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dc.contributor.author陳力輔en_US
dc.contributor.authorLeaf Chenen_US
dc.contributor.author李建平en_US
dc.contributor.authorC.P. Leeen_US
dc.date.accessioned2014-12-12T02:24:03Z-
dc.date.available2014-12-12T02:24:03Z-
dc.date.issued2004en_US
dc.identifier.urihttp://140.113.39.130/cdrfb3/record/nctu/#GT009211546en_US
dc.identifier.urihttp://hdl.handle.net/11536/66179-
dc.description.abstract本研究中,針對氮化鎵異質結構場效電晶體之結構特性,探討利用感應耦合電漿蝕刻改變閘極位置,以達成臨界電壓調整及改善元件特性之目的。蝕刻時,考慮之方向分兩部分,首先是為避免過度蝕刻導致主動區被挖穿,故蝕刻速率不可過快。其次是避免閘極在蝕刻中受到過多損傷導致特性衰減。 實驗中採用兩種不同掘入蝕刻(recess etch)條件,分別是純氯(Cl2)蝕刻與氯氬(Cl2/Ar)蝕刻,分別將閘極掘入(gate recess)50Å與80Å 處,臨界電壓由-7V調整至-6V及-4V,掘入蝕刻後分析元件特性之衰減主要受到surface trap及etch damage所導致,利用passivation 消除surface trap並量測current collapse驗證後,可分別評估surface trap 與etch damage對元件特性所造成之影響。 實驗中使用undoped Al0.3Ga0.7N/GaN HFET 閘極長度1μm閘極寬度50μm之元件作為比較基準,量測未加上閘極前之Vds-Id分佈判斷掘入蝕刻程度,並在元件完成後量測C-V來判斷蝕刻深度,量測元件之各項直流特性與高頻特性,並相互比較以評估掘入蝕刻所造成之影響。未經蝕刻之原始試片臨界電壓-7V,室溫下之最大通道電流高達37mA,單位閘極寬度之電流密度達到740mA/mm,最大外部轉導117mS/mm,元件之崩潰電壓大於100V扣除Pad寄生效應後之ft與 fmax分別達7.5GHz與13GHz。 相同尺寸之元件經過掘入蝕刻並passivation後,臨界電壓縮小至-4V,室溫下最高通道電流20.55mA,單位閘極寬度之電流密度達到411mA/mm,最大外部轉導為112 mS/mm,崩潰電壓為61V。在高頻特性上扣除Pad寄生效應後的ft達到9GHz,fmax達到12.5GHz。 因此可明白,除了崩潰電壓亦會因passivation下降外,etch damage 所造成之特性影響主要是外部轉導、通道電流及崩潰電壓。zh_TW
dc.description.abstractIn this study, we focus on structure characteristics of GaN heterostructure FET Gate recess can change gate position to modify threshold voltage and to optimize device performance.During recess etching, two things are concerned. One is to avoid active layer being over etched. And therefore the etching rate can not be too fast. The other is to avoid gate being over damaged, which causes degradation of device characteristics. In this experiment, we use two different recess etching recipes. One is pure Cl2, which induces gate recess to reach 50A and threshold voltage to change from -7V to -6V;the other is CL2/Ar, which induces gate recess to reach 80A and threshold voltage to change from -7V to -4V.After recess etching, we found that the degradation of device characteristics is mainly caused by surface trap and etching damage. Therefore, by removing surface trap with passivation, and measuring current collapse, the influences of surface trap and etch damage on device characteristics can be evaluated respectively. In this experiment, we use undoped Al0.3Ga0.7N/GaN HFET with gate length 1 µm and gate width 50µm as the basis. Vds-Id curves of the device are measured to determine recess etching degree. After the device is completed, C-V curves are measured to determine depth of etching. We measure DC characteristics and RF performance of the device to evaluate the influence of recess etching. Threshold voltage of no recess sample is -7V, maximum channel current is 37mA under room temperature, current density of unit gate width is 740mA/mm,maximum extrinsic transconductance is 117 mS/mm. breakdown voltage >100V.After deembedding, ft is 7.5GHz and fmax is 13GHz. Recess sample after passivation, Threshold voltage of no recess sample is -4V, maximum channel current is 20.55mA under room temperature, current density of unit gate width is 411mA/mm,maximum extrinsic transconductance is 112 mS/mm. breakdown voltage is 61V.After deembedding, ft is 9GHz and fmax is 12.5GHz. Therefore, etch damage influences extrinsic transconductance, channel current, and breakdown voltage of its characteristics, however, breakdown voltage also reduces due to passivation.en_US
dc.language.isozh_TWen_US
dc.subject氮化鎵zh_TW
dc.subject蝕刻zh_TW
dc.subject臨界電壓zh_TW
dc.subjectGaNen_US
dc.subjectHEMTen_US
dc.subjectHFETen_US
dc.subjectgate recessen_US
dc.subjectthreshold voltageen_US
dc.title氮化鎵異質結構場效電晶體之研究zh_TW
dc.titleStudies of AlGaN/GaN Heterostructure Field Effect Transistorsen_US
dc.typeThesisen_US
dc.contributor.department電子研究所zh_TW
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