, Edward-Yien_US
dc.date.accessioned2014-12-12T03:08:36Z-
dc.date.available2014-12-12T03:08:36Z-
dc.date.issued2009en_US
dc.identifier.urihttp://140.113.39.130/cdrfb3/record/nctu/#GT009018548en_US
dc.identifier.urihttp://hdl.handle.net/11536/81880-
dc.description.abstract本論文最主要是研究含閘極電場板之氮化鋁鎵/氮化鎵高電子遷移率電晶體製作及線性度分析,雙通道訊號及寬頻分碼多工存取訊號將用作線性度分析之依據。相較於一般高電子遷移率電晶體,閘極電場板之高電子遷移率電晶體的擁有較高的崩潰電壓160伏。此外,閘極電場板之高電子遷移率電晶體偏壓在30伏時,在頻率2 GHz下,亦有較高的功率25.4 dBm,其效率為43%。當偏壓在30伏,電流為15 mA/mm時,其2 GHz下的三階互調失真及鄰近通道功率溢出分別為-27.1 dBc及-33.8 dBc。量測的結果顯示當元件操作於較高的輸出時,閘極電場板之高電子遷移率電晶體的線性度較一般佳,故適合用於為高功率操作。 當氮化鋁鎵/氮化鎵高電子遷移率電晶體的閘極線寬為0.5微米時,閘極總長100微米的元件之直流飽和電流密度為823 mA/mm,最大電導值為225 mS/mm。截止頻率和最大振盪頻率分別為33和57GHz。該元件偏壓在30伏時,其功率輸出為27 dBm,線性增益為21.2 dB,效率為50%。 在本研究中,閘極總長為1.2和2.4厘米之氮化鋁鎵/氮化鎵高電子遷移率電晶體偏壓在30伏時,總功率輸出分別為31.34 dBm (1.36W)及34.38 dBm (3.74W)。功率密度分別為1.13及1.14 W/mm,其功率密度遠小於閘極總長100微米元件的4.3 W/mm。主要是由於大尺寸元件因散熱不良,而使得元件的功率輸出大為下降。zh_TW
dc.description.abstractA field-plated (FP) AlGaN/GaN high electron mobility transistor (HEMT) was fabricated. Investigations on the linearity characteristics were performed through two-tone and wide band code division multiple access (WCDMA) modulated excitations. The FP-HEMT exhibited an improved breakdown voltage of 160 V compared with that of the conventional HEMT. Additionally, a higher output power of 25.4 dBm with 43% power added efficiency at a 30 V drain bias at 2 GHz was achieved. When biased at 30 V and 15 mA/mm current density, the third-order intermodulation (IMD3) level was measured to be -27.1 dBc (at P1dB) and the adjacent channel power rejection (ACPR) was -33.8 dBc (at P1dB) under WCDMA modulation at 2 GHz. Measurement results revealed that the field-plated structure improved the linearity performance over the conventional structure at high output power levels even beyond P1dB. 0.5×100 μm2 AlGaN/GaN HEMT has a drain saturation current density of 823 mA/mm and and maximum transconductance of 225 mS/mm. The cut-off frequency and maximum oscillating frequency are 33 and 57 GHz. The device has output power of 27 dBm with power added efficiency of 50%, and the linear gain was 21.2 dB. The output power of 1.2 mm and 2.4 mm AlGaN/GaN HEMTs demonstrated, respectively, 31.34 dBm (1.27 W) and 34.38 dBm (2.74 W) of output power when biased at a drain voltage of 30 V. The power densities of 1.2 mm and 2.4 mm large periphery devices were 1.13 and 1.14 W/mm which were lower than 4.3 W/mm of 100 μm AlGaN/GaN HEMT. This implies that self-heating problem affected the large periphery devices and degraded their power performance.en_US
dc.language.isozh_TWen_US
dc.subjectGaNzh_TW
dc.subjectHEMTzh_TW
dc.subjecttransistorzh_TW
dc.subjectpowerzh_TW
dc.subjectmicrowavezh_TW
dc.subjectLinearityzh_TW
dc.subject氮化鎵en_US
dc.subject高電子遷移率電晶體en_US
dc.subject電晶體en_US
dc.subject功率en_US
dc.subject微波en_US
dc.subject線性度en_US
dc.title微波功率元件應用含場效電極板之氮化鋁鎵/氮化鎵高電子遷移率電晶體之製作與線性度分析zh_TW
dc.titleFabrication and Linearity Analysis of Field-Plated AlGaN/GaN High Electron Mobility Transistors for Microwave Applicationsen_US
dc.typeThesisen_US
dc.contributor.department材料科學與工程學系zh_TW
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