TWI362747B - Semiconductor device edge termination structure and method - Google Patents
Semiconductor device edge termination structure and method Download PDFInfo
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- TWI362747B TWI362747B TW094140266A TW94140266A TWI362747B TW I362747 B TWI362747 B TW I362747B TW 094140266 A TW094140266 A TW 094140266A TW 94140266 A TW94140266 A TW 94140266A TW I362747 B TWI362747 B TW I362747B
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- semiconductor layer
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Classifications
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- H01L29/41725—Source or drain electrodes for field effect devices
- H01L29/41766—Source or drain electrodes for field effect devices with at least part of the source or drain electrode having contact below the semiconductor surface, e.g. the source or drain electrode formed at least partially in a groove or with inclusions of conductor inside the semiconductor
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- H01L29/423—Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions not carrying the current to be rectified, amplified or switched
- H01L29/42312—Gate electrodes for field effect devices
- H01L29/42316—Gate electrodes for field effect devices for field-effect transistors
- H01L29/4232—Gate electrodes for field effect devices for field-effect transistors with insulated gate
- H01L29/42372—Gate electrodes for field effect devices for field-effect transistors with insulated gate characterised by the conducting layer, e.g. the length, the sectional shape or the lay-out
- H01L29/42376—Gate electrodes for field effect devices for field-effect transistors with insulated gate characterised by the conducting layer, e.g. the length, the sectional shape or the lay-out characterised by the length or the sectional shape
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Description
1362747 九、發明說明: 【發明所屬之技術領域】 本發明一般有關半導體裝置,尤其有關功率切換裝置及 其製造方法》 【先前技術】 金氧半導體場效電晶體(MOSFET)為常見的功率切換裝 置類型^ MOSFET裝置包括:源極區域、汲極區域、在源 極區域及汲極區域之間延伸的通道區域、及鄰接通道區域 提供的閘極結構。閘極結構包括布置鄰接通道區域且和通 道區域以介電薄層隔開的導電閘極層。 當MOSFET裝置在開啟狀態中,會對閘極結構施加電壓 以在源極區域及汲極區域之間形成傳導通道區域,讓電流 流動通過裝置。在關閉狀態中,對閘極結構所施加的任何 電厘將低到使傳導通道無法形成,因而無法形成電流。在 關閉狀態期間,裝置必須支援源極區域及汲極區域之間的 向壓。 【發明内容】 有兩個主要參數駕馭今日的高壓功率開關市場:崩潰電 壓(BVdss)與開啟狀態電阻(Rds〇n)。對於特定應用而言, 需要使用最小崩潰電壓,而實際上,設計者通常能夠達成 dSS規格的要求。然而’這通常會犧牲Rdson。對高磨功 率刀換裝置的製造者及使用者而言’此效能上的權衡是主 要的設計挑戰。 L來為了改進Rdson及BVdss間的權衡,超接合裝置漸 106084.doc 1362747 獲重視。在習用的n通道超接合裝置中,多個高濃度推雜 之擴散的η型及p型區域取代一個輕微摻雜的η型蟲晶區 域。在開啟狀態中,電流流動通過高濃度摻雜的η型區 域,因而降低Rds〇n ^在關閉狀態或閉鎖狀態中,高濃卢 摻雜的n型及P型區域彼此耗盡或彼此補償以提供高 BVdss。雖然超接合裝置的前景看好,但在製造時仍有重 大挑戰。 目前高壓功率切換產品的另一個問題是其通常需要大量 輸入(如,閘極或控制電極)電荷,以從_個狀態切換至= -個狀態。除了別的以夕卜,此需求對於周邊控制電路造成 額外負擔。 因此,需要高壓功率切換裝置結構及其製造方法,以提 供較低的Rdson、高B Vdss並減少輸入電荷。 【實施方式】 為了便於瞭解’圖式中的元件未必按比例繪製,及所有 不同圖式中視需要使用相同的元件。儘管下文說明η通道 裝置,但本發明亦有關藉由顛倒所述薄層及區域之導電率 類型來形成的ρ通道裝置。 此外,本發明的裝置可執行蜂巢式設計(其中本體區域 為複數個蜂巢式區域)或單—本體設計(其中本體區域由按 通常為蛇形圖案之伸長圖案形成的單—區域组成”缺 而,為便於瞭解’在整個說明中皆將本發明之裝置說明為 =式設計。應明自’本發明希望既包括锋巢式設計又包 括單一的基本設計。 106084.doc 1362747 圖1顯示根據本發明之絕緣閘極場效電晶體(IGFET)、 MOSFET、超接合裝置或切換裝置或單元1〇的局部放大橫 截面圖。舉例而言’裝置10係屬於在半導體晶片中整合邏 輯組件及/或其他組件作為功率積體電路之部分的許多此 類裝置。或者,裝置10屬於啓A —扣丨、,π上& 躅於蹩σ起以形成離散電晶體裝 置的許多此類裝置。 裝置1G包括半導體材料11的區域,該區域包含如具有範 #圍介於約0·001至約0·0〇5 0hm-cm之電阻率的η型石夕基板12 並可以石申進行摻雜。在所示的具體實施例中,基板12提供 沒極接觸。半導體層14係形成於基板12中或形成於其上, 且根據本發明為輕微摻雜的η型或?型或含有極少量的雜質 (即,為本質半導體層)。在示範性具體實施例中,半導體 層14係使用&用的磊晶生長技術來形成。在適於伏特 裝置的不範性具體實施例中,半導體層14為摻雜物濃度約 1·0χ10η atoms/cm3至約 5 〇χ1〇〗3 at〇ms/cm3 的 ρ型具有等 φ 級約40微米的厚度。半導體層14的厚度隨著裝置10的所需 BVdss額定值而增加或減少。應明白,半導體材料u的本 體或其部分可使用其他材料,包括矽_鍺、矽_鍺_碳、摻雜 碳的矽或其類似物。 裝置10亦包括形成於半導體材料u之區域之上表面或主 表面18中或與其鄰接的η型區域或毯狀層17» N型區域17提 供裝置1 〇低電阻電流路徑,其詳細說明如下◦在示範性具 體實施例中’ η型區域17具有最大濃度等級約6 〇χ1〇〗6 atoms/cm3及深度約0 4微米。視情況,ρ型區域或毯狀層19 106084.doc 1362747 係形成於主表面18之中或與其鄰接,且在n型區域η之下 或與其鄰接βΡ型區域19對„型區域17及半導體層Μ間的pn 接合面提供較佳控制,且在完全耗盡條件下提供η型區域 17電荷補償。在示範性具體實施例中,p型區域19具有表 面浪度約5.(^1〇丨5以011^/(;1113及深度約〇8微米。 根據本發明,裝置10進一步包括填充溝渠、半導體材料 填充溝渠、蟲晶填充區域或溝渠、電荷補償溝渠區域、深 鲁溝式電,補償區域、電荷補償填充溝渠或電荷補償區域 電荷補償填充溝渠22包括複數個層或多個半導體材料 層,其包括相反導電率類型的層,其較佳是以本質或緩衝 半導體層來隔開。除了別的以外,本質層作用可防止混合 相反導電率類型的層(即,兩個電荷層),因這在開啟狀態 中,對裝置10的傳導效率有不利的影響。 在示範性具體實施例中,填充溝渠22包括使用磊晶生長 技術形碑之多個層或堆疊的半導體材料層。例如,填充溝 • 渠22包括形成於鄰接半導體材料11之本體之溝渠壁面或表 面上、或其上方、或和其鄰接的η型層23。本質半導體或 緩衝層24係形成於η型層23上、或其上方、或和其鄰接,ρ 型層26係形成於本質半導體層24上、或其上方、或和其鄰 接’及本質半導·體或緩衝層27係形成於ρ型層26上、或其 上方、或和其鄰接。除了別的以外,本質層24作用可防止 混合薄層23及26,其如先前所述,改良裝置1〇的傳導效 率。除了別的以外,本質層27作用可填充其餘溝渠。對於 η通道裝置及根據本發明’ η型層23在裝置1〇處於開啟狀熊 I06084.doc 1362747 時提供通道至沒極的主要垂直低電阻電流路徑。當裝置ι〇 處於關閉狀態時,根據本發明,n型層23及p型層Μ彼此補 償,以提供增加的BVdss特性。應明白.,可使用附加的η型 層及pf_層,且較佳疋以附加的本質層或缓衝層隔開。 舉例而έ,η型層23及p型層26各具有摻雜物濃度等級約 2.0x10至約4·0χ10ΐ6 at〇ms/cm3及各具有厚度約微米至 約0.3微米。在示範性具體實施例中,本質半導體或緩衝 層24及27為未摻雜或極輕微推雜的㈣,其榜雜物濃度低 於約2.0x1〇m at〇ms/cm3,及各具有厚度約〇 $微求至約以 微米。調整本質層27的厚度以如填充溝渠的剩餘部分。 在填充溝渠22間及在其附近或和其鄰接,本體或摻雜區 域31係形成於半導體層14中,並自主表面18延伸。在示範 拴具體貫施例中,本體區域31包含卩型導電率,具有適於 形成操作為裝置10之傳導通道45之反向層的摻雜物濃度, 其說明如下。本體區域31自主表面18延伸至深度約10至 φ 約5,0微米。η型源極區誠33係於本體區域3〗内或其中形 成且自主表面18延伸至深度約〇.2微米至約〇5微米。ρ型 本體接觸或接觸區域36亦形成於本體區域31中,並提供較 低接觸電阻至主表面18的本體區域31。此外,接觸區域% 可降低源極區域33下之本體區域31的薄片電阻,以抑制寄 生雙極效應。 第一介電層41係形成於主表面18的部分之上或與其鄰 接。在示範性具體實施例中,介電層41包含具有厚度約 〇·1微米至約0.2微米的熱氧化層。第二介電層42係形成於 J06084.doc 1362747 介電層41之上。在示範性具體實施例中,第二介電層包 含氮化石夕,具有厚度約〇丨微米。 閘極介電層43俾形於主表.面18鄰接本體區域31的其他部 分之上或與其鄰接。在示範性具體實施例中,閘極介電層 43包含氧化矽,具有厚度約〇〇5微米至約〇」微米。在替代 性具體實施例中,閘極介電層43包含:氮化矽、五氧化 钽、二氧化鈦、鈦酸鳃鋇、或其組合(包括氧化矽之組合) 或其類似物。 σ _ 根據本發明的-項具體實施例,摻雜的多晶半導體層、 導電層、或接地平面層46係形成於介電層41及42之上,且 透過形成於介電層41及42的開口 47接觸?型層26。在示範 性:體實施例中’導電層46包含多晶石夕層,具有厚度約 0.1微米,且具有η通道裝置的卩型導電率。在進行熱處理 時,導電層46的ρ型摻雜物擴散至填充溝渠22以形成ρ型摻 雜區域52,因而強化ρ型層26的歐姆接觸。在替代性具體 籲實施例中,導電層46包含非晶石夕 '金屬、石夕化物、或其中 包括多晶石夕之組合的組合。如果導電層46使用金屬,則先 透過開口 47植入或沉積ρ型摻雜物以形成ρ型摻雜區域, 以強化Ρ型層26層的歐姆接觸。導電層“較佳是直接或間 接地連結或耦合至導電接觸或源極接觸層〇,如圖」所 示0 根據本發明,除了別的以外,導電層46可作為接地平 I 、决速且有效地提供要自裝置清除或清除於裝置外之 少數載子的路徑,以減少切換裝置1〇從一個狀態至另—個 I06084.doc 1362747 狀態所需的輸入電荷及提高切換速度。另外,如下文詳細 說明,另外使用導電層46作為根據本發明之邊緣终止結構 的部分。 第三介電層48係形成於導電層46之上,及第四介電層” 係形成於第三介電層48之上。在示範性具體實施例中,介 電層48包含氮化石夕(如,厚度約〇 ()5微米),及介電層^包 含沉積氧化梦(如,厚度約〇 7微米導電層53係形成於介 電曰之上且包含如n型多晶矽(如,厚度約〇 3微米)。 >導電間隔物閉極區域、垂直間隔物間極區域、或間隔物 定義閘極區域57係形成於閘極介電層43之上,並以介電質 間隔物59而和導電層46隔離。導電間隔物閘極區域57連同 閘極介電層43形成控制電極或閘極結構58 d導電間隔物閉 極區域57包含如n型多晶矽,厚度約〇 8微米。在示範性具 體實施例中,介電質間隔物59包含氮化石夕,厚度約〇」微 米。間隔物閘極區域57係耦合至導電層53以提供導電閘極 結構,以在裝置10中控制通道45的形成及電流的傳導。在 所不的具體實施例中,導電連接部分77將間隔物開極區域 5、7耦合至導電層53。導電連接部分77包含如η型多晶矽。 間隔物閘極區域是指以在一表面上之沉積閘極材料形成的 控制電極,以控制在另一垂直表面上形成的通道。至於裝 置1〇,通道45係形成於視為水平表面的表面18。用以形成 間隔物閘極區域57的控制電極薄膜係沿著和表面18垂直的 垂直表面68沉積。 根據本發明的導電間隔物閘極區域57和習用的裝置相 106084.doc …‘/4/ :’提供最小的閘極至汲極重疊’藉此大幅減少閘極電 仃另外,在裝置ίο中,由高出主表面18上的導電層”提 供閘極的電選路,藉此進-步減少閘極電荷。此外,除了 別的以外,導電層46可作為***於閘極及沒極區域間的接 地平面,以進一#減少間極至沒極電容。本發明的這些特 色可%高切換速度及減少輸入電荷需求。 第五介電層6】係形成於裝置1〇的部分之上且包含如具 魯有厚度約G.G5微米的氮化碎。層間介電(助)層62係形成 於裝置10的部分之上’且包含如具有厚度約〇 8微米的沉 積氧化石夕。在介電層中形成開口以提供源極接觸層63對裝 置1〇的接觸。如圖所示,钱刻主表面㈣部分,致使源極 接觸層63接觸源極區域33及本體區域%。在示範性具體實 施例中,源極接觸層63包含紹石夕合金或其類似物。沒極接 觸層66係形成於半導體材料u之區域的相對表面,且包含 如可焊接的金屬結構,如鈕_鎳_銀、鉻_鎳_金或其類似 物。 裝置10的操作說明如下。假設源極終端63操作於零伏特 的電位Vs,間隔物閘極區域57接收大於裝置1〇之傳導臨限 值的控制電壓VG = 5.〇伏特,及汲極終端66操作於沒極電位 VD 5.0伏特。VdVs的值導致本體區域31在間隔物開極區 域57下反向,以形成使源極區域%電連接至層17的通道 45。裝置電流is流自源極終端63並透過源極區域33、通道 45層17、n型層23選路至汲極終端66。因此,電流“垂 直地流動通過n型層23 ,以產生低導通電阻。在一項具體 106084.doc *14- 1362747 實施例中’ Is=l.〇安培。要將裝置10切換至關閉狀態,將 小於裝置之傳導臨限值的控制電壓VG施加於間隔物閘極 57(如’ VG<5.0伏特)。這將移除通道45,Is不再流動通過 裝置10,且導電層46將少數載子清除於裝置外。在關閉狀 匕、中’ η型層23及p型層26彼此補償為主要阻擋接合面散布 耗盡區域,以提高BVdss。在一項具體實施例中,在半 導體層14為η型時,由本體區域31及半導體層〗4形成主要 φ 阻擋接合面。在另一項具體實施例中,在半導體層“為卩 型時’由半導體層14及基板12形成主要阻擋接合面。 現在參考圖2-7說明形成根據本發明之裝置1〇的程序。 圖2顯示裝置10在初期製造階段的局部放大橫截面圖。在 初期步驟’介電層40係形成於主表面18之上,及透過介電 層40將選擇性ρ型區域19離子植入半導體層14。在示範性 具體貫施例中,以劑量約5.0x10" atoms/cm2及植入能量 600 KeV植入硼以形成p型層19。接著,透過介電層40將η • 型層1 7離子植入半導體層14。在示範性具體實施例中,以 劑量約2.OxlO】2 atoms/cm2及植入能量6〇〇 KeV植入磷以形 成η型層17。 然後,在主表面18之上形成及圖案化遮罩層71以形成開 口 72。然後,使用習用的技術蝕刻介電層4〇,以透過開口 72曝露半導體材料11之本體的部分。舉例而言,開口 72具 有等級約3.0微米至約5.0微米的寬度74。接著,透過層 1 7、19、及14餘刻溝渠122。在示範性具體實施例中,溝 渠122延伸至基板12的至少一部分。溝渠122的深度係由半 106084.doc -15· 1362747 導體層14的厚度(為BVdss的函數)決定。在示範性具體實 施例中’使用以氟或氯為主之化學物蝕刻的深反應性離子 蝕刻(DRIE)形成溝渠122。DRIE#刻可使用若干技術包 括低溫、高密度電漿、或B〇sch DRIE處理。在示範性具體 實施例中,溝渠122具有實質上為垂直的側壁。在替代性 具體實施例中,溝渠122具有溝渠在溝渠下表面的寬度小 於寬度74的倒錐形輪廓。在使用習用的蝕刻技術形成溝渠 122後移除遮罩層71。雖然說明溝渠122為複數,但應明 白,溝渠122可以是單一連續溝渠或連接的溝渠矩陣(如圖 ίο所不,其說明如下)。或者,溝渠122可以是複數個具有 封閉末端及以半導體材料丨丨之本體之部分隔開的個別溝 渠。 圖3顯不裝置1〇在進一步處理階段的局部放大橫戴面 圖。此時,如形成填充溝渠22的第一階段,在溝渠122中 形成、生長或沉積半導體材料層。在示範性具體實施例 中,使用半導體磊晶生長技術來填充溝渠丨22。 在第一步驟,在溝渠122的側壁上形成薄的熱氧化物, 以移除因DRIE步驟所損壞的任何表面。然後,使用習用 的各向同性蝕刻技術移除薄的熱氧化物。接著,如磊晶生 長程序的第一步驟,將半導體材料丨丨的本體置入磊晶生長 反應器並進行預清洗。當填充層(如,層23、、%及27) 的所選半導體材料是矽時,如smci3、SiH2Cl2、siH4或 Si2%的矽來源氣體適於形成這些層。在所示的具體實施 例中,生長毯狀層(即’除了溝渠122之外,在主表面18之 106084.doc 1362747 ^長:這些層卜在替代性具體實施例中,使用選擇的 猫曰曰生長技術以形成層23、24、26及27,致使這 在介電層40之上形成。 —不0 :沿著溝渠m的表面生長N型層23,以坤為合適的摻雜 =源。在示範性具體實施例中,n型層23具有摻雜物濃 二:約2.GX1G16至約4.GX1G丨6 at()ms/em3,及厚度約〇」微 米至約0.3微米。 接著,在η型層23之上生長本質或緩衝層“,其未經摻 "通常在先前生長步驟後留在反應器隔室中之矽來 源材料及/或殘餘摻雜物氣體中出現的這些微量雜質之 外),或為摻雜物濃度低於約2加〇】4 at〇msW的輕微捧 雜P型。層24具有厚度約〇·5微米至約1〇微米。然後,在層 24之上生長p型層26,明摻雜物來源為合適的摻雜物^ 源。在示範性具體實施例中,p型層26 約〇·3微米。然後在?型層26之上生長本質或緩衝層η, 其未經摻雜(除了通常在先前生長步驟後留在反應器隔室 中之石夕來源材料及/或殘餘摻雜物氣體中出現的這些微量 雜質之外),或為摻雜物濃度低於約2 〇χ1〇Μ at〇ms/cm3的 輕微掺雜p型。層27具有厚度約〇·5微米至I 〇微米。應明 白,將根據溝渠122的寬度來調整層23、24、26及27的厚 度。在不範性具體實施例中’這些層的厚度將使所形成的 蟲晶層填滿溝渠122。當使用毯狀蟲晶生長程序時,其後 以化學機械拋光技術、回触技術、其組合或其類似物平坦 106084.doc 1362747 化層27、26、24及23。在平坦化程序中,將磊晶層27、 26、24及23向下或往回平坦化至主表面18,以形成填充溝 渠22 »在示範性具體實施例中,平坦化程序亦移除介電層 40。可使用附加的蝕刻步驟,以進一步移除層4〇的任何殘 餘介電材料。如果使用選擇的磊晶生長或選擇的回蝕技 術,介電層40可留下並將取代層41,其說明如下。 圖4顯示裝置1〇在進一步處理後的局部放大橫截面圖。 第一介電層41係形成於主表面18之上,且包含如氧化矽約 0.1微米至約0.2微米厚。生長於攝氏75〇度的熱氧化物將為 合適的熱氧化物。在選擇性步驟,使用濺鍍蝕刻步驟讓第 一介電層41的上表面或曝露表面光滑。接著,第二介電層 42係形成於介電質41之上,且包含如約〇1微米的氮化 石夕。然後,使用接觸微影钱刻及钱刻步驟以形成通過第二 介電層42及第一介電層41的開口 47。這將曝露主表面以在 填充溝渠22之上的部分,如圖4所示。在示範性具體實施 • 例中,開口47具有等級約〇.5微米至約1〇微米的寬度49。 然後,導電層46係形成於第二介電層42之上,並透過開 口 47接觸或耦合至填充溝渠22。在示範性具體實施例中, 導電層46包含約(M微米的多晶矽’且為沉積摻雜或未摻 雜。如果初始沉積導電層46時並未摻雜,則其後使用如離 子植入技術摻雜導電層46 ^在此示範性具體實施例中,以 硼摻雜導電層46,以提供p型層26的接觸。硼離子植入劑 量約5.0x10”至約i.ouW at〇ms/cm2及植入能量約μ 將足以摻雜導電層26»在後續的熱處理步驟,導電層“的 -1S- 106084.doc 1362747 摻雜物擴散至填充溝渠22以形成p型區域52。 接著’第三介電層48係形成於導電層46之上,及第四介 電層51係形成於第三介電層48之上。第三介電層48包含如 氮化矽(如,厚度約〇.〇5微米),及介電層51包含沉積氧化 矽(如’厚度約〇·7微米)。然後,導電層53係形成於第四介 電層51之上’且包含如^型多晶矽(如,厚度約〇3微米)。 電層54係形成於導電層53之上,且包含如約〇15微米的 氮化石夕。 ® 執行微影蝕刻及蝕刻步驟以蝕刻通過層54、53、5!、 48、46及42的部分,以提供開口 7(^這亦形成基座堆疊結 構56 ’其包含層42、46、48、51、53及54的部分。在示範 性具體實施例中,開口 70具有等級約5.〇微米至約8〇微米 的寬度73。 圖5顯示裝置1〇在形成介電質間隔物59之附加處理步驟 後的局部放大橫截面圖。在示範性具體實施例中,在基座 φ 堆疊結構56及第一介電層41之上沉積氮化矽薄膜。舉例而 言,使用化學汽相沉積技術沉積約0>1微米厚的氮化矽薄 膜。接著,使用習用的各向異性回蝕步驟移除氮化矽層在 基座堆疊結構56及第一介電層41之上的部分,並留下氣化 石夕層在基座堆疊結構56之側壁或垂直表面68上的部分,以 形成介電質間隔物59。 然後,使用氧化矽濕式蝕刻來移除介電層41在開口 内 的部分。舉例而言,使用稀釋的氫氟酸(如,5〇:ι)來蝕刻 介電層41。在示範性具體實施例中,延長蝕刻時間(如,\ 106084.doc •19· 1362747 至15分鐘)以從介電質間隔物59下底切或移除介電層41的 材料,以形成凹陷部分74。凹陷的介電層41依此方式確保 在本體區域31中形成的通道45(如圖1所示)延伸至層17,以 允許通道電流更有效地流動。在示範性具體實施例中,部 分74在介電質間隔物59之下凹陷距離約〇1微米。然後, 在開口 70内的主表面丨8上生長熱氧化矽至厚度約〇 〇8微 米,以形成間極介電層43 »
圖6顯示裝置〗〇在進一步處理後的局部放大橫截面圖。 在裝置10之上沉積半導體材料的保形層至厚度約〇丨微米 至約0.15微球。然後,透過開口 7〇及半導體材料的保形層 將删摻雜物引進主表面18,以提供本體區域31心型擦雜 物。在示範性具體實施例中,半導體材料的保形層包含未 摻雜的多晶石夕,及硼係透過未播雜的多晶石夕植入層η。離 子植入劑量約LOUOn at〇ms/cm2及植入能量約ΐ6〇 μ適 於650伏特裝置。在植入步驟後,使用清洗或姓刻程序以 清洗半導體材料之保形層的表面。 然後,在第一保形層之上沉積_導體材料的第二保形 層’並蝕刻此二層以提供間隔物閘極57。在示範性具體實 ,例中導體材料的第二保形層包含約〇.8微米的^型多 在沉積料中進行摻誠在其後❹離子植入 =他摻雜技術進行摻雜。在形成間隔物間 的表面上加入附加之0.015微米的開極介電質 (° ’氧切)並曝露間極氧化物43的部分。 、 在示範性具體實施例中,钱刻步驟曝露介電層“及介電 I06084.doc /4/ 質間隔物59的上古如八 。刀然後,钱刻保護層5 4及介電質間 隔物59的上方部公wy 丨电貝间 移除保護層54,及在間隔物閘極57與 導電層53之間移除介電質間隔物的上方部分。 在進纟的步肆,沉積如多晶石夕的導電材料’以提供連 接導電部分77。連接導電部分77使間隔物閘極57耦合至或 電連接^電層53。然後,執行n型摻雜步驟以摻雜連接 f電部分77及以提供源極區域33的摻雜物。在示範性具體 貫施例中’此摻雜步驟使料植人劑量3.0xlG15 at〇ms/cm2 及植入能量80 。 圖7顯不裝置1G在進—步製造步驟後的局部放大橫截面 圖’儿積第五介電層61,其包含如約〇 〇5微米的氮化矽。 =後’在第五介電層61之上沉積肋層62。在示範性具體 貫施例中ILE)層62包含沉積氧化石夕厚度約〇 8微求。使用 選擇性ILD錐形物㈣使IU^62的部分心成錐形,這有 助於其後所形成層的階梯覆蓋率。 接者’使用習用的微影蝕刻及蝕刻步驟以形成接觸開口 81 ’其將曝露主表面18的部分,,透過開口 8ι,使用 P5L離子植入步驟形成接觸區域36。舉例而言,使用硼離 子植入劑量3.(^1〇】、_/(^2及植入能量8〇0。然後, 沉積及钱刻等形間隔物層,以形成間隔物82。纟示範性具 體實施例中,沉積及姓刻0.3微米的氮化石夕層,以形成間 隔物82。此時使用快速退火步驟以活化及擴散各種離子植 入。例如,曝露裝置10於溫度約攝氏1〇3〇度約45秒。 然後,使用蝕刻步驟以移除主表面18的部分,以形成凹 106084.doc 1362747 陷部分84。运允許源極接觸層63接觸源極區域33及接觸區 域36,以使這些區域一起短路。然後,移除間隔物82。在 後續處理中,沉積及圖案化源極接觸層63。然後,視情況 薄化基板12,及沉積汲極接觸層66,以提供圖丨所示的結 構。雖然在圖2-7中未顯示,但在所述製造階段中可使用 微影㈣及姓刻步驟,例如,在圖4·6中㈣露導電層Μ 的部分,以提供源極接觸區域63耦合至導電層46的開口, φ 如®1所*。此外,應日月白,在沉積源極接觸層63之前可 形成其他導電層,如石夕化物層。 圖8為描繪根據本發明及根據本文所述處理參數之裝置 1〇之崩潰電壓(BVdss)特性的曲線圖。如圖8所示,裝置ι〇 呈現汲極及源極的標稱崩潰電壓約75〇伏特。另外,如圖名 所示,裝置進-步呈現在崩潰之下的低洩漏。 圖9為描繪根據本發明及根據本文所述處理參數之裝置 10之開啟狀態電阻(RdSon)特性的曲線圖。和習用之具相 •似BVdss的超接合裝置相比,裝置10呈現極佳的Rds〇n特 性,其具有等級36 mUli-ohm Cm2的典型Rds〇n值。 圖10顯示適於根據本發明之裝置1〇之單元結構3〇〇的局 部放大橫截面圖。根據本發明的一項具體實施例,顯示單 元結構300具有圍繞半導體層14之複數個多角形區域314的 填充溝渠322,其中形成主動裝置或單元。應明白,多角 形區域具有圓角,及應明白’包括圓形、方形、矩形或其 類似物的其他形狀為合適的形狀。蜂巢結構3〇〇的一個特 色是其提供用於高封裝密度,以改良Rdson及電流載送能1 I06084.doc •22· 1362747 力。根據本發明,填充溝渠322包括η型層23、本質層24與 27、及Ρ型層26。 圖11為裝置10之另一部分的局部放大橫截面圖,其顯示 根據本發明的選擇性邊緣终止結構1〇〇。終止結構1〇〇的特 色之一是其併入裝置1〇的基本組件,因而節省了處理成 本。終止結構100包括導電接觸層或導電半導體層、146,其 係形成於主表面18之上且與其鄰接。在示範性具體實施例 中導電接觸半導體層140包含和導電層46相同的材料且 係同時形成。例如,導電接觸半導體層146包含ρ型多晶 矽。在熱處理後,ρ型摻雜物從導電接觸半導體層146擴散 以形成Ρ型摻雜層.152,其反向摻雜η型肩17及耦合至選擇 性Ρ型層19。圓丨丨進一步顯示透過開口 91而耦合至源極接 觸層63的導電接觸半導體層丨46。 隔離溝渠103係形成於裝置1〇的周邊,且包含如以介電 材料1〇8填充的蝕刻溝渠1〇6。視情況’先形成熱氧化層 110以排列隔離溝渠1〇3的側壁及/或下表面。 在替代性具體實施例中及如圖丨丨所示’隔離溝渠103進 一步包括和填充溝渠22同時形成的半導體材料層。舉例而 吕,半導體材料層包括:如參考圖1所述的η型層23、本質 或緩衝層24、ρ型層26、及本y或緩衝層27。如果不使用 半導體材料層’則在製S中和填充溝渠22分開形成溝渠 106 ° 在不範性具體實施例中,介電材料1〇8包含使用旋塗式 玻璃(SOG)、BPSG、PSG及/或丁咖沉積技術形成的氧 106084.doc •23· 1362747 化石夕。在形成氧化物後,使用回银或化學機械平坦化技 t、其組合、或其類似物平坦化介電區域的上表面。在示 範性具體實施例中’溝渠刚具有寬度約观米至約_微 未,且係使用和形成參考圖2所述之溝渠〗22所用技術的類 似技術來形成。溝渠106的側壁實質上為垂直、或為倒錐 形,致使溝渠H)6之底部的寬度小於溝渠1〇6之頂部的寬 度。舉例而言,介電材料108及/或介電層110延伸至半導 體層14下的深度或距離,如圖11所示。 在包括層23、24、26、27及隔離溝渠1G3的替代性且體 實施例中,將η型區域109併入溝渠1〇6下的基板12,.以減 少和晶粒分割相關聯的任何電流洩漏。 根據本發明,當半導體層14包含ρ型導電率時,则㈣ 主要接合面為半導體層14及„型基板12所形成的ρη接合面 14此特色可簡化邊緣終止結構100並可節省空間。例 如’習用裝置需要距離約終止結構之蟲晶層的厚度m 倍。在本發明中,此距離將減為約此厚度的·ι/2χ倍。 在此具體實施例中,接合面114比在習用裝置中的接合 面^平’因接合面從基板12耗盡,而非從本體區域31向下 及橫跨耗盡。此外’由於導電接觸半導體層146係透過摻 雜區域152及19而搞合至半導體層14,因此接合面u4橫向 U申至|置10的邊緣。依此方式’得以最佳化達成 最佳化平面接合。除了別的以外,隔離溝渠1〇3作用可鈍 化接合面114。 頁示根據本發明之替代性溝渠隔離2〇3的局部放大 106084.doc -24- 1362747 俯視圖。區域131代表裝置则於參考圖u所述之終止結 構的部分’及區域132代表裝置1G用於圖W述之主動結構 的部分。當姓刻隔離溝渠203時,該隔離溝渠包括所形成 之複數個柱狀矩陣或形狀117。在示範性具體實施例中, 鄰接列的形狀ι17為相對於彼此偏移,如圖12所示,致使 开7狀117彼此實|上為等距離。在示範性具體實施例中, 柱狀物11 7相隔約5微米至約丨5微米。
舉例而言,形狀117為半導體材料u之本體之部分的柱 狀物或區域。在示範性具體實施例中,形狀117包含:基 板12、半導體層14、p型層19、n型層17及介電層“,且具 有寬度或直徑約0.8微米至社^微米。這如_清楚所 不’圖13為沿著圖12之參考線13_13截取之隔離溝渠加之
部分的放大橫截面圖 離 H /|叮月,』的隔 溝渠203。使用習用的微影蝕刻及蝕刻技術以形成溝渠 206及形狀117。例如 DRIE。 使用以氟或氯為主之化學物的 在形成溝渠206及形狀117後,形成介電層21〇,如圖14 =示。舉例而言,介電層21〇包含熱生長的氧化矽。接 著’沉積及平坦化介電層208。在示範性具體實施例中, 介電層208包含旋塗式玻璃。根據本發明,形狀ιΐ7在沉積 介電層208時減少碟化效應,因而提供更平坦的表面、較 佳鈍化、及更可靠的裝置。形狀117可為圓形、方形、矩 形' 多邊形、梯形、橢圓形、三角形、其組合或其類似 物。這些形狀可進一步包括圓角。 106084.doc •25- 1362747 圖15顯示鄰接或複數個隔離溝渠2〇3a&2〇3b的局部放大 仏截面圖,如兩個以劃分格柵或區域461隔開之裝置的部 刀所示。在此具體實施例中’半導體晶圓上的鄰接裝置1 〇 包括劃分格栅461 ’其包含半導體材料U的本體,而非在 鄰接晶粒間為連續的介電材料208及210。這允許如切割機 的晶粒分割裝置晶粒沿著中線463分割,以提供更強健的 晶粒分割。 〜之’已說明具有深溝式電荷補償的新型切換裝置結 構,包括其製造方法。還有,也已說明適於本發明之裝置 及八他半導體裝置的接地平面結構。此外,還說明適於本 發明之裝置及其他半導體裝置的邊緣終止結構。 雖Λ、;、本發明已參考其特定具體實施例加以說明及解說, 但是不希望本發明限於該等解說性具體實施例。熟習此項 技術者應明白,可進行修改與變更而不背離本發明之精 神。因此,本發明係有意涵蓋符合隨附申請專利範圍之所 有該等變更及修改。 【圖式簡單說明】 圖1說明根據本發明之切換裝置的局部放大橫截面圖; 圖2 - 7說明圖1之切換裝置在各種製造階段的局部放大橫 截面圖; 圖8為顯示圖1之切換裝置之崩潰電壓特性的曲線圖; 圖9為顯示圖1之切換裝置之開啟狀態電阻特性的曲線 圖; 圖10說明適於根據本發明之切換裝置之蜂巢結構的局部 106084.doc •26- 1362747 放大俯視圖; 圖π說明本發明之切換裝置及邊緣終止結構之放大的局 部橫截面圖; ° 圖12說明根據本發明之替代性溝渠隔離結構的局部放大 俯視圖; 圖13說明圖12之沿著參考線13_13截取之溝渠隔離結構 在初期製造階段的局部放大橫截面圖; 、°
圖14說明圖13之結構在進一步處理後的局 圖;及 %戴面 圖15說明根據本發明之進一步溝渠隔離結構的局部放 橫截面圖。 【主要元件符號說明】
10 11 12 14 17 18 19 22 23 24 ' 27 26 31 切換裝置 半導體材料 矽基板 半導體層 η型區域 主表面 Ρ型區域 電荷補償填充溝渠 η型層 本質層 Ρ型層 本體區域 106084.doc 27- 1362747 η
33 源極區域 36 接觸區域 40 、 208 ' 210 介電層 41 第一介電層 42 第二介電層 43 閘極介電層 45 傳導通道 46、53 導電層 47 、 70 、 72 、 91 開口 48 第三介電層 49 寬度 51 第四介電層 52 P型掺雜區域 54 保護層 56 基座堆疊結構 57 導電間隔物閘極區域 58 控制電極或閘極結構 59 介電質間隔物 61 •第五介電層 62 層間介電層 62a ILD層的部分 63 源極接觸層 66 汲極接觸層 68 垂直表面 106084.doc ·28· 1362747 •i
71 遮罩層 74(圖 2) 寬度 74(圖 5) 、 84 凹陷部分 77 導電連接部分 81 接觸開口 82 間隔物 100 終止結構 103、203、203a、203b 隔離溝渠 106 钱刻溝渠 108 、 208 介電材料 114 pn接合面 117 柱狀物 122 ' 206 溝渠 131 用於裝置終止結構之部分的區域 132 用於裝置之主動結構之部分的區域 146 導電接觸半導體層 152 P型摻雜層 300 單元結構 322 填充溝渠 461 劃分格柵 463 中線 106084.doc -29-
Claims (1)
- ί命私日修正本 1362747 Λ 十、申請專利範圍: 第094140266號專利申請案 中文申請專利範圍替換本(1〇〇年 一種半導體裝置,其包含: 第導電率類型的半導體基板’其具有一邊緣部 分; 一第二導電率類型的半導體層,其形成覆蓋於該半導 體基板之上,使得該半導體層與該半導體基板為該半導 體裝置形成一主要阻擋接合面; Φ 主動裝置,其形成於該半導體層之一部分,其中該 主動震置包含: 該第二導電率類型的一第一摻雜區域; ▲該第導電率類型的一第二摻雜區域,其形成於 該第一摻雜區域中;及 电極其形成於鄰接該等第一及第二彳參雜 區域處;及邊’·彖終止結構,其形成於該邊緣部份,其中該 邊緣終止結構包含: °亥第一V電率類型的一第三摻雜區域,其形成 於該半導體層; 一第一導電層 —隔離溝渠, 該半導體層》 ,其輕合至該第三摻雜區域;及 其形成於鄰接該第三摻雜區域之 2 ·如請求項1之裝置, 層之部分之形狀的一 3.如請求項2之裝置, 其中該隔離溝渠包括包含該半導體 矩陣。 其中5亥形狀矩陣包括複數個圓形柱 106084-1001223.doc 4. 狀物。 如請求項2之裝置,其 再中該形狀矩陣包括相 的一形狀矩陣。 州幻马偏移 如。月求項1之裝置,其進一步包含一電 電荷補償區域形成於相鄰該主動裝置之該半導^域,該 •如請求項5之裝置,其令該電荷補償區域包含層。 溝渠,其形成於該半導體層; 渠該第-導電率類型的一第一半導體層,其形成於該溝 -第-緩衝層,其形成於該第—半導體層之上及 該第二導電率類型的一第二半導體層,其形成於該第 一緩衝層之上。 .如請求項5之裝置 區域的第二導電層 8. 如請求項7之裝置 層輕合一起。 9. 如請求項1之裝置 結構。 如明求項9之裝置’其進一步包含一耦合至該間隔物閘 極結構的第三導電層’其中該第二導電層位在該第三導 %層及。亥半導體層之間,及其中該等第二及第三導電層 為彼此隔離β 11’ 求項丨之裝置,其進一步包含一耦合至該第二摻雜 區域的接觸層’其中該接觸層係進一步耦合至該第一導 其進一步包含一耦合至該電荷補償 其中將該等第一傳導層及第二傳導 其中該控制電極包含一間隔物閘極 106084-1001223.doc -2- 12. 電層 種半導體裝置,其包含: -第-導電率類型的半導體基板,其具有一邊 分; ~第二導電率類 板之上; 緣部 型的半導體層’其形成於該半導體基 δ玄第二導電率類划的_ # _协&社、备 ^•的一第一摻雜區域,其形成於鄰接 〜邊緣部分之該半導體層; 第導電層’其耦合至該第—摻雜區域; 離區域’其形成於鄰接該第_摻雜區域之該半導 體層; 一電荷補償區域,其形成於該半導體層; 該第二導電率類型的一第二摻雜區域,其形成於鄰接 °Λ電荷補償區域之該半導體層;-該第-導電率類型的一第三摻雜區域,其形成於該第 一摻雜區域;及 -控制電S,其形成於鄰接該等第1摻雜區域及第三 摻雜區域處。 13 •如請求項12之裝置,其中該電荷補償區域包含: —溝渠,其形成於該半導體層; 該第一導電率類型的一第一半導體層,其形成於該溝 渠; 一第一本質層,其形成於該第一半導體層之上;及 該第二導電率類型的一第二半導體層,其形成於該第 106084-1001223.doc 一本質層之上。 14. 15. 16. 其進一步包含一 耦合至該電荷補償 如請求項12之裝置, 區域的第二導電層。 耦合至該第三摻雜 步耦合至該等第— 如請求項14之裝置,其進一步包含— 區域的接觸層,其中該接觸層係進— 導電層及第二導電層β 一卿成一半導體裝置的方法,其包含以下步驟: 提供具有-邊緣部分之一第一導電率類型的半導體 基板及一形成於一主表面之卜夕一 ^ 帛—導電率類型的半 導體層’其巾該半導體層與該半導體基板為 置形成一主要阻擋接合面; 在鄰接該邊緣部分的該半導體層形成該第二導電率類 型的一第一摻雜區域; 在該半導體層形成一隔離溝渠,其中該隔離溝渠與該 第一摻雜區域相鄰; 在該半導體層中形成該第二導電率類型的—第二摻雜 區域; ^ ' 在δ玄第二摻雜區域中形成該第一導電率類型的一第三 摻雜區域; 形成一鄰接該等第二及第三摻雜區域的控制電極,其 中該第二摻雜區域、第三摻雜區域及該控制電極形成一 主動裝置;及 形成一耦揭至該第一摻雜區域的第一導電層,其中該 第—摻雜區域、該隔離溝渠及該第一導電層於該半導體 •06084-100l223.doc -4 * 1362747 -裝置之一周圍形成一邊緣終止結構。 17. 如請求項16之方法,其中形成該隔離溝渠的步驟包括在 該溝渠中形成包含該半導體層之部分的一形狀矩陣。 18. 如請求項16之方法,其進一步包含在該半導體層中形成 一電荷補償區域的步驟。 19_如請求項18之方法,其進一步包含以下步驟:形成一耦 合至該電荷補償區域的第二導電層。 ^ 20.如請求項18之方法,其中形成該電荷補償區域的步驟包 括以下步驟: 在該半導體層中形成一溝渠; 在該溝渠中形成該第一導電率類型的一第一半導體 層; 在該第一半導體層之上形成一第一缓衝層;及 在該第一缓衝層之上形成該第二類型的一第二半導體 層。 馨 106084-1001223.doc
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