TWI311371B - Double gate semiconductor device having separate gates - Google Patents

Double gate semiconductor device having separate gates Download PDF

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TWI311371B
TWI311371B TW092130612A TW92130612A TWI311371B TW I311371 B TWI311371 B TW I311371B TW 092130612 A TW092130612 A TW 092130612A TW 92130612 A TW92130612 A TW 92130612A TW I311371 B TWI311371 B TW I311371B
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Taiwan
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gate
fin
semiconductor device
layer
electrode
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TW092130612A
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TW200421595A (en
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Ahmed Shibly S S
Haihong Wang
Bin Yu
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Advanced Micro Devices Inc
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/68Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
    • H01L29/76Unipolar devices, e.g. field effect transistors
    • H01L29/772Field effect transistors
    • H01L29/78Field effect transistors with field effect produced by an insulated gate
    • H01L29/785Field effect transistors with field effect produced by an insulated gate having a channel with a horizontal current flow in a vertical sidewall of a semiconductor body, e.g. FinFET, MuGFET
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/41Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions
    • H01L29/423Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions not carrying the current to be rectified, amplified or switched
    • H01L29/42312Gate electrodes for field effect devices
    • H01L29/42316Gate electrodes for field effect devices for field-effect transistors
    • H01L29/4232Gate electrodes for field effect devices for field-effect transistors with insulated gate
    • H01L29/42384Gate electrodes for field effect devices for field-effect transistors with insulated gate for thin film field effect transistors, e.g. characterised by the thickness or the shape of the insulator or the dimensions, the shape or the lay-out of the conductor
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/43Electrodes ; Multistep manufacturing processes therefor characterised by the materials of which they are formed
    • H01L29/49Metal-insulator-semiconductor electrodes, e.g. gates of MOSFET
    • H01L29/4908Metal-insulator-semiconductor electrodes, e.g. gates of MOSFET for thin film semiconductor, e.g. gate of TFT
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/66007Multistep manufacturing processes
    • H01L29/66075Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials
    • H01L29/66227Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials the devices being controllable only by the electric current supplied or the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched, e.g. three-terminal devices
    • H01L29/66409Unipolar field-effect transistors
    • H01L29/66477Unipolar field-effect transistors with an insulated gate, i.e. MISFET
    • H01L29/66787Unipolar field-effect transistors with an insulated gate, i.e. MISFET with a gate at the side of the channel
    • H01L29/66795Unipolar field-effect transistors with an insulated gate, i.e. MISFET with a gate at the side of the channel with a horizontal current flow in a vertical sidewall of a semiconductor body, e.g. FinFET, MuGFET
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/68Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
    • H01L29/76Unipolar devices, e.g. field effect transistors
    • H01L29/772Field effect transistors
    • H01L29/78Field effect transistors with field effect produced by an insulated gate
    • H01L29/786Thin film transistors, i.e. transistors with a channel being at least partly a thin film
    • H01L29/78645Thin film transistors, i.e. transistors with a channel being at least partly a thin film with multiple gate

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  • Engineering & Computer Science (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Physics & Mathematics (AREA)
  • Ceramic Engineering (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Computer Hardware Design (AREA)
  • Manufacturing & Machinery (AREA)
  • Thin Film Transistor (AREA)
  • Insulated Gate Type Field-Effect Transistor (AREA)
  • Testing Or Measuring Of Semiconductors Or The Like (AREA)

Description

1311371 玖、發明說明 .................. 【發明所屬之技術領域】 本發明係關於半導體裝置以及製造該半導體裝置的方 法’尤指一種適用於雙閘極裝置者。 【先前技術】 超大型積體半導體裝置在高密度與高性能的加速需求 上,需如100奈米(nm)以下的閘極長度,高可靠度與製 造產里的增加專結構特性。而結構特性達1 〇〇nln以下時, 則面臨習知技術的極限。 例如’當習知平面金屬氧化物半導體場效電晶體 (MOSFET )之閘極長度小於i 〇〇nm時,與短通道效應有 關的問題,譬如源極與汲極之間的過度漏損,則會變得越 來越難克服。此外,遷移率的降低以及許多製程上的問題, 同樣會難以縮小習知M〇SFETs標有以包括更小的裝置特 性。因此,新的裝置結構乃因運而生,改善FET性能並進 一步縮小裝置。 雙閘極MOSFETs代表已經被視為取代現存平面 MOSFETs的新結構。在許多態樣中,雙閘極m〇sfeTs提 供比習知塊狀矽M0SFETs較佳的特性,其改良處在於雙 閘極MOSFET在通道的兩侧上具有—閘極電極,而不是如 在習知MOSFETs中僅位於一邊側上。當具有兩㈣時, 沒極所產生的電場會較佳地由該通道的源極端過渡。同樣 地,兩閘極能控制之電流約為單一問極的兩倍,而產生更 92454(修正版) 6 1311371
FinFET ( 1式場效電晶體)是目前顯現出良好短通道 行為的·雙間極結構。雖然習知的FinFET稱為、、雙閘極" MOSFETs,但是該兩閘極基本上係實f與電性地連接,從 而形成單-邏輯化的可定㈣極。FinFET包括形成於垂直 鰭部中的通道,FinFET結構可使用類似於製造習知平面 MOSFETs的電路佈局與製程技術來製造。 【發明内容】 本發明之實現在於提供具有雙閘極的FinFET裝置, 該閘極係藉導電鰭部(conductivefin)而有效彼此隔開, 該閘極可獨立地偏置以增加電路設計彈性。 本發明之其餘優點與其它特徵一部分將陳述於下述說 明中,而另-部份對熟諳該技藝者於審查下文時即能瞭 解或者可從實施本發明而知悉。本發明的優點與特徵可 依所附之申請專利範圍指出者而予實現與取得。 根據本發明,以上與其它優點能部份地由包括基板盘 ^成於該基板上之絕緣層的—種半導體裝置達成。縛部可 形成於該絕緣層上’並可包括頂表面與多數個側表 二 1極可形成於該絕緣層上且鄰近該縛部之多數側表面: 一者。第厂閘極可形成在該絕緣層上且與該第一 並且鄰近该鰭部之多數側表面之另外一者。 汗
根據本發明另—誓A & H 貫&心、枚,一種製造半導體裝 法可包括形成絕緣層於A 铲置的方
、土板上,以及形成鰭部結構於哕P 緣層上。該鰭部結構可包括第—側表面、第面= 頂表面。該方法亦可包 表面u及 括將源極與汲極區域形成於該鰭部 92454(修正版) 7 1311371 結構的末端,以及將閘極材料沈積於 極材料圍繞著該頂表面及該第:吉構上。該閘 料可予以㈣’以在該韓部的相對側上該閑極材 極電極。該沈積的問極材料可於鄰近該鰭部處予 很艨本發明 人 ㈣成"其士 …樣’半導體裝置係包括基板 广於該基板上的絕緣層。導電鰭部可形成於該絕緣声 =閑極介電層則可形成料導電鰭部的侧表面上。; =極電極可形成㈣絕緣層上。第—閘極電㈣可位在 :近該閘極介電層之-之導電鰭部的第—側上。第二閑極 電極可形成於該絕緣層i。第二閑極電極可位於導電妹部 的相對側上,鄰近該閘極介電層之另一者,並且與該第一 閘極電極相隔開。 &從下述詳細說明中,本發明的其它優點與特徵將為熟 相該項技藝者所清楚得知。所顯示與用以說明的具體實施 例提供欲實施本發明之最佳模式的說明。本發明能夠以各 種明顯的態樣來修改,而皆未背離本發明。因而,該等圖 式係用以說明本發明之本質而非限定之。 【實施方式】 本發明以下的詳細說明乃參考附圖’在不同圖式中的 相同標號可代表相同或類似的元件。同樣地,以下的詳細 說明並非用以限定本發明。相對地,本發明的範圍係由所 附之申請專利範圍及其等效者所定義出。 本發明之實施態樣係提供雙閘極FinFET裝置與此種 92454(修正版) 1311371 裝置的l造方法。根據本發明所製成之FinFET (鰭式場效 電晶體)f置裡的閘極係有效地彼此.關,且可個別地偏 置。 第1圖說明根據本發明_I體實*例而形成之半導體 裝置100的』面圖。參考第J圖’半導體裝置⑽係包括 石夕在絕緣體上(S0I)之結構,該結構包括—石夕基板110、 -埋設氧化物4120以及在該埋設氧化物層12〇上的一矽 層別。埋設氧化㈣12〇與石夕| 13〇係以一習知方式而 形成於基板11 0上。 在一實施例中,埋設氧化物層 物 ’並且具有從大約咖埃至大約3刪埃範圍的厚度。 石夕層230係包括厚度範圍從3⑽埃至〗埃的單晶或多晶 二,:步詳細於下者’係該石夕層13〇乃用來形成一雙閑 極電晶體裝置用的一鰭部結構。 —本發明之另實施例中,基板110與梦層13G可包括 其它的半導材料,譬如鍺,或者 ^ 干等材枓之組合,嬖如矽 錯。埋設氧化物層12G亦可包括其它的介電材料。= 如石夕氮化物層或者石夕氧化物層(例如,二氧 介電層140係形成於矽層13〇上,以 、 作為保護罩用。在一實施例中 的蝕刻製程中 為約15G埃至約f14G之沈積厚度得 化,以形成一光阻遮罩150用於後續製程 :?圖案 何習知的方式來沈積與圖荦化。 、^光阻係以任 半導體裝置100隨後係予钱刻,再移除該光阻遮軍 92454(修正版) 9 1311371 150。在一實施例中,矽層13〇可以習知的方式來蝕刻,而 該钱刻則終止於埋設氧化物層120上以形成一鰭部。在該 鰭部形成後,源極與汲極區域係形成於鄰近該鰭部的各別 端處。例如,在一具體實施例中,一矽、鍺、或矽與鍺組 合層則可以習知的方式予以沈積、圖案化與蝕刻以形成 源極與汲極區域。 弟2A圖係說明以此方式形成之半導體上,之縛 部結構俯視圖。根據本發明之一具體實施例,源極區域22〇 與汲極區域230係在埋設氧化物層12〇上鄰近鰭部2ι〇的 端處形成。 第2B圖係沿第2A圖之A-A’線所取的剖視圖,以說 明本發明之具體實施例的鰭部結構。介電層14〇與矽層13〇 係予蝕刻以形成鰭部210,該鰭部210係包括矽層13〇與 介電層140。 第3圖係根據本發明之一具體實施例之閘極介電層與 閘極材料形成於鰭部210上的剖視圖。一介電層係形^ 鰭部210上。例如,如第4圖所示,一薄氧化膜3ι〇得熱 生長於鰭部210上。氧化膜310係長至約1〇埃至約5〇埃 的厚度,且形成在鰭部210之矽層130之外露的侧表面上, 以作為一用於後續形成之閘極電極的介電層。類似於該氧 化膜310,介電層14〇得對該鰭部210之頂表面提供電性 絕緣。 在开> 成氧化膜3 1 0後’得沈積一閘極材料層3 2 〇於半 導體裝置1 00上。而該閘極材料層32〇得包含後續形成之 92454(修正版) 10 1311371 閘極電極所用的材料 係包括使用習知化例中,該閘極材料層320 其厚度範圍約3〇〇:二目沈積(CVD)而沈積出的多晶矽, 辟 、至約15〇〇埃。另外,其它的车道从止丨 言如鍺或切與錯的組 、::材料’ 極材料。 个』旳i屬,亦得做為閘 極材系藉由微影術(例如,光學微影)而定義於 極材枓層320中。 〜取玎、 带置HH) ^ 層320得選擇性地钮刻,以
=:。。上的閑極材料層32。形成出一問極結構。如第 者丁存極結構’得使部分閘極材料. $廿A "罨層1 40的頂部上。 第4圖係說明根據本發明具體實施例之閘極材料32〇 千面化的剖視圖。多餘的M極材料得予料(例如,從介 電们40上)’以平面化半導體裝置1〇〇的鰭部區域。例如, 可進灯化學機械式拋光(CMp ),以使該閘極材料(亦即,
閉極材料層320)纟垂直方向上甚至具有或者幾乎甚至具 有介電層140。 參考第4圖’在半導體裝置1〇〇通道區域中的閘極材 料層320係緊靠著鰭部21〇之兩側表自,以形成一第一閘 極41〇與第二閘極42〇。然而,鰭部21〇的頂表面係為: 電層140所覆蓋。此結構亦示於第5圖中,其係說明本發 明之半導體裝置1〇〇的俯視圖。在第5圖中,第一閑極41〇 與第二閘極420係鄰靠但未覆蓋鰭部2丨〇。 該閘極材料層320隨後可予圖案化與蝕刻,以形成雙 閘極電極。如第5圖所示,半導體裝置1〇〇包括具有閘極 92454(修正版) 11 1311371 m51〇肖52〇的雙_結構。如以下所詳述者,閑極電 虽51〇與52〇係有效地由鰭部21。所隔開,並可個別偏置。 為f曰1化起見’圍繞鰭部21〇之側表面之閘極介電 化膜31〇(如第4圖所示)未示於第5圖中。 隨後可將源極/汲極區域22〇與23〇播雜,例如η型或 Ρ型雜質可植入源極/汲極區域22〇與23〇中。特定的植入 劑量與能量可依據特別之終端裝置的需求而選定。一般熟 諳該技藝者將能依電路規格最佳化源極/汲極植入製程,: 該等步驟在此不予揭露,以不致於不當地混淆本發明的重 :。此外’侧壁隔片(未圖示)可在源極/汲極離子植入以 刖選擇14地φ成,以依據特定電路規格而來控制源極/及極 接合的位置。隨後’進行活化退火,以將源極Λ及極區域 220與230活化。 如第5圖所示,閘極電極51〇與閘極電極52〇係實質 以及電性地彼此隔開。根據本發明之—具體實施例,當使 用於電路中時’每—閘極電極510與520係以不同電壓個 別地偏置。獨立偏置第一閘極41〇與第二閘極42〇 (經由 閘極電極5 1 〇與520 )的能力會增加使用半導體裝置j 〇〇 之電路設計的彈性 第5圖中所示之製成的半導體裝置1〇〇係為具有第一 閘極4 1 0與第二閘極42〇的雙閘極裝置。相較於習知的雙 閘極裝置,閘極材料層32〇 (第3圖與第4圖)鄰接鰭部 210的兩表面,並提供半導體裝置1〇〇增大之通道寬度/裝 置之值。該鰭部2 1 0同樣可保留在閘極蝕刻中保護鰭部2 i 〇 12 92454(修正版) 1311371 的介電層140。 第一及第二閘極410與42〇同樣由鰭部21〇有效地隔 開,且係依半導體裝置1〇〇的特定電路規格而個別地偏置 (經由個別的閘極電極51〇與52〇)。相對於包括單閘極連 接的習知FinFETs’此種隔開的雙閘極結構在電路設計的 期間内提供增改的彈性。 因此,根據本發明,雙閘極FinFET裝置在該裝置的 通道區域中形成有兩㈣的_。所製成之結構會呈現出 良好的短通道表現。此外,本發明提供較大的彈性,並能 易於與習知的製程整合。 [其它實施例] 、在二實施例中,係欲將張力應變引入到FinFET (鰭 切效電晶體)的鰭部裡。第6A_6D圖係為說明本發明另 —具體實施例之將張力應變引入到鰭部裡的剖視圖。第6A 圖係示半導體裝置600的剖視圖。參照第6八圖,半導體 裝置600可包括埋設氧化物層(BOX) 610、.鳍部620以及 氧化矽罩63〇。如上述,元件61〇_63〇係依第圖所 逑者而形成。鰭部620係包括矽、鍺、或矽與鍺的組合。 如第6B圖所示,厚的去除式氧化物層得受熱生 :在鰭部620上。厚(例如,2〇〇_4〇〇埃)去除式氧化物 曰640會導入張力應變於鰭部62〇中。如第6c圖所示, 接而,將去除式氧化物層64〇移除,再生成薄閘極氧化物 層650。如第6D圖所示。閘極材料66〇隨後沈積於鰭部 2〇上。FmFET係以典型的方式而由第6D圖中的結構所 92454(修正版) 13 1311371 620將具有一張力應變 性質植入鰭部620中。 形成。在此一 FinFET中的鰭部 而會將熟諳該技藝者所能理解的 在其它的實施例中,係欲—完全石夕化閑極的 此- FinFET可具有-合併的金屬閘㉟,該金屬閘極能移 除多晶石夕消耗效應並且有助於得到用於跑·的適當極 限電壓。第7A圖與第7B圖係用來形成具有完切化閑極 之FinFET之示範性製程的圖式。參照第7A圖,裝置700 包括一鰭部710、源極區域72〇與汲極區域73〇。如上述, 這些層/結構係依第⑽圖所述者而形成。如第7B圖所 不鰭4 71 〇可包括—頂部氧化物罩以及圍繞一石夕結 構的閘極氧化物7 5 0。雜立β 71 η -Γ ·π^ π 710可形成於一埋設氧化(Β〇Χ) 層705上。 第7C圖所示,薄多晶矽層76〇係沈積於鰭部7】〇 上。接而,如第7D圖所示,沈積出一厚,底部抗反射(barc) 層770。如帛7E圖頂部所示,該閘極區域與接觸部780隨 後則可予以圖案化與蝕刻。 ^沒有移除BARq 77G的情形下源極與沒極區域 ;、730可植入離子。因此,所使用的摻雜質會為驗。 θ 所止檔而無法穿透入通道内(例如,鰭部71 〇 )。 =第7Ε圖與第7F圖所示,BARC層770得予以移除, 夕晶石夕760能完全地石夕化以形成金屬閑極彻。該閉 。材料71:亦可以類似上述第4圖所述之方式來平面化。 材料在的說明中’種種特定細節已予說明,譬如特定 、°、化學物、製程等等,以提供對本發明完整的 92454(修正版) 14 1311371 理解。總言之’本發明可在未藉在此所述之特定細節下實 施。在其它情形中’已知的製程結構說明並未細述,以免 不當地混淆本發明的標的。 用以製造本發明之半導體裝置的介電與導電層可藉由 習知的沈積技術而沈積。例如,可應用金屬化技術,譬如 不同型態的CVD製程’包括低壓CVD ( LPCVD )與增強 型 CVD (ECVD)。 本發明可實施於雙閘極半導體裝置的製造上,特別是 具有lOOnm以及以下之結構特徵的FinFET裝置。本發明 可應用於任一不同型態半導體裝置的形成,因而在此不予 夤述,以避免混淆本發明之標的。在實施本發明上,得使 用習知之光學微影術與蝕刻技術,因此,該等技術的細節 在此不另贅述。 本說明書僅將本發明的較佳具體實施例與其部分多用 j實例示出並說明。應理解的是,本發明能用於不同之其 匕組合與環境中’其並能在此所示的發明範内進行修改。 【圖式簡單說明】 以附圖為參考,其中具有相同標號的元件可代表全部 的相同元件。 第1圖係為說明根據本發明具體實施例所形成之鰭部 的剖視圖; 第2A圖係說明本發明之一具體實施例之鰭部結構的 俯視圖; 第2B圖係本發明之一具體實施例之第2A圖所示鰭部 15 92454C修正版) 1311371 結構的剖視圖; 第3圖係本發明一具體實施例之第2b圖所示裝置上 問極介電層舆閘極材料的形成之示意圖; 第4圖係根據本發明—具體實施例之第3圖所示閘極 材料平面化的剖視圖; 具體實施例之第4圖所示之 第5圖係為說明本發明 半導體裝置的俯視圖; 第6A至6D圖係為說明本發明另一實施例之將應變張 力應用導入於一鰭部中的剖視圖;以及 又 第7A至7F圖係為說明本笋 ^ 个知明另一具體實施例而將 全矽化閘極形成於FinFET中的价、 J俯現圖與剖視圖。
[元件符號說明J 100 半導體裝置 120 埋設氧化層 140 介電層 210 鰭部 230 汲極區域 320 閘極材料層 420 第二閘極 520 閘極電極 61〇 埋設氧化(BOX) 620 鰭部 640 犧牲氧化層 660 閘極材料 110 矽基板 13〇 矽層 150 光阻遮罩 220 源極區域 3 1 〇 氧化膜 41〇 第一閘極 51〇 閘極電極 6〇〇 半導體裝置 630 二氧化矽罩 65〇 薄閘極氧化層 7〇0 裝置 92454(修正版) 16 1311371 705 埋 設 氧化 (BOX) 層 710 鰭 部 720 源 極 區 域 730 汲 極 區域 740 頂 部 氧 化罩 750 閘 極 氧化 物 760 薄 多 晶 石夕層 770 BARC 層 80 屬 閘 極 17 92454(修正版)

Claims (1)

1311371 拾、申請專利範圍: 1,一種半導體裝置(100),包括: 基板(11 0 ); 絕緣層(120),形成於該基板(110)上; 鰭部(21G)’形成於該絕緣層(12G)上並且包 括頂表面與複數個側表面; 第一閘極(410),形成於該絕緣層(12〇)上,並 鄰近於該鰭部(210)之複數側表面之一者;以及 第一閘極(420),形成於該絕緣層(12〇)上,並 與該第一閘極(410)隔開且鄰近該鰭部(21〇)之複數 侧表面之另一個側表面。 2·如申請專利範圍第1項的半導體裝置(100),其中,該 第一閘極(420 )係形成在該鰭部(21 〇 )之相對側而遠 離該第一閘極(410)。 3.如申請專利範圍第2項的半導體裝置(1〇〇),其中,該 第與第一閘極(410、42〇)分別包括第一與第二間極 接觸件(510、520)。 4·如申請專利範圍第1項的半導體裝置(100),復包括: 複數個介電層(3 1 0 ),分別沿該鰭部(2 1 〇 )的複 數個側表面而形成,其中該第一與第二閘極(410、420) 分別緊鄰該複數個介電層(310)之不同者。 5.如申請專利範圍第1項的半導體裝置(1〇〇),復包括: 介電層(140),包含形成於該鰭部(210)之該頂 表面上之氮化物與氧化物之至少一者,其中該介電層 18 92454(修正版) 1311371 (14〇)的頂表面、該第一閘極(wo)的頂表面、與該 第二閘極(420 )的頂表面係實質上共平面。 6· —種製造半導體裝置(1〇〇)的方法,包括下列步驟: 形成絕緣層(120)於基板(U0)上; 形成轉部結構(210)於該絕緣層(12〇)上,該鰭 部結構(2 1 0 )包括第一側表面、第二側表面、以及頂 表面; 形成源極與汲極區域(220、23 0 )於該鰭部結構 (210 )的末端; 沈積閘極材料(320)於該鰭部結構(21〇)上,該 閘極材料(320 )圍繞著該頂表面以及該第一與第二側 表面; 將該閘極材料(320 )蝕刻,以將第一閘極電極(41 〇 ) 與第二閘極電極(420 )形成於該鰭部結構(21 〇 )的相 對侧上;以及 將鄰近該鰭部所沈積的閘極材料(32〇 )平面化。 7. 如申凊專利範圍第6項的方法’復包括下列步驟: 將介電層(140)形成於該鰭部結構(210)的該頂 表面上’其中該平面化之步驟包括: 將該閘極材料(320)拋光’俾使該閘極材料(320 ) 不致殘留在該介電層(140)上。 8. 一種半導體裝置(100 ),包括基板(110)、形成於該基 板(11 〇 )上的絕緣層(12〇 )、形成於該絕緣層(1 2〇 ) 上的導電鰭部(2 1 0 )、形成於該導電鰭部(2 1 〇 )之側 19 92454(修正版) 1311371 表面上的間極介電層(310)、以及形成於該絕緣層(120) 上的第—閘極電極(41 0 )’該第一閘極電極(41 0 )係 置在該導電‘鰭部(2 1 0 )之第一側上,且鄰近該閘極 "電層(310)之—者,其特徵在於: : 第二閉極電極(410)係形成於該絕緣層(120)上, 該第二閘極電極(42〇)係配置在該導電鰭部(21〇)的 ’子側上而鄰近該閘極介電層(HQ)之另一者,且與 該第一閘極電極(410)隔開。 9·如申请專利範圍第8項的半導體裝置(ι〇〇),復包括: 介電蓋狀物(140),形成於該導電鰭部(21〇)的 頂表面上,其中該第一閘極電極(41〇)與該第二閘極 電極( 420 )兩者均未延伸超出該介電蓋狀物(14〇)。 1〇·如申請專利範圍第9項的半導體裝置(1〇〇),其中,該 第閘極電極(410)、該第二問極電極(42〇)與該介 電蓋狀物〇4〇)的頂表面係實質上共平面。 92454(修正版) 20 1311371 柒、指定代表圖: (一) 本案指定代表圖為:第(4 )圖。 (二) 本代表圖之元件代表符號簡單說明: 100 半導體裝置 110 矽基板 120 埋設氧化層 130 矽層 140 介電層 310 氧化膜 410 第一閘極 420 第二閘極
捌、本案若有化學式時,請揭示最能顯示發明特徵的化學式:
92454(修正版)
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KR101029383B1 (ko) 2011-04-15
WO2004044992A1 (en) 2004-05-27
KR20050062656A (ko) 2005-06-23
CN1711644A (zh) 2005-12-21
JP2006505950A (ja) 2006-02-16
GB2408849A (en) 2005-06-08
US6611029B1 (en) 2003-08-26
GB2408849B (en) 2006-06-28
AU2003291641A1 (en) 2004-06-03
DE10393687T5 (de) 2005-10-06
GB0504833D0 (en) 2005-04-13
CN100459166C (zh) 2009-02-04
TW200421595A (en) 2004-10-16
US20040126975A1 (en) 2004-07-01
DE10393687B4 (de) 2012-12-06

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