TWI446532B - A structure of high electron mobility transistor, a device comprising the structure and a metnod of producing the same - Google Patents
A structure of high electron mobility transistor, a device comprising the structure and a metnod of producing the same Download PDFInfo
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- TWI446532B TWI446532B TW98134015A TW98134015A TWI446532B TW I446532 B TWI446532 B TW I446532B TW 98134015 A TW98134015 A TW 98134015A TW 98134015 A TW98134015 A TW 98134015A TW I446532 B TWI446532 B TW I446532B
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- 239000004065 semiconductor Substances 0.000 claims description 42
- 229910001218 Gallium arsenide Inorganic materials 0.000 claims description 24
- 238000000034 method Methods 0.000 claims description 22
- 239000002131 composite material Substances 0.000 claims description 18
- 229910018072 Al 2 O 3 Inorganic materials 0.000 claims description 15
- 238000000231 atomic layer deposition Methods 0.000 claims description 14
- 150000001875 compounds Chemical class 0.000 claims description 13
- 239000000758 substrate Substances 0.000 claims description 13
- 238000000151 deposition Methods 0.000 claims description 10
- 239000000463 material Substances 0.000 claims description 10
- 229910000530 Gallium indium arsenide Inorganic materials 0.000 claims description 9
- 229910000980 Aluminium gallium arsenide Inorganic materials 0.000 claims description 8
- 230000008021 deposition Effects 0.000 claims description 7
- 238000004519 manufacturing process Methods 0.000 claims description 7
- 229910052751 metal Inorganic materials 0.000 claims description 7
- 239000002184 metal Substances 0.000 claims description 7
- 229910052802 copper Inorganic materials 0.000 claims description 6
- 229910021193 La 2 O 3 Inorganic materials 0.000 claims description 4
- 229910052782 aluminium Inorganic materials 0.000 claims description 4
- 229910004166 TaN Inorganic materials 0.000 claims description 3
- 229910052737 gold Inorganic materials 0.000 claims description 3
- 229910052763 palladium Inorganic materials 0.000 claims description 3
- 229910052697 platinum Inorganic materials 0.000 claims description 3
- 229910052719 titanium Inorganic materials 0.000 claims description 2
- 239000004575 stone Substances 0.000 claims 1
- JBRZTFJDHDCESZ-UHFFFAOYSA-N AsGa Chemical compound [As]#[Ga] JBRZTFJDHDCESZ-UHFFFAOYSA-N 0.000 description 17
- 239000010408 film Substances 0.000 description 8
- 238000002955 isolation Methods 0.000 description 5
- 239000007789 gas Substances 0.000 description 4
- -1 GaAs metal oxide Chemical class 0.000 description 3
- 239000002019 doping agent Substances 0.000 description 3
- 238000005530 etching Methods 0.000 description 3
- 230000005669 field effect Effects 0.000 description 3
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 2
- 238000005229 chemical vapour deposition Methods 0.000 description 2
- 238000007796 conventional method Methods 0.000 description 2
- 239000013078 crystal Substances 0.000 description 2
- 238000010894 electron beam technology Methods 0.000 description 2
- 238000003780 insertion Methods 0.000 description 2
- 230000037431 insertion Effects 0.000 description 2
- 229910044991 metal oxide Inorganic materials 0.000 description 2
- TWNQGVIAIRXVLR-UHFFFAOYSA-N oxo(oxoalumanyloxy)alumane Chemical compound O=[Al]O[Al]=O TWNQGVIAIRXVLR-UHFFFAOYSA-N 0.000 description 2
- 229910005191 Ga 2 O 3 Inorganic materials 0.000 description 1
- 229910003855 HfAlO Inorganic materials 0.000 description 1
- 229910010052 TiAlO Inorganic materials 0.000 description 1
- 229910010413 TiO 2 Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 238000001312 dry etching Methods 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 238000001459 lithography Methods 0.000 description 1
- 238000001451 molecular beam epitaxy Methods 0.000 description 1
- 230000003647 oxidation Effects 0.000 description 1
- 238000007254 oxidation reaction Methods 0.000 description 1
- 239000000376 reactant Substances 0.000 description 1
- 239000012495 reaction gas Substances 0.000 description 1
- 239000011435 rock Substances 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 238000012360 testing method Methods 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Chemical compound O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
- 238000001039 wet etching Methods 0.000 description 1
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Description
本發明大致係關於一種製造在第III-V族複合半導體晶圓上之結構,及一種製造此結構的方法;上述之晶圓適合作為一種半導體元件來使用,例如做為開關或單石微波積體電路元件(monolithic microwave integrated circuit,MMIC)之放大器。The present invention generally relates to a structure fabricated on a Group III-V composite semiconductor wafer, and a method of fabricating the same; the wafer described above is suitable for use as a semiconductor component, for example as a switch or a single rock microwave product An amplifier of a monolithic microwave integrated circuit (MMIC).
習知的複合半導體元件,例如高電遷性電晶體(high electron mobility transistor,HEMT),通常會使用蕭特基二極體閘極來進行電流的調控。但是,這類元件的缺點是具有較高的閘極漏電流。因此,此領域中亟需一種可克服上述缺點的改良結構,以及可製造出此種改良結構的方法。Conventional composite semiconductor components, such as high electron mobility transistors (HEMTs), typically use Schottky diode gates for current regulation. However, such components have the disadvantage of having a higher gate leakage current. Accordingly, there is a need in the art for an improved structure that overcomes the above disadvantages, and a method of making such an improved structure.
基於上述缺點,本發明目地之一在於提供一種製造可應用在微波及雷達領域之半導體元件上的改良結構,使用此改良結構的半導體元件將表現出較低的閘極漏電流、較少的直流電力損耗、較少的衰減損耗以及較佳的隔絕性質。Based on the above disadvantages, one of the objects of the present invention is to provide an improved structure for fabricating semiconductor components applicable in the microwave and radar fields, and semiconductor devices using the improved structure will exhibit lower gate leakage current and less DC. Power loss, less attenuation loss, and better isolation.
因此,本發明是有關於一種製造在第III-V族複合半導體晶圓(其適合用在半導體元件上)上的結構,一種包含此結構的半導體元件以及一種製造此結構的方法。Accordingly, the present invention is directed to a structure fabricated on a Group III-V compound semiconductor wafer suitable for use on a semiconductor device, a semiconductor device including the structure, and a method of fabricating the structure.
在本發明一態樣中,提供一種GaAs金氧半導體假型高電遷性電晶體(GaAs metal oxide semiconductor pseudomorphic high electron mobility transistor,MOS-PHEMT)結構。此結構包括:一基板;一第III-V族複合半導體;一閘極介電質,其係經由原子層沉積法(atomic layer deposition,ALD)而沉積覆蓋在該第III-V族複合半導體上;複數個歐姆接點,耦接至該第III-V族複合半導體;以及一閘極電極,位在該閘極介電質上。在一實例中,此閘極介電質乃是一層厚度介於8nm至20nm間的氧化鋁(Al2 O3 )薄膜。In one aspect of the present invention, a GaAs metal oxide semiconductor pseudomorphic high electron mobility transistor (MOS-PHEMT) structure is provided. The structure comprises: a substrate; a III-V compound semiconductor; a gate dielectric deposited on the III-V compound semiconductor via atomic layer deposition (ALD) deposition a plurality of ohmic contacts coupled to the III-V compound semiconductor; and a gate electrode positioned on the gate dielectric. In one example, the gate dielectric is an aluminum oxide (Al 2 O 3 ) film having a thickness between 8 nm and 20 nm.
在本發明第二態樣中,提供一種製造上述結構的方法。此方法包括以下步驟:在一基板上形成一第III-V族複合半導體;以原子層沉積法在該第III-V族複合半導體上形成一閘極介電質;以電子槍沉積法(electron gun deposition,E-gun)形成多個與該第III-V族複合半導體耦接之歐姆接點;及以施加一層金屬在該閘極介電質上以形成一閘極電極。In a second aspect of the invention, a method of making the above structure is provided. The method comprises the steps of: forming a III-V compound semiconductor on a substrate; forming a gate dielectric on the III-V compound semiconductor by atomic layer deposition; and electron gun deposition (electron gun) Deposition, E-gun) forming a plurality of ohmic contacts coupled to the III-V compound semiconductor; and applying a layer of metal on the gate dielectric to form a gate electrode.
在本發明第三態樣中,提供一種GaAs MOS-PHEMT單刀雙擲(single-pole-double-throw,SPDT)開關,其包含以前述方法製成的GaAs MOS-PHEMT結構。相較於習知的PHEMT開關來說,此GaAs MOS-PHEMT SPDT開關的特徵在於具有較低的閘極漏電流、較少的直流電力損耗、較少的衰減損耗以及較佳的隔絕性質。In a third aspect of the invention, a GaAs MOS-PHEMT single-pole-double-throw (SPDT) switch comprising a GaAs MOS-PHEMT structure fabricated in the foregoing manner is provided. Compared to conventional PHEMT switches, the GaAs MOS-PHEMT SPDT switches are characterized by lower gate leakage current, less DC power loss, less attenuation loss, and better isolation properties.
透過以下的詳細明與附隨之申請專利範圍將可更了解本揭示內容的這些及其他特徵。需知以上的概述及以下的詳細說明僅為例示,用來闡述本揭示內容,而非用以限制本揭示內容之範疇。These and other features of the present disclosure will become more apparent from the following detailed description. The above summary and the following detailed description are merely illustrative, and are not intended to limit the scope of the disclosure.
以下,將參照附圖詳細說明本發明實施方式。在說明附圖時,相同元件符號代表相同或對應的元件。Hereinafter, embodiments of the present invention will be described in detail with reference to the accompanying drawings. In the description of the drawings, the same element symbols represent the same or corresponding elements.
本發明是有關於一種製造在第III-V族複合半導體晶圓上的MOS-PHEMT結構;以及一種製造此結構的方法,其中該第III-V族複合半導體晶圓可做為一種半導體元件來使用,例如當作MOS-PHEMT SPDT開關來使用。The present invention relates to a MOS-PHEMT structure fabricated on a Group III-V composite semiconductor wafer; and a method of fabricating the same, wherein the III-V compound semiconductor wafer can be used as a semiconductor component Use, for example, as a MOS-PHEMT SPDT switch.
在本發明之較佳實施方式中,一種製造在第III-V族複合半導體晶圓上之砷化鎵金氧半導體假型高電遷性電晶體(GaAs metal oxide semiconductor pseudomorphic high electron mobility transistor,GaAs MOS-PHEMT)結構,其特徵在於具有一層經由原子層沉積法(atomic layer deposition,ALD)所沉積而成的氧化鋁閘極介電質。此高k值之氧化鋁介電質可提供較低的閘極漏電流與較佳的熱安定性,因此可讓所製成的半導體元件(例如,MOS-PHEMT SPDT開關)具有較少的直流電損失,較少的衰減損失(insertion loss),並可使高頻開關元件具有較佳的隔絕效果。In a preferred embodiment of the present invention, a GaAs metal oxide semiconductor pseudomorphic high electron mobility transistor (GaAs) fabricated on a III-V composite semiconductor wafer is used. A MOS-PHEMT) structure characterized by having a layer of an aluminum oxide gate dielectric deposited by atomic layer deposition (ALD). This high-k alumina dielectric provides lower gate leakage current and better thermal stability, thus allowing the fabricated semiconductor components (eg, MOS-PHEMT SPDT switches) to have less DC current Loss, less loss of insertion, and high-frequency switching elements have better insulation.
在一實施方式中,提供一種製造在第III-V族複合半導體晶圓上之MOS-PHEMT元件10。此元件是以習知的微影蝕刻和剝離(lift-off)技術製成,包括台面蝕刻(mesa etch)、凹陷蝕刻(recess etch)、介電質沉積、形成歐姆接點和閘極等技術。表1詳細列出有關此製造在第III-V族複合半導體晶圓上之砷化鎵金氧半導體假型高電遷性電晶體(GaAs MOS-PHEMT)之特定實例的細節。表1各欄中分別列出此特定實例中每一層的功能、厚度()及各成分的莫耳比例。In one embodiment, a MOS-PHEMT device 10 fabricated on a Group III-V compound semiconductor wafer is provided. This component is fabricated using conventional lithography and lift-off techniques, including mesa etch, recess etch, dielectric deposition, ohmic contacts, and gates. . Table 1 details details of a specific example of the gallium arsenide oxy-semiconductor pseudo-high-reactive transistor (GaAs MOS-PHEMT) fabricated on the III-V composite semiconductor wafer. The functions and thicknesses of each layer in this particular example are listed in the respective columns of Table 1. And the molar ratio of each component.
第1A圖繪示出尚未完全完成之GaAs MOS-PHEMT結構的橫斷面示意圖。依據此實施方式,可在基板100上依序生長出各種磊晶層。可以任何一種第III-V族材料(例如,GaAs、InP或其他類似物,且較佳是GaAs或任一種以GaAs為基礎的材料)來製造此基板100,也可使用任何已知的技術(例如,金屬有機化學氣相沉積法(metal-organic chemical vapor deposition,MOCVD)、或分子束磊晶(molecule beam epitaxy,MBE))在基板100上成長上述的各種磊晶層。在本發明一態樣中,先在基板100上創造出一層緩衝層101。在第1A圖的實例中,此特定的緩衝層101是一種不含摻質的GaAs層。接著,依序在該緩衝層101上磊晶生長厚度為13nm之無摻質的InGaAs層102、及厚度為40nm且含有δ-摻雜106於其中之無摻質的AlGaAs層103。在第1A圖中,此δ-摻雜106係以虛線表示。在第1A圖之特定實施方式中,此不含摻質的InGaAs層102是一種無摻質的In0.2 Ga0.8 As層,且此含有δ-摻雜106於其中之無摻質的AlGaAs層103是一種無摻質的Al0.25 Ga0.75 As層103。接著,也可於第1A圖之特定結構上生長約1.5nm之AlAs層104,接著生長約60nm之含有n+型摻質的GaAs層105。Figure 1A depicts a cross-sectional view of a GaAs MOS-PHEMT structure that has not been fully completed. According to this embodiment, various epitaxial layers can be sequentially grown on the substrate 100. The substrate 100 can be fabricated from any of the Group III-V materials (eg, GaAs, InP, or the like, and preferably GaAs or any GaAs-based material), and any known technique can be used ( For example, metal-organic chemical vapor deposition (MOCVD) or molecular beam epitaxy (MBE) grows various epitaxial layers described above on the substrate 100. In one aspect of the invention, a buffer layer 101 is first created on the substrate 100. In the example of Figure 1A, this particular buffer layer 101 is a GaAs layer that does not contain dopants. Next, a non-doped InGaAs layer 102 having a thickness of 13 nm and an undoped AlGaAs layer 103 having a thickness of 40 nm and containing δ-doping 106 therein are epitaxially grown on the buffer layer 101. In Figure 1A, this δ-doping 106 is indicated by a dashed line. In a particular embodiment of FIG. 1A, the dopant-free InGaAs layer 102 is a non-doped In 0.2 Ga 0.8 As layer, and the δ-doped 106 has no dopant-doped AlGaAs layer 103 therein. It is a non-doped Al 0.25 Ga 0.75 As layer 103. Next, an AlAs layer 104 of about 1.5 nm may be grown on the specific structure of FIG. 1A, followed by an GaAs layer 105 containing an n+ type dopant of about 60 nm.
接著,以任何適當之已知的蝕刻技術來蝕刻第1A圖之特定結構,以形成如第1B圖所示具有凹槽的結構。可以任何標準的蝕刻技術來執行此蝕刻步驟,包括濕蝕刻或乾蝕刻。接著,再利用原子層沉積法(ALD)沉積一層閘極介電質107於第1B圖之結構中。適合做為閘極介電質的材料可選自由Al2 O3 、HfO2 、La2 O3 、ZrO2 、Ga2 O3 、Y2 O3 、TiO2 、Ta2 O5 、HfAlO、TiAlO和LaAlO所組成的群組中。適合做為閘極介電質的材料較佳是選自以下任一者:Al2 O3 、HfO2 、La2 O3 ,或ZrO2 。在第1C圖的結構中,係以原子層沉積法在約300℃的溫度下沉積出約8nm至約20nm的Al2 O3 層。較佳是,從包含有三甲基鋁(trimethylalumium,TMA)和水蒸氣的來源氣體中,沉積出約16nm的Al2 O3 層。在一實施方式中,執行由TMA、N2 、H2 O及N2 組成之氣體循環,其中該TMA、N2 、H2 O及N2 的時間分別被設定為1、10、1及10秒,且在此氣體循環中,氧化鋁的沉積速率約為1.3/循環。在一實施方式中,用以執行ALD製程的腔室是由儀器科技研究中心(台灣)所提供,但是也可使用其他適當的製程腔室來實施此ALD製程。相較於習知用來形成Al2 O3 薄膜的方法來說,例如,濺鍍、化學氣相沉積法或是將純鋁膜氧化,由ALD法沉積而成的Al2 O3 薄膜,其品質較佳。ALD是一種利用依序使用氣相反應物來進行沉積的技術,其可沉積出超薄薄膜。透過使生長表面重複地暴露在反應氣體下,可使每一次循環中所沉積出來的膜層量維持不變(即,固定),因此,可在原子層的層級上來控制沉積膜層的厚度。在所示的實施例中,所沉積出來的Al2 O3 介電膜具有極低的漏電流,對厚度約16nm的膜層來說,漏電流的密度約在10-8 A/cm2 。Next, the specific structure of FIG. 1A is etched by any suitable known etching technique to form a structure having a recess as shown in FIG. 1B. This etching step can be performed by any standard etching technique, including wet etching or dry etching. Next, a layer of gate dielectric 107 is deposited in the structure of FIG. 1B by atomic layer deposition (ALD). Suitable materials for the gate dielectric are Al 2 O 3 , HfO 2 , La 2 O 3 , ZrO 2 , Ga 2 O 3 , Y 2 O 3 , TiO 2 , Ta 2 O 5 , HfAlO, TiAlO. And the group consisting of LaAlO. A material suitable as the gate dielectric is preferably selected from the group consisting of Al 2 O 3 , HfO 2 , La 2 O 3 , or ZrO 2 . In the structure of Fig. 1C, an Al 2 O 3 layer of about 8 nm to about 20 nm is deposited by atomic layer deposition at a temperature of about 300 °C. Preferably, an Al 2 O 3 layer of about 16 nm is deposited from a source gas containing trimethylalumium (TMA) and water vapor. In one embodiment, a gas cycle consisting of TMA, N 2 , H 2 O, and N 2 is performed, wherein times of TMA, N 2 , H 2 O, and N 2 are set to 1, 10, 1, and 10, respectively. Seconds, and in this gas cycle, the deposition rate of alumina is about 1.3 /cycle. In one embodiment, the chamber used to perform the ALD process is provided by the Instrument Technology Research Center (Taiwan), but other suitable process chambers may be used to implement the ALD process. Compared with the conventional method for forming an Al 2 O 3 film, for example, sputtering, chemical vapor deposition, or oxidation of a pure aluminum film, an Al 2 O 3 film deposited by an ALD method, Better quality. ALD is a technique that utilizes sequential gas phase reactants for deposition, which deposits ultra-thin films. By repeatedly exposing the growth surface to the reaction gas, the amount of the film deposited in each cycle can be maintained constant (i.e., fixed), and therefore, the thickness of the deposited film layer can be controlled at the level of the atomic layer. In the illustrated embodiment, the deposited Al 2 O 3 dielectric film has a very low leakage current, and the density of the leakage current is about 10 -8 A/cm 2 for a film having a thickness of about 16 nm.
接著,在所示的實例中,於第III-V族複合半導體結構中一活性區域109的兩相對立側邊附近,形成與此複合結構(即,基板100及其上之多層磊晶層)耦接的兩個歐姆接觸108,如第1D圖所示。這些歐姆接觸108是透過電子束槍(E-gun)方式,以一種選自Ni、Ge、Cu、Pd、Au及其之組合的金屬所沉積而成的。在所示的實例中,係以Ge-Au來形成所述的歐姆接觸108。此外,也可利用電子束槍法在上述的閘極介電質107上形成金屬閘極電極110,且其包含選自Ti、Pt、Cu、Al、TaN、Au及其之組合的金屬(其與用來形成該些歐姆接觸108之材料不盡相同)所製成的電極。在所揭示的實施例中,該閘極電極110是由Ti-Au所製成。Next, in the illustrated example, a composite structure (ie, the substrate 100 and the multilayer epitaxial layer thereon) is formed in the vicinity of the opposite sides of an active region 109 in the III-V compound semiconductor structure. Two ohmic contacts 108 are coupled as shown in FIG. 1D. These ohmic contacts 108 are deposited by means of an electron beam gun (E-gun) in a metal selected from the group consisting of Ni, Ge, Cu, Pd, Au, and combinations thereof. In the example shown, the ohmic contact 108 is formed with Ge-Au. In addition, the metal gate electrode 110 may be formed on the gate dielectric 107 by using an electron beam gun method, and it may include a metal selected from the group consisting of Ti, Pt, Cu, Al, TaN, Au, and combinations thereof (which is The electrodes used to form the ohmic contacts 108 are not identical. In the disclosed embodiment, the gate electrode 110 is made of Ti-Au.
在此揭示的實施方式均可應用在第III-V族複合半導體晶圓上。依據本發明實施方式之方法而形成的複合半導體結構可用來製造各種MMICs,包括SPDT開關。可依據所揭示方法實施方式來製造適當的高電遷性電晶體(HEMT),其包括,但不限於,假型高電遷性電晶體(PHEMT)、金氧半導體場效電晶體(metal-oxide-semiconductor field effect transistor,MOSFET)、金屬半導體場效電晶體(metal-semiconductor field effect transistor,MESFET)和改性高電遷性電晶體(metamorphic high electron mobility transistor,MHEMT)。The embodiments disclosed herein can be applied to a Group III-V compound semiconductor wafer. Composite semiconductor structures formed in accordance with the methods of embodiments of the present invention can be used to fabricate a variety of MMICs, including SPDT switches. Suitable high-reactive electro-optical crystals (HEMTs) can be fabricated in accordance with the disclosed method embodiments, including, but not limited to, pseudo-high-reactive electro-optical crystals (PHEMT), MOS field-effect transistors (metal- Oxide-semiconductor field effect transistor (MOSFET), metal-semiconductor field effect transistor (MESFET) and modified high electron mobility transistor (MHEMT).
在一較佳實施方式中,以上述方法製造出閘極長度為0.5μm之MOS-PHEMT結構。在此實例中,此MOS-PHEMT結構的特徵是具有約16nm的Al2 O3 閘極介電質。接著利用測量漏電流、控制電流和微波頻率特徵等方式來評估所製造出來的開關。結果示於第2圖中。In a preferred embodiment, a MOS-PHEMT structure having a gate length of 0.5 μm is fabricated by the above method. In this example, this MOS-PHEMT structure is characterized by having an Al 2 O 3 gate dielectric of about 16 nm. The resulting switch is then evaluated by measuring leakage current, control current, and microwave frequency characteristics. The results are shown in Figure 2.
參照第2圖,相較於以習知方法製成的PHEMT結構來說,包含本發明MOS-PHEMT結構的開關在各種電位下,對各種閘極偏壓的容忍度較大(第2圖),在VG =-25V時,幾乎沒有漏電流;然而,同樣電壓下,具有習知PHEMT結構的開關之漏電流則高達約-0.5mA/mm。Referring to Fig. 2, the switch including the MOS-PHEMT structure of the present invention has a high tolerance to various gate biases at various potentials compared to the PHEMT structure fabricated by the conventional method (Fig. 2). At V G = -25 V, there is almost no leakage current; however, at the same voltage, the leakage current of the switch having the conventional PHEMT structure is as high as about -0.5 mA/mm.
第3圖繪示出SPDT開關的控制電流與控制電壓間的關係。相較於以習知PHEMT結構所製造而成的開關來說,具有本發明MOS-PHEMT結構的SPDT開關在整個1.5V至5.0V的測試範圍,都表現出較低的控制電流。Figure 3 depicts the relationship between the control current of the SPDT switch and the control voltage. The SPDT switch having the MOS-PHEMT structure of the present invention exhibits a lower control current over the entire 1.5V to 5.0V test range compared to a switch fabricated using the conventional PHEMT structure.
SPDT開關元件的衰減損失(insertion loss)和隔絕性繪示於第4圖中。具有本發明MOS-PHEMT結構的SPDT開關在2.5GHz(控制電壓=+3/0V)下的衰減損失大約為0.3dB,隔絕性約33.4dB。此外,RF特性也顯示使用本發明MOS-PHEMT結構可顯著的改善開關的隔絕效果,表示可使用本發明MOS-PHEMT結構來製造MMICs。The insertion loss and isolation of the SPDT switching elements are shown in Figure 4. The SPDT switch having the MOS-PHEMT structure of the present invention has an attenuation loss of about 0.3 dB at 2.5 GHz (control voltage = +3/0 V) and an isolation of about 33.4 dB. In addition, the RF characteristics also show that the use of the MOS-PHEMT structure of the present invention can significantly improve the isolation of the switch, indicating that the MMOSs can be fabricated using the MOS-PHEMT structure of the present invention.
雖然已參照特定實施例詳細敘述本發明精神,然而該等實施例僅是用於說明本發明,而非限制本發明。須了解熟悉此技術者可在不偏離本發明範圍及精神的情況下變化或修改該實施例。The present invention has been described in detail with reference to the preferred embodiments thereof. It is to be understood that those skilled in the art can change or modify the embodiment without departing from the scope and spirit of the invention.
100...基板100. . . Substrate
101...緩衝層101. . . The buffer layer
102...無摻質的InGaAs層102. . . Non-doped InGaAs layer
103...無摻質的AlGaAs層103. . . Non-doped AlGaAs layer
104...AlAs層104. . . AlAs layer
105...含有n+型摻質的GaAs層105. . . GaAs layer containing n+ type dopant
106...δ-摻雜106. . . Δ-doping
107...閘極介電質107. . . Gate dielectric
108...歐姆接觸108. . . Ohmic contact
109...活性區域109. . . Active area
110...金屬閘極電極110. . . Metal gate electrode
為讓本揭示內容之上述和其他目的、特徵、優點與實施例能更明顯易懂,所附圖式之說明如下:The above and other objects, features, advantages and embodiments of the present disclosure will become more apparent and understood.
第1A~1E圖示出依據本發明方法所製造出來的GaAs MOS-PHEMT結構在各製造階段中的截面示意圖;1A to 1E are schematic cross-sectional views showing the GaAs MOS-PHEMT structure fabricated in accordance with the method of the present invention in various stages of fabrication;
第2圖示出在(a)習知PHEMT元件,與(b)依據本發明一較佳實施方式所製造出來的GaAs MOS-PHEMT元件上,所分別量測到的閘極漏電流隨電壓變化的情形;Figure 2 shows the gate leakage current measured with voltage difference between (a) a conventional PHEMT device and (b) a GaAs MOS-PHEMT device fabricated in accordance with a preferred embodiment of the present invention. Situation
第3圖示出在(a)習知PHEMT元件,與(b)依據本發明一較佳實施方式所製造出來的GaAs MOS-PHEMT元件上,所分別量測到的控制電流隨控制電壓變化的情形;和Figure 3 shows the control current measured by the (a) conventional PHEMT element, and (b) the GaAs MOS-PHEMT element fabricated in accordance with a preferred embodiment of the present invention. Situation; and
第4圖示出在(a)習知PHEMT元件,與(b)依據本發明一較佳實施方式所製造出來的GaAs MOS-PHEMT元件上,所分別量測到的衰減損失隨頻率變化的情形。Figure 4 shows the variation of the attenuation loss measured with frequency on (a) a conventional PHEMT device, and (b) a GaAs MOS-PHEMT device fabricated in accordance with a preferred embodiment of the present invention. .
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