TWI619249B - High electron mobility transistor structure and forming method thereof - Google Patents
High electron mobility transistor structure and forming method thereof Download PDFInfo
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- 238000000034 method Methods 0.000 title claims abstract description 22
- 229910052751 metal Inorganic materials 0.000 claims abstract description 46
- 239000002184 metal Substances 0.000 claims abstract description 46
- 239000004065 semiconductor Substances 0.000 claims abstract description 34
- 239000000758 substrate Substances 0.000 claims abstract description 27
- 239000011295 pitch Substances 0.000 claims abstract description 22
- 239000002127 nanobelt Substances 0.000 claims abstract description 10
- 229910002601 GaN Inorganic materials 0.000 claims description 82
- JMASRVWKEDWRBT-UHFFFAOYSA-N Gallium nitride Chemical compound [Ga]#N JMASRVWKEDWRBT-UHFFFAOYSA-N 0.000 claims description 49
- RNQKDQAVIXDKAG-UHFFFAOYSA-N aluminum gallium Chemical compound [Al].[Ga] RNQKDQAVIXDKAG-UHFFFAOYSA-N 0.000 claims description 39
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 claims description 14
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 claims description 10
- 229910052710 silicon Inorganic materials 0.000 claims description 10
- 239000010703 silicon Substances 0.000 claims description 10
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 claims description 7
- 239000010931 gold Substances 0.000 claims description 7
- 229910052737 gold Inorganic materials 0.000 claims description 7
- 229910052759 nickel Inorganic materials 0.000 claims description 7
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 claims description 6
- XLOMVQKBTHCTTD-UHFFFAOYSA-N Zinc monoxide Chemical compound [Zn]=O XLOMVQKBTHCTTD-UHFFFAOYSA-N 0.000 claims description 5
- 239000012212 insulator Substances 0.000 claims description 5
- 229910052594 sapphire Inorganic materials 0.000 claims description 5
- 239000010980 sapphire Substances 0.000 claims description 5
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 claims description 5
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical group [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 claims description 4
- 229910052782 aluminium Inorganic materials 0.000 claims description 4
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 claims description 4
- 238000000151 deposition Methods 0.000 claims description 4
- 238000002207 thermal evaporation Methods 0.000 claims description 4
- 239000010936 titanium Substances 0.000 claims description 4
- 229910052719 titanium Inorganic materials 0.000 claims description 4
- 229910052757 nitrogen Inorganic materials 0.000 claims description 3
- 229910001218 Gallium arsenide Inorganic materials 0.000 claims description 2
- 238000000609 electron-beam lithography Methods 0.000 claims description 2
- 239000002074 nanoribbon Substances 0.000 claims description 2
- 238000001020 plasma etching Methods 0.000 claims description 2
- 229910052785 arsenic Inorganic materials 0.000 claims 1
- RQNWIZPPADIBDY-UHFFFAOYSA-N arsenic atom Chemical compound [As] RQNWIZPPADIBDY-UHFFFAOYSA-N 0.000 claims 1
- 230000000694 effects Effects 0.000 abstract description 19
- 238000013461 design Methods 0.000 abstract description 8
- 239000008186 active pharmaceutical agent Substances 0.000 description 18
- 230000010287 polarization Effects 0.000 description 8
- 229910002704 AlGaN Inorganic materials 0.000 description 6
- JBRZTFJDHDCESZ-UHFFFAOYSA-N AsGa Chemical compound [As]#[Ga] JBRZTFJDHDCESZ-UHFFFAOYSA-N 0.000 description 5
- 239000000463 material Substances 0.000 description 4
- 230000015572 biosynthetic process Effects 0.000 description 3
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- 230000005684 electric field Effects 0.000 description 2
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- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 description 1
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 description 1
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- 239000000969 carrier Substances 0.000 description 1
- 229910052804 chromium Inorganic materials 0.000 description 1
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- 229910052733 gallium Inorganic materials 0.000 description 1
- MSNOMDLPLDYDME-UHFFFAOYSA-N gold nickel Chemical compound [Ni].[Au] MSNOMDLPLDYDME-UHFFFAOYSA-N 0.000 description 1
- 238000013508 migration Methods 0.000 description 1
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- 150000004767 nitrides Chemical class 0.000 description 1
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- -1 titanium aluminum nickel gold Chemical compound 0.000 description 1
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- 230000005533 two-dimensional electron gas Effects 0.000 description 1
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Abstract
一種高電子遷移率電晶體結構及其形成方法,係以半導體基材為基 底的磊晶堆疊結構中形成奈米帶,該奈米帶形成於磊晶堆疊結構的閘極區,以及閘極金屬層形成於閘極區以構成具有奈米帶結構設計的閘極結構。且又本發明係利用變更奈米帶的複數個間距的長度和寬度,可減少高電子遷移率電晶體結構的熱效應,而可提高臨界電壓。 A high electron mobility transistor structure and its forming method, based on a semiconductor substrate A nano-belt is formed in the bottom epitaxial stack structure. The nano-belt is formed in the gate region of the epitaxial stack structure, and a gate metal layer is formed in the gate region to form a gate structure with a nano-belt structure design. Moreover, the present invention uses the change of the length and width of the plurality of pitches of the nano-belt to reduce the thermal effect of the high electron mobility transistor structure and increase the critical voltage.
Description
本發明涉及一種高電子遷移率電晶體結構及其形成方法,特別是涉及一種增強型(Enhancement-mode)氮化鋁鎵/氮化鎵高電子遷移率電晶體之結構及其形成方法。 The invention relates to a high electron mobility transistor crystal structure and a formation method thereof, in particular to an enhancement-mode aluminum gallium nitride / gallium nitride high electron mobility transistor crystal structure and a formation method thereof.
「高電子遷移率電晶體(HEMT)」,又稱為「異質接面場效電晶體(HFET)」,或是「調制摻雜場效應電晶體(MODFET)」,一般係利用兩種不同能帶寬度的材料而形成接面,例如以「異質接面」替代「摻雜區」而作為「溝道」。 "High electron mobility transistor (HEMT)", also known as "heterojunction field effect transistor (HFET)" or "modulated doped field effect transistor (MODFET)", generally uses two different energy A material with a width is used to form a junction. For example, a "heterojunction" replaces a "doped region" as a "channel".
在氮化鋁鎵/氮化鎵(AlGaN/GaN)體系中,氮化鋁鎵/氮化鎵介面的極化效應可分為兩種,第一種是由晶格不匹配的應力所產生的壓電極化效應,第二種是由於三族氮化物的晶格並非完全中心對稱,導致的自發極化。而「高電子遷移率電晶體」的通道主要由壓電極化效應主導,應力產生壓電極化效應,進而產生通道。 In the aluminum gallium nitride / gallium nitride (AlGaN / GaN) system, the polarization effect of the aluminum gallium nitride / gallium nitride interface can be divided into two types, the first one is caused by the stress of the lattice mismatch The second type of piezoelectric polarization effect is spontaneous polarization due to the fact that the crystal lattice of Group III nitrides is not completely centrosymmetric. The channel of the "high electron mobility transistor" is mainly dominated by the piezoelectric polarization effect, and the stress produces the piezoelectric polarization effect, which in turn generates channels.
承前述極化場量效應與異質接面之位能井能帶結構,會產生一自然導通之二維電子氣通道,是故為空乏型(Depletion mode)元件。但在電路 上的應用,為了簡化電路設計的複雜度,並且降低不必要的功率耗損,使用增強型(Enhancement Mode)是不可或缺的選擇。 The energy band structure of the potential well, which bears the aforementioned polarization field effect and heterojunction, will produce a naturally conducting two-dimensional electron gas channel, so it is a depletion mode device. But in the circuit In order to simplify the complexity of circuit design and reduce unnecessary power consumption, the use of enhanced mode is an indispensable choice.
「奈米帶」的寬度改變會使得臨界電壓發生變化,其因是由於應力的改變造成臨界電壓的改變,「奈米帶」的寬度愈小則應力愈小。若應力愈小,壓電極化愈小,則「高電子遷移率電晶體」的通道則可以愈小,進而讓臨界電壓上升,同時增加了該「高電子遷移率電晶體」結構的熱效應,更因此嚴重影響「高電子遷移率電晶體」結構的效能。 A change in the width of the "nano band" will cause the threshold voltage to change. This is because the change in the stress causes the threshold voltage to change. The smaller the width of the "nano band", the smaller the stress. If the stress is smaller and the piezoelectric polarization is smaller, the channel of the "high electron mobility transistor" can be smaller, which will increase the critical voltage and increase the thermal effect of the "high electron mobility transistor" structure. Therefore, the performance of the "high electron mobility transistor" structure is seriously affected.
其次,當壓電極化效應變小,則載子濃度會下降(通道變小),而於傳統習知先前技術中,即有Kota Ohi等人於「Japanese Journal of Applied Physics」期刊發表相關論文,該論文抬頭名稱為「Drain Current Stability and Controllability of Threshold Voltage and Subthreshold Current in a Multi-Mesa-Channel AlGaN/GaN High Electron Mobility Transistor」,Kota Ohi等人於論文中提出利用改變「奈米帶」的通道寬度,以調變臨界電壓的運用原理,當要調變氮化鎵高電子遷移率電晶體(GaN HEMT)的臨界電壓時,提出多蝕刻通道(multi-mesa-channel),以及調整通道寬度(Modulation channel width)的方法,進行調變「氮化鎵高電子遷移率電晶體」的臨界電壓。該論文所提供之作法雖可讓元件臨界電壓往正臨界電壓偏移,可提升元件熱穩定度,但其缺點卻是大大降低元件的電流密度。 Second, when the piezoelectric polarization effect becomes smaller, the carrier concentration will decrease (the channel becomes smaller), and in the conventional prior art, Kota Ohi et al. Published related papers in the "Japanese Journal of Applied Physics". The title of the paper is titled "Drain Current Stability and Controllability of Threshold Voltage and Subthreshold Current in a Multi-Mesa-Channel AlGaN / GaN High Electron Mobility Transistor", and Kota Ohi et al. Proposed to use the channel to change the "nano band" in the paper Width, according to the application principle of modulating the threshold voltage, when the threshold voltage of GaN HEMT transistor is to be adjusted, multi-mesa-channel is proposed, and the channel width is adjusted ( Modulation channel width) method to adjust the critical voltage of "GaN high electron mobility transistor". Although the method provided in this paper can shift the critical voltage of the device to the positive critical voltage and improve the thermal stability of the device, its disadvantage is that it greatly reduces the current density of the device.
承前述,傳統習知先前技術多通道閘極3D電場披覆,雖可提升半導體材料的「表面釘紮效應(surface pinning effect)」,但因「通道上的邊壁效應(Sidewall effect on the channel)」未善用元件的表面釘紮效應,故必須將元件寬度(width)減低到100奈米(nm)以下的寬度,才能產生如「增強型氮化鎵高電子遷移率電晶體(E-mode GaN HEMT)」的效果,又因元件寬度太小則甚難製作,且因中性區不足夠,而使得元件通道的阻抗變大,更無法達到 真正的實用性。 According to the foregoing, the conventional prior art multi-channel gate 3D electric field coating can improve the "surface pinning effect" of semiconductor materials, but due to the "Sidewall effect on the channel" ) "The surface pinning effect of the device is not used properly, so the width of the device must be reduced to a width below 100 nanometers (nm) to produce such as" enhanced GaN high electron mobility transistor (E- mode GaN HEMT), because the width of the device is too small, it is very difficult to produce, and because the neutral region is not enough, the impedance of the device channel becomes larger and cannot be achieved Real practicality.
因此,有鑒於前述的「高電子遷移率電晶體」之缺陷,針對未來之半導體工業需求,亟需開發一種「高電子遷移率電晶體」結構,期能積極應用而能促進積體電路之發展。 Therefore, in view of the aforementioned shortcomings of "high electron mobility transistors", in view of the future needs of the semiconductor industry, there is an urgent need to develop a "high electron mobility transistors" structure that can be actively applied to promote the development of integrated circuits .
故為了提高臨界電壓,本發明提供一種「高電子遷移率電晶體」結構及其形成方法,其閘極結構包括「奈米帶」結構設計,並變更「奈米帶」結構的間距長度或連同變更間距寬度,利用閘極側面的空乏來調變臨界電壓。 Therefore, in order to increase the threshold voltage, the present invention provides a "high electron mobility transistor" structure and its forming method. The gate structure includes a "nano-belt" structure design, and changes the pitch length of the "nano-belt" structure or together Change the pitch width and use the vacancy on the side of the gate to adjust the critical voltage.
本發明之一種「高電子遷移率電晶體」結構,包括:一半導體基材,其中該半導體基材包括藍寶石(sapphire)、矽(Si)、碳化矽(SiC)、氮化鎵(GaN)、氧化鋅(ZnO)、砷化鎵(GaAs)、SOI(Silicon on Insulator)或其他商用供磊晶用之半導體基材;一氮化鎵層覆蓋於該半導體基材上;一氮化鋁鎵層位於該氮化鎵層上,該氮化鋁鎵層區分為一源極區、一汲極區以及位於該源極區和該汲極區之間的一閘極區,該閘極區具有複數個溝槽,其中,每一該溝槽暴露出部分該氮化鎵層,相鄰的任二溝槽間的複數個間距具有相同的長度和相同的寬度,且任一該間距的長度大於等於0.8微米(um);一歐姆金屬層覆蓋於該氮化鋁鎵層的該源極區和該汲極區上;以及一閘極金屬層位於該氮化鋁鎵層的該閘極區上,該閘極金屬層覆蓋住每一該溝槽的至少一部分。 A "high electron mobility transistor" structure of the present invention includes: a semiconductor substrate, wherein the semiconductor substrate includes sapphire, silicon (Si), silicon carbide (SiC), gallium nitride (GaN), Zinc oxide (ZnO), gallium arsenide (GaAs), SOI (Silicon on Insulator) or other commercial semiconductor substrates for epitaxial use; a gallium nitride layer covering the semiconductor substrate; an aluminum gallium nitride layer Located on the gallium nitride layer, the aluminum gallium nitride layer is divided into a source region, a drain region, and a gate region between the source region and the drain region, the gate region has a plurality of A plurality of trenches, wherein each of the trenches exposes a portion of the gallium nitride layer, and the plurality of pitches between any two adjacent trenches have the same length and the same width, and any length of the pitch is greater than or equal to 0.8 micrometers (um); an ohmic metal layer covers the source region and the drain region of the aluminum gallium nitride layer; and a gate metal layer is located on the gate region of the aluminum gallium nitride layer, The gate metal layer covers at least a portion of each trench.
本發明之一種「形成高電子遷移率電晶體」結構的方法,包括:提供一磊晶堆疊結構,該磊晶堆疊結構包括一半導體基材,其中該半導體基材包括藍寶石(sapphire)、矽(Si)、碳化矽(SiC)、氮化鎵(GaN)、氧化鋅(ZnO)、砷化鎵(GaAs)、SOI(Silicon on Insulator)或其他商用供磊晶用之半導體基材; 形成一氮化鎵層覆蓋於該半導體基材上;形成一氮化鋁鎵層位於該氮化鎵層上;形成一圖案化遮罩層於該磊晶堆疊結構上,其中該圖案化遮罩層覆蓋部分該氮化鋁鎵層;形成一「奈米帶」於該氮化鋁鎵層中,其中該「奈米帶」包括複數個溝槽,並以該圖案化遮罩層為一遮罩移除部分該氮化鋁鎵層和氮化鎵層;形成一歐姆金屬層於該「奈米帶」以外的該氮化鋁鎵層上;以及形成一閘極金屬層於該「奈米帶」上。 A method of "forming a high electron mobility transistor" structure of the present invention includes: providing an epitaxial stack structure including a semiconductor substrate, wherein the semiconductor substrate includes sapphire and silicon ( Si), silicon carbide (SiC), gallium nitride (GaN), zinc oxide (ZnO), gallium arsenide (GaAs), SOI (Silicon on Insulator) or other commercial semiconductor substrates for epitaxial use; Forming a gallium nitride layer covering the semiconductor substrate; forming an aluminum gallium nitride layer on the gallium nitride layer; forming a patterned mask layer on the epitaxial stack structure, wherein the patterned mask The layer covers part of the aluminum gallium nitride layer; a "nano band" is formed in the aluminum gallium nitride layer, wherein the "nano band" includes a plurality of trenches, and the patterned mask layer is used as a mask Removing part of the cover of the aluminum gallium nitride layer and the gallium nitride layer; forming an ohmic metal layer on the aluminum gallium nitride layer outside the "nano band"; and forming a gate metal layer on the "nanometer" Bring on.
本發明之一主要目的,則是利用閘極側面空乏(Gate side wall deplete)的方法,藉以調變「高電子遷移率電晶體」的臨界電壓(Vth)。 One of the main objectives of the present invention is to use the gate side wall depletion method to modulate the threshold voltage (Vth) of the "high electron mobility transistor".
本發明之另一主要目的,係利用變更「奈米帶」的複數個間距的長度和寬度,而減少「高電子遷移率電晶體」結構的熱效應,且同時具有提高臨界電壓的功效。 Another main object of the present invention is to reduce the thermal effect of the "high electron mobility transistor" structure by changing the length and width of a plurality of pitches of the "nano band", and at the same time have the effect of increasing the critical voltage.
本發明之主要特徵,係具有帶狀(ribbon)的三維(3D)立體條狀結構,故可提昇「高電子遷移率電晶體」元件側壁的表面態(surface states)密度,進而提高半導體材料的「表面釘紥效應(surface pinning effect)」。其主要原理係因為當半導體的「表面態」密度較高的時候,半導體表面上的「費米能階」會被固定在半導體的「表面態」上,而產生「表面釘紥效應」的現象。 The main feature of the present invention is that it has a three-dimensional (3D) three-dimensional (3D) strip structure, which can increase the surface state density of the side wall of the "high electron mobility transistor" device, thereby improving the semiconductor material. "Surface pinning effect". The main principle is that when the density of the "surface state" of the semiconductor is high, the "Fermi energy level" on the surface of the semiconductor will be fixed to the "surface state" of the semiconductor, and the phenomenon of "surface pinning" will occur. .
10‧‧‧高電子遷移率電晶體結構 10‧‧‧High electron mobility transistor structure
12‧‧‧半導體基材 12‧‧‧Semiconductor substrate
14‧‧‧氮化鎵層 14‧‧‧GaN layer
16‧‧‧氮化鋁鎵層 16‧‧‧AlGaN layer
162‧‧‧源極區 162‧‧‧Source
164‧‧‧閘極區 164‧‧‧Gate area
166‧‧‧汲極區 166‧‧‧ Jiji District
18‧‧‧金屬層 18‧‧‧Metal layer
182‧‧‧歐姆金屬層 182‧‧‧ohm metal layer
184‧‧‧閘極金屬層 184‧‧‧Gate metal layer
20‧‧‧溝槽 20‧‧‧Groove
22‧‧‧間距 22‧‧‧spacing
40‧‧‧圖案化遮罩層 40‧‧‧patterned mask layer
L‧‧‧長度 L‧‧‧Length
Lg‧‧‧長度 Lg‧‧‧Length
Lt‧‧‧長度 Lt‧‧‧Length
W‧‧‧寬度 W‧‧‧Width
Wt‧‧‧寬度 Wt‧‧‧Width
第1圖為本發明的「高電子遷移率電晶體」結構實施例的立體側視示意圖。 Fig. 1 is a schematic perspective side view of an embodiment of the "high electron mobility transistor" structure of the present invention.
第2圖為形成本發明的「高電子遷移率電晶體」方法實施例的流程示意圖。 FIG. 2 is a schematic flowchart of an embodiment of a method for forming a "high electron mobility transistor" of the present invention.
第3A、3B、3C、3D圖為依據第2圖的流程中各步驟的「高電子遷 移率電晶體」或是「氮化鋁鎵/氮化鎵高電子遷移率電晶體」結構剖面示意圖。 Figures 3A, 3B, 3C, and 3D are the "high electron migration" steps in the flow of Figure 2. Schematic diagram of the structure of the "Transfer Transistor" or "AlGaN / GaN High Electron Mobility Transistor" structure.
第4A、4B、4C、4D圖為依據第2圖的流程中各步驟的「高電子遷移率電晶體」結構俯視立體示意圖。 Figures 4A, 4B, 4C, and 4D are schematic top perspective views of the structure of the "high electron mobility transistor" according to the steps in the flow of Figure 2.
第5圖顯示本發明之奈米帶寬度為100奈米之電晶體正規化汲極電流(IDS)-閘極電壓(V)曲線特性。 Figure 5 shows the normalized drain current (I DS ) -gate voltage (V) curve characteristics of a transistor with a nano-band width of 100 nanometers according to the present invention.
第6圖顯示本發明之奈米帶寬度為300奈米之電晶體正規化汲極電流(IDS)-閘極電壓(V)曲線特性。 FIG. 6 shows the normalized drain current (I DS ) -gate voltage (V) curve characteristics of a transistor with a nano-band width of 300 nm according to the present invention.
第7圖顯示本發明之奈米帶寬度500為奈米之電晶體正規化汲極電流(IDS)-閘極電壓(V)曲線特性。 FIG. 7 shows the normalized drain current (I DS ) -gate voltage (V) curve characteristics of a transistor with a nano-band width of 500 according to the present invention.
第8圖顯示本發明之奈米帶長度為0.8微米之電晶體正規化汲極電流(IDS)-閘極電壓(V)曲線特性。 FIG. 8 shows the normalized drain current (I DS ) -gate voltage (V) curve characteristics of a transistor with a nanometer length of 0.8 μm according to the present invention.
第9圖顯示本發明之奈米帶長度為1微米之電晶體正規化汲極電流(IDS)-閘極電壓(V)曲線特性。 Figure 9 shows the normalized drain current (I DS ) -gate voltage (V) curve characteristics of a transistor with a nanometer length of 1 micrometer according to the present invention.
第10圖顯示本發明之奈米帶長度為2微米之電晶體正規化汲極電流(IDS)-閘極電壓(V)曲線特性。 FIG. 10 shows the normalized drain current (I DS ) -gate voltage (V) curve characteristics of a transistor with a nanometer length of 2 μm according to the present invention.
第11圖顯示本發明元件在前述第5圖至第10圖中,具有不同「奈米帶」長度(NRs length)及「奈米帶」寬度(NRs width)下的臨界電壓。 FIG. 11 shows the threshold voltages of the device of the present invention with different “NRs length” and “NRs width” in the foregoing FIGS. 5 to 10.
第12圖為本發明「奈米帶」的面積(Area)與「元件臨界電壓」趨勢圖。 FIG. 12 is a trend diagram of the area of the “nano band” and the “device threshold voltage” of the present invention.
本發明以下所稱的溝槽間的間距,基本上可以視為矩形,並以氮化鋁鎵層表面來測量長度和寬度。而本發明以下所稱的溝槽,基本上 為矩形體,具有長、寬和深度,但可以理解的,可能因製程的影響,使得溝槽可能在高倍放大下顯示為非矩形體,但此並不影響本發明定義溝槽間的間距。 The pitch between trenches referred to below in the present invention can be basically regarded as a rectangle, and the length and width are measured on the surface of the aluminum gallium nitride layer. The groove referred to below in the present invention is basically It is a rectangular body with length, width and depth, but it is understandable that the groove may be displayed as a non-rectangular body under high magnification due to the influence of the manufacturing process, but this does not affect the distance between the grooves defined by the present invention.
請參考第1圖所示,本發明之「高電子遷移率電晶體」結構10具有半導體基材12,其中該半導體基材12包括藍寶石(sapphire)、矽(Si)、碳化矽(SiC)、氮化鎵(GaN)、氧化鋅(ZnO)、砷化鎵(GaAs)、SOI(Silicon on Insulator)或其他商用供磊晶用之半導體基材12,氮化鎵層14,氮化鋁鎵層16和金屬層18,其中氮化鎵層14形成於半導體基材12上,氮化鋁鎵層16形成於氮化鎵層14上,以及金屬層18形成於氮化鋁鎵層16上。 Please refer to FIG. 1, the “high electron mobility transistor” structure 10 of the present invention has a semiconductor substrate 12, wherein the semiconductor substrate 12 includes sapphire, silicon (Si), silicon carbide (SiC), Gallium nitride (GaN), zinc oxide (ZnO), gallium arsenide (GaAs), SOI (Silicon on Insulator) or other commercial semiconductor substrates for epitaxial use 12, gallium nitride layer 14, aluminum gallium nitride layer 16 and a metal layer 18, in which the gallium nitride layer 14 is formed on the semiconductor substrate 12, the aluminum gallium nitride layer 16 is formed on the gallium nitride layer 14, and the metal layer 18 is formed on the aluminum gallium nitride layer 16.
首先,為方便說明,仍請參考第1圖所示,於此將覆蓋住氮化鎵層14的氮化鋁鎵層16區分成源極區162、閘極區164以及汲極區166,其中,閘極區164位於源極區162和汲極區166之間,各區在氮化鋁鎵層16上的比例不限,於第1圖上各區的面積大小僅為例示而非以限制。其次,在可同時跨越源極區162、閘極區164以及汲極區166的延伸方向上,可定義的是:閘極區164具有「長度L」,且閘極區164亦具有「寬度W」。 First, for convenience of description, please still refer to FIG. 1, where the aluminum gallium nitride layer 16 covering the gallium nitride layer 14 is divided into a source region 162, a gate region 164, and a drain region 166, wherein The gate region 164 is located between the source region 162 and the drain region 166, and the ratio of each region on the aluminum gallium nitride layer 16 is not limited. The area size of each region in FIG. 1 is only an example and not a limitation. . Secondly, in the extending direction that can span the source region 162, the gate region 164 and the drain region 166 at the same time, it can be defined that the gate region 164 has a "length L" and the gate region 164 also has a "width W" ".
續參考第1圖所示,複數個溝槽20形成於閘極區164,且暴露出部分的氮化鎵層14,其中,該複數個「溝槽20」在「寬度W」上排成一列並彼此之間保持「間距22」。於本發明中,該複數個「溝槽20」具有相同的「長度Lt」,並用該「長度Lt」作為「間距22」的「長度Lt」,且該「間距22」具有「寬度Wt」。其中,值得注意的是「長度Lt」小於「長度L」,「寬度Wt」小於「寬度W」。是以,該複數個「間距22」在閘極區164中形成一「奈米帶」(nanoribbon structure),而較佳範圍之分佈係,「長度Lt」大於等於0.8微米(um)且可小於等於6微米,「寬度Wt」則大於等於100奈米(nm)並小於等於500奈米。是以,當該「高電子遷移率電晶體結構10」的磊晶結構具有前述「奈米帶」的結構設計時,則可以改善半導體基材結構的散熱問題,減少 熱效應以維持高電流高電壓下運作的效能,而於「氮化鋁鎵/氮化鎵高電子遷移率電晶體」中,其源極(Source)與汲極(Drain)元件的長度L不會小於3微米(um),主要原因係由於「操作電場下降」以及「製程技術」的限制。而於一般市面上,「射頻氮化鎵高電子遷移率電晶體(RF GaN HEMT)」的元件「長度L」為4微米(28伏特)到6微米(50伏特)。但若是「氮化鋁鎵/氮化鎵高電子遷移率電晶體」功率元件,目前市面上,則有50伏特(V),200伏特,以及650伏特等規格,而若耐壓要超過650伏特時,則元件「長度L」可能須達幾十微米。 With continued reference to FIG. 1, a plurality of trenches 20 are formed in the gate region 164 and expose a portion of the gallium nitride layer 14, wherein the plurality of "trenches 20" are arranged in a row on the "width W" And maintain a "spacing 22" between each other. In the present invention, the plurality of "grooves 20" have the same "length Lt", and the "length Lt" is used as the "length Lt" of the "pitch 22", and the "pitch 22" has a "width Wt". Among them, it is worth noting that "Length Lt" is smaller than "Length L" and "Width Wt" is smaller than "Width W". Therefore, the plurality of "spacings 22" form a "nanoribbon structure" in the gate region 164, and the preferred range of distribution is that the "length Lt" is greater than or equal to 0.8 microns (um) and can be less than Is equal to 6 microns, "width Wt" is greater than or equal to 100 nanometers (nm) and less than or equal to 500 nanometers. Therefore, when the epitaxial structure of the "high electron mobility transistor structure 10" has the aforementioned "nano band" structure design, the heat dissipation problem of the semiconductor substrate structure can be improved and reduced The thermal effect maintains the performance of high current and high voltage operation. In the "aluminum gallium nitride / gallium nitride high electron mobility transistor", the length L of the source and drain elements does not Less than 3 microns (um), the main reason is due to "operating electric field decline" and "process technology" restrictions. In the general market, the "Length L" of the "RF GaN HEMT" device is 4 microns (28 volts) to 6 microns (50 volts). However, if it is an "aluminum gallium nitride / gallium nitride high electron mobility transistor" power device, there are currently 50 volt (V), 200 volt, and 650 volt specifications on the market, and if the withstand voltage should exceed 650 volts At this time, the component "length L" may have to reach several tens of microns.
續參考第1圖所示,位於氮化鋁鎵層16上的金屬層18係作為電極之用。於實施例中,金屬層18包括歐姆金屬層182和閘極金屬層184,其中,歐姆金屬層182為鈦鋁鎳金層,而閘極金屬層184則可為鎳金層。其次,歐姆金屬層182覆蓋於氮化鋁鎵層16的源極區162和汲極區166上,閘極金屬層184則覆蓋住每一溝槽20和間距22的至少一部分。又於實施例中,閘極金屬層184的「長度Lg」為2微米(um),如於第1圖所顯示,是以,本發明的溝槽20和間距22可以整個為閘極金屬層184所覆蓋,亦可以因溝槽20和間距22的「長度Lt」大於閘極金屬層184的「長度Lg」而暴露出來,但本發明並不限於何種形式。 With continued reference to FIG. 1, the metal layer 18 on the aluminum gallium nitride layer 16 is used as an electrode. In an embodiment, the metal layer 18 includes an ohmic metal layer 182 and a gate metal layer 184, wherein the ohmic metal layer 182 is a titanium aluminum nickel gold layer, and the gate metal layer 184 may be a nickel gold layer. Second, the ohmic metal layer 182 covers the source region 162 and the drain region 166 of the aluminum gallium nitride layer 16, and the gate metal layer 184 covers at least a portion of each trench 20 and the pitch 22. In the embodiment, the "length Lg" of the gate metal layer 184 is 2 micrometers (um). As shown in FIG. 1, the trench 20 and the pitch 22 of the present invention can be the entire gate metal layer The coverage of 184 may also be exposed because the "length Lt" of the trench 20 and the pitch 22 is greater than the "length Lg" of the gate metal layer 184, but the invention is not limited to any form.
請參考第2圖之步驟30,並配合第3A圖與第4A圖所示,在第2圖步驟30中係「首先提供磊晶堆疊結構」之步驟,而本發明的磊晶堆疊結構可包括第1圖中的半導體基材12,其中該半導體基材包括藍寶石(sapphire)、矽(Si)、碳化矽(SiC)、氮化鎵(GaN)、氧化鋅(ZnO)、砷化鎵(GaAs)、SOI(Silicon on Insulator)或其他商用供磊晶用之半導體基材,而氮化鎵層(GaN layer)14形成於該半導體基材12上,以及氮化鋁鎵層(AlGaN layer)16形成於氮化鎵層(GaN layer)14上,其中氮化鎵層14的厚度可為2微米,氮化鋁鎵層16的厚度可為21.8奈米,但本發明不限於此,而前述結構亦顯示於第3A圖與第4A圖 中。 Please refer to step 30 in FIG. 2 and cooperate with FIG. 3A and FIG. 4A. In step 30 in FIG. 2 is the step of “firstly provide an epitaxial stack structure”, and the epitaxial stack structure of the present invention may include The semiconductor substrate 12 in FIG. 1, wherein the semiconductor substrate includes sapphire, silicon (Si), silicon carbide (SiC), gallium nitride (GaN), zinc oxide (ZnO), gallium arsenide (GaAs) ), SOI (Silicon on Insulator) or other commercial semiconductor substrates for epitaxial use, and a gallium nitride layer (GaN layer) 14 is formed on the semiconductor substrate 12 and an aluminum gallium nitride layer (AlGaN layer) 16 It is formed on the gallium nitride layer (GaN layer) 14, wherein the thickness of the gallium nitride layer 14 can be 2 microns, the thickness of the aluminum gallium nitride layer 16 can be 21.8 nanometers, but the invention is not limited thereto, and the aforementioned structure Also shown in Figures 3A and 4A in.
接著,如第2圖之步驟32,並配合第3A圖與第4A圖所示,在第2圖步驟32中係「形成一圖案化遮罩層40於磊晶堆疊結構上」之步驟,本發明的圖案化遮罩層(Mask layer)40可以為金屬鉻層(Cr layer)40,其圖案則為第1圖中的「奈米帶」結構設計,可選擇合適的製程方式於氮化鋁鎵層16的閘極區定義「奈米帶」圖案,此合適的製程方式,舉例但不限地,可以選擇例如電子束微影方法(E-beam lithography)。另要說明的是,仍如第3A圖與第4A圖所示,其中前述的圖案化遮罩層40,亦可以形成薄的圖案化遮罩層(GaN)40,而圖案化遮罩層(GaN)40的厚度約為2奈米,但本發明不限於此。 Next, as shown in step 32 of FIG. 2 and in conjunction with FIGS. 3A and 4A, in step 32 of FIG. 2 is the step of “forming a patterned mask layer 40 on the epitaxial stack structure”. The patterned mask layer 40 of the invention may be a metal chromium layer (Cr layer) 40, and its pattern is the "nano band" structure design shown in FIG. 1, and a suitable manufacturing method may be selected for aluminum nitride The gate region of the gallium layer 16 defines a "nano-belt" pattern. This suitable manufacturing method can be selected from, but not limited to, for example, E-beam lithography. In addition, as shown in FIGS. 3A and 4A, the aforementioned patterned mask layer 40 can also form a thin patterned mask layer (GaN) 40, and the patterned mask layer ( The thickness of GaN) 40 is about 2 nm, but the invention is not limited thereto.
接著,如第2圖之步驟34,並配合第3B圖與第4B圖所示,在第2圖步驟34中係「移除部分的氮化鋁鎵層16和氮化鎵層14以形成複數個溝槽」之步驟,其中移除的方式,包括例如乾式蝕刻方式的反應式離子蝕刻,以圖案化的遮罩層做為蝕刻遮罩,而蝕刻深度約130奈米,蝕刻完畢後,移除圖案化的遮罩層。再者,該複數個溝槽暴露出溝槽下方的氮化鎵層,溝槽之間的間距大小可參考第1圖的對應說明,但本發明不限於上述尺寸。 Next, as shown in step 34 of FIG. 2, and in conjunction with FIGS. 3B and 4B, in step 34 of FIG. 2, "a part of the aluminum gallium nitride layer 16 and the gallium nitride layer 14 are removed to form a plurality of "Trench" step, where the removal method includes reactive ion etching such as dry etching, using a patterned mask layer as an etching mask, and the etching depth is about 130 nm. After etching, move In addition to the patterned mask layer. Furthermore, the plurality of trenches expose the gallium nitride layer under the trenches. For the distance between the trenches, refer to the corresponding description in FIG. 1, but the present invention is not limited to the above dimensions.
續參考第2圖之步驟36,並配合第3C圖與第4C圖所示,在第2圖步驟36中係「於部分的氮化鋁鎵層16上形成一歐姆金屬層182」之步驟,於本發明中,係利用電子鎗(E-gun)沉積方法,或是熱沉積方法形成鈦/鋁/鎳/金層作為歐姆金屬層182,其中鈦/鋁/鎳/金的厚度分別為30/120/20/80奈米,但本發明不限於此。其次,歐姆金屬層是形成於氮化鋁鎵層16的源極區和汲極區上。 Continuing to refer to step 36 of FIG. 2, and as shown in FIGS. 3C and 4C, in step 36 of FIG. 2 is the step of "forming an ohmic metal layer 182 on a portion of the aluminum gallium nitride layer 16", In the present invention, a titanium / aluminum / nickel / gold layer is formed as an ohmic metal layer 182 by using an electron gun (E-gun) deposition method or a thermal deposition method, wherein the thickness of titanium / aluminum / nickel / gold is 30 / 120/20/80 nm, but the invention is not limited to this. Second, the ohmic metal layer is formed on the source region and the drain region of the aluminum gallium nitride layer 16.
接著,參考第2圖之步驟38,並配合第3D圖與第4D圖所示,在第2圖步驟38中係「於部分暴露出的氮化鋁鎵層16上形成一閘極金屬層184」之步驟。於本發明中,亦利用電子鎗(E-gun)沉積方法,或是熱沉積方法形成閘極金屬層184,其可以為厚度分別為20/80奈米的鎳/金層所形成。其次, 閘極金屬層184是形成在介於源極區和汲極區之間的閘極區,閘極金屬層184其長度Lg約為2微米,如於第4D圖所顯示。是以,在當間距22的「長度Lt」大於2微米時,該閘極金屬層184僅能形成覆蓋住每一該溝槽20的一部分。但相對而可以理解的是,仍如第4D圖所示,當間距22的「長度Lt」係小於閘極金屬層184的長度Lg設計時,閘極金屬層184則可以完全覆蓋住溝槽20,即閘極金屬層184得以完全形成覆蓋住被暴露出的氮化鎵層14,而形成本發明具有「奈米帶」的「高電子遷移率電晶體」或是「氮化鋁鎵/氮化鎵高電子遷移率電晶體」結構。 Next, referring to step 38 of FIG. 2, and in conjunction with FIGS. 3D and 4D, in step 38 of FIG. 2, a gate metal layer 184 is formed on the partially exposed aluminum gallium nitride layer 16 "Steps. In the present invention, the gate metal layer 184 is also formed by an E-gun deposition method or a thermal deposition method, which can be formed by a nickel / gold layer with a thickness of 20/80 nm, respectively. Secondly, The gate metal layer 184 is formed in the gate region between the source region and the drain region. The length Lg of the gate metal layer 184 is about 2 microns, as shown in FIG. 4D. Therefore, when the “length Lt” of the pitch 22 is greater than 2 μm, the gate metal layer 184 can only form a part covering each of the trenches 20. However, it is relatively understandable that, as shown in FIG. 4D, when the “length Lt” of the pitch 22 is smaller than the length Lg of the gate metal layer 184, the gate metal layer 184 can completely cover the trench 20 That is, the gate metal layer 184 can be completely formed to cover the exposed gallium nitride layer 14 to form the "high electron mobility transistor" or "aluminum gallium nitride / nitrogen" with the "nano band" of the present invention GaAs high electron mobility transistor "structure.
第5圖顯示本發明之「奈米帶」寬度為100奈米(nm)之電晶體正規化汲極電流(IDS)-閘極電壓(V)曲線特性,即如第5圖顯示本發明之「奈米帶」的「寬度Wt」為100奈米(nm)電晶體,固定汲極偏壓(VDS)為8伏特(V),得到汲極電流(IDS)對不同閘極偏壓(VG)的變化關係,該閘極偏壓係於「奈米帶」的「長度Lt」從1微米(μm)到2微米(μm),元件臨界電壓從-0.14伏特到0.79伏特,取值在汲極電流為1mA/mm時的閘極電壓。 Figure 5 shows the normalized sink current (I DS ) -gate voltage (V) curve characteristics of the transistor with a width of 100 nanometers (nm) in the "nano band" of the present invention, as shown in FIG. 5 The "width Wt" of the "nano band" is 100 nanometers (nm) transistors, the fixed drain bias (VDS) is 8 volts (V), and the drain current (IDS) is obtained for different gate biases ( VG), the gate bias is dependent on the "length Lt" of the "nano band" from 1 micrometer (μm) to 2 micrometers (μm), and the critical voltage of the device is from -0.14 volts to 0.79 volts The gate voltage when the drain current is 1mA / mm.
第6圖顯示本發明之「奈米帶」寬度為300奈米(nm)之電晶體正規化汲極電流(IDS)-閘極電壓(V)曲線特性,即如第6圖顯示本發明之「奈米帶」的「寬度Wt」為300奈米電晶體,固定汲極偏壓(VDS)為8伏特,汲極電流對不同閘極偏壓的變化關係,該閘極偏壓係於「奈米帶」的「長度Lt」從1微米到6微米,元件臨界電壓從-2.12伏特到0.46伏特,取值在汲極電流為1mA/mm時的閘極電壓。 Figure 6 shows the normalized drain current (I DS ) -gate voltage (V) curve characteristics of the transistor with a width of 300 nanometers (nm) in the "nano band" of the present invention, as shown in FIG. 6 The "width Wt" of the "nano band" is 300 nanometer transistors, the fixed drain bias (VDS) is 8 volts, and the relationship between the drain current and the different gate bias is changed. The gate bias is based on The "length Lt" of the "nano band" is from 1 micrometer to 6 micrometers, and the critical voltage of the device is from -2.12 volts to 0.46 volts. The value is the gate voltage when the drain current is 1 mA / mm.
第7圖顯示本發明之「奈米帶」寬度為500奈米(nm)之電晶體正規化汲極電流(IDS)-閘極電壓(V)曲線特性,即如第7圖顯示本發明之「奈米帶」的「寬度Wt」為500奈米電晶體,固定汲極偏壓(VDS)為8伏特,汲極電流對不同閘極偏壓的變化關係,該閘極偏壓係於「奈米帶」的「長度Lt」從1微米到6微米,元件臨界電壓從-2.52伏特到-1.62伏特,取值在汲極電流為1 mA/mm時的閘極電壓。 Figure 7 shows the normalized drain current (I DS ) -gate voltage (V) curve characteristics of the transistor with a width of 500 nanometers (nm) in the "nano band" of the present invention, as shown in FIG. 7 The "width Wt" of the "nano-belt" is a 500-nanometer transistor, the fixed drain bias (VDS) is 8 volts, and the relationship between the drain current and the different gate bias is changed. The gate bias is based on The "length Lt" of the "nano band" is from 1 micrometer to 6 micrometers, and the critical voltage of the device is from -2.52 volts to -1.62 volts. The value is the gate voltage when the drain current is 1 mA / mm.
第8圖顯示本發明之「奈米帶」長度為0.8微米之電晶體正規化汲極電流(IDS)-閘極電壓(V)曲線特性,即如第8圖顯示本發明之「奈米帶」的「長度Lt」為0.8微米電晶體,固定汲極偏壓(VDS)為8伏特,汲極電流(IDS)對不同閘極偏壓(VG)的變化關係。在「奈米帶」的「寬度Wt」從100奈米到500奈米時,元件臨界電壓從-0.41伏特到-2.62伏特,取值在汲極電流1mA/mm時的閘極電壓。 Figure 8 shows the normalized drain current (I DS ) -gate voltage (V) curve characteristics of the transistor with a length of 0.8 micrometers of the "nano band" of the present invention, as shown in FIG. 8 The "length Lt" of the band "is 0.8 micron transistor, the fixed drain bias (V DS ) is 8 volts, and the relationship between the drain current (I DS ) and different gate bias (V G ). When the "width Wt" of the "nano band" is from 100 nm to 500 nm, the critical voltage of the device is from -0.41 volts to -2.62 volts, and the value is the gate voltage at the drain current of 1 mA / mm.
第9圖顯示本發明之「奈米帶」長度為1微米之電晶體正規化汲極電流(IDS)-閘極電壓(V)曲線特性,即如第9圖顯示本發明之「奈米帶」的「長度Lt」為1微米電晶體,固定汲極偏壓(VDS)為8伏特,汲極電流(IDS)對不同閘極偏壓(VG)的變化關係。在「奈米帶」的「寬度Wt」從100奈米到500奈米時,元件臨界電壓從-0.14伏特到-2.52伏特,取值在汲極電流1mA/mm時的閘極電壓。 FIG. 9 shows the normalized drain current (I DS ) -gate voltage (V) curve characteristics of the transistor with a length of 1 micron of the “nano band” of the present invention, as shown in FIG. 9 The "length Lt" of "band" is a 1 micron transistor, the fixed drain bias (V DS ) is 8 volts, and the relationship between the drain current (I DS ) and different gate bias (V G ). When the "width Wt" of the "nano band" is from 100 nm to 500 nm, the critical voltage of the device is from -0.14 volts to -2.52 volts, which is the gate voltage at the drain current of 1 mA / mm.
第10圖顯示本發明之「奈米帶」長度為2微米之電晶體正規化汲極電流(IDS)-閘極電壓(V)曲線特性,即如第10圖顯示本發明之「奈米帶」的「長度Lt」為2微米電晶體,固定汲極偏壓(VDS)為8伏特,汲極電流(IDS)對不同閘極偏壓(VG)的變化關係。在「奈米帶」的「寬度Wt」從100奈米到500奈米時,元件臨界電壓從0.79伏特到-2.18伏特,取值在汲極電流1mA/mm時的閘極電壓。 Figure 10 shows the normalized drain current (I DS ) -gate voltage (V) curve characteristics of a transistor with a "nanometer zone" length of 2 micrometers according to the present invention, as shown in FIG. 10 The "Lt" of the "band" is a 2 micron transistor, the fixed drain bias (V DS ) is 8 volts, and the relationship between the drain current (I DS ) and different gate bias (V G ). When the "width Wt" of the "nano band" is from 100 nm to 500 nm, the critical voltage of the device is from 0.79 volts to -2.18 volts, and the value is the gate voltage at the drain current of 1 mA / mm.
於第11圖所顯示,猶如前述第5圖至第10圖中所顯示,本發明元件在不同「奈米帶」的長度(NRs length)及「奈米帶」的寬度(NRs width)之條件下,所產生的臨界電壓。而由該第11圖可以得知,當「奈米帶」寬度越窄,「奈米帶」長度越長時,元件的臨界電壓會往正方向偏移,故而可以推測奈米寬度在100奈米下,且奈米長度在4微米(μm),以及6微米(μm)的條件下,元件的臨界電壓亦會大於零。 As shown in Figure 11, as shown in Figures 5 to 10, the conditions of the device of the present invention at different "NRs length" and "NRs width" conditions Under the critical voltage. It can be seen from Figure 11 that when the width of the "nano band" is narrower and the length of the "nano band" is longer, the threshold voltage of the device will shift in the positive direction, so it can be speculated that the nano width is 100 nanometers Under the condition that the nanometer length is 4 microns (μm) and 6 microns (μm), the critical voltage of the device will also be greater than zero.
仍請參考第11圖所示,係本發明「側面面積(長度*深度)」變大時,會提高較多的表面狀態(Surface states)密度,故而本發明之結構可以運用來控制載子(carrier)。 Still referring to FIG. 11, as the "side area (length * depth)" of the present invention becomes larger, it will increase the density of more surface states (Surface states), so the structure of the present invention can be used to control carriers ( carrier).
參考第12圖所示,亦請參考第11圖「面積」對「臨界電壓」作圖所繪製顯示,於第12圖所示之橫軸,係為「奈米帶」中單一間距的「面積(NR area)」,縱軸為「臨界電壓(Vth)」。又單一間距的「面積」為「長度Lt」與「寬度Wt」的乘積,而「臨界電壓Vth」為「汲極電流」於1mA/mm下的「閘極電壓」。故由第12圖可知,當「寬度Wt」固定時,挖洞間距的「長度Lt」愈大,即單一間距的面積愈大,則其「臨界電壓Vth」升高。是以,本發明的「高電子遷移率電晶體結構10」的磊晶結構具有前述「奈米帶」的結構設計時,不僅可以減少元件的熱效應,亦可提高「臨界電壓Vth」,並且在具有固定間距的「寬度Wt」情形下,倘能增加間距的「長度Lt」,即可以提高「臨界電壓Vth」。 Refer to Figure 12 and also refer to Figure 11 "Area" plotted against "Critical Voltage". The horizontal axis shown in Figure 12 is the single-area "area" of the "nano zone" (NR area) ", the vertical axis is" critical voltage (Vth) ". The "area" of a single pitch is the product of "length Lt" and "width Wt", and "threshold voltage Vth" is the "gate voltage" of the "drain current" at 1 mA / mm. It can be seen from Figure 12 that when the "width Wt" is fixed, the larger the "length Lt" of the hole spacing, that is, the larger the area of the single spacing, the higher the "threshold voltage Vth". Therefore, when the epitaxial structure of the "high electron mobility transistor structure 10" of the present invention has the aforementioned "nano band" structure design, not only can the thermal effect of the device be reduced, but also the "critical voltage Vth" can be increased. In the case of a "width Wt" with a fixed pitch, if the "length Lt" of the pitch can be increased, the "threshold voltage Vth" can be increased.
依據前述,本發明之「高電子遷移率電晶體」結構包括具有「奈米帶」設計的閘極結構,其可提高半導體基材結構的散熱效果,維持較佳的性能,並且提高臨界電壓。且本發明利用變更「奈米帶」的複數個間距的長度和寬度,可減少高電子遷移率電晶體結構的熱效應,且同時具有提高臨界電壓的功效。又本發明具有「奈米帶」設計的閘極結構,故只需透過更改遮罩層的圖案即可得到,不須複雜的製程變更,有利於高電子遷移率電晶體的形成。 According to the foregoing, the "high electron mobility transistor" structure of the present invention includes a gate structure with a "nano band" design, which can improve the heat dissipation effect of the semiconductor substrate structure, maintain better performance, and increase the threshold voltage. In addition, the present invention can reduce the thermal effect of the high electron mobility transistor structure by changing the length and width of the plurality of pitches of the "nano band", and at the same time has the effect of increasing the critical voltage. In addition, the present invention has a gate structure with a "nano band" design, so it can be obtained only by changing the pattern of the mask layer, without complicated process changes, and is beneficial to the formation of high electron mobility transistors.
依前述說明,本發明之主要特徵,係具有帶狀(ribbon)的三維(3D)立體條狀結構,故可提昇「氮化鎵高電子遷移率電晶體(GaN HEMT)」元件側壁的表面態(surface state)密度,進而提高半導體材料的「表面釘紥效應(surface pinning effect)」。 According to the foregoing description, the main feature of the present invention is that it has a three-dimensional (3D) three-dimensional (ribbon) stripe structure, so the surface state of the side wall of the "GaN HEMT" device can be improved (surface state) density, which in turn improves the "surface pinning effect" of semiconductor materials.
以上所述僅為本發明的較佳實施例,並非用以限定本發明的權利 要求範圍,因此凡其他未脫離本發明所揭示的精神下所完成的等效改變或修飾,均應包含于本發明的範圍內。 The above are only the preferred embodiments of the present invention and are not intended to limit the rights of the present invention The scope is required, so any other equivalent changes or modifications made without departing from the spirit disclosed by the present invention should be included in the scope of the present invention.
10‧‧‧高電子遷移率電晶體結構 10‧‧‧High electron mobility transistor structure
12‧‧‧半導體基材 12‧‧‧Semiconductor substrate
14‧‧‧氮化鎵層 14‧‧‧GaN layer
16‧‧‧氮化鋁鎵層 16‧‧‧AlGaN layer
162‧‧‧源極區 162‧‧‧Source
164‧‧‧閘極區 164‧‧‧Gate area
166‧‧‧汲極區 166‧‧‧ Jiji District
18‧‧‧金屬層 18‧‧‧Metal layer
182‧‧‧歐姆金屬層 182‧‧‧ohm metal layer
184‧‧‧閘極金屬層 184‧‧‧Gate metal layer
20‧‧‧溝槽 20‧‧‧Groove
22‧‧‧間距 22‧‧‧spacing
L‧‧‧長度 L‧‧‧Length
Lg‧‧‧長度 Lg‧‧‧Length
Lt‧‧‧長度 Lt‧‧‧Length
W‧‧‧寬度 W‧‧‧Width
Wt‧‧‧寬度 Wt‧‧‧Width
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