TW201034185A - Metal-insulator-semiconductor tunneling contacts - Google Patents

Metal-insulator-semiconductor tunneling contacts Download PDF

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Publication number
TW201034185A
TW201034185A TW098142486A TW98142486A TW201034185A TW 201034185 A TW201034185 A TW 201034185A TW 098142486 A TW098142486 A TW 098142486A TW 98142486 A TW98142486 A TW 98142486A TW 201034185 A TW201034185 A TW 201034185A
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Taiwan
Prior art keywords
transistor
contact
insulator
source
conductive
Prior art date
Application number
TW098142486A
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English (en)
Inventor
Niloy Mukherjee
Gilbert Dewey
Matthew V Metz
Jack Kavalieros
Robert S Chau
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Intel Corp
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Publication date
Application filed by Intel Corp filed Critical Intel Corp
Publication of TW201034185A publication Critical patent/TW201034185A/zh

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  • Electrodes Of Semiconductors (AREA)
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201034185 六、發明說明: L 明所屬技領3 本發明係有關於金屬-絕緣體-半導體穿隧接點。 背景 本發明之背景 在積體電路的製造中,諸如電晶體的裝置形成於一晶
圓上,且使用多個金屬化層連接在一起。該等金屬化層包 括通孔及互連體,如在該技藝中已知的,其等作為用以互 連該等裝置的電氣路徑發揮作用。接點將該等通孔及互連 體連接至該等裝置。 【明内j 依據本發明之一實施例,係特地提出一種裝置,其包 含有.-電晶體’其具有_源極區域及—汲極區域;—第 層間電介質層,其相鄰於該電晶體;一溝槽,兑穿過該 第-層間電介質層至該源極區域;及—傳導源極接點,: 該溝槽巾’簡極接㈣自—歸層與賴極區域相分離。 圖式之簡單描述 圖,=圖是緣示具有—電氣接點之—裝置的1面側視 、.該傳導接點材料藉由—絕緣體與該正受接觸的區 场I分離; 第2圖是繪示可用以製造第1圖所示之該裝置的一方 法的一流程圖; 第3圖是繪示沈積於該電晶體上之該第-ILD層的一 3 201034185 截面側視圖; 第4圖是繪示形成於該第一 ILD層中之溝槽的一截面 側視圖; 第5圖是繪示沈積於該等溝槽中之該絕緣層的一截面 側視圖; 第6圖是繪示沈積於該絕緣層上之該傳導層的一截面 側視圖; 第7圖是繪示該填充材料的一截面側視圖; 第8圖是繪示額外的ILD及傳導層的一截面側視圖; 第9圖是繪示一多閘極電晶體的一等角視圖; 第10圖是穿過該鰭片之該源極區域部分,且繪示該第 一 ILD層的一截面側視圖; 第11圖是繪示形成於該第一 ILD層中之一溝槽的一截 面側視圖; 第12圖是繪示形成於該鰭片之該頂面及側壁上的該絕 緣層、形成於該絕緣層上的該傳導層116及實質上填充該 溝槽之剩餘容積的該填充材料的一截面側視圖; 第13圖是繪示缺乏填充材料之一實施例的一截面側視 圖;以及 第14圖是繪示在同一基體上的一第一電晶體及一第二 電晶體的一截面側視圖。 C實施方式3 詳細描述 在下面的描述中,至一半導體裝置的一接點的各種實 201034185 ⑽料以討論,其中―絕緣體將—傳導接點與該裝置分 離彡該相關技株中具有通常知識者將認識到的是,該等 各種實施例可以不由該等特定細節中—或多個細節來實 行,或由其他替代及/或額外的方法、材料或元件來實行。 在其他實例中’已知的結構、材料或操作沒有予以詳細地 顯示或描述’以避免模糊本發明之各種實施例的層面。類 似地,以解釋為目的,特定的數目、材料及組態被提出, • α提供對本發明的透徹理解。然而,本發明可不由特定的 細節來實行。再者,應理解的是,在該等圖中所示的各種 實施例是說雜的範例表示,且不_定按照比例缚製。 貫穿此說明書對“—實施例,,之參照意指結合該實施例 ‘ 所述之一特定的特徵、結構、材料或特性包括於本發明的 ' 至少—個實施例中,但是不表示其等出現於每一實施例 中因而,在貫穿此說明書出現於各種地方的短語“在一實 施例中’’不-定是指本發明的同_實施例。再者,該等特定 • ㈣徵、結構、材料或特性可以任何適當的方式結合於-或多個實施例中。可包括各種額外的層及/或結構 ,及/或在 其他實施例中可省略所述的特徵。 各種操作將依:欠以最㈣助理解本發明之^•式,而描 述為多個分離的操作。然而,描述的次序不該理解為是暗 =,此等操作必須是:欠序相依的。特制是此等操作不 而要以陳述的次序來執行。與該所述實施例相比,所述操 作可以+同的次序,串聯地或並行地予以執行。各種額 卜的操作可予以執行,及/或在額外實施例中所述操作可予 5 201034185 以省略。 第1圖是繪示具有一電氣接點之一裝置丨00的一截面 側視圖,其中該傳導接點材料116藉由一絕緣體114與正 受接觸的該等區域106、108分離。在一實施例中,該裝置 100是一電晶體。該電晶體包括一源極區域1〇6及一汲極區 域108。存在至該等源極及汲極區域106、1〇8的接點。此 等接點包括藉由一絕緣材料114與該等源極及汲極區域 106、108分離的一傳導材料116。此一安排避免了需要一 般用於電晶體的一矽化物或鍺化物接點。 透過避免一矽化物或鍺化物接點的使用,裝置100的 一些實施例可允許使用保形的接點形成製程,其允許接點 形成於較小的溝槽中’使裝置100能夠縮小尺寸。該裝置 100的一些實施例較容易製造,因為不需要一矽化物或鍺化 物所需的超純的金屬沈積。而且,隨著裝置100變得越來 越小’較少的半導體材料可用來形成一矽化物或鍺化物。 該裝置100的一些實施例透過不使用一矽化物或鍺化物, 而避免了過度消耗形成該裝置1〇〇之一部分的半導體材 料。而且,矽化物等的形成可能將應力施予該裝置,或限 制可能由其他結構及材料所引起的應力。透過省略該石夕化 物’可能增加該等可用應力修改的可能性,且從而允許一 性能較佳的裝置100。 在該所繪示範例中,該裝置1〇〇包括一基體102。此基 體102可包含作為可建立一半導體裝置之基礎的任何材 料。在一範例中,基體102是一包含矽的基體,儘管在其 201034185 :财也可使用其他的材料。該基想ι〇2可使用 緣層切結構來形成。在其財施中,該基想1〇2 他㈣枓形成’該等其他的材料可與或不與石夕結 括{不限於鍺、録化銦、碲化船、_化銦、鱗化姻、 珅:鎵:。綈化鎵或其他的第三至五族材料。該基體1〇2可 =-早「的材料’或具有多個層及/或具有多個結構。雖 ,,、、此知述了可形成該基冑102之材料的-些範例,但是
可作為建立—裝置之基礎的任何材料都在本Μ的精神及 範圍中。 “所、會下之範例中的該裝置_包括一電晶體。該 電的體匕#閘極1〇4、一源極區域_及一没極區域 1〇8/β該電晶體可包括多個其他的區域及結構,但是此等為 了簡單及月晰而予以省略。儘管所緣示的—平面電晶體虫 型地建立於—縣體上,但找電晶體可錢-多閘極電 曰曰體’可以疋基於不同類型的材料(諸如-第三至五族材 料)在此所述的該等接點不限於一特定類型的裝置1〇〇或 電晶體。 在該所繪示的範例中,在該電晶體上存在一第一層間 電介質(ILD)廣110。至該源極區域106及沒極區域108的 接點穿過該第-⑽層UG形成於溝射。應注意的是, 為了清晰,至該閘極1〇4的接點在此沒有予以顯示,但是 其通常是存在的。與所示及所述之至源極及汲極區域1〇6、 108之接點相似,至該閘極104的接點可用於各種實施例 中。在此所述接點不限於用於源極及汲極區域1〇6、1〇8 , 7 201034185 而是可與該閘極H)4或其他元件—起制。料接點允許 操作該電晶體,及在各種電晶體之間及在該裝置1〇〇與外 部裝置之間的電氣通訊。 在該所繪示之實施例中,該接點包括與該溝槽保形且 相鄰於該等源極及汲極區域106、1〇8的一絕緣層ιΐ4。相 鄰於該絕緣層114的是一傳導層116。該絕緣層114將該傳 導層116與該等源極及汲極區域1〇6、1〇8分離(或與該接 點所接觸的任何元件分離)。儘管該傳導層116不直接地與 該等源極及汲極區域106、1〇8相接觸,但是其仍作為一電 氣接點發揮作用。此可藉由該絕緣層114整體或部分地解 釘扎來自該半導體源極或汲極區域1〇6、1〇8的金屬費米能 階而發生。因而,在一傳導體直接地與該源極或汲極區域 106、108相接觸的情況下,若一絕緣層1丨4包含在該傳導 層116與該源極或汲極區域106、1〇8之間,則可實際上減 小該接點的電阻。在一些實施例中,此等接點可允許在低 摻雜(摻雜位準〜1 X 1017 at/cm3)矽上具有接近於】X ι〇_7 ohm-μηι2(歐姆-平方微米)或更小的一特定接點電阻率e c, 其比在相同摻雜位準之Si上的傳統矽化物接點(例如 NiSi、TiSi2、CoSi2)小5X-10X。此類型的接點也可允許按 照所期望的最佳裝置100性能,來調整該蕭特基能障高度 與接點電阻。 在該所繪示之實施例中,存在實質上填充穿過該第一 ILD層11〇之該溝槽的不由該絕緣層114及傳導體層η6 所佔據的剩餘容積的一填充材料118。該填充材料U8可以 201034185 是一金屬或其他的傳導體, 以疋另—類型的材料。在 i體不存在—分離的填充材料•而是,該傳 V體層116可實質上填充穿過 的不由該絕緣層114所佔據的剩餘容積。110之該溝槽 的Γ圖是綠示可製造第1圖所示之裝置咖的一方法 的一流程圖200。其他的方、、玄 干筋方;、 其他的實施射。在此 不範方法開始處,包括該閘 B ^ 104 /原極 10ό 及沒極 1〇8 ❿ 的该電日日體已經形成於該基 沈積搬於該電晶體上。 該第一1⑶層110 第冑疋根據本發明之_實施例,纷示沈積於該 電晶體上之該第-ILD層陶一截面側視圖。該第一⑽ 層110可使用已知地適用於積體電路結構之電介質層中的 材料(諸如低介電常數電介質材料)來形成。此等電介質材料 包括但不限於諸如二氧切(sio·氧化物、及碳摻雜氧化 物(CDO)、氛化石夕、諸如全敦環丁燒或聚四氟乙稀的有機 聚合物、氟石夕酸鹽玻璃(FSG)及諸如倍半石夕氧燒、妙氧 烷或有機矽酸鹽玻璃的有機矽酸鹽。該電介質第一 ild層 110可包括氣孔或其他空隙,以進一步減小其電介質常數。 回顧第2圖,一開口形成2〇4於該第一 ILD層11〇中。 第4圖是繪示形成204於該第一 ild層11〇中之溝样H2 的一裁面側視圖。諸如一或多個濕式或乾式蝕刻的任何適 當方法可用以形成204該等溝槽112〇如所繪示該等溝槽 112僅至該等源極及汲極區域106、108。然而,至間極1〇4 的溝槽112及接點也可予以形成,儘管其等在此沒有予以 9 201034185 特定地顯示及描述。 如第2圖所示,在該等溝槽112形成204之後,一絕 緣層114可沈積206於該等溝槽112中。第5圖是繪示沈 積於該等溝槽112中之該絕緣層114的一截面側視圖。在 一些實施例中,該絕緣層114可藉由諸如化學汽相沈積 (CVD)、原子層沈積(ALD)的一保形沈積製程予以沈積 206 ’可藉由一熱長成製程(諸如該基體材料之一氧化物、 氮化物或氮氧化物的熱長成)來形成206,或藉由另一適當 的沈積製程來形成206。該絕緣層114可包含諸如Hf〇2、 A10、ZrO、Si3N4、Si〇2、SiON或另一絕緣電介質材料的 一電介質材料。在一些實施例中,該絕緣層114的厚度被 選擇’以允許不釘扎隨後所沈積之傳導體的費米能階。在 一些實施例中,該絕緣層114可能極其薄以實現此,諸如 在各種實施例中小於大約4奈米,小於大約3奈米或大約i 奈米或更小。在一實施例中,該絕緣層114在大約5與 埃之間。也可以使用其他厚度的絕緣層114。應注魚的a 儘管該絕緣層114說明成予以保形沈積,但是此不是_、、 要條件。在一些實施例中,諸如具有一熱長成絕緣層Η* 的實施例,該絕緣層114可予以不保形地形成。 再次參照第2圖’一傳導層116沈積208於該絕緣層 114上。第6圖是繪示沈積208於該絕緣層114上的j傳導 層116的一截面側視圖。該傳導層116可藉由諸如化風士 相沈積(CVD)、原子層沈積(ALD)、無電電鍍或另—適也、、尤 積製程的一保形沈積製程予以沈積208。在一些實施例中 10 201034185 ^ ^傳導層116用以填充該等溝槽112的剩餘容 13圖是續示+ —杏 '、此一貫施例的一截面侧視圖)或該等溝槽112足 夠大的實施例中,諸如的非保形沈積技術可用以沈積 208該傳導層。
在-些實施例中,該傳導層ιΐ6可以是一金屬或包含 各種金屬可予以使用。在一些實施例中,該傳導 料1Γ材料可基於該難電晶體的—適當功函數(高功函 於PM〇S電晶體,低功函數金屬帛於-]STMOS 曰曰體其中“功函數在大約5電子伏特以上且“低”功 函數為大約3.2電子伏特歧低)來轉,儘管此並非必要 X用於該傳導層116的材料包括銘、錄、鎮、銅或其他 傳導金屬碳化物、氮化物或其他材料也可用於該傳 16。任何適當的厚度可驗該傳導層則。在一些實 施=中’該傳導層U6大於刚埃,其 該傳導層m遠遠厚於100埃。 -貫 在—些實施例中,該閘極⑽可以是遭移除的一犧牲 及在該第—ILDI11G予以沈積之後所形成的-新 在此一實施例中,該新閉極可由與形成該傳導層m 製程’且在形成該傳導層…相同時間予以形成。 在此所述之該絕緣層114及傳導層ιΐ6的形成可允許 在極其狹㈣溝槽112中形成接點。心形成切化物及 錄化物中所使狀極純金相料製程可能導致在與極其 狹窄的溝槽112 一起使用時出現的問題。因而,透過如在 此所述在絕緣雜社㈣料體,如於如果使时化 11 201034185 物或鍺化物接點,可能將該等溝槽112縮小尺寸。 再次參考第2圖,該溝槽112的剩餘容積予以填充 210。第7圖是繪示該填充材料118的一戴面侧視圖。此填 充材料118可以是一傳導材料或任何其他適當的材料,可 以是一單一材料或多個材料,且可以由任何適當的方法予 以沈積。如先前所述,在實施例中該傳導層116可填充哕 溝槽。一分離的填充材料118不用於如第13圖所綠示之此 等實施例中。 回顧第2圖,額外的ILD及傳導層可接著予以形成 _ 212。第8圖是緣示額外ILD及傳導層的一截面側視圖。在 第8圖中,該絕緣層U4、傳導層116及填充材料118予以 平坦化’以實質上與該第一 ILD層110的一頂面共平面。 在平坦化之後,至該源極區域106的溝槽112中的該傳導 層116不與至該汲極區域108的溝槽112中的該傳導層116 連續。該傳導層116可從而被認為是在該源極區域1〇6之 左側的該溝槽112中的一第一傳導層,及在該沒極區域1〇8 之右側的該溝槽中的一第二傳導層。 參 一第二ILD層120已經沈積於該第一 ild層110上。 s亥第二ILD層120中的通孔122及線124藉由該等溝槽112 中的接點傳導地連接於該等源極及汲極區域106、108。一 第二ILD層126已經沈積於該第二ILD層120上。該第三 乩〇層126中的通孔122及線124藉由該等溝槽112中的 接點傳導地連接於該等源極及汲極區域106、108。額外的 ILD層及傳導體可出現於其他實施例中。 12 201034185 第9圖是繪示一多閘極電晶體的一等角視圖。儘管第1 及3-8圖繪示了對於平面電晶體所形成的接點,但是相同 的絕緣層上傳導體接點也可用於其他類型的電晶體,諸如 二閉極電晶體。第9圖所料之該三閘極電晶體包括-韓 片13〇。在該·辖片130的任一側上存在隔離區域138。在該 ‘铸片130上存在相鄰於該韓# 130之頂部及相對側壁的-閘極電極132。在該難電極132之—側上的是—源極區域 134’且在該閘極電極132之另一側上的是一汲極區域。應 注意的是,儘管對於該等源極及汲極區域134、136,第9 圖僅具有指向朗片132之頂面的㈣,但是該等源極及 汲極區域134、136可沿著該鰭片13〇的頂面及側壁延伸。 第ίο圖是穿過該鰭片130的源極區域134部分,且繪 示忒第一 ILD層11〇的一載面側視圖,該第一 ILD層11〇 以與第3圖所示之-第-1LD層110可能形成於-平面電 晶體上相似的方式來形成。第11圖是繪示形成於該第一 ILD層11〇中之一溝槽112的一截面側視圖。該源極區域 134藉由此溝槽112而暴露。 第12圖是繪示形成於該鰭片130之該源極區域134的 頂面及側壁上的該絕緣層114、形成於該絕緣層U4上之該 傳導層116、及實質上填充該溝槽112之剩餘容積的該填充 材料118的—戴面側視圖。此等材料可與上面針對於一平 面電晶體所述相似地予以形成。因為對於該平面電晶體, 該絕緣層114將該傳導層116與該源極區域134分離,所 以相比於如果—傳導體經由穿隧與該源極區域相接觸,此 13 201034185 可允許-較低電阻的接點。而且,絕緣體ιΐ4及傳導體116 的保形沈積使該鰭片130實質上完整。如果—石夕化物緒 化物或相似接點獲得形成,則該接點將消耗該鰭片的 大量半導體材料,其可能在該韓片13〇是極小的情況下, 製成一無功能的裝置。 第14圖是緣示在同一基體1〇2上的—第—電晶體3〇2 及一第二電晶體304的一截面側視圖。電晶體3〇4具有包 含一矽化物、鍺化物等的接點3〇6,或以另外的方式具有與 該等源極及汲極區域1〇6、108相接觸的—傳導體。曲線 參 A-A表示’該等電晶體302、3〇4可相互分離,而非鄰接於 彼此。在-些實施例中,在-基體1〇2上諸如電晶體3〇2 的-些電晶體可包括具有該傳導體116的接點,該傳導體 116藉由一絕緣層114與該等源極及/或汲極區域1〇6、1〇8 — 相分離,而在同一基體上諸如電晶體3〇4的其他電晶體可 包括由-石夕化物、鍺化物或其他材料所形成,具有與該等 源極及/或汲極區域106、108相接觸之一傳導體的接點 306。例如,具有接點(其具有藉由_絕緣體114輿該等源 〇 極及汲極區域106、108相分離的_傳導體116)的電晶體 302可以是一 NMOS電晶體’而電晶體3〇4可以是一 pM〇s 電晶體’或反之亦然。在一實施例中,—基體上之一種類 型(N-型或P-型)的所有電晶體可具有一種類型的接點,而 該相反類变的所有電晶體可具有另—類型的接點。在另_ 實施例中,-些選定的電晶體可具有多個接點,該等接點 具有藉由一絕緣層114與該等源極及/或汲極區域丨〇6、川8 14 201034185
相分離的傳導體116’而該等電晶體的剩餘部分可具有較多 的傳統接點306。此等選定的電晶體可以是一種類型(N_型 或P-型),或可包括多種類型的電晶體(N-型及Ρ·型)。在其 他實施例中,一基體102上的所有電晶體可具有多個接點, 該等接點具有藉由一絕緣層114與該等源極及/或汲極區域 106、108相分離的傳導體Π6。在再—實施例中,一種類 型的一些或所有電晶體可具有絕緣、傳導及(如果可用的話) 填充層114、116、U8,與其他類型的電晶體的絕緣、傳導 及(如果可用的話)填充層114、116、118相比,其等包含不 同的材料。例如,N-型電晶體可具有包含該等絕緣、傳導 及(如果可用的話)填充層114、116、118的一第一組材料, 且同一基體102上的P-型電晶體可具有包含該等絕緣、傳 導及(如果可用的話)填充層114、116、118的一第二不同組 材料。 本發明之實施例的先前描述已經以說明及描述為目的 予以呈現。其不打算是詳盡的,或將本發明限制為所揭露 的精確形式。此描収料㈣專鄕圍在下面包括諸如 士、右、頂部、底部、在…上、在…下、上方、下方、第 -、第二等的習語’其等僅驗描述之目的且残 是限制性的。例如,表示相對垂直位置的習語是指下面的 情況:其中-基體或積體電路的一裝置側(或主動表面)在此 基體的“頂”面;該基财實際上在任何方財,使得在一 標準的參考地面座標系中—基體的―“頂,,面可低於該“底” 側,且仍在該習語“頂部”的意義卜在此所(包括在該等申 15 201034185 請專利範圍中)所使用之該習語“在…上”不表示“在”一第二 層“上”的一第一層直接地在該第二層上,及直接地與該第 二層相接觸,除非予以特定地描述;在該第一層上可能有 在該第一層與該第二層之間的一第三層或其他結構。在此 所述之一裝置或物品的實施例可以多個位置及方位予以製 造、使用或載運。在該相關技藝中具有通常知識者可理解 的是,根據上面的教示,多個修改及變化是可能的。在該 技藝中具有通常知識者將認識到的是,該等圖中所示之各 種元件的各種等效結合及替換。因而,其企圖在於本發明 之範圍不是由此詳細描述來限制,而是由附加的申請專利 範圍來限制。 I:圖式簡單說明3 第1圖是繪示具有一電氣接點之一裝置的一截面側視 圖,其中該傳導接點材料藉由一絕緣體與該正受接觸的區 域分離; 第2圖是繪示可用以製造第1圖所示之該裝置的一方 法的一流程圖; 第3圖是繪示沈積於該電晶體上之該第一 ILD層的一 截面側視圖; 第4圖是繪示形成於該第一 ILD層中之溝槽的一截面 側視圖; 第5圖是繪示沈積於該等溝槽中之該絕緣層的一截面 側視圖; 第6圖是繪示沈積於該絕緣層上之該傳導層的一截面 16 201034185 側視圖; 第7圖是繪示該填充材料的一截面側視圖; 第8圖是繪示額外的ILD及傳導層的一截面側視圖; 第9圖是繪示一多閘極電晶體的一等角視圖; 第10圖是穿過該鰭片之該源極區域部分,且繪示該第 一 ILD層的一截面側視圖; 第11圖是繪示形成於該第一 ILD層中之一溝槽的一截 面側視圖; 第12圖是繪示形成於該鰭片之該頂面及側壁上的該絕 緣層、形成於該絕緣層上的該傳導層116及實質上填充該 溝槽之剩餘容積的該填充材料的一截面側視圖; 第13圖是繪示缺乏填充材料之一實施例的一截面側視 圖;以及 第14圖是繪示在同一基體上的一第一電晶體及一第二 電晶體的一截面側視圖。 【主要元件符號說明】 100…裝置 122...通孔 102...基體 124…線 104...閘極 126·.·第三ILD層 106、134...源極區域 130...鰭片 108、136...汲極區域 132...閘極電極 110...第一層間電介質/ILD層 138…隔離區域 112...溝槽 200...流程圖 114...絕緣體/絕緣材料 302…第一電晶體 116...傳導層/傳導材料 304…第二電晶體 118...填充材料 306...接點 120...第二 ILD 層 202〜212·.·步驟 17

Claims (1)

  1. 201034185 七、申請專利範圍: 1. 一種裝置,包含: 一電晶體,其具有一源極區域及一汲極區域; 一第一層間電介質層,其相鄰於該電晶體; 一溝槽,其穿過該第一層間電介質層至該源極區 域;及 一傳導源極接點,在該溝槽中,該源極接點藉由一 絕緣層與該源極區域相分離。 2. 如申請專利範圍第1項所述之裝置,其中該電晶體是包 括一鰭片的一多閘極電晶體。 3. 如申請專利範圍第2項所述之裝置,其中該絕緣層在該 鰭片之一頂面及側壁上。 - 4. 如申請專利範圍第1項所述之裝置,其中該絕緣層具有 _ 大約4奈米或更小的一厚度。 5. 如申請專利範圍第1項所述之裝置,其更包含: 一第二層間電介質層; _ 一第一金屬化層,其相鄰於該第二層間電介質層, 且具有多個傳導通孔及多個傳導線; 一第三層間電介質層,其在該第二層間電介質層 上; 一第二金屬化層,其相鄰於該第三層間電介質層, 且具有多個傳導通孔及多個傳導線;及 其中,該第一金屬化層之該等傳導通孔及該等傳導 線中的至少一些及該第二金屬化層之該等傳導通孔及 18 201034185 該等傳導線中的至少一些,傳導地連接於該傳導源極接 點。 6. 如申請專利範圍第1項所述之裝置,其中該傳導源極接 點具有小於100奈米的一厚度。 7. 如申請專利範圍第6項所述之裝置,其更包含在該傳導 源極接點上且實質上填充該溝槽的一填充傳導體。 8. 如申請專利範圍第1項所述之裝置,其中該電晶體是一 P-型電晶體,且該傳導源極接點包含具有在大約5電子 伏特以上之一功函數的一金屬。 9. 如申請專利範圍第1項所述之裝置,其中該電晶體是一 N-型電晶體,且該傳導源極接點包含具有在大約3.2電 子伏特以下之一功函數的一金屬。 10. 如申請專利範圍第1項所述之裝置,其中該傳導源極接 點包含A1或Ni。 11. 一種製成接點的方法,包含以下步驟: 將一電介質層沈積於具有一電晶體的一基體上; 餘刻在該電介質層中延伸至一源極區域的一第一 開口; 在該源極區域上形成一絕緣體; 在該絕緣體上形成一接點金屬,該絕緣體將該接點 金屬與該源極區域相分離;及 填充實質上所有的該第一開口,其中在該第一開口 予以填充之後,該接點金屬保持與該源極區域相分離。 12. 如申請專利範圍第11項所述之方法,其中該絕緣體具 19 201034185 有大約4奈米或更小的一厚度。 13·如申請專利範圍第12項所述之方法,其中該絕緣體具 有大約1奈米或更小的一厚度。 14. 如申請專利範圍第12項所述之方法,其中形成該絕緣 體之步驟包含形成該絕緣體的一保形層。 15. 如申請專利範圍第n項所述之方法,其中該電晶體是 一多閘極電晶體,其中該絕緣體形成於該多閘極電晶體 之一 ·鰭片的一頂部上及側雙上,以產生一絕緣體頂部及 絕緣體側壁,且其中該接點金屬形成於該絕緣體頂部上 及該等絕緣體側壁上。 16. —種裝置,包含: 一電晶體,其具有一源極區域及一没極區域; 一源極接點,其中該源極接點不直接地相鄰於該源 極區域,且其中一第一絕緣層將該源極接點與該源極區 域相分離;及 一汲極接點,其中該汲極接點不直接地相鄰於該汲 極區域’且其中一第二絕緣層將該汲極接點與該汲極區 域相分離。 17. 如申請專利範圍第16項所述之裝置,其中該電晶體是 一多閘極電晶體,該源極區域具有一頂部及側壁,且該 沒極區域具有一頂部及側壁。 18. 如申請專利範圍第μ項所述之裝置,其中該源極接點 及該汲極接點都不包含一石夕化物。 19. 如申請專利範圍第16項所述之裝置,其中該第一及第 20 201034185 二絕緣層包含ΗίΌ2。 20.如申請專利範圍第16項所述之裝置,其中該電晶體具 有包令—第三至五族材料的一通道區域。
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US8110877B2 (en) 2008-12-19 2012-02-07 Intel Corporation Metal-insulator-semiconductor tunneling contacts having an insulative layer disposed between source/drain contacts and source/drain regions
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