TWI503969B - High electron mobility transistor and manufacturing method thereof - Google Patents

High electron mobility transistor and manufacturing method thereof Download PDF

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TWI503969B
TWI503969B TW102124851A TW102124851A TWI503969B TW I503969 B TWI503969 B TW I503969B TW 102124851 A TW102124851 A TW 102124851A TW 102124851 A TW102124851 A TW 102124851A TW I503969 B TWI503969 B TW I503969B
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electron mobility
high electron
mobility transistor
barrier layer
thickness
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TW102124851A
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TW201503364A (en
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Jung Ruey Tsai
Kuo Sue Wei
Yi Sheng Chang
Guo Cheng Lin
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Univ Asia
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高電子遷移率電晶體及其製造方法 High electron mobility transistor and method of manufacturing same

本發明是有關於一種高電子遷移率電晶體及其製造方法,特別是有關於一種障礙層包含閘極下方之第一部分以及與其相鄰之第二部分,且障礙層的第一部分和第二部分具有Al和Ga的不同莫耳分率的高電子遷移率電晶體及其製造方法。 The present invention relates to a high electron mobility transistor and a method of fabricating the same, and more particularly to a barrier layer including a first portion under the gate and a second portion adjacent thereto, and the first portion and the second portion of the barrier layer A high electron mobility transistor having a different molar fraction of Al and Ga and a method of manufacturing the same.

氮化鋁鎵/氮化鎵高電子遷移率電晶體(AlGaN/GaN HEMT),由於擁有卓越的載子傳輸特性,因此常被應用在高功率、高溫度以及高頻率的電路操作中。 Aluminum gallium nitride/gallium nitride high electron mobility transistors (AlGaN/GaN HEMTs) are often used in high power, high temperature, and high frequency circuit operations due to their excellent carrier transport characteristics.

然而,現有之高電子遷移率電晶體,由於障礙層與通道層之間會形成二維電子氣(2DEG),因此能達到非常快的切換速度。但相對地,因電子通過路徑隨時存在,即使閘極電壓為零,電流仍會通過,而造成高電子遷移率電晶體常開(Normally-On)的問題,亦即,在作為電路操作元件時,即使閘極沒有施加電壓,通道仍然存在,亦即仍然會有電流通過,造成電路操作上之不便。 However, in the existing high electron mobility transistor, since a two-dimensional electron gas (2DEG) is formed between the barrier layer and the channel layer, a very fast switching speed can be achieved. But relatively, because the electron transit path exists at any time, even if the gate voltage is zero, the current will pass, causing the problem of the high electron mobility transistor normally-on, that is, when operating as a circuit operation component. Even if no voltage is applied to the gate, the channel still exists, that is, there is still current passing, which causes inconvenience in circuit operation.

有鑒於此,本發明之發明人思索並設計一種高電子遷移率電晶體及其製造方法,以針對現有技術之缺失加以改善,使得高電子遷移率電晶體能夠常閉(Normally-Off),進而增進產業上之實施利 用。 In view of the above, the inventors of the present invention have conceived and designed a high electron mobility transistor and a manufacturing method thereof to improve the defect of the prior art, so that the high electron mobility transistor can be normally closed (Normally-Off). Improve the implementation of the industry use.

有鑑於上述習知技術之問題,本發明之目的就是在提供一種高電子遷移率電晶體及其製造方法,以解決習知技術之高電子遷移率電晶體之常開(Normally-On)問題。 In view of the above problems of the prior art, it is an object of the present invention to provide a high electron mobility transistor and a method of fabricating the same that solve the problem of the normally-on problem of the high electron mobility transistor of the prior art.

根據本發明之目的,提出一種高電子遷移率電晶體,其包含基材、通道層、障礙層、源極、汲極及閘極。通道層形成於基材上。障礙層形成於通道層上。源極形成於障礙層上,源極與通道層之間形成歐姆接觸(Ohmic Contact)。汲極形成於障礙層上,汲極與通道層之間形成歐姆接觸。閘極形成於障礙層上,以形成蕭基接觸(Schottky Contact),其中閘極位於源極與汲極之間。其中,障礙層包含位於閘極下方之第一部分,以及位於源極與汲極下方且與第一部分相鄰之第二部分,第一部分以AlxGa1-xN形成且具有第一厚度,第二部分以AlyGa1-yN形成且具有第二厚度。其中,第一厚度小於第二厚度,x值小於y值。 In accordance with the purpose of the present invention, a high electron mobility transistor is disclosed that includes a substrate, a channel layer, a barrier layer, a source, a drain, and a gate. The channel layer is formed on the substrate. A barrier layer is formed on the channel layer. The source is formed on the barrier layer, and an ohmic contact is formed between the source and the channel layer. The drain is formed on the barrier layer and an ohmic contact is formed between the drain and the channel layer. A gate is formed on the barrier layer to form a Schottky Contact, wherein the gate is located between the source and the drain. Wherein the barrier layer comprises a first portion under the gate and a second portion below the source and the drain and adjacent to the first portion, the first portion being formed of Al x Ga 1-x N and having a first thickness, The two portions are formed of Al y Ga 1-y N and have a second thickness. Wherein the first thickness is less than the second thickness and the x value is less than the y value.

較佳者,通道層可以GaN形成。 Preferably, the channel layer can be formed of GaN.

較佳者,x值可為0.02至0.5,且y值可為0.2至0.7。 Preferably, the value of x can be from 0.02 to 0.5 and the value of y can range from 0.2 to 0.7.

較佳者,第一厚度可介於1nm至4nm,且第二厚度可介於1.5nm至40nm。 Preferably, the first thickness may be between 1 nm and 4 nm, and the second thickness may be between 1.5 nm and 40 nm.

根據本發明之目的,另提出一種高電子遷移率電晶體之製造方法,其包含下列步驟:提供基材;形成通道層於基材上;形成障礙層於通道層上;形成源極於障礙層上,源極與通道層之間形成歐姆接觸;形成汲極於障礙層上,汲極與通道層之間形成歐姆接觸 ;以及形成閘極於障礙層上,以形成蕭基接觸,其中閘極位於源極與汲極之間;其中,障礙層包含位於閘極下方之第一部分,以及位於源極與汲極下方且與第一部分相鄰之第二部分,第一部分以AlxGa1-xN形成且具有第一厚度,第二部分以AlyGa1-yN形成且具有第二厚度;其中,第一厚度小於第二厚度,x值小於y值。 According to the purpose of the present invention, a method for manufacturing a high electron mobility transistor is further provided, which comprises the steps of: providing a substrate; forming a channel layer on the substrate; forming a barrier layer on the channel layer; forming a source in the barrier layer Forming an ohmic contact between the source and the channel layer; forming a drain on the barrier layer, forming an ohmic contact between the drain and the channel layer; and forming a gate on the barrier layer to form a Schottky contact, wherein the gate Located between the source and the drain; wherein the barrier layer includes a first portion under the gate and a second portion below the source and the drain and adjacent to the first portion, the first portion being Al x Ga 1-x N is formed and has a first thickness, and the second portion is formed of Al y Ga 1-y N and has a second thickness; wherein the first thickness is less than the second thickness and the x value is less than the y value.

承上所述,依本發明之高電子遷移率電晶體及其製造方法,其可具有下述優點:此高電子遷移率電晶體及其製造方法可藉由降低閘極下方之障礙層之莫耳分率及厚度,以改善高電子遷移率電晶體Normally-On的問題。 According to the present invention, the high electron mobility transistor and the method of manufacturing the same can have the following advantages: the high electron mobility transistor and the method of fabricating the same can reduce the barrier layer under the gate Ear fraction and thickness to improve the problem of high electron mobility transistor Normally-On.

1‧‧‧高電子遷移率電晶體 1‧‧‧High Electron Mobility Transistor

11‧‧‧基材 11‧‧‧Substrate

12‧‧‧通道層 12‧‧‧Channel layer

13‧‧‧障礙層 13‧‧‧ obstacle layer

131‧‧‧第一部分 131‧‧‧Part 1

132‧‧‧第二部分 132‧‧‧Part II

14‧‧‧源極 14‧‧‧ source

15‧‧‧汲極 15‧‧‧汲polar

16‧‧‧閘極 16‧‧‧ gate

S1~S6‧‧‧步驟流程 S1~S6‧‧‧Step process

第1圖 係為本發明之高電子遷移率電晶體之結構圖。 Fig. 1 is a structural view of a high electron mobility transistor of the present invention.

第2圖 係為本發明之高電子遷移率電晶體之製造方法之步驟流程圖。 Fig. 2 is a flow chart showing the steps of the method for producing a high electron mobility transistor of the present invention.

為利 貴審查員瞭解本發明之技術特徵、內容與優點及其所能達成之功效,茲將本發明配合附圖,並以實施例之表達形式詳細說明如下,而其中所使用之圖式,其主旨僅為示意及輔助說明書之用,未必為本發明實施後之真實比例與精準配置,故不應就所附之圖式的比例與配置關係解讀、侷限本發明於實際實施上的權利範圍,合先敘明。 The technical features, contents, and advantages of the present invention, as well as the advantages thereof, can be understood by the present inventors, and the present invention will be described in detail with reference to the accompanying drawings. The subject matter is only for the purpose of illustration and description. It is not intended to be a true proportion and precise configuration after the implementation of the present invention. Therefore, the scope and configuration relationship of the attached drawings should not be interpreted or limited. First described.

請參閱第1圖,係為本發明之高電子遷移率電晶體之結構圖。如圖所示,本發明之高電子遷移率電晶體1包含基材11、通道層12、障礙層13、源極14、汲極15以及閘極16。通道層12及障礙層13 係可例如以物理氣相沉積(physical vapor deposition,PVD)法或化學氣相沉積(chemical vapor deposition,CVD)法依序形成於基材11上,其中基材11可例如為藍寶石(Sapphire)基板;源極14係形成於障礙層13上,且源極14與通道層12之間形成歐姆接觸;汲極15形成於障礙層13上,汲極15與通道層12之間形成歐姆接觸。 Please refer to FIG. 1 , which is a structural diagram of a high electron mobility transistor of the present invention. As shown, the high electron mobility transistor 1 of the present invention comprises a substrate 11, a channel layer 12, a barrier layer 13, a source 14, a drain 15 and a gate 16. Channel layer 12 and barrier layer 13 The substrate 11 can be sequentially formed on the substrate 11 by, for example, a physical vapor deposition (PVD) method or a chemical vapor deposition (CVD) method, wherein the substrate 11 can be, for example, a sapphire substrate. The source 14 is formed on the barrier layer 13 and an ohmic contact is formed between the source 14 and the channel layer 12; the drain 15 is formed on the barrier layer 13 and an ohmic contact is formed between the drain 15 and the channel layer 12.

接著,可例如以習知之微影及蝕刻製程對障礙層13進行蝕刻以形成凹槽,並且利用同一光罩圖形將閘極16形成於障礙層13之凹槽中,以形成蕭基接觸。其中,閘極16位於源極14與汲極15之間,而閘極16之材料可例如選自於Al及Ni所組成之族群。 Next, the barrier layer 13 can be etched to form a recess, for example, by conventional lithography and etching processes, and the gate 16 is formed in the recess of the barrier layer 13 using the same mask pattern to form a Schottky contact. The gate 16 is located between the source 14 and the drain 15 , and the material of the gate 16 can be selected, for example, from the group consisting of Al and Ni.

值得注意的是,障礙層13可分為第一部分131以及第二部分132。第一部分131係位於閘極16下方,其厚度較薄,第二部分132則位於源極14及汲極15下方,與第一部分131相鄰,第二部分132的厚度較厚。此外,障礙層13整體係以Al、Ga及N之化合物形成,然而,其第一部分131與第二部分132,關於所添加的Al含量的多寡,而使得Al的莫耳分率不同。當以AlxGa1-xN表示第一部分131,且以AlyGa1-yN表示第二部分132時,x值係小於y值,亦即,第一部分131的Al的莫耳分率小於第二部分132的Al的莫耳分率。 It is to be noted that the barrier layer 13 can be divided into a first portion 131 and a second portion 132. The first portion 131 is located below the gate 16 and has a relatively thin thickness. The second portion 132 is located below the source 14 and the drain 15 adjacent to the first portion 131. The second portion 132 is thicker. Further, the barrier layer 13 is entirely formed of a compound of Al, Ga, and N, however, the first portion 131 and the second portion 132 have different Mo content of Al depending on the amount of Al added. When the first portion 131 is represented by Al x Ga 1-x N and the second portion 132 is represented by Al y Ga 1-y N, the value of x is less than the value of y, that is, the molar fraction of Al of the first portion 131 Less than the molar fraction of Al of the second portion 132.

如此一來,藉由降低第一部分131的厚度及Al的莫耳分率改變通道層12及障礙層13之間的極化效應,使得障礙層13之第一部分131下方與通道層12介面之間的二維電子氣(2DEG)的濃度降低,並且提高電晶體之臨界電壓,進而使得高電子遷移率電晶體1較趨向為Normal-Off狀態,亦即,當閘極未施加電壓時,通道不存在,亦即不會有電流通過,使得電路操作上將較為方便。此外, 本發明之高電子遷移率電晶體1之結構亦使得其臨界電壓高於1V,藉此則較不易造成漏電流之問題,以減少功率耗損。 In this way, by reducing the thickness of the first portion 131 and the molar fraction of Al, the polarization effect between the channel layer 12 and the barrier layer 13 is changed, so that the lower portion of the first portion 131 of the barrier layer 13 and the channel layer 12 interface The concentration of the two-dimensional electron gas (2DEG) is lowered, and the threshold voltage of the transistor is increased, so that the high electron mobility transistor 1 tends to be in a Normal-Off state, that is, when the gate is not applied with a voltage, the channel is not Existence, that is, no current will pass, making the circuit more convenient to operate. In addition, The structure of the high electron mobility transistor 1 of the present invention also makes the threshold voltage higher than 1V, thereby making it less susceptible to leakage current problems and reducing power consumption.

順帶一提的是,通道層12可以GaN形成。由於GaN具有自發極化效應(spontaneous polarization)與壓電極化效應(piezoelectric polarization),因此相較於習知之Si及GaAs具有更高的電子濃度,更可提高本發明之高電子遷移率電晶體1之輸出功率。 Incidentally, the channel layer 12 can be formed of GaN. Since GaN has spontaneous polarization and piezoelectric polarization, it has higher electron concentration than conventional Si and GaAs, and can improve the high electron mobility transistor 1 of the present invention. Output power.

此外,當以AlxGa1-xN表示第一部分131,且以AlyGa1-yN表示第二部分132時,則x值係小於y值,且x值可為0.02至0.5,y值可為0.2至0.7。再者,於較佳的實施例中,第一部分131較第二部分132為薄,且第一部分131之厚度可介於1nm至4nm,第二部分132之厚度可介於1.5nm至40nm。 Further, when the first portion 131 is represented by Al x Ga 1-x N and the second portion 132 is represented by Al y Ga 1-y N, then the value of x is less than the value of y, and the value of x may be 0.02 to 0.5, y The value can be from 0.2 to 0.7. Moreover, in a preferred embodiment, the first portion 131 is thinner than the second portion 132, and the first portion 131 may have a thickness of 1 nm to 4 nm, and the second portion 132 may have a thickness of 1.5 nm to 40 nm.

簡單地說,藉由將障礙層13形成如第1圖所示之凹槽,並使得第一部分131其Al之莫耳分率小於第二部分132之Al之莫耳分率,將大幅度的改善傳統高電子遷移率電晶體皆具有之Normally-On問題,使得本發明之高電子遷移率電晶體1作為電路操作元件時,可更具有方便性與準確性。 Briefly, by forming the barrier layer 13 into a groove as shown in Fig. 1, and making the first portion 131 have a molar fraction of Al lower than that of the second portion 132, it will be substantially large. Improving the Normally-On problem of conventional high electron mobility transistors makes the high electron mobility transistor 1 of the present invention more convenient and accurate as a circuit operation component.

儘管於前述說明本發明之高電子遷移率電晶體之過程中,亦已同時說明本發明之高電子遷移率電晶體之製造方法之概念,但為求清楚起見,以下另繪示步驟流程圖以詳細說明。 Although the concept of the method for manufacturing a high electron mobility transistor of the present invention has been simultaneously described in the foregoing description of the high electron mobility transistor of the present invention, for the sake of clarity, the flow chart of the steps is further illustrated below. To explain in detail.

請參閱第2圖,其係為本發明之高電子遷移率電晶體之製造方法之步驟流程圖。如圖所示,本發明之高電子遷移率電晶體之製造方法可包含下列步驟:在步驟S1中,提供基材。 Please refer to FIG. 2, which is a flow chart of the steps of the method for manufacturing a high electron mobility transistor of the present invention. As shown, the method of manufacturing a high electron mobility transistor of the present invention may comprise the step of providing a substrate in step S1.

在步驟S2中,形成通道層於基材上。 In step S2, a channel layer is formed on the substrate.

在步驟S3中,形成障礙層於通道層上。 In step S3, a barrier layer is formed on the channel layer.

在步驟S4中,形成源極於障礙層上,源極與通道層之間形成歐姆接觸。 In step S4, a source is formed on the barrier layer, and an ohmic contact is formed between the source and the channel layer.

在步驟S5中,形成汲極於障礙層上,汲極與通道層之間形成歐姆接觸。 In step S5, a drain is formed on the barrier layer, and an ohmic contact is formed between the drain and the channel layer.

在步驟S6中,形成閘極於障礙層上,以形成蕭基接觸,其中閘極位於源極與汲極之間。 In step S6, a gate is formed on the barrier layer to form a Schottky contact, wherein the gate is located between the source and the drain.

其中,障礙層包含位於閘極下方之第一部分,以及位於源極與汲極下方且與第一部分相鄰之第二部分,第一部分係以AlxGa1-xN形成且具有第一厚度,第二部分係以AlyGa1-yN形成且具有第二厚度。且其中,第一厚度係小於第二厚度,x值係小於y值。 Wherein the barrier layer comprises a first portion under the gate and a second portion under the source and the drain and adjacent to the first portion, the first portion being formed of Al x Ga 1-x N and having a first thickness, The second portion is formed of Al y Ga 1-y N and has a second thickness. And wherein the first thickness is less than the second thickness, and the x value is less than the y value.

綜上所述,本發明之主要精神,係將障礙層13形成如第1圖所示之凹槽,並使得第一部分131其Al之莫耳分率小於第二部分132之Al之莫耳分率。藉此改善傳統高電子遷移率電晶體皆具有之Normally-On問題,使得本發明之高電子遷移率電晶體1作為電路操作元件時,可更具有方便性與準確性。 In summary, the main spirit of the present invention is that the barrier layer 13 is formed into a groove as shown in FIG. 1 such that the Mo portion of the first portion 131 having Al is smaller than the Al portion of the second portion 132. rate. Thereby, the Normally-On problem of the conventional high electron mobility transistor is improved, and the high electron mobility transistor 1 of the present invention can be more convenient and accurate as the circuit operation component.

以上所述僅為舉例性,而非為限制性者。任何未脫離本發明之精神與範疇,而對其進行之等效修改或變更,均應包含於後附之申請專利範圍中。 The above is intended to be illustrative only and not limiting. Any equivalent modifications or alterations to the spirit and scope of the invention are intended to be included in the scope of the appended claims.

1‧‧‧高電子遷移率電晶體 1‧‧‧High Electron Mobility Transistor

11‧‧‧基材 11‧‧‧Substrate

12‧‧‧通道層 12‧‧‧Channel layer

13‧‧‧障礙層 13‧‧‧ obstacle layer

131‧‧‧第一部分 131‧‧‧Part 1

132‧‧‧第二部分 132‧‧‧Part II

14‧‧‧源極 14‧‧‧ source

15‧‧‧汲極 15‧‧‧汲polar

16‧‧‧閘極 16‧‧‧ gate

Claims (8)

一種高電子遷移率電晶體,其包含:一基材:一通道層,係形成於該基材上;一障礙層,係形成於該通道層上;一源極,係形成於該障礙層上,該源極與該通道層之間形成歐姆接觸;一汲極,係形成於該障礙層上,該汲極與該通道層之間形成歐姆接觸;以及一閘極,係形成於該障礙層上,以形成蕭基接觸,其中該閘極位於該源極與該汲極之間;其中,該障礙層包含位於該閘極下方之一第一部分,以及位於該源極與該汲極下方且與該第一部分相鄰之一第二部分,該第一部分係以AlxGa1-xN形成且具有一第一厚度,該第二部分係以AlyGa1-yN形成且具有一第二厚度;其中,該第一厚度係小於該第二厚度,x值係小於y值,以令該第一部分的Al的莫耳分率小於該第二部分的Al的莫耳分率。 A high electron mobility transistor comprising: a substrate: a channel layer formed on the substrate; a barrier layer formed on the channel layer; and a source formed on the barrier layer An ohmic contact is formed between the source and the channel layer; a drain is formed on the barrier layer, the drain electrode forms an ohmic contact with the channel layer; and a gate is formed on the barrier layer Forming a Schottky contact, wherein the gate is between the source and the drain; wherein the barrier layer comprises a first portion below the gate and under the source and the drain a second portion adjacent to the first portion, the first portion being formed of Al x Ga 1-x N and having a first thickness, the second portion being formed of Al y Ga 1-y N and having a first portion The thickness is less than the second thickness, and the value of x is less than the value of y such that the molar fraction of Al of the first portion is less than the molar fraction of Al of the second portion. 如申請專利範圍第1項所述之高電子遷移率電晶體,其中該通道層係以GaN形成。 The high electron mobility transistor according to claim 1, wherein the channel layer is formed of GaN. 如申請專利範圍第1項所述之高電子遷移率電晶體,其中x值係介於0.02至0.5,且y值係介於0.2至0.7。 The high electron mobility transistor according to claim 1, wherein the value of x is between 0.02 and 0.5, and the value of y is between 0.2 and 0.7. 如申請專利範圍第1項所述之高電子遷移率電晶體,其中該第一厚度係介於1nm至4nm,且該第二厚度係介於1.5nm至40nm。 The high electron mobility transistor according to claim 1, wherein the first thickness is between 1 nm and 4 nm, and the second thickness is between 1.5 nm and 40 nm. 一種高電子遷移率電晶體之製造方法,其包含下列步驟:提供一基材;形成一通道層於該基材上;形成一障礙層於該通道層上;形成一源極於該障礙層上,該源極與該通道層之間形成歐姆接觸;形成一汲極於該障礙層上,該汲極與該通道層之間形成歐姆接 觸;以及形成一閘極於該障礙層上,以形成蕭基接觸,其中該閘極位於該源極與該汲極之間;其中,該障礙層包含位於該閘極下方之一第一部分,以及位於該源極與該汲極下方且與該第一部分相鄰之一第二部分,該第一部分係以AlxGa1-xN形成且具有一第一厚度,該第二部分係以AlyGa1-yN形成且具有一第二厚度;其中,該第一厚度係小於該第二厚度,x值係小於y值,以令該第一部分的Al的莫耳分率小於該第二部分的Al的莫耳分率。 A method for manufacturing a high electron mobility transistor, comprising the steps of: providing a substrate; forming a channel layer on the substrate; forming a barrier layer on the channel layer; forming a source on the barrier layer Forming an ohmic contact between the source and the channel layer; forming a drain on the barrier layer, forming an ohmic contact between the drain and the channel layer; and forming a gate on the barrier layer to form a Schottky contact, wherein the gate is between the source and the drain; wherein the barrier layer includes a first portion below the gate and is located below the source and the drain and with the first portion Adjacent one of the second portions, the first portion is formed of Al x Ga 1-x N and has a first thickness, the second portion is formed of Al y Ga 1-y N and has a second thickness; The first thickness is less than the second thickness, and the x value is less than the y value such that the Mo content of Al of the first portion is less than the Mo content of Al of the second portion. 如申請專利範圍第5項所述之高電子遷移率電晶體之製造方法,其中該通道層係以GaN形成。 The method of manufacturing a high electron mobility transistor according to claim 5, wherein the channel layer is formed of GaN. 如申請專利範圍第5項所述之高電子遷移率電晶體之製造方法,其中x值係介於0.02至0.5,且y值係介於0.2至0.7。 The method for producing a high electron mobility transistor according to claim 5, wherein the value of x is between 0.02 and 0.5, and the value of y is between 0.2 and 0.7. 如申請專利範圍第5項所述之高電子遷移率電晶體之製造方法,其中該第一厚度係介於1nm至4nm,且該第二厚度係介於1.5nm至40nm。 The method of manufacturing a high electron mobility transistor according to claim 5, wherein the first thickness is between 1 nm and 4 nm, and the second thickness is between 1.5 nm and 40 nm.
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US20030157776A1 (en) * 2000-12-01 2003-08-21 Smith Richard Peter Methods of fabricating aluminum gallium nitride/gallium nitride high electron mobility transistors having a gate contact on a gallium nitride based cap segment
EP2282346A2 (en) * 2001-05-11 2011-02-09 Cree, Inc. Group-III nitride based high electron mobility transistor (HEMT) with barrier/spacer layer

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US20030157776A1 (en) * 2000-12-01 2003-08-21 Smith Richard Peter Methods of fabricating aluminum gallium nitride/gallium nitride high electron mobility transistors having a gate contact on a gallium nitride based cap segment
EP2282346A2 (en) * 2001-05-11 2011-02-09 Cree, Inc. Group-III nitride based high electron mobility transistor (HEMT) with barrier/spacer layer

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