TW557567B - Double channel pseudomorphic high electron mobility transistor - Google Patents
Double channel pseudomorphic high electron mobility transistor Download PDFInfo
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557567 A7 ,----- B7 經濟部智慧財產局員工消費合作社印製557567 A7, ----- B7 Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs
五、發明説明() 發明領域: #發日月係有關於一種具有雙層通道(D〇uble channel) 結構之擬晶性高電子移動率電晶體(Pseud〇m〇rphic HighV. Description of the invention () Field of invention: # 发 日月 is related to a pseudo-crystalline high electron mobility transistor (Pseud〇m〇rphic High) with a double channel structure.
EleeUon Mobility Transist〇r ; phemt),特別是有關於一種 利用雙層由例如磷化銦鎵(InGaP)/砷化銦鎵(InGaAs)/砷化 蘇(GaAs)所構成之堆疊結構作為電晶體之通道結構的擬晶 性高電子移動率電晶體。 發明背景: 般而σ ’由於石申化銦鎵材料具有較低的有效質量、 較高的電子移動率以及飽和速度等優點,因此為了得到更 佳的几件效能,以砷化鎵為基板之異質結構場效電晶體 中,利用砷化銦鎵取代砷化鎵作為通道材料已經成為一種 趨勢。 在以砷化鎵為基板且以砷化銦鎵為通道材料之異質結 構場效電晶體中,由於砷化鎵與砷化銦鎵這兩層材料之間 的晶格常數差異,在砷化鎵基材上磊晶成長薄砷化銦鎵層 時,會在砷化銦鎵層上產生相當大的應變。如同熟習此技 藝者所知,此在砷化銦鎵層上所產生之應變將更進一步地 深化量子井(Quantum Well)’此現象乃係由於例如擬晶性高 電子移動率電晶體中之二維電子氣(Tw〇 Electron Gas ; 2DEG)受到電子大量增加的影響所形成。藉 由量子井所產生之二維電子氣’可提高元件之載子移動^ 以及速度。(t著銦含量的增加’石申化鎵基材肖砂化姻鎵通EleeUon Mobility Transistor; phemt), in particular, relates to a type of transistor that uses a double-layer stack structure composed of, for example, indium gallium phosphide (InGaP) / indium gallium arsenide (InGaAs) / thallium arsenide (GaAs). Pseudocrystalline high electron mobility transistor with channel structure. Background of the invention: In general, σ 'is due to the low effective mass, high electron mobility, and saturation speed of the Shishenhua indium gallium material. Therefore, in order to obtain better performance, gallium arsenide is used as the substrate. In field-effect transistors with heterostructures, it has become a trend to use indium gallium arsenide instead of gallium arsenide as the channel material. In a heterostructure field effect transistor using gallium arsenide as a substrate and indium gallium arsenide as a channel material, due to the lattice constant difference between the two layers of gallium arsenide and indium gallium arsenide, When epitaxial growth of a thin indium gallium arsenide layer on a substrate results in considerable strain on the indium gallium arsenide layer. As the person skilled in the art knows, the strain generated on the indium gallium arsenide layer will further deepen the quantum well. This phenomenon is due to, for example, two of the pseudo-crystalline high electron mobility transistors Two-dimensional electron gas (TwO Electron Gas; 2DEG) is formed by the large increase in electrons. The two-dimensional electron gas generated by the quantum well can increase the carrier movement ^ and speed of the element. (The increase in indium content ’
本紙張尺度適用中國國家標準(CNS)A4規格(210X297公楚) 6 5 7 5 5 發明説明() =材料之間的晶格不匹配也隨之提升,而使得電晶體中之 里子井更為加深,可進一步地提升電晶體元件之性能。缺 而,當銦含量過高時,將造成砷化銦鎵材料產生晶格=弛W 其中’此晶格鬆弛現象乃係因過大之累積應變在晶格: :成後受到釋放所產生。此肖’所形成之晶格缺陷如同‘ 多散射中心、。而這些晶格缺陷所產生之散射中心將導致栽: 子之移動率與速度下降。因由於材料間晶格常 配的影響,將會使得砷化銦鎵通道材料之厚度與銦(In)含量 雙到限制,而引發臨界厚度的問題。 1 而由於材料間晶袼常數不匹配所造成的臨界厚度問 題’導S電晶豸元件無法利用車交厚且具有高姻纟量的砷化This paper size applies the Chinese National Standard (CNS) A4 specification (210X297). 6 5 7 5 5 Description of the invention () = The lattice mismatch between the materials has also increased, making the neutron well in the transistor even more Deepening can further improve the performance of transistor components. However, when the content of indium is too high, it will cause the lattice of the indium gallium arsenide material to relax = where W is the phenomenon that the relaxation of the lattice is caused by the excessive accumulated strain in the lattice: after the release. The lattice defect formed by this Shao ’is like a multiple scattering center. The scattering centers generated by these lattice defects will cause the mobility and velocity of the seed to decrease. Due to the influence of the lattice configuration between materials, the thickness of the indium gallium arsenide channel material and the content of indium (In) are doubled to the limit, which causes the problem of critical thickness. 1 The critical thickness problem caused by the mismatch of the crystal rhenium constants between the materials ’’ S ’crystal rhenium elements cannot be made thick and have a high arsenic content.
銦鎵材料。如此一來,將使得電晶體元件在未來更高效能 的應用中受到限制。 I 發明目的及概述: 鑒於上述之發明背景中,由於材料間晶格常數不匹配 所引發之臨界厚度問題,會導致砷化銦鎵通道材料之厚度 與銦含量受到限制,而無法有效提升電晶體元件之效Z 2 應用。 Μ 因此,本發明的主要目的之一就是在提供一種擬晶性 兩電子移動率電晶體,使用雙層磷化銦鎵(InGap)/砷化銦鎵 (InGaAs)/砷化鎵(GaAs)堆疊結構作為電晶體元件之通道結 構。如此一來,可利用較厚且銦含量較高之砷化銦鎵材料 做為通道層。因此,可增加載子傳輸特性,並提升閘極電 本紙張尺度適用中國國家標準(CNS)A4規格(210X297公爱) 請 先 閱 讀 背’ 意 事 項 再Indium gallium material. As a result, transistor components will be limited in future higher-efficiency applications. I Purpose and summary of the invention: In view of the above background of the invention, the critical thickness problem caused by the lattice constant mismatch between the materials will cause the thickness and indium content of the indium gallium arsenide channel material to be limited, and the transistor cannot be effectively improved. Component effect Z 2 application. Μ Therefore, one of the main objects of the present invention is to provide a pseudomorphic two-electron mobility transistor using a double-layer Indium Gallium Phosphide (InGap) / InGaAs / GaAs stack Structure as the channel structure of the transistor element. In this way, a thicker indium gallium arsenide material with a higher indium content can be used as the channel layer. Therefore, the carrier transmission characteristics can be increased and the gate current can be improved. The paper size is applicable to the Chinese National Standard (CNS) A4 specification (210X297 public love).
訂 經濟部智慧財產局員工消費合作社印製 557567 A7 B7 五、發明説明( 壓擺幅。 之擬曰=之另一目的就是在提供-種具有雙層通道結構 平面:::…移動率電晶體’其係利用上、中、下三層 =雜層做為載子供應層。如此一來,可使得雙層通道 及交流線性度。 電-體疋件獲得優良的直流 明之另一目的就是在提供一種高電子移動率電晶 特基接=用Γ隙之碟化姻錄等材料作為缓衝層以及蕭 M :曰’、中通道結構上方之磷化銦鎵層可提供電晶 之蕭特基特性,而通道結構下方之碟化銦錄層 p J攸基板漏失之基板漏電流。 件具有相當優良之夾正特性。 了使電B曰體兀 訂 之雷月之再一目的就是在提供一種具有雙層通道結構 體’其通道結構中之碟化銦鎵材料層與石申化鋼嫁材 偈曰=間大的導電帶不連續度eEc)可以將載子有效地 電=在又層通道結構中’因此可降低順向偏壓操作時的漏 、根據以上所述之目的,本發明更提供了一種具有雙層通 道結構之擬晶性高電子移動率電晶體,至少包括:一 ^絕 緣基板;-第-未摻雜緩衝層位於上述之半絕緣基板上、’、£ 一第二未摻雜緩衝層位於上述之第—未摻雜緩衝層上一 第一平面摻雜層位於上述之第二未摻雜緩衝層上y一第一 未摻雜隔離層位於上述之第一平面摻雜層上;一第一未摻 本紙張尺度適用中國國家標準(CNS)A4規格(210X297公釐) 557567Ordered by the Intellectual Property Bureau of the Ministry of Economic Affairs, printed by employee consumer cooperatives 557567 A7 B7 V. Description of the invention (Pressure swing. The other purpose of = is to provide-a plane with a double-layered channel structure ::: ... 'It uses the upper, middle, and lower layers = the heterogeneous layer as the carrier supply layer. In this way, double-layer channels and AC linearity can be made. Another purpose of the electrical-body components to obtain excellent DC light is to Provide a high-electron mobility transistor crystal base = using Γ-gap material such as a disc as a buffer layer and Xiao M: said, the indium gallium phosphide layer above the middle channel structure can provide the transistor Basic characteristics, and the substrate leakage current under the channel structure of the indium recording layer p. The substrate has a very good sandwiching characteristic. Another purpose of making the electrical system is to provide A kind of double-layered channel structure with a layer of indium-gallium material in the channel structure and Shishenhua Steel's bridging material (the large discontinuity of the conductive band eCc) can effectively charge the carrier = in another layer Channel structure 'therefore reduces forward bias operation According to the above-mentioned purpose, the present invention further provides a pseudo-crystallized high electron mobility transistor having a double-layered channel structure, including at least: an insulating substrate; On the above semi-insulating substrate, a second undoped buffer layer is located on the first-undoped buffer layer, a first planar doped layer is located on the second undoped buffer layer, and An undoped isolation layer is located on the above-mentioned first planar doped layer; a first un-doped paper size is applicable to China National Standard (CNS) A4 (210X297 mm) 557567
、發明說明( 雜通道層位於上述 隔離層位於上述之:未摻雜隔離層上;-第二未摻1 層位於上述之第-一未摻雜通道層上;一第二平面摻痒 位於上述之第未摻雜隔離層上;一第三未摻雜隔離; 上迷之楚二土Μ平面摻雜層上;一第二未摻雜通道層位方2. Description of the invention (The hetero-channel layer is located on the above isolation layer: on the undoped isolation layer;-the second undoped layer is on the first-undoped channel layer; a second planar doped layer is on the above On the first undoped isolation layer; a third undoped isolation; on the second doped layer of the second earth M; a second undoped channel layer side
述之4始 離層上;一第四未摻雜隔離層位於J <第一未摻雜通 第四未摻雜隔❹上日,—第三平面#雜層位於上心 第三平面摻雜;:上,-未換雜蕭特基接觸層位於… 蕭特基接觸層:,而::四平面摻雜層位於部分之未摻· 層;一第五去# 暴路出另一部分之未摻雜簫特基接海 一捭 》雜隔離層位於上述之第四平面摻雜層上; 擦雜歐姆接觸屉你Μ ^ 日上, 極 ";上述之第五未摻雜隔離層上;一泛 及1極位於部分之摻雜歐姆接觸層上;以及一問和 、所暴路之未摻雜蕭特基接觸層上。 在此擬晶性高雷· -JL ·<Ατ jc~ 層、第-未摻雜Λ 電晶體中’第—未摻雜隔萄 m 層、以及第二未掺雜隔離層構成本# 明之第-層通道結構,而第三未擦雜隔離層、第二 =餐 通道層、第四未摻雜隔離層則構成首· 經濟部智慧財產局員工消費合作社印製 粗八、未摻雜隔離層以及第四未摻雜隔離層之未 /可例如為磷化銦鎵、砷化鋁鎵(A1GaAs)、或磷化鋁金 ⑽謂,π第二未摻雜隔離層以及第三未摻雜隔離〜 材料可例如為砷化鎵或磷化銦(ΙηΡ)等。此外,第一曰 通道層以及第二未摻雜通道層之材料均為砷化銦:摻· 此,第_未掺雜通道層《及第二未摻雜通道層可利用較: 本紙張尺度適用中國國家標準(CNS)A4規格(210X297公楚) 557567 A7The fourth layer is described above; a fourth undoped isolation layer is located on the J < first undoped through fourth undoped spacer, and the third plane is doped on the third plane. Miscellaneous:-, Unchanged Schottky contact layer is located in ... Schottky contact layer :, and :: Four-plane doped layer is located in part of the undoped layer; The undoped insulating layer is located on the fourth planar doped layer described above; the ohmic contact layer is wiped on the electrode, and the electrode is on the fifth undoped isolation layer described above. ; A pan and 1 pole is located on a part of the doped ohmic contact layer; and a non-doped Schottky contact layer that is harmonized and exposed. Here, the pseudo-crystalline high thunder ·· JL · < Aτ jc ~ layer, the first-undoped spacer layer in the-undoped Λ transistor, and the second undoped spacer layer constitute this # 明 之The first layer of the channel structure, while the third unblended isolation layer, the second = meal channel layer, and the fourth undoped isolation layer constitute the first The layers and the fourth undoped isolation layer may be, for example, indium gallium phosphide, aluminum gallium arsenide (A1GaAs), or aluminum phosphide. The second un-doped isolation layer and the third undoped Isolation ~ The material may be, for example, gallium arsenide or indium phosphide (InP). In addition, the material of the first channel layer and the second undoped channel layer are both indium arsenide: doped. Therefore, the _th undoped channel layer and the second undoped channel layer are available: Applicable to China National Standard (CNS) A4 specification (210X297), 557567 A7
五、發明説明() 且銦含量較高之砷化銦鎵材料做為通道層,而達到增加載 子傳輪特性,以及提升閘極電壓擺幅之目的。 其中,上述之第一平面摻雜層、第二平面摻雜層、以及 第三平面摻雜層係用以作為載子供應層。藉由此三層載子 供應層可使付上述之雙層通道結構内的載子均勻分佈,而 使電晶體元件獲得優良的直流及交流線性度。 發明詳細說明: 本發明揭露一種具有雙層通道結構之擬晶性高電子移 動率電晶體,其係使用雙層由例如磷化銦鎵/砷化銦鎵/珅化 叙堆疊結構來構成電晶體之通道結構,並利用上、中、下 三層平面掺雜層來作為載子供應層。因此,除了可利用較 厚且銦含量較高之砷化銦鎵來作為通道層材料,而達到增 加載子傳輸特性以及提升閘極電壓擺幅的目的外,更可使 得雙層通道結構内之載子均勻分佈,而使電晶體元件獲得 優良的直流及交流線性度,進而達到提升元件效能之目 的。為了使本發明之敘述更加詳盡與完備,可參照下列描 述並配合第1圖至第9圖之圖示。 經濟部智慧財產局員工消費合作社印製 請參照第1圖,第1圖係繪示本發明之一較佳實施例 之具有雙層通道結構之擬晶性高電子移動率電晶體的剖面 圖。本發明之電晶體丨00的結構係先利用例如低壓金屬有 機化學氣相沉積(Low Pressure Metal Organic Chemical Vapor Deposition ; LP-MOCVD)或分子束磊晶成長法 (Molecular Beam Epitaxy ; MB E)在半導體之基板 ii2 上依 6 本紙張尺度適用中國國家標準(CNS)A4規格(210X297公釐) 557567 A7 B7 五 經濟部智慧財產局員工消費合作社印製 發明説明( 序形成未摻雜之緩衝層114覆蓋在基板112上;未摻雜之 緩衝層116覆蓋在緩衝層Η#;平面換雜層us覆蓋在緩 衝層116上;未摻雜之隔離層12〇覆蓋在平面摻雜層ιι8 上;未摻雜之通道層122覆蓋在隔離層12〇上;未摻雜之 隔離層124覆蓋在通道層122上;平面摻雜層126覆蓋在 隔離層124上;未摻雜之隔離層128覆蓋在平面摻雜層126 上;未摻雜之通道層130覆蓋在隔離層128上;未摻雜之 隔離層132覆盍在通道層130上;平面摻雜層134覆蓋在 隔離層132上,未摻雜之蕭特基接觸層丨36覆蓋在平面摻 雜層134上;平面摻雜層138覆蓋在蕭特基接觸層136上; 未摻雜之隔離層140覆蓋在平面摻雜層138上;以及歐姆 接觸層142覆蓋在隔離層140上。 其中’隔離層120、通道層122、與隔離層124構成電 晶體100之一層通道結構,而隔離層128、通道層13〇、與 隔離層1 3 2則構成電晶體1 〇 〇之另一層通道結構,亦即, 隔離層120 /通道層122 /隔離層124以及隔離層128 /通道層 1 3 0/隔離層1 3 2堆疊構成本發明之雙層通道結構。 接著,利用例如真空蒸鍍的方式形成源極144與汲極 146之金屬層(僅繪示其中之源極144與汲極146)覆蓋在歐 姆接觸層142上’其中此金屬層可例如為金(Au) /錯(Ge)/ 鎳(Ni)之堆疊結構。再於約250°C之環境下進行約10秒鐘 之熱退火(Annealing)步驟,藉以使源極144以及汲極146 之金屬層與歐姆接觸層1 42形成歐姆接觸。然後,利用例 本紙張尺度適用中國國家標準(CNS)A4規格(210X297公釐) 557567 A7 ----- B7 五、發明說明() (請先閲讀背面之注意事項再填寫本頁) 如微影(Photolithograph)以及蝕刻,例如濕蝕刻,的方式定 義源極1 44以及汲極丨46之金屬層,而去除部分之金屬層, 並暴露出部分之歐姆接觸層丨42,藉以在歐姆接觸層142 上分別形成源極1 44以及汲極1 46。 源極1 44以及汲極146形成後,利用例如微影以及濕 姓刻製程進行定義,而將所暴露出之歐姆接觸層142及其 底下部分之隔離層1 40、部分之平面摻雜層1 3 8、以及部分 之蕭特基接觸層136去除,直至暴露出蕭特基接觸層136 為止’而在蕭特基接觸層136上之歐姆接觸層142、隔離 層140、以及平面摻雜層138中形成開口 ι5〇。待暴露出蕭 特基接觸層1 36之開口 1 50形成後,利用例如蒸鍍的方式 形成閘極148位於所暴露出之蕭特基接觸層136上,而形 成如第1圖所示之結構。其中’閘極148之材料可例如為 鋁、鈦(Ti)、鉬(Mo)、鉑(Pt)、金及其合金,例如鈦/金合金 或鉑/金合金等。 經濟部智慧財產局員工消費合作社印製 在本發明之電晶體100結構中,基板112之材料可例 如為砷化鎵或磷化銦。緩衝層丨14之材料可例如為砷化鎵 或磷化銦,且此緩衝層114之厚度較佳是介於01人至 m之間。緩衝層1 16之材料可例如為磷化銦鎵 (In0 49 Ga().5lP)、珅化銘鎵(AlxGabxAs),χ 介於 〇」至 ^ 〇 之間、磷化鋁鎵(AluGauP)、或砷化鋁銦(Α1〇 “η。52As) 等,且此緩衝層116之厚度較佳是介於2〇〇 A至5〇〇〇a之 間。平面摻雜層118係用以作為載子供應層,且平面摻雜 本紙張尺度適用中國國家標準(CNS)A4規格(21〇χ297公釐)一---- 557567 五、發明説明( 經濟部智慧財產局員工消費合作社印製 層118之摻雜濃度5 (N + )較佳是介於1χ 1〇11公分_2(cm·2) cm 隔離層120之材料可例如為碟化銦鎵 (In〇.49Ga〇5lP)、坤化銘鎵(AlxGai_xAs)、,X 介於 〇」至!·〇 ^間、磷化鋁銦(Α10.5ΐη〇 5P)、或砷化鋁銦(A1〇 “InmAs) 等,且隔離層120之厚度較佳是介於3〇 A至8〇人之間。 而通道層122之材料可例如為厚度介於5〇 A至15〇人 之砷化銦鎵(InxGai-xAs),χ介於〇.〇5至〇3之間、或厚度 介於100 Α至300Α之砷化銦鎵(InxGai xAs),χ介於〇 3至 0·7之間。隔離層124之材料可例如為4化鎵或罐化铜,且 隔離層124之厚度較佳是介於3〇入至8〇人之間。平面摻雜 1 126係用以作為載子供應層,且平面摻雜層&之摻雜 濃度5 (Ν + )較佳是介於1χ 1〇ucm-2至5χ 1〇13⑽入隔離層 128之材料可例如為砷化鎵或磷化銦,且 度較佳是介於3。人一間。通道層13。之材料= 為厚度介於50Α至150Α之砷化銦鎵(InxGaixAs),X介於 〇.〇5至0.3之間、或厚度介於1〇〇 A至3〇〇A之坤化姻鎵 (InxGa丨·xAs),x介於〇·3至〇 7之間。隔離層m之材料可 例如為磷化銦鎵(In〇 49GaG 5iP)、砷化鋁鎵(α1χ^ι As),X 介於〇·1至1.0之間、碗化銘銦(A1〇5ln〇5P)、或石申化叙銦 (Al^InmAs)等,且隔離層132之厚度較佳是介於3〇 a 至80A之間。 此外,平面摻雜層134係用以作為载子供應層,且平 面摻雜層134之摻雜濃度5 (N + )較佳是介於1χ 1〇1】咖_2至 本紙張尺度適用中國國家標準(CNS)A4規格(210X297公楚) ' -------- (請先閲讀背面之注意事項再 I I 填寫本頁) 訂· 557567 五 經濟部智慧財產局員工消費合作社印製 發明説明() 5χ 10 cm2。蕭特基接觸層】 1 3 6之材料可例如為磷化銦鎵V. Description of the invention () Indium gallium arsenide material with higher indium content is used as the channel layer, so as to increase the characteristics of the carrier wheel and increase the gate voltage swing. The first planar doped layer, the second planar doped layer, and the third planar doped layer are used as carrier supply layers. The three-layer carrier supply layer can uniformly distribute the carriers in the above-mentioned double-layered channel structure, so that the transistor element can obtain excellent DC and AC linearity. Detailed description of the invention: The present invention discloses a pseudo-crystallized high electron mobility transistor having a double-layered channel structure, which uses a double-layered structure to form a transistor using, for example, an indium gallium phosphide / indium gallium arsenide / thallium halide stack structure. Channel structure, and the top, middle and bottom plane doping layers are used as the carrier supply layer. Therefore, in addition to using thicker and higher indium gallium indium gallium arsenide as the material of the channel layer, in order to increase the carrier transmission characteristics and increase the gate voltage swing, it can also make the The carriers are evenly distributed, so that the transistor element obtains excellent DC and AC linearity, thereby achieving the purpose of improving the element performance. In order to make the description of the present invention more detailed and complete, reference may be made to the following descriptions in conjunction with the diagrams in FIGS. 1 to 9. Printed by the Consumer Cooperative of Intellectual Property Bureau of the Ministry of Economics Please refer to FIG. 1. FIG. 1 is a cross-sectional view of a pseudo-crystallized high electron mobility transistor having a double-layered channel structure according to a preferred embodiment of the present invention. The structure of the transistor of the present invention 00 is firstly applied to a semiconductor using, for example, Low Pressure Metal Organic Chemical Vapor Deposition (LP-MOCVD) or Molecular Beam Epitaxy (MB E). The substrate ii2 is based on the 6 paper standards applicable to the Chinese National Standard (CNS) A4 specification (210X297 mm) 557567 A7 B7 Five printed by the Intellectual Property Bureau of the Ministry of Economic Affairs and the Consumer Cooperatives printed the invention description (in order to form an undoped buffer layer 114 to cover On the substrate 112; the undoped buffer layer 116 covers the buffer layer Η; the planar doping layer us covers the buffer layer 116; the undoped isolation layer 120 covers the planar doped layer ι8; The impurity channel layer 122 covers the isolation layer 120. The undoped isolation layer 124 covers the channel layer 122. The planar doped layer 126 covers the isolation layer 124. The undoped isolation layer 128 covers the planar doped layer. On the impurity layer 126; the undoped channel layer 130 covers the isolation layer 128; the undoped isolation layer 132 covers the channel layer 130; the planar doped layer 134 covers the isolation layer 132; Schottky contacts The layer 36 covers the planar doped layer 134; the planar doped layer 138 covers the Schottky contact layer 136; the undoped isolation layer 140 covers the planar doped layer 138; and the ohmic contact layer 142 covers the The isolation layer 140. Among them, the 'isolation layer 120, the channel layer 122, and the isolation layer 124 constitute a one-layer channel structure of the transistor 100, and the isolation layer 128, the channel layer 13 and the isolation layer 1 32 constitute the transistor 1'. 〇 Another layer of channel structure, that is, the isolation layer 120 / channel layer 122 / isolation layer 124 and the isolation layer 128 / channel layer 130 / isolation layer 13 2 are stacked to form the double-layer channel structure of the present invention. For example, a vacuum evaporation method is used to form a metal layer of the source electrode 144 and the drain electrode 146 (only the source electrode 144 and the drain electrode 146 are shown) and cover the ohmic contact layer 142. The metal layer may be, for example, Au / Ge (Ge) / nickel (Ni) stacked structure. Then under the environment of about 250 ° C for about 10 seconds Annealing step, so that the source electrode 144 and drain electrode 146 metal layer and ohms The contact layer 1 42 forms an ohmic contact. Then, using an example paper size Use Chinese National Standard (CNS) A4 specification (210X297 mm) 557567 A7 ----- B7 V. Description of the invention () (Please read the precautions on the back before filling this page) Photolithograph and etching, For example, wet etching defines the metal layers of source 1 44 and drain 46, and removes part of the metal layer, and exposes part of the ohmic contact layer 42, thereby forming source 1 on the ohmic contact layer 142, respectively. 44 and drain 1 46. After the source electrode 44 and the drain electrode 146 are formed, they are defined using, for example, lithography and a wet etching process, and the exposed ohmic contact layer 142 and the isolation layer 1 40 and a part of the planar doped layer 1 underneath are defined. 3, and part of the Schottky contact layer 136 is removed until the Schottky contact layer 136 is exposed, and the ohmic contact layer 142, the isolation layer 140, and the planar doped layer 138 on the Schottky contact layer 136 are removed. In the opening ι5〇. After the opening 150 of the Schottky contact layer 1 36 is formed, a gate electrode 148 is formed on the exposed Schottky contact layer 136 by, for example, evaporation, and a structure as shown in FIG. 1 is formed. . The material of the gate 148 may be, for example, aluminum, titanium (Ti), molybdenum (Mo), platinum (Pt), gold, and alloys thereof, such as titanium / gold alloy or platinum / gold alloy. Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs In the transistor 100 structure of the present invention, the material of the substrate 112 may be, for example, gallium arsenide or indium phosphide. The material of the buffer layer 14 may be, for example, gallium arsenide or indium phosphide, and the thickness of the buffer layer 114 is preferably between 01 and m. The material of the buffer layer 116 can be, for example, indium gallium phosphide (In0 49 Ga (). 5lP), AlxGabxAs, χ is between 0 ″ to ^ 〇, aluminum gallium phosphide (AluGauP), Or indium aluminum arsenide (Al 1O "η. 52As), and the thickness of the buffer layer 116 is preferably between 2000A and 5000a. The planar doped layer 118 is used as a carrier. Sub-supply layer, and the plane is doped. The paper size is applicable to the Chinese National Standard (CNS) A4 specification (21 × 297 mm). ---- 557567 V. Description of the invention (Printing layer 118, Consumer Cooperatives, Intellectual Property Bureau, Ministry of Economic Affairs) The doping concentration 5 (N +) is preferably between 1 × 1011 cm_2 (cm · 2) cm. The material of the isolation layer 120 may be, for example, indium gallium indium (In.49Ga〇5lP), Kunhua Indium gallium (AlxGai_xAs), X is between 0 ″ to! 0 ^, indium aluminum phosphide (A10.5ΐη〇5P), or indium aluminum arsenide (A1〇 ”InmAs), etc., and the thickness of the isolation layer 120 Preferably, it is between 30A and 80. The material of the channel layer 122 may be, for example, indium gallium arsenide (InxGai-xAs) with a thickness of 50A to 150. 〇5 to 〇3, or thickness between 100 InxGai xAs (A to 300A), χ is between 03 and 0.7. The material of the isolation layer 124 may be, for example, gallium 4 g or canned copper, and the thickness of the isolation layer 124 is preferably Between 30 and 80 people. The plane doping 1 126 is used as a carrier supply layer, and the doping concentration 5 (N +) of the plane doping layer & preferably is between 1 × 1. The material of ucm-2 to 5χ 1〇13 inserted into the isolation layer 128 may be, for example, gallium arsenide or indium phosphide, and the degree is preferably between 3. One for one. The channel layer 13. The material = is a thickness between 50A InxGaixAs up to 150A, InxGa 丨 xAs with X between 0.05 and 0.3, or thickness between 100A and 300A, x Between 0.3 and 0.7. The material of the isolation layer m may be, for example, indium gallium phosphide (In〇49GaG 5iP), aluminum gallium arsenide (α1χ ^ As), and X is between 0.1 and 1.0. , Indium indium (AlO5InO5P), or indium indium (Al ^ InmAs), etc., and the thickness of the isolation layer 132 is preferably between 30a and 80A. In addition, planar doping The layer 134 is used as a carrier supply layer, and the doping concentration of the planar doped layer 134 is 5 (N +) is preferably between 1x 1〇1] Coffee_2 to this paper size applies Chinese National Standard (CNS) A4 specifications (210X297). -------- (Please read the back Note II, please fill in this page) Order · 557567 Five Intellectual Property Bureau of the Ministry of Economic Affairs printed a description of the invention () 5 × 10 cm2. Schottky contact layer] The material of 1 3 6 may be, for example, indium gallium phosphide
(In〇.49Ga().51P)、砷化鋁鎵(μ G 碎山abxAs),χ介於〇」至u 之間、碟化鋁銦(Al〇 5ln。5ρ)、或# 請 先 閱 讀 背 之 注 意 事 項 再 Α 申化銘銦(AlG48ln〇.52As) 等,且蕭特基接觸層136之厚声鈐杜θ a 9 ?(In〇.49Ga (). 51P), aluminum gallium arsenide (μ G broken mountain abxAs), χ is between 0 ″ to u, aluminum indium (Al〇5ln.5ρ), or # Please read first Note on the back, and then apply Α Shin Huaming Indium (AlG48ln〇.52As), etc., and the thick sound of the Schottky contact layer 136, θ a 9?
7子從較佳是介於100A至1 000A 之間。平面摻雜層13 8之摻雜澧_ a /χτ+ 人 心雜/辰度占(Ν + )較佳是介於1χ ΙΟ1、]!!2 至 5x 1013cm·2。隔雜思 1/1Γν &離層1 40之材料可例如為磷化The 7 sub is preferably between 100A and 1,000A. The doped 澧 _ a / χτ + of the planar doped layer 13 8 is preferably between 1 × 10101 and 2 × 5 × 1013cm · 2. Imagination 1 / 1Γν & separation layer 1 40 material can be, for example, phosphating
1.0之間、磷化鋁銦(Al〇 5lnn冲八七成yL •5 G·5。或砷化鋁銦(Al〇 48In〇.52As) 等’且隔離層14G之厚度較佳是介於3以至祕之間。歐 姆接觸層142之材料則可例如為摻雜濃度介於ΐχ 1〇1、-2 至 1 x 1 0 19 c πΓ2之石申化鉉痞石φ各如力、/ τ 棘Α甲化銦鎵(In 0 5 3 Ga0 4 7 As),且歐 姆接觸層142之厚度較佳是介於2〇〇 A至5〇〇〇A之間。 請參照f 2 @ ’帛2 _係'、%示本發明之一較佳實施例 之電晶體的相對應導電帶能帶圖,其中Ερ為費米能階。在 此貫施例中,緩衝層1 1 6之材料係採用厚度3 〇〇人之磷化銦 鎵(InowGa^P);隔離層120係採用厚度5〇人之磷化銦鎵 (InowGao qP);通道層122係採用厚度1〇〇人之砷化銦鎵 (In〇 2Ga〇 sAs);隔離層124係採用厚度4〇a之砷化鎵;隔 離層128係採用厚度40A之砷化鎵;通道層13〇係採用厚 度100A之砷化銦鎵(In〇 jGao.sAs);隔離層132係採用厚度 50入之填化銦鎵(Ino.oGamP);而蕭特基接觸層136係採 用厚度450人之磷化銦鎵(In〇 49 p)。在此實施例中, 電晶體100利用InGaP/InGaAs/GaAs雙層通道結構,亦即 10 本紙張尺度適用中國國家標準(CNS)A4規格(210X297公楚) 557567 A7 B7 五、發明説明() 隔離層120/通道層122/隔離層124以及隔離層132/通道層 ^0/隔離層丨28,因此可利用較厚且較高銦含量的神化銦錄 材料做為通道層1 22與通道層丨3 〇,進而達到改善載子傳 輸特性及提升閘極工作電壓擺幅的目的。 此外,上、中、下三層脈波摻雜之平面摻雜層i 34、平 面摻雜層126、以及平面摻雜層118做為载子供應層,可 使在雙層通道結構内的載子均勻分佈,進而使電晶體i⑽ 獲得良好的直流及交流線性度。另外,利用大能隙之鱗化 姻鎵材料作為蕭特基接觸層1 3 6以及緩衝層丨丨6,更可分 別提供電晶體1 〇 〇良好之蕭特基特性及抑制從基板丨丨2漏 失之漏電流以改善元件之夾止特性。另一方面,藉由Between 1.0, indium aluminum phosphide (Al〇5lnn, 87% yL • 5 G · 5. Or indium arsenide (Al〇48In〇.52As), etc.) and the thickness of the isolation layer 14G is preferably between 3 The material of the ohmic contact layer 142 may be, for example, a stone with a doping concentration ranging from ΐχ 101, -2 to 1 x 1 0 19 c πΓ2. Indium gallium (In 0 5 3 Ga0 4 7 As), and the thickness of the ohmic contact layer 142 is preferably between 2000A and 5000A. Please refer to f 2 @ '帛 2 _ 系' And% show the corresponding conductive band energy band diagram of a transistor of one of the preferred embodiments of the present invention, where Eρ is a Fermi level. In this embodiment, the material of the buffer layer 1 16 is a thickness of 3 〇 〇InowGaP (Powder Indium GaP); the isolation layer 120 is made of InowGao qP with a thickness of 50; the channel layer 122 is made of InGaGa (Powder) with a thickness of 100. 2Ga〇sAs); the isolation layer 124 is made of gallium arsenide with a thickness of 40a; the isolation layer 128 is made of gallium arsenide with a thickness of 40A; the channel layer 13 is made of indium gallium arsenide (In〇jGao.sAs) with a thickness of 100A ); The isolation layer 132 is made of 50 Filled with indium gallium (Ino.oGamP); and the Schottky contact layer 136 is made of indium gallium phosphide (In〇49 p) with a thickness of 450 people. In this embodiment, the transistor 100 uses InGaP / InGaAs / GaAs dual Layer channel structure, that is, 10 paper sizes are applicable to Chinese National Standard (CNS) A4 specifications (210X297 Gongchu) 557567 A7 B7 V. Description of the invention () Isolation layer 120 / channel layer 122 / isolation layer 124 and isolation layer 132 / channel Layer ^ 0 / isolation layer 丨 28, so thicker and higher indium content of the indium recording material can be used as the channel layer 1 22 and channel layer 丨 3, to achieve improved carrier transmission characteristics and increase the gate operating voltage In addition, the pulse doping plane doping layer i 34, the plane doping layer 126, and the plane doping layer 118 of the upper, middle, and lower three layers are used as the carrier supply layer, so that The carriers in the channel structure are evenly distributed, so that the transistor i⑽ obtains good DC and AC linearity. In addition, a large band gap galvanic material is used as the Schottky contact layer 1 3 6 and the buffer layer 丨 6 , Can also provide good Schottky characteristics and suppression of transistor 100 Shushu leak off the substrate 2 of the element to improve the leakage current characteristics of clipping the other hand, by
InGaP/InGaAs(亦即通道層122/隔離層120以及通道層13〇/ 隔離層132)界面間大的導電帶不連續度(AEc),可將載子有 效地侷限在雙層通道結構内,藉以降低順向偏壓操作時的 漏電流’並提升順向偏壓操作的能力。此外,利用大能隙 之碌化麵鎵等材料作為緩衝層1 1 6以及蕭特基接觸層 1 3 6,位於通道結構上方之磷化銦鎵層可提供電晶體元件優 良之蕭特基特性,位於通道結構下方之磷化銦鎵層則可抑 制從基板1 1 2漏失之基板漏電流。因此,可使電晶體元件 之夾止特性更為增強。 請一併參照第3圖至第5圖,其中第3圖係繪示本發 明之一較佳實施例之電晶體的兩端閘極電流(Ig)對閘-汲 極電壓(VGD)之關係圖,第4圖係繪示第3圖之電晶體的 11 (請先閲讀背面之注意事項再?本頁} -、一一-口 #· 經濟部智慧財產局員工消費合作社印製The large conduction band discontinuity (AEc) between the interfaces of InGaP / InGaAs (that is, channel layer 122 / isolation layer 120 and channel layer 130 / isolation layer 132) can effectively confine carriers to a two-layer channel structure. This reduces the leakage current during forward bias operation and improves the ability of forward bias operation. In addition, using materials such as gallium with a large band gap as buffer layers 1 16 and Schottky contact layers 1 36, the indium gallium phosphide layer above the channel structure can provide excellent Schottky characteristics of transistor elements. The indium gallium phosphide layer located under the channel structure can suppress the substrate leakage current leaked from the substrate 1 12. Therefore, the pinch-off characteristic of the transistor element can be further enhanced. Please refer to FIG. 3 to FIG. 5 together, where FIG. 3 is a diagram showing a relationship between a gate current (Ig) and a gate-drain voltage (VGD) of a transistor of a preferred embodiment of the present invention. Figure, Figure 4 shows the transistor 11 of Figure 3 (please read the precautions on the back first? This page}-、 一一-口 # · Printed by the Employees ’Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs
557567 五 經濟部智慧財產局員工消費合作社印製 發明説明( 問-沒極漏電流(IGL)對溫度的關係圖,而第5圖係繪示第3 圖之電晶體的閘-汲極起始電壓(v〇n)對溫度的關係圖。在 第3圖中’電晶體元件之閘極面積為丨χ 8 〇 #㈤2 ,且溫 度為3 00K。由第3圖可知本發明之電晶體元件擁有良好 的閘極蕭特基特性。當閘-汲極電壓為1 5 v時,閘-汲極 漏電流在溫度為 300K、330K、360K、390K、420K、450K、 、及 480K 時刀別為 60# A/mm、96/z A/mm、110// A/mm、 114# A/mm、203 # A/mm、367 a A/mm、以及 600 // A/mm,如第4圖所示;另一方面,在上述之溫度下,相 對應之起始電壓則分別為1.46V、my、1.38V、1.35V、 1.31V、1.25V、以及lmv,如第5圖所示。電晶體元件 在高溫時依然擁有低的閘-汲極漏電流及高的起始電壓。 因此,這也就說明了本發明之電晶體元件之結構設計不但 擁有良好的蕭特基特性,更可以確實將電子偏限在通道層 内,而降低漏電&,並增加崩潰電壓,進而增進元件的高 溫特性。 請參照第6圖,第6圖係繪示本發明之一較佳實施例 之電晶體在室溫下之共源極輸出電流·電壓三端特性圖。此 電晶體元件之㈣面㈣! χ 8 〇 “ m 2,每一階段之閘-源極 電壓(VGS)差距為·〇.5ν’ x臨界電壓^為]5ιν,而溫 度則為3 00K。由“圖中可發現本發明之電晶體元件擁 有良好的電晶體放大、飽和、以及失止特性,帛明了本設 計結構具有良好的載子揭限能力。此外,由於大的順向起 12 本紙張尺度適用中國國家標準(CNS)A4規格(210X297公楚) 五、發明説明() 1以诛作在閘·源極電壓為 時’本發明之電晶體元件並 的線…1.5〜 件特性。 玍月,.肩的漏電流而影響元 請參照第7圖’第7圖係繪示本發 之電晶體在室溫下沒極飽和月之一較佳實施例 源極電壓(VGS)之關係圖,農 轉導值(gm)對閘- 與閘-源極電壓之間的關係,曲線、代表没極飽和電流 電壓之間的關係。此電曰Μ 一、 、導值與閘-源極 2 , 日日肢兀件之閘極面積為:1x8ο# m2,沒-源極電壓(Vds)固定 β Q υ ν,/皿度則為3 0 〇 κ。由 第 7 圖可知,此時電晶辦_ _ 吁冤日日體兀件之最大輸出電流為 460mA/mm,最大耱違_佶目丨丨劣 取人轉導值則為162mS/mm。當線性操作區 定義在最大轉導值9G%以上時1極工作飽和電流區域可 大於310mA/mm’而閘·源極工作電壓區域則可大於2V, 元件有相當優良之線性操作特性。這也正說明了藉由利用 雙層通道結構及上'中、下三層平面摻雜層做為載子供應 層’可使得在通道内的載子能夠均句分饰,因此元件可以 獲得寬廣的線性㈣區n面,^平行傳導的消 除’在大的順向閘-源極電壓+2.0 V操作_,元件依然保 有大的轉導值135 mS/mm。 經濟部智慧財產局員工消費合作社印製 請參照第8圖,第8圖係繪示本發明之一較佳實施例 之電晶體在室溫下之轉導值(gm)、輸出電導(gds)及電壓增 益(Av)對汲-源極電壓(Vl)s)的關係圖,其中曲線d代表轉 導值與汲-源極電壓之間的關係,曲線e代表輸出電導與 13 本紙張尺度適用中國國家標準(CNS)A4規格(210X297公釐) 557567557567 The Intellectual Property Bureau of the Five Ministry of Economic Affairs printed a description of the invention of the Consumer Cooperative of the Consumers (Q-Grade Leakage Current (IGL) vs. Temperature, and Figure 5 shows the gate-drain of the transistor in Figure 3 Voltage (v〇n) vs. temperature. In Figure 3, 'the gate area of the transistor element is χχ 8〇 # ㈤2, and the temperature is 3 00K. From Figure 3, the transistor element of the present invention is known. Have good Schottky characteristics of the gate. When the gate-drain voltage is 15 v, the gate-drain leakage current is at 300K, 330K, 360K, 390K, 420K, 450K, and 480K. 60 # A / mm, 96 / z A / mm, 110 // A / mm, 114 # A / mm, 203 # A / mm, 367 a A / mm, and 600 // A / mm, as shown in Figure 4 On the other hand, at the above temperatures, the corresponding starting voltages are 1.46V, my, 1.38V, 1.35V, 1.31V, 1.25V, and lmv, as shown in Figure 5. The crystal element still has low gate-drain leakage current and high starting voltage at high temperatures. Therefore, this also illustrates that the structural design of the transistor element of the present invention not only has good Schottky characteristics, It is also possible to confine the electrons in the channel layer, reduce the leakage & and increase the breakdown voltage, thereby improving the high temperature characteristics of the device. Please refer to FIG. 6, which illustrates a preferred embodiment of the present invention. The three-terminal characteristic diagram of the common source output current and voltage of the transistor at room temperature. The surface of this transistor element! Χ 8 〇 "m 2, the gate-source voltage (VGS) gap at each stage is · 0.5v 'x critical voltage is 5mv, and the temperature is 300K. "It can be found from the figure that the transistor element of the present invention has good transistor amplification, saturation, and stop characteristics, which clarifies the design. The structure has a good ability to lift the limit of the carrier. In addition, due to the large forward direction, 12 paper sizes are applicable to the Chinese National Standard (CNS) A4 specification (210X297). 5. Description of the invention () When the pole voltage is at the same time, the line of the transistor element of the present invention is 1.5 to 1.5. The characteristics of the leakage current of the shoulder, please refer to Figure 7 '. Figure 7 shows the transistor in the room. One of the preferred embodiments of the source voltage (VGS) month Relationship diagram, the relationship between agricultural transduction value (gm) and gate-to-gate voltage, and the curve, which represents the relationship between the non-polar saturation current and voltage. The pole area of the pole 2 is as follows: 1x8ο # m2, and the source voltage (Vds) is fixed β Q υ ν, and the degree is 3 0 〇κ. As can be seen from Figure 7, at this time, The Office of the Electronic Crystal _ _ appealed that the maximum output current of the Japanese body components was 460mA / mm, and the maximum value was 162mS / mm. When the linear operating area is defined above the maximum transmissive value of 9G%, the saturation current area of one pole can be greater than 310mA / mm 'and the operating voltage area of the gate and source can be greater than 2V. The device has excellent linear operating characteristics. This also illustrates that by using a double-layered channel structure and the upper 'middle and lower three planar doped layers as the carrier supply layer', the carriers in the channel can be evenly decorated, so the component can be broad In the n-plane of the linear chirp region, the elimination of parallel conduction is operated at a large forward gate-source voltage +2.0 V, and the component still maintains a large transduction value of 135 mS / mm. Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs, please refer to FIG. 8. FIG. 8 shows the transconductance value (gm) and output conductance (gds) of the transistor at room temperature according to a preferred embodiment of the present invention. And voltage gain (Av) versus drain-source voltage (Vl) s), where curve d represents the relationship between transconductance value and drain-source voltage, and curve e represents the output conductance and 13 paper sizes are applicable China National Standard (CNS) A4 specification (210X297 mm) 557567
五、發明説明( 經濟部智慧財產局員工消費合作社印製 及-源極電壓之間的關係, ,,^ M 則代表電壓增益與汲. 源極電壓之間的關係。此 ,2 ―从 ®疋件之閘極面積為lx8C 偏壓在閘-源極電壓(Vos)為+0.5 V,溫度則為 3〇〇K。從第8圖可知,由 -度則為 ..^ ^ , 位佳之载子侷限能力及低的 /扁電机’在汲-源極電壓大 n4l 2·5 V時,可得到低的輸出 電導力為0·41 mS/mm’而配合高的轉導值i6〇ms/mm, 可以得到相當高之電壓增益(Av = gm/gd。值390。而由於本 發明疋件擁有相當高之電壓增益值’因此相當適合在放大 電路中使用。 請參照第9圖,第9圖係綠示本發明之一較佳實施例 之,晶體在室溫下頻率特性對沒極電流(Id)的關係圖。此 電晶體70件之閘極面積為lxl0〇# m2,汲-源極電壓(Vds) 為β 、 /Ja度則為3 0 0 κ。此時,當偏壓條件在汲__源極 電壓為3·5 V、閘.源極電壓(Vgs)為+〇·25 v下,其最大之 單位電流增益截止頻率(Unity Current Gain Cut_off FreqUenCy,/τ)為 13GHz,最大之震盪·頻率(Maximum Oscnllation Frequency ; /max)則為 32GHz,因此可知此電 晶體το件具有相當良好之頻率特性表現。同樣地,由於在 通道内的載子能夠均勻分佈,本發明元件也保有寬廣而線 性的頻率表現特性,如同第9圖所示,當汲極電流在6 0 至3 60mA/mm之操作範圍時,此電晶體元件之頻率操作 特性保持在其最大單位電流增益截止頻率及最大震盪頻 率值的90%以上。這也說明了本發明之電晶體元件相當適 14 本紙張尺度適用中國國家標準(CNS)A4規格(210X297公釐) (請先閲讀背面之注意事項再本頁) ’!· 装· 訂· #· 557567 經濟部智慧財產局員工消費合作社印製 五、發明説明( 合於高頻電路之應用。 综上戶…本發明具有雙層通道結構之擬麽增 移動率電晶體不但具有低漏電流、低輸出電導、: 盈、以及極佳之頻率表現等優點,更具有策廣而線 流、交流操作區域之優勢。因此,非常適用於微波… 通訊、微電子、及光電之領域與產業,例如光殲通訊系,·· 功率放大器、可攜式通訊器材、防撞雷達、衛星通訊、以 及區域無線通訊網路等。 如熟悉此技術之人員所瞭解的,以上所述僅為本發明 之鬏佳貫施例而已,並非用以限定本發明之申請專利範 $,、凡其它未脫離本發明所揭示之精神下所完成之等效改 艾或修飾’均應包含在下述之申請專利範圍内。 圓式簡單說明: 本發明的較佳實施例已於前述之說明文字中輔以下列 圖形做更詳細的闡述,其中·· 第1圖係繪示本發明之一較佳實施例之具有雙層通道 結構之擬晶性高電子移動率電晶體的剖面圖; 第2圖係繪示本發明之一較佳實施例之電晶體的相對 應導電帶能帶圖; 第3圖係繪示本發明之__齡4廉 乃(鬏佳貫施例之電晶體的兩端 閘極電流(iG)對閘-汲極電壓(Vgd)之關係圖; 第4圖料示第3圖之電晶體的閘極漏電師 對溫度的關係圖; 晶 性 高 電 孑 15 557567 A7 ------- B7 五、發明説明() ~" — -- 第5圖係繪示第3圖之電晶體的閘-汲極起始電壓(v。。) 對溫度的關係圖; 第6圖係繪示本發明之一較佳實施.例之電晶體在室溫 下之共源極輸出電流-電壓三端特性圖; 第7圖係繪不本發明之一較佳實施例之電晶體在室溫 下汲極飽和電流(IDS)及轉導值(gm)對閘_源極電壓(ν〇 關係圖; 第8圖係繪示本發明之一較佳實施例之電晶體在室溫 下之轉導值(gm)、輸出電導(gds)及電壓增益對汲·源 極電壓(V D s )的關係圖;以及 第9圖係繪示本發明之一較佳實施例之電晶體在室溫 下頻率特性對汲極電流(ID)的關係圖。 圈號對照說明: 經濟部智慧財產局員工消費合作社印製 100 電晶體 1 12 基板 1 14 緩衝層 116 緩衝層 118 平面摻雜層 120 隔離層 122 通道層 124 隔離層 126 平面摻雜層 128 隔離層 130 通道層 132 隔離層 134 平面摻雜層 136 蕭特基接觸層 138 平面摻雜層 140 隔離層 142 歐姆接觸層 144 源極 146 汲極 148 閘極 16V. Description of the invention (The relationship between the printed source and the source voltage of the consumer cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs, ,, M represents the relationship between the voltage gain and the source voltage. This, 2 ―From® The gate area of the component is lx8C. The bias voltage at the gate-source voltage (Vos) is +0.5 V, and the temperature is 300K. As can be seen from Figure 8, the degree of-is ^^, which is better. Carrier confinement capability and low / flat motor 'When the drain-source voltage is large n4l 2 · 5 V, a low output conductance of 0.41 mS / mm' can be obtained in conjunction with a high transduction value i6. ms / mm, you can get a very high voltage gain (Av = gm / gd. Value 390. And because the file of the present invention has a very high voltage gain value ', it is quite suitable for use in amplifier circuits. Please refer to Figure 9, Figure 9 is a green diagram showing the relationship between the frequency characteristics of the crystal and the non-polar current (Id) at room temperature in a preferred embodiment of the present invention. The gate area of 70 transistors of this transistor is lxl0〇 # m2. -The source voltage (Vds) is β, and / Ja degrees is 3 0 0 κ. At this time, when the bias condition is at the drain source voltage is 3.5V, the gate. Source voltage (Vgs) is + 〇 · 2 Under 5 v, its maximum unit current gain cut-off frequency (Unity Current Gain Cut_off FreqUenCy (/ τ)) is 13GHz, and the maximum oscillation frequency (Maximum Oscnllation Frequency; / max) is 32GHz, so it can be known that this transistor το component has Quite good frequency performance. Similarly, because the carriers in the channel can be evenly distributed, the element of the present invention also maintains a wide and linear frequency performance, as shown in Figure 9, when the drain current is 60 to 3 When the operating range is 60mA / mm, the frequency operating characteristics of this transistor element remain above 90% of its maximum unit current gain cut-off frequency and maximum oscillation frequency value. This also shows that the transistor element of the present invention is quite suitable for 14 papers. Standards are applicable to China National Standard (CNS) A4 specifications (210X297 mm) (Please read the precautions on the back before this page) '! · Binding · Order · 557567 Printed by the Intellectual Property Bureau of the Ministry of Economic Affairs Consumer Cooperatives V. Inventions Description (Suitable for the application of high-frequency circuits. To sum up ... the present invention has a double-layer channel structure of the proposed mobility-increasing transistor not only has low leakage current, The advantages of output conductance, profit, and excellent frequency performance have the advantages of wide and linear flow and AC operation area. Therefore, it is very suitable for microwave ... communication, microelectronics, and optoelectronics fields and industries, such as optical J Communication Department, · Power amplifiers, portable communication equipment, anti-collision radar, satellite communication, and regional wireless communication networks, etc. As understood by those familiar with this technology, the above is only a good idea of the present invention The examples are not intended to limit the patent application scope of the present invention, and any other equivalent alterations or modifications that have been made without departing from the spirit disclosed by the present invention should be included in the scope of the patent application described below. Brief description of the round form: The preferred embodiment of the present invention has been described in more detail in the preceding explanatory text with the following figures, of which: Figure 1 shows a preferred embodiment of the present invention with a double layer A cross-sectional view of a pseudo-crystalline high electron mobility transistor with a channel structure; FIG. 2 is a diagram showing a corresponding conductive band energy band of a transistor according to a preferred embodiment of the present invention; FIG. 3 is a diagram showing the present invention Zhi_Ling 4 Lian Nai (The relationship between the gate current (iG) and the gate-drain voltage (Vgd) at both ends of the transistor of the Jia Jiaguan example; Figure 4 shows the transistor of Figure 3 The relationship diagram of the gate leakage technician's temperature; crystalline high voltage 孑 15 557567 A7 ------- B7 V. Description of the invention () ~ "--Figure 5 shows the transistor of Figure 3 Gate-drain starting voltage (v ..) vs. temperature; Figure 6 shows a preferred embodiment of the present invention. The common source output current of the transistor at room temperature-voltage three Terminal characteristics diagram; FIG. 7 is a drawing showing the saturation current (IDS) and transconductance value (gm) of the transistor at a room temperature according to a preferred embodiment of the present invention. Relation diagram of voltage (ν〇; Figure 8 is a graph showing the transconductance value (gm), output conductance (gds) and voltage gain vs. source of the transistor at room temperature of a preferred embodiment of the present invention) The relationship diagram of voltage (VD s); and FIG. 9 is a diagram showing the relationship between the frequency characteristics of the transistor and the drain current (ID) at room temperature according to a preferred embodiment of the present invention. Printed by the Intellectual Property Bureau Staff Consumer Cooperative 100 Transistor 1 12 Substrate 1 14 Buffer layer 116 Buffer layer 118 Plane doped layer 120 Isolation layer 122 Channel layer 124 Isolation layer 126 Plane doped layer 128 Isolation layer 130 Channel layer 132 Isolation layer 134 planar doped layer 136 Schottky contact layer 138 planar doped layer 140 isolation layer 142 ohmic contact layer 144 source 146 drain 148 gate 16
557567 A7 B7 五、發明説明() 150 開口 a 曲線 b 曲線 C 曲線 d 曲線 e 曲線 f 曲線 (請先閱讀背面之注意事項再塡寫本頁) 、τ 經濟部智慧財產局員工消費合作社印製 17 本紙張尺度適用中國國家標準(CNS)A4規格(210X297公釐)557567 A7 B7 V. Description of the invention (150) Opening a Curve b Curve C Curve d Curve e Curve f Curve (Please read the precautions on the back before writing this page), τ Printed by the Employees ’Cooperative of Intellectual Property Bureau of the Ministry of Economic Affairs 17 This paper size applies to China National Standard (CNS) A4 (210X297 mm)
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Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
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TWI404209B (en) * | 2009-12-31 | 2013-08-01 | Univ Nat Chiao Tung | High electron mobility transistor and method for fabricating the same |
TWI637516B (en) * | 2017-08-07 | 2018-10-01 | 世界先進積體電路股份有限公司 | Semiconductor devices and methods for forming the same |
US10217854B1 (en) | 2017-09-29 | 2019-02-26 | Vanguard International Semiconductor Corporation | Semiconductor device and method of manufacturing the same |
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Cited By (3)
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TWI404209B (en) * | 2009-12-31 | 2013-08-01 | Univ Nat Chiao Tung | High electron mobility transistor and method for fabricating the same |
TWI637516B (en) * | 2017-08-07 | 2018-10-01 | 世界先進積體電路股份有限公司 | Semiconductor devices and methods for forming the same |
US10217854B1 (en) | 2017-09-29 | 2019-02-26 | Vanguard International Semiconductor Corporation | Semiconductor device and method of manufacturing the same |
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