TW586165B - Self-aligned nanotube field effect transistor and method of fabricating same - Google Patents

Self-aligned nanotube field effect transistor and method of fabricating same Download PDF

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TW586165B
TW586165B TW092104050A TW92104050A TW586165B TW 586165 B TW586165 B TW 586165B TW 092104050 A TW092104050 A TW 092104050A TW 92104050 A TW92104050 A TW 92104050A TW 586165 B TW586165 B TW 586165B
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carbon nanotube
gate
metal
effect transistor
dielectric layer
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Joerg Appenzeller
Phaedon Avouris
Kevin K Chan
Philip G Collins
Richard Martel
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    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y10/00Nanotechnology for information processing, storage or transmission, e.g. quantum computing or single electron logic
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    • 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
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    • H10K10/40Organic transistors
    • H10K10/46Field-effect transistors, e.g. organic thin-film transistors [OTFT]
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    • H10K10/462Insulated gate field-effect transistors [IGFETs]
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Description

586165
一、【發明所屬之技術領域】 本發明係有關於-種場效電晶體,特別有關於一種碳 奈米管場效電晶體。 二、【先前技術】 在分子奈米電子學(molecular nanoelectronics) 領域中,很少有材料像奈米管那麼有希望,特別是碳奈米 管,其包含有埃米等級直徑的石墨中空圓柱。奈米管可被 使用於電子元件中,如二極體及電晶體,視奈米管的電子 特性而定。奈米管具有特殊的尺寸、形狀以及物理特性。 結構上碳奈米管類似碳的六角形晶格滾入一圓柱中。 除了有趣的低溫下量子行為,碳奈米管具有至少兩項 重要特性:奈米管可以是金屬或是半導體的,依其對掌性 (chirality )而定(即構造幾何,conf〇rmati〇nai geometry)。金屬奈米管可以固定電阻率傳載極大電流。 半導體奈米管則可以電切換開或關,類似一場效電晶體 (field-effect transistor,FET)。這兩種奈米管可共價 連接(分享電子)。這些特性使得奈米管成為製作奈米等 級半導體電路之良好材料。 -此外,碳奈米管為——維電導體,意即僅有一維量子 ‘ 力學模式傳載電流。因為材料内之散射(scattering )被· 強烈壓抑,而使得使用碳奈米管之電晶體的元件效能具有
第5頁 586165
強大的優勢。元件具有較低之散射 代表具有較好之效
…對一個三端元件而言,例如場效電晶體,一閘極(第 二端)需要與主動通道區、源極以及汲極絕緣。因此需要 使用例如是二氧化矽等介電材料。要改善矽元件内之元件 特性介電層厚度可降低。而介電層厚度減少,使得閘極 電谷i曰加,且促進閘極對通道— channei)之耦 合。對標準矽場效應元件而言,閘極電容之大小與介電能 厚度成反比。現今製造的高效能處理器中,二氧化矽之厚 度低於4nm。重要的是,不易達到更低之厚度,因為當氧 化層厚度低於4nm時,閘極透過介電層之漏電流指數增 加0 ;、、、、而’對於一碳奈米管電晶體而言,閘極電容與介電 f厚度不呈反比關係。&而代之的是,碳奈米管依循-對 =關,。與-般標準之發場效電晶體相較,因為其圓柱狀 成何外形,碳奈米管電晶體之閘極電容可以更大。 未有已知系統或方法在一場效電晶體中使用奈米管以 Φ : 5表現與較小尺寸。因11匕,需要-製作-奈米管場效 電日日體的系統及方法。 三
發明内容
第6頁
ου 丄 CO
自對準碳奈米管場效 根據本發明之一實施例,提供_ 電晶體半導體元件。此元件包二 山 _ -基板。-源極形成於上述碳太::一:示米管放置於 形成於上述碳奈米管之-第::未官之H -沒極 上述碳奈米管之一部分上,」及-閘極實質形成於 述碳奈米管隔開。 、’"電層使上述閘極與上 上述基板包括一I之厚度約為150nm ‘ 热礼化層沉積於 帘丞敗上 以 此元件更包括一保護介電層於元件上。 此半導體元件更包括一對準記號於基板上,供源極以 上述閘極披覆於介電層以及碳奈米管,並與碳奈米管 之一背面接觸。 ” & 根據本發明之一實施例,提供一自對準碳奈米管場效 電aa體半導體元件。此元件包括以下。一垂直碳奈米管, 以一介電材料纏繞。一源極,形成於上述碳奈米管之一第 586165
第8頁 586165
五、發明說明(5) 金屬接點係利用一光阻形成。 根據本發明之一實施例,提供一形成自對準碳奈米管 場效電晶體半導體元件的方法。此方法包括以下步驟。放 置一碳奈米管於一熱氧化物基板上,其中基板包括一對準 "己號。以反應式離子#刻(reactive ion etch)方式, ^碳奈米管之每一端形成一金屬接點,其中一第一金屬接 點係一源極,且一第二金屬接點係一汲極。形成一氮化間 ^壁於每一金屬接點之兩側。沉積具有高介電常數(high 之了介電層’於自對準碳奈米管場效電晶體半導體元件 上。以及形成一閘極,實質位於源極以及汲極之間,並於 碳奈米管上。 上述方法更包含一步驟:沉積一保護介電層於元件 場效ί f 5::之一實施例,提供-形成自對準碳奈米管 置-件的方法。此方法包括以下步驟。激 記號。在碳I米管:mi: 基板包括-對準 層使非晶矽柱絕緣。 : 虱化 間。形成-閉^實質位於間於ί晶:柱之― 上。形成-氮化層,於閘極上。於 ^二:奴奈米官 氧化間隙壁。以金屬接點取代非…第2屬 586165 五、發明說明(6) 以及沉積一 接點係一源極,且一第二金屬接點係一汲極。 保護介電層於元件上。 …根據本發明之另一實施例,提供一形成自對準碳 管場效電晶體半導體元件的方法’此方法包括以下? 沉積-金屬催化劑於-熱氧化物基板。沉積一低 於元件上。姓刻形成一溝槽(trench),溝槽通過氧化^ 以及金屬催化劑,並進入位於金屬催化劑下方之一埶氧化 層。蝕刻低溫氧化層以形成氧化物島。剝除 … (stripping )暴露之金屬催化劑。成長一奈米管,位於 該等氧化物島之下的該金屬催化劑之間。以一閘極介電層 包覆碳奈米管。形成氮化物間隙壁於氧化物島相對之表 面。以化學氣相沉積方式形成一閘極,實質位於氧化物島 之間,並位於奈米管上。以及沉積一保護介電層於元件 上。 根據本發明之一實施例,提供一形成自對準碳奈米管 場效電晶體半導體元件的方法,此方法包括以下步驟。成 長一奈米管垂直於該半導體元件之一表面所形成之一金屬 催化劑。形成一氮化物塊結構。以一閘極介電層包覆破奈 米管。沉積一閘極金屬’並以閘極介電層使閘極金屬與金 屬催化劑隔開。沉積一氮化層。形成閘極金屬柱,被氮化 層所覆蓋。形成氮化物間隙壁,包覆閘極金屬柱。沉積一 >及極金屬’實質位於閘極金屬柱之間,以介電層使汲極金
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586165 五、發明說明(8) 1 〇 9以形成金屬接點1 〇 6、1 〇 7之側的間隙壁11 〇。而非晶石夕 1 08可以選擇性方式移除或以濕式化學方法氧化之。一@問 極介電層111形成於元件上。這裡以及以下的方法中,介 電層可以是二氧化矽或是任何高介電常數之材料,例如: Hf〇2。閘極112可利用化學氣相沉積以及蝕刻法實質形成金 屬接點106、107、源極以及汲極之間。一保護介電層113 沉積於元件上。源極、汲極以及閘極皆自對準於 ^呓號 101。 〇
在另一實施例中,在形成閘極之前,源極以及汲極以 反應式離子蝕刻方法而成。請參閱第2a〜2b圖,形成源 極、汲極以及金屬接點1〇6、107之方法,首先利用反應式 離子钱刻方式定義源極以及汲極之金屬。其中,反應式離 子餘刻需絕緣於碳奈米管104。一氮化層2〇ι沉積於^牛 上,並自金屬接點周圍區域蝕刻之。氮化物間隙壁2〇2形 成於金屬接點之側邊。一閘極介電層2 〇 3沉積於元件上。 閘極金屬204實質形成於源極以及閘極1〇6、1〇7之門。一 保護介電層205可沉積於元件上。熱氧化層厚度約。
、,根據本發明之另一實施例,閘極可形成於源極/汲極 之丽。非晶矽301可沉積於碳奈米管1〇4之兩端。此非晶矽 可以一氧化物層302覆蓋。一閘極介電層3〇3沉積於非晶矽 層,例如301,之間。一閘極304實質形成於此非晶矽柱 301之間。一氮化層3 0 5形成覆蓋閘極3〇4。氧化物間隙壁
586165 五、發明說明(9) 306形成於閘極304金屬之兩端。而暴露出之非晶石夕/ 物之角^,可以被剝除以露出非晶石卜餘下之非晶秒乳化费 閘極金屬,可以反應式離子㈣方式移除之。金屬接^ 307、308與奈米管1〇4連接,奈米管1〇4部分位於閘極3〇4 以及閘極介電層3 03下方。金屬接點3〇7、3〇8形成此半 體兀,之源極以及汲極。金屬接點3〇7、3〇8可以對準沉 於熱氧化層102以及矽基板103内之對準記號1〇1。最貝 保護介電層3 0 9於此元件上。 、,根據本發明之一實施例,一碳奈米管場效電晶體可於 適當處成長。其中源極/汲極形成於閘極之前,一非晶石夕 層401/儿積於一熱氧化層1Q2上。一低溫氧化層jog (lt〇) 可沉積於金屬催化劑上。蝕刻低溫氧化層4〇2、非晶矽層 4〇1以及熱氧化層1〇2以形成一溝槽。則部分位於氧化層 402下方之非晶石夕層4〇1被底切(un(jer cut)。一金屬催 化劑40 1B則進入非晶矽4〇1被底切之邊緣,其中,金屬催 化劑可以為Fe、Co、Ni或是Fe/Mo。一碳奈米管403可成長 於金屬催化劑40 1B之間,其中一部分奈米管懸吊於熱氧化 層1 02上。一閘極介電層4〇4以化學氣相沉積方式沉積並包 覆奈米管403。因此奈米管403可完全以閘極介電層覆蓋。 間隙壁405可形成於氧化層402之側邊。一閘極40 6可實質 形成於氧化層402之間。若是熱氧化層102被蝕刻的夠深, 則閘極金屬406可包覆整個碳奈米管403以及介電層404。 為達到此目的’閘極金屬可以化學氣相沉積之方式,以覆
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蓋奈米管/介電層堆疊之背面。此一包覆方式,提供較佳 之閘極與奈米管之耦合。一保護介電層4〇6沉積於表 面上。 、根據本發明之另一實施例,一碳奈米管於適當處垂直 成長。成長一奈米管垂直於例如於基部的一金屬源極戍一 金屬催化劑。請參閱第5a〜5n圖,一金屬催化劑5〇1形1於 矽基板502上。一氮化物503之第一層沉積於半導體元件 上。在氮化物503上沉積一氧化層504,再在氧化層5〇4上 >儿積第二層氮化物5 0 5。一光阻5 0 6以一般微影製程形成於 此半導體元件,且曝露出金屬催化劑5 〇 1之部分。將複數 個第二金屬催化劑5 0 7沉積於此元件上。再將光阻5 〇 6剝 離,使得第二金屬催化劑507僅存在於第一金屬催化劑5〇1 上。而在每一第二金屬催化劑5〇7上,垂直地成長一奈米 管5 0 8,如此形成奈米管的二維以及三維陣列。 當分子金屬催化劑設置對準於基板上之細孔 (pore ) ’則碳奈米管垂直於基板成長。在此情形下,成 長空間被偈限,並使奈米管之成長僅在垂直方向。原則 上,垂直之細孔,如第5b圖所示,可利用光阻及圖案轉移 製作。 一非晶矽層5 0 9形成覆蓋元件。元件可被平坦化至與 氮化層5 0 5齊。再移除部分之氮化物—氧化物-氮化物層5 0 3
第14頁 586165 五、發明說明(11) -- 〜505。奈米管5〇8周圍以及金屬催化劑5〇ι、5〇7周圍留下 ,狀物(Pillar )。一犧牲層51〇覆蓋氮化物5〇5、碳夺 官508以及非晶州9。接觸層可以為η或是w。移除氮化、 ”03以及505間之氧化物5〇4。接著非晶矽5〇9同時自 = 5 08周圍被移除。非晶㈣9亦可以在移除氧化物之、 後被移除。一閘極介電層5n ,形成於奈米管5〇8周圍 於犧牲層51〇下,金屬催化劑51()上。若為二維奈米管陣位· 列,閘極介電層511可形成於碳奈米管間。犧牲層51〇可 Π方5移除。接著沉積於元件表面上。沉積第三氮化層 13於閘極金屬512上。接著移除部份氮化物513以及閘^
512,而形成柱狀之氮化物513以及閘極512仍包覆前述 I 屬催化劑-奈米管結構。氮化物間隙壁514形成於柱狀两 圍。汲極接點5 1 5形成於金屬催化劑_奈米管結構上,形二 一場效電晶體。沉積一保護介電層516於各個場效電晶體 之間。 、必須注意的是,自金屬催化劑成長奈米管之確實機 並不被知道。不過此一金屬催化劑成長單壁奈米管之過, 程,例如鈷於氧化鋁支撐之鉬顆粒上(c〇baU Mer之 alumina-supported Molybdenum particles),可採用不 根據本發明之另一實施例,可採用應用組裝之 而非如前所述放置或成長的方式來擺放奈米管。應 方 用 式, 組裝
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可用於垂直或是水平之奈米管放置,此放置係利用化學或 物f方式驅動之選擇性設置。此一選擇性放置包括形成一 黏著層或是化學基團(chemical gr〇ups)作為接收體, 用以幫助奈米管放置在所需之位置上。第6a〜6b圖分別顯 示水平以及垂直應用組裝之方法。其中,一奈米管6〇1兩 端包括預設之化學基團602,例如DNA股(strand )或是醇 類。奈米管601被帶到靠近具有接收體6〇4之基板6〇3,若 用DNA,則使用互補之DNA股。而若用醇類,則金粒或包含 金的接點可用以作為鏈結具有此類化學基團6 〇 2之奈米管 601。而奈米管601可以此組裝方式設置於基板6〇3内。 效能較佳之高介電常數介電層可作為閘極之絕緣層。 了碳奈米管場效電晶體之電容不會隨介電層厚度產生巨 變化,因此較難達到所需之電容,甚至是較薄之閘極介 層。Abo〆介電常數k = 9)以及Hf〇2(介電常數k = 2〇)在此背旦 之下,則有希望可以作為介電層用。化學氣相沉積銘,‘ 氧化以形成高介電常數之閘極介電層,或是直接沉積八 (則2亦可以直接沉積)。與二氧切相較,使用上述材^ 約可增加五倍之問極電$,且對半導體元件之效能比減少 介電層厚度具有較大之影響效果。纟於奈米管在—空 境下為PFET,而在真空下通入氬氣並經過退火後,會轉變 為nFET,0此在介電層沉積前,可對此半導體元件進 火,使^奈米管轉變為nFET。在原處Un以汕)以一介 電層加蓋此一半導體元件’以防止奈米管再次轉換為
586165 五、發明說明(13) pFET。對^互補技術而言,應轉為矸^的場效電晶體上的 介電層可被移除,且仍可摻雜此些場效電晶體。再在低溫 下利用-化學氣相沉積塗佈此些元件,不需額外之退 驟0 適结Λ,或是nm)皆以氧化層 適田之"電層)覆盍’目此在閘極電極製造時,並不 ΠΪ之沉積可使用化學氣相沉積。如第4以及第5 學氣相沉積法進行此-製程可確定介電層 :王二;官丄同時閘極金屬亦完全包覆介電層,而形 Ϊ: Π 管輕合之條件。閘極金屬可以在所需 可以開放(。pen)以供電接觸。疋移除而源極和汲極 雖然本發明已以一較佳青祐 以限定本發明,任何熟習此技藝j揭:並非用 二圍;當可作些許之更動與潤飾,因此本發 乾圍s視後附之申請專利範圍所界定者為準。 ’、凌 586165 圖式簡單說明 五、【圖式簡單說明】 第1 a〜1 i圖顯示本發明一實施例之一源/閘極第一碳奈米管 場效電晶體, 第2 a〜2 b圖顯示本發明另一實施例之一源/閘第一碳奈米管 場效電晶體; 第3 a〜3 g圖顯示本發明一實施例之一閘極第一碳奈米管場 效電晶體; 第4 a〜4 d圖顯示本發明一實施例之一碳奈米管場效電晶體 包含適當地方成長之一奈米管; 第5 a〜5 η圖顯示本發明一實施例之一碳奈米管場效電晶體 包含適當地方垂直成長之一奈米管;以及 第6 a〜b圖顯示本發明一實施例奈米管之應用組裝。 元件符號說明 1 (Π〜對準記號; 1 0 2〜熱氧化層; 103、 502、603〜石夕基板; 104、 403、508、601〜奈米管; 105、 506〜光阻; 106、 107、307、308、515〜接點; 108、 301、401、50 9〜非晶石夕層; 109、 201、30 5、503、50 5、513〜氮化層; 110、 2 0 2、30 6、40 5、514〜間隙壁; 111 、113 、203 、205 、303 、309 、404 、 511、 516〜介電
第18頁 586165 圖式簡單說明 層; 1 1 2、2 0 4、3 0 4、4 0 6、5 1 2 〜問極; · 3 0 2、4 0 2、5 0 4〜氧化物層; , 4 0 1 B、5 0 1、5 0 7〜金屬催化劑; 5 1 0〜犧牲層; 6 0 2〜化學基團; , 604〜接收體。
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Claims (1)

  1. 586165 六、申請專利範圍 1. 一種自對準碳奈米管場效電晶體半導體元件,包括: 一碳奈米管放置(deposited)於一基板; 一源極形成於該碳奈米管之一第一端; 一汲極形成於該碳奈米管之一第二端;以及 一閘極實質形成於該碳奈米管之一部分上,並以一介 電層使該閘極與該碳奈米管隔開。
    2. 如申請專利範圍第1項所述之自對準碳奈米管場效電晶 體半導體元件,其中該基板包括一熱氧化層沉積於一矽基 板。 3. 如申請專利範圍第2項所述之自對準碳奈米管場效電晶 體半導體元件,其中該熱氧化層之厚度約為150 nm。 4. 如申請專利範圍第1項所述之自對準碳奈米管場效電晶 體半導體元件,其中一部分之該閘極更以一氧化層與該碳 奈米管隔開。
    5. 如申請專利範圍第1項所述之自對準碳奈米管場效電晶 體半導體元件,其中該閘極以一氮化物間隙壁 (spacer ),與該源極和沒極隔開。 6.如申請專利範圍第1項所述之自對準碳奈米管場效電晶 體半導體元件,更包括一保護介電層(passivation
    第20頁 586165 六、申請專利範圍 dielectric layer)覆蓋該元件。 7 ·如申請專利範圍第1項所述之自對準碳奈米管場效電晶 體半導體元件,更包括一對準記號於該基板上,供該源極 以及該汲極對準。 8 ·如申請專利範圍第1項所述之自對準碳奈米管場效電晶 體半導體元件,其中該閘極披覆於(wraps around )該介 電層以及該碳奈米管,以與該碳奈米管之一背面接觸。 9. 一種碳奈米管場效電晶體半導體元件,包括: 一垂直碳奈米管,以一介電材料纏繞(wrap ); 一源極,形成於該碳奈米管之一第一端; 一汲極,形成於該碳奈米管之一第二端; 一雙層氮化物複合體(bilayer nitride complex ),供形成該源極以及該汲極各自之一捆帶 (band strap),並使該源極以及該汲極與該介電材料纏 繞之該碳奈米管連接;以及 一閘極’實質形成於該碳奈米管之一部分上。 1 0 ·如申請專利範圍第9項所述之碳奈米管場效電晶體半導 體元件’其更包括—金屬催化劑於該碳奈米管之一基部 (base ) °
    586165 六、申請專利範圍 11·、種形成一自對準碳奈米管場效電晶體半導體元件的 方法,包括下列步驟: 放置一奈米管於一熱氧化物基板上,其中該基板包括 一對準記號; 於该奈米官之每一端形成一金屬接點,其中一第一金 屬接點係一源極,且一第二金屬接點係一汲極; 沉積一非晶矽層於該元件上; 形成一氮化間隙壁,於每一該等金屬接點之兩側 (oppos i ng sides); 沉積具有高介電常數(high k)之一介電層於該元件 上; 氧化该非晶秒層;以及 形成一閘極,實質上位於該源極以及該汲極之間,並 位於該奈米管上。 1 2·如申請專利範圍第11項所述之方法,其更包含一步 驟··沉積一保護介電層於該元件上。 1 3 ·如申請專利範圍第丨丨項所述之方法,其中該奈米管係 一單壁(single-waiied)奈米管。 1 4 ·如申請專利範圍第丨丨項所述之方法,其中該等金屬接 點係利用一光阻形成。
    第22頁 586165 六、申請專利範圍 1 5 · —種形成一自對準碳奈米管場效電晶體半導體元件的 方法,包括下列步驟: 散I 奈米管於一熱氧化物基板上,其中該基板包括 一對準記號; 以反應式離子餘刻(reactive i〇n etch)方式,於 ΰ玄示米’之母一端形成一金屬接點,其中一第一金屬接點 係一源極,且一第二金屬接點係一汲極; 形成一氮化間隙壁於每一該等金屬接點之兩側; >冗積具有高介電常數之一介電層於該元件上;以及
    形成一閘極,實質位於該源極以及該汲極之間,且位 於該奈米管上。 16.如申請專利範圍第15項所述之方法,其更包含一步 驟:沉積一保護介電層於該元件上。 1 7 · —種形成一自對準碳奈米管場效電晶體半導體元件的 方法,包括下列步驟: 放置一奈米管於一熱氧化物基板上,其中該基板包括 一對準記號; 在邊奈米管之每一端上,形成一非晶矽柱 (amorphous silicon pillar ) \ 以一氧化層使該等非晶矽柱絕緣(丨s〇丨at i叫); 形成一閘極介電層於該等非晶矽柱之間; 升/成閘極貝貝位於该專非晶石夕柱之間,且位於該
    第23頁 586165 六、申請專利範圍 奈米管上; 形成一氮化層於該閘極上; 於该閘極之每一邊,形成一氧化間隙壁; 以i屬接點取代該等非晶矽柱,其中一第一金屬接點 係一源極,且一第二金屬接點係一汲極;以及 沉積一保護介電層於該元件上。 18· —種形成一自對準碳奈米管場效電晶體半導體元件的 . 方法,包括下列步驟: 沉積一金屬催化劑於一熱氧化物基板上; · 沉積一低溫氧化層於該元件上; I虫刻形成一溝槽,該溝槽通過該氧化層以及該金屬催 化劑,並進入位於該金屬催化劑下方之一熱氧化層; 蝕刻該低溫氧化層以形成氧化物島; 剝除暴露之該金屬催化劑; 成長一奈米管,位於該等氧化物島之下的該金屬催化 劑之間; 以一閘極介電層包覆該奈米管; 形成氮化物間隙壁於該等氧化物島相對之表面; 以化學氣相沉積方式形成一閘極,實質位於該等氧化 | 物島之間,並位於該奈米管上;以及 沉積一保護介電層於該元件上。 . 1 9 · 一種形成一自對準碳奈米管場效電晶體半導體元件的
    586165 六、申請專利範圍 方法,包括下列步驟: 成長一奈米管垂直於該半導體元件之一表面所形成之 一金屬催化劑; 形成一氮化物塊結構(n i t r i d e b 1 〇 c k structure ); 以一閘極介電層包覆該奈米管; 沉積一閘極金屬,並以該閘極介電層使該閘極金屬與 該金屬催化劑隔開; 沉積一氮化層; 形成閘極金屬柱,被該氮化層所覆蓋; 形成氮化物間隙壁於該柱周圍; 沉積一汲極金屬,實質位於該柱之間,以該介電層使 該汲極金屬與該閘極金屬分開;以及 沉積一保護介電層於該元件上。
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