TW493280B - DMOS transistor structure having improved performance - Google Patents
DMOS transistor structure having improved performance Download PDFInfo
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- TW493280B TW493280B TW090103825A TW90103825A TW493280B TW 493280 B TW493280 B TW 493280B TW 090103825 A TW090103825 A TW 090103825A TW 90103825 A TW90103825 A TW 90103825A TW 493280 B TW493280 B TW 493280B
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- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
- H01L21/18—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
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- H01L29/76—Unipolar devices, e.g. field effect transistors
- H01L29/772—Field effect transistors
- H01L29/78—Field effect transistors with field effect produced by an insulated gate
- H01L29/7801—DMOS transistors, i.e. MISFETs with a channel accommodating body or base region adjoining a drain drift region
- H01L29/7802—Vertical DMOS transistors, i.e. VDMOS transistors
- H01L29/7813—Vertical DMOS transistors, i.e. VDMOS transistors with trench gate electrode, e.g. UMOS transistors
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- H01L29/0615—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by particular constructional design considerations, e.g. for preventing surface leakage, for controlling electric field concentration or for internal isolations regions for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse biased devices by the doping profile or the shape or the arrangement of the PN junction, or with supplementary regions, e.g. junction termination extension [JTE]
- H01L29/0626—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by particular constructional design considerations, e.g. for preventing surface leakage, for controlling electric field concentration or for internal isolations regions for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse biased devices by the doping profile or the shape or the arrangement of the PN junction, or with supplementary regions, e.g. junction termination extension [JTE] with a localised breakdown region, e.g. built-in avalanching region
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- H01L29/06—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
- H01L29/08—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions with semiconductor regions connected to an electrode carrying current to be rectified, amplified or switched and such electrode being part of a semiconductor device which comprises three or more electrodes
- H01L29/0843—Source or drain regions of field-effect devices
- H01L29/0847—Source or drain regions of field-effect devices of field-effect transistors with insulated gate
- H01L29/0852—Source or drain regions of field-effect devices of field-effect transistors with insulated gate of DMOS transistors
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- H01L29/02—Semiconductor bodies ; Multistep manufacturing processes therefor
- H01L29/06—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
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- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/68—Types 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
- H01L29/76—Unipolar devices, e.g. field effect transistors
- H01L29/772—Field effect transistors
- H01L29/78—Field effect transistors with field effect produced by an insulated gate
- H01L29/7801—DMOS transistors, i.e. MISFETs with a channel accommodating body or base region adjoining a drain drift region
- H01L29/7802—Vertical DMOS transistors, i.e. VDMOS transistors
- H01L29/7811—Vertical DMOS transistors, i.e. VDMOS transistors with an edge termination structure
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Description
493280 Λ7 Β7 五、發明說明(1) 技術領域 (請先閱讀背面之注意事項再填寫本頁) 本發明與閘極成形在槽中之電流切換的D Μ〇S電晶 體有關,且特別是當裝置在接通時具有低電阻的槽式 D Μ〇S電晶體有關。 發明背景 功率D Μ 0 S電晶體的用途極爲廣泛,包括自動電子 裝置,磁碟機及電源供應器等。一般言之,這些裝置的功 能如同開關,它們用來將電源供應連接到負載。很重要的 一點是,當開關閉路時,裝置的電阻要儘量低。否則,電 力將被浪費,且會產生過量的熱。 經濟部智慧財產局員工消費合作社印製 典型的分立DMO S電路包括兩或多個各自獨立的 D Μ 0 S電晶體格,它們被平行製造。各自獨立的 D Μ〇S電晶體格共同使用一共用的汲極接點(基底), 同時,它們的源極也全都以金屬短路在一起,它們的閘極 以複矽短路在一起。因此,即使分立的D Μ〇S電路是由 較小電晶體的矩陣所構成,它們的行爲也如同一個大型電 晶體。對分立的D Μ〇S電路而言,當電晶體矩陣被閘極 接通時,希望每單位面積的導電率最大化。 此裝置說明於圖1,它是單格D Μ〇S電晶體1 0〇 的剖面圖,圖2是格的斜視截面圖。閘極1 0 2及1〇4 成形在槽中,且四周分別被閘氧化物層1 0 6及1 0 8包 圍。槽式的閘極通常是形成格子的樣式,格子代表一個互 連的閘極,不過,槽式閘極也可成形爲一連串不連續的平 -4- 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 493280 ------- A7 B7 五、發明說明(2) 行條狀。 DM〇S電晶體1 〇 〇是一雙擴散的裝置,它成形在 N —磊晶層1 1 1中。N +源極區1 1 2成形在磊晶層 1 1 1的表面,做爲P+接點區1 1 4 ° P —本體1 1 6 位於N +源極區1 1 2與P +接點區1 1 4的下方。金屬 的源極接點1 1 8與N +源極區1 1 2接觸,並短路N + 源極區1 1 2、P+接點區1 1 4及P區1 1 6。 N —磊晶層1 1 1成形在N +基底1 2 0上,汲極接 點(未顯示)位於N +基底1 2 0的底部。圖2中顯示閘 極1 0 2及1 0 4的接點1 2 1,它是導電的閘極材料延 伸到槽的外部,並在各格遠方的位置成形金屬接點。圖3 也顯示閘金屬接點1 2 1形成與閘極1 0 2及1 〇 4的連 接。典型上,閘極是由複矽摻雜磷或硼而成。須注意,當 一連串的電晶體格成形之時,閘接點1 2 1僅從構造之周 邊的格延伸,不是從內部的格。 N-磊晶層111中位於N+基底120與P—本體 1 1 6之間的區域1 1 〇中,一般是摻雜濃度比N +基底 1 2 0輕的N —型雜質。此可增加DM〇S電晶體1〇〇 忍受高電壓的能力。區域1 1 0有時稱爲”輕度摻雜”或 ”漂移”區(”漂移”是指載子在電場中移動)。漂移區 1 1 0與N+基底1 2〇構成DMOS電晶體1 〇 0的汲 極。 DM〇S電晶體1 〇 0是N —通道的電晶體。當正電 壓施加於閘極1 0 2時,毗鄰閘氧化物1 〇 6之P -本體 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) --♦---;--------^--- (請先閱讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製 言·
-5- 493280 A7 B7 經濟部智慧財產局員工消費合作社印製 五、發明說明(3) 116內一通道區反轉,在N+源極區112與N+基底 1 2 0間提供一電壓差,電子流從源極區經過通道區進入 漂移區1 1 0。在漂移區1 1 〇中,某些電子流以一角度 對角線地分開,直到它撞擊到N +基底1 2 0,並接著垂 直地流到汲極。另一部分的電子流直接向下通過漂移區 1 1 0 ,以及,某些電子流在閘極1 〇 2的下方流動,並 直接通過漂移區1 1 〇。 閘極1 0 2與1 〇 4中摻雜導電材料。由於D Μ〇S 電晶體1 0 0是Ν -通道的裝置,因此閘極1 〇 2與 1 0 4是複矽摻雜磷。閘極1 〇 2與1 0 4分別以閘氧化 物層1 0 6及1 0 8與DM 0S電晶體1 〇 〇的其餘部分 隔離。選擇閘氧化物層1 〇 6及1 0 8的厚度即可設定 D Μ〇S電晶體1 〇 〇的門檻電壓,也影響到D μ〇S電 晶體1 0 0的崩潰電壓。 在圖1 一 3所示的DM〇S電晶體1〇〇中,Ρ+接 點區1 1 4向下延伸低於槽的底部,在格的中央形成一深 層一重度摻雜的P+本體1 1 6。在其它的已知DM〇S 電晶體(未顯示)中,P +接點區1 1 4非常淺,其延伸 並未低於槽的底部。易言之,在這些裝置中沒有P +本體 1 1 6。淺的P +接點區有助於確保p 一型雜質不會進入 通道區,它傾向使裝置的門檻電壓增加,並致使裝置的接 通特性相互間不同,視P +接點區1 1 4的排列而定。不. 過,沒有P+本體116的淺P+接點區114,當裝置 關閉時,它所能忍受的電壓較低(例如i 〇伏)。這是因 (請先閱讀背面之注意事項再填寫本頁) 11丨裝
ϋ ·ϋ _§· tMMe 一口τ I I— 11 flu Hi n n tmMmm I %· 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) -6 - 493280 A7 B7 五、發明說明(4) 爲在P +接點區1 1 4與漂移區1 1 0之接面附近的耗盡 擴散不適合保護槽的角落(例如圖1中所示的角落1 2 2 )。結果,在槽的附近會發生崩落擊穿,導致很高的載子 產生率,它會對閘氧化物層1 0 6充電或使其劣化,甚至 ,在極端的情況,致使閘氧化物1 0 6破裂。因此,此種 已知的D Μ〇S電晶體最好是用於低電壓裝置。 不過,如前所述,在如圖1 一 3所示的D Μ〇S電晶 體1 0 0中,由於Ρ +接點區1 1 4向下延伸低於槽的底 部,在格的中央形成一深且重度-摻雜的Ρ本體區1 1 6 ,因此崩潰電壓增加。此提供了角落1 2 2額外的遮蔽, 同時,它的主要優點是,載子的產生主要是發生在Ρ+本 體1 1 6的底部尖端3 0 2。這是因爲在尖端3 0 2下方 的電場加強,藉以致使載子是沿著接面彎曲的點產生,而 非毗鄰閘氧化物1 0 6。此減少了對閘氧化物1 0 6的應 力,並增進了 DMO S電晶體1 〇 〇在高電壓時的可靠度 ,雖然這會降低裝置實際的接面擊穿。關於向下延伸之Ρ 接點區的其它細節,可見於例如美國專利5,0 7 2, 266及5,688,725° 經濟部智慧財產局員工消費合作社印製 ---;---·--------裳--- (請先閱讀背面之注意事項再填寫本頁) 在D Μ〇S電晶體1 〇 〇中的深Ρ +本體1 1 6,雖 然大幅地降低了崩潰的不利影響,但也有一些有害的效果 。第一,產生了格密度的上限,因爲隨著格密度增加,Ρ 離子可能會進入通道區。如前所述,此傾向增加D Μ〇S 電晶體的門檻電壓。第二,由於深Ρ +接點本體1 1 6的 出現,當電子流離開通道進入漂移區1 1 0時傾向被擠壓 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 經¾部智慧財產局員工消費合作社印製 493280 A7 B7___ 五、發明說明(5 ) 。在沒有深p +本體1 1 6的已知電晶體中,當電子流到 達漂移區1 1 0時是擴散開的。電流擴散開可增加漂移區 1 1 〇中每單位面積的平均電流,並因此使D Μ〇S電晶 體的接通電阻降低。深Ρ +本體1 1 6的出現限制了此電 流的擴散,且接通電阻隨著格密度的增加而增加。 因此,吾人需要的D Μ〇S電晶體是結合深ρ +本體 的優點與低的接通電阻。 發明槪述 按照本發明,提供一種槽式D Μ〇S電晶體構造,它 包括至少3個獨立的槽式D Μ 0 S電晶體格,成形在第一 導電類型的基底上。複數個獨立的D Μ 0 S電晶體劃分成 周邊電晶體格與內部電晶體格。每一個獨立的電晶體格包 括位於基底上的本體區,該本體區具有第二導電類型。至 少一條槽延伸通過本體區與基底,一絕緣層襯於槽內。一 導電電極位於槽內,覆於絕緣層上。每一個內部電晶體格 在本體區中毗鄰槽邊還包括第一導電類型的源極區,但周 邊電晶體格則無。因此,周邊的電晶體格是無作用的,而 內部電晶體格是有源的電晶體。結果,可得到低的門檻電 壓,同時也不需要深的Ρ +接點區。 按照本發明的一態樣,本體區實質平坦地橫過電晶體 格的寬度,它們個別地位於其中。或者,本體區可以是雙 峰(bimodal )分布橫過電晶體格的寬度,它們個別地位於 其中。 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) -8- (請先閱讀背面之注意事項再填寫本頁) · --------訂·--------· 493280 A7 B7 五、發明說明(6) 按照本發明的另一態樣,槽延伸的深度深於本體區。 按照本發明的另一態樣,周邊電晶體格之本體區的摻 雜遠比內部電晶體格的本體區輕。 按照本發明的另一態樣,提供~種槽式〇 Μ 0 S電晶 體構造,它包括至少3個獨立的槽式D Μ〇S電晶體格, 成形在第一導電類型的基底上。複數個獨立的DM0 S電 晶體劃分成周邊電晶體格與內部電晶體格。每一個獨立的 電晶體格包括位於基底上的本體區,本體區具有第二導電 類型。本體區是以雙峰分布橫過電晶體格的寬度,它們個 別地位於其中。至少一條槽延伸通過本體區與基底,一絕 緣層襯於槽內。一導電電極位於槽內,覆於絕緣層上。內 部電晶體格每一個還包括第一導電類型的源極區。源極區 位於本體區中毗鄰槽邊。 圖式簡單說明 圖1及2分別是習知垂直槽N -通道DM〇S電晶體 格的剖面圖及斜視圖,它具有較深的中央P +接點區。 (請先閱讀背面之注意事項再填寫本頁) --裝 訂---------%· 經濟部智慧財產局員工消費合作社印製 道之 。 通格圖 I 體 面 N晶平 知電 的 習部 造 之內 構 區及體 點邊 晶。 接周 電例 + 之 之施 P 。 構 構實 央圖架 架一 中面明 明另 深剖發 發的 較一本 本明 有另照 照發 具的按 按本 明體明。明明 說晶說圖說說 是電是面是是 3 S 4 0 5 6 圖〇 圖的圖圖 Μ 造 D 構 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) -9- 493280 A7 _ B7 五、發明說明(7) 元件表 1〇〇 DMOS電晶體 (請先閱讀背面之注意事項再填寫本頁) 1 0 2 閘極 1〇4 閘極 10 6 閘氧化物層 10 8 閘氧化物層 111 N —磊晶層 112 N +源極區 114 P +的接點區 1 1 8 源極接點 116 P +本體 121 閘極接點 11〇 漂移區 12 2 角落 302 P+本體的底部尖端 200 DMOS構造 21 電晶體格 2 2 0 η +基底 經濟部智慧財產局員工消費合作社印製 2 11 -摻雜磊晶層 214 本體區 2 4 0 η -摻雜磊晶層 2 0 2 槽 2 0 4 槽 2 3 0 閘氧化物層 本紙張尺度適用中國國家標準(CNS)A4規格(210 x 297公釐) _ 1〇 _ 493280 經濟部智慧財產局員工消費合作社印製 A7 --— _ B7____五、發明說明(8 ) 218 源極電極 2 2 1 閘電極 6 14 ρ +接點區 圖4說明槽式D Μ〇S構造2 〇 0之實施例的剖面圖 ,圖5是平面圖,其中,獨立格21在水平方向的截面是 長方形。本實施例的構造包括η +基底2 2 0,在基底上 生長輕度的η -摻雜磊晶層2 1 1。在η —摻雜的磊晶層 2 1 1中配置導電極性相反的接點與本體區2 1 4。覆於 部分本體區2 1 4上方的η -摻雜磊晶層2 4 0做爲源極 。長方形的槽2 0 2及2 0 4配置在磊晶層內,它在構造 的上表面開放,並定義電晶體格的周界。閘氧化物層 230襯於槽202及204的內壁。槽202及2〇4 內塡以複矽,即複晶矽。汲極電極連接到半導體基底 2 2 0的背表面,源極電極2 1 8連接到兩個源極區 2 4 0及接點區2 1 4,閘電極2 2 1連接到塡充於槽 2〇2中的複矽。襯於槽內的複矽連續地連接於基底 2 0 0的表面,。此外,如圖4及5所示,複砂接點2 2 1 延伸超出基底200的表面,做爲與周邊電晶體格的互連 ,如電晶體格2 1 i、2 1 2、及2 1 3。內部電晶體格, 如格2 1 4、2 1 5、及2 1 6經由槽的本身相互連接並連 接到周邊格。在圖4中,槽2 0 2與周邊格有關,槽 2 0 4與內部格有關。 (請先閱讀背面之注意事¾再填寫本頁) :·丨
I a HI an —ϋ ϋ— ϋ ϋ n 一口、馨 ΜΜ Μ··· I ΜΒΗ I MM· HW % 本紙張尺度適用中國國家標準(CNS)A4規格(210 x 297公釐) -_ 493280 A7 ___B7 五、發明說明(9) (請先閱讀背面之注意事項再填寫本頁) 須注意,就基本的電晶體工作而言,電晶體格2 1並 不需要是長方形,它可以是任何的多邊形。不過,以配置 而言,正規的長方形及正規的六角形最方便。或者,不一 定需要如圖中所示之封閉-格的幾何形狀,電晶體格也可 以是開放或條形。 如前所述,習知D Μ 0 S電晶體技術所使用的深p + 接點區致使門檻電壓隨著格密度增加而增加。深的中央 Ρ +區致使裝置的接通電阻增加。不過,沒有深的ρ +接 點區,裝置的崩潰電壓會低到在很多應用中都無法接受。 經濟部智慧財產局員工消費合作社印製 按照本發明,經由提供其內爲無作用之電晶體的周邊 電晶體格以及其內爲有源電晶體的內部電晶體格,即可做 到低門檻電壓同時不需要深的ρ +接點區。如圖4所示, 槽2 0 2與周邊電晶體格有關,同時,槽2 0 4與內部電 晶體格有關。無作用的周邊電晶體格與有源的內部電晶體 間的區別在於無作用的電晶體沒有源極。例如,如圖4所 示,與槽2 0 2有關的周邊電晶體格沒有任何源極區。此 外,與周邊電晶體格有關的Ρ +接點區2 1 4的摻雜遠低 於與內部格有關的Ρ +接點區。由於摻雜較輕,在這些周 邊格中將不會發生崩潰。更正確地說,此種配置確保在內 部格內發生崩落擊穿。因此,所發明的D Μ〇S電晶體陣 列可用於較高電壓。此外,由於不需要深的ρ +接點區, 不受歡迎的門檻電壓與接通-電阻的增加也得以避免。 圖6顯示本發明的另一特定實施例,其中,ρ +接點 區6 1 4具有雙峰的分布,而非沿著電晶體格之寬度實質 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) -12- 493280 A7 ______B7____ 五、發明說明(10) 平坦的分布。在本發明的此實施例中,崩落擊穿通常發生 在標示爲6 1 0之點的附近。 雖然本文特別說明與描述了各種實施例,但須瞭解, 對本發明的各種修改與變化也包涵在上述的教導中,且在 所附申請專利範圍的範圍中,不會偏離本發明所欲的精神 與範圍。例如,本發明也一體適用於各半導體區域之導電 特性與本文描述相反的槽式D Μ〇S。 (請先閱讀背面之注意事項再填寫本頁) 1 --------訂·------- 經濟部智慧財產局員工消費合作社印製 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) -13-
Claims (1)
- 493280 Α8 Β8 C8 D8 申請專利範圍 1 · 一種槽D Μ〇S電晶體構造,它包括至少3個獨 立的槽式D Μ〇S電晶體格,成形在第一導電類型的基底 上,該複數個獨立的D Μ〇S電晶體劃分成周邊電晶體格 與內部電晶體格,每一個獨立的電晶體格包括 位於基底上的本體區,該本體區具有第二導電類型; 至少一條槽延伸通過本體區與基底; 一絕緣層,襯於槽內; 一導電電極,位於槽內,覆於絕緣層上;以及 其中,每一個內部電晶體格在本體區中Η比鄰槽邊還包 括第一導電類型的源極區,但周邊電則無。 2 .如申請專利範圍第1項的電晶 實質平坦地橫過電晶體格的寬度,它於 3 .如申請專利範圍第1項的電中 一條槽延伸的深度深於本體區的深度; / 4 ·如申請專利範圍 本體區 們個別 —----------裝---- * - (請先閱讀背面之注意事項再填寫本頁) —訂------ 經濟部智慧財產局員工消費合作社印製 每一個都具有一雙峰分布橫過電晶體格的寬度,它 地位於其中。 ,蟲 5 ·如申請專利範圍第1項的電晶¾,該周邊 ^等丨:::管^ 電晶體格之本體區的摻雜遠比內部電晶體格ίτ%/體區輕。 6 ·如申請專利範圍第1項的電晶體構造,還包括一 汲極電極,配置在基底相對於本體區的表面。 7 ·如申請專利範圍第1項的電晶體構造,其中該絕 緣層是氧化物層。 8 ·如申請專利範圍第1項的電晶體構造,其中該導 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公爱·) -14 - 493280 Α8 Β8 C8 D8 六、申請專利範圍 電電極包括複砂。 9 ·如申請專利範圍第1 個該槽式D Μ 〇 s電晶體格的 1 0 ·如申請專利範圍第 之格的幾何形狀是長方形。 項的電晶 幾何形狀是 9項的電晶.如申請專利範圍第1項的電晶(請先閱讀背面之注意事項再填寫本頁) 中,至少 1項的電晶一步包括 周邊電晶體格的每一個導電 4項的電晶進一步包括 周邊電晶體格Mg—個導電 個該槽式D Μ 0 S電晶體格的幾何形肤最 1 2 .如申請專利範圍第 複數個複矽接點,分別連接到 電極。 1 3 ·如申請專利範圍第 複數個複矽接點,分別連接到 電極。 1 4 ·如申請專利範圍第 複數個複矽接點,分別連接到 電極。 3項的電晶 周邊電晶體格的個導電 經濟部智慧財產局員工消費合作社印製 1 5 · —種槽式D Μ〇S電晶體構造,它包括至少3 個獨立的槽式D Μ〇S電晶體格,成形在第一導電類型的 基底上,該複數個獨立的D Μ〇S電晶體劃分成周邊電晶 體格與內部電晶體格,每一個獨立的電晶體格包括: 位於基底上的本體區,該本體區具有第二導電類型, 其中該本體區是以雙峰分布橫過電晶體格的寬度,它們個 別地位於其中; 至少一條槽延伸通過本體區與基底; 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公爱·) 15 493280 Α8 Β8 C8 D8 申請專利範圍 一絕緣層襯於槽 —導電電極位於 內 其中, 中毗鄰槽邊 槽內,覆於絕緣層上;以及 至少該內部電晶體格每一個還包括位於本體區 之第一導電類型的源極區。 1 6 ·如申請專 至少一條槽延伸的深 1 7 ·如申請專 格之本體 利範圍第1 5項的電晶其中,該 度深於本體區的深度。經濟部智慧財產局員工消費合作社印製 周邊電晶體 輕° 1 8 . 括一汲極電 19. 該絕緣層是 2 0 . 該導電電極 2 1 . 少一個該槽 2 2 . 閉之格的幾 2 3 . 少一個該槽 2 4·· 括複數個複 電電極。 如申請專 極,配置 如申請專 氧化物層 如申請專 包括複矽 如申請專 式D Μ〇 如申請專 何形狀是 如申請專 式f) Μ〇 如申請專 矽接點, 利範圍第1 5項的電晶齡中,該 區的摻雜遠比內部電晶體格的本體區 利範圍第1 5項的電晶體構造,還包 在基底相對於本體區的表面。 利範圍第1 5項的電晶體構造,其中 0 利範圍第1 5項的電晶體構造,其中 0 利範圍第1 5項的電晶 S電晶體格的幾何形狀 利範圍第2 1項的電晶 長方形。 /, 利範圍第1 5項的電晶1¾¾其中,至 S電晶體格的幾何形狀的格。 利範圍第1 5項的電晶—步包 分別連接到周邊電晶體格的每一個導(請先閱讀背面之注意事項再填寫本頁) I裝 II---------备丨 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公爱’) -16- 493280 A8 B8 C8 D8 申請專利範圍 2 5 .如申請專利範圍第 項的電晶步包 括複數個複矽接點,分別連接到周邊電晶體格個導 極I电 -----------_-裝— -·* (請先閱讀背面之注意事項再填寫本頁) 訂------- 經濟部智慧財產局員工消費合作社印製 -17 - 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐‘)
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EP (2) | EP1266406B1 (zh) |
JP (1) | JP2003529209A (zh) |
KR (1) | KR20020079919A (zh) |
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DE10127885B4 (de) * | 2001-06-08 | 2009-09-24 | Infineon Technologies Ag | Trench-Leistungshalbleiterbauelement |
US6838722B2 (en) * | 2002-03-22 | 2005-01-04 | Siliconix Incorporated | Structures of and methods of fabricating trench-gated MIS devices |
US8629019B2 (en) * | 2002-09-24 | 2014-01-14 | Vishay-Siliconix | Method of forming self aligned contacts for a power MOSFET |
US7494876B1 (en) | 2005-04-21 | 2009-02-24 | Vishay Siliconix | Trench-gated MIS device having thick polysilicon insulation layer at trench bottom and method of fabricating the same |
US7583485B1 (en) | 2005-07-26 | 2009-09-01 | Vishay-Siliconix | Electrostatic discharge protection circuit for integrated circuits |
US7544545B2 (en) * | 2005-12-28 | 2009-06-09 | Vishay-Siliconix | Trench polysilicon diode |
CN101361193B (zh) * | 2006-01-18 | 2013-07-10 | 维西埃-硅化物公司 | 具有高静电放电性能的浮动栅极结构 |
DE102006029750B4 (de) * | 2006-06-28 | 2010-12-02 | Infineon Technologies Austria Ag | Trenchtransistor und Verfahren zur Herstellung |
US20080206944A1 (en) * | 2007-02-23 | 2008-08-28 | Pan-Jit International Inc. | Method for fabricating trench DMOS transistors and schottky elements |
US10600902B2 (en) | 2008-02-13 | 2020-03-24 | Vishay SIliconix, LLC | Self-repairing field effect transisitor |
US9230810B2 (en) | 2009-09-03 | 2016-01-05 | Vishay-Siliconix | System and method for substrate wafer back side and edge cross section seals |
US9425305B2 (en) | 2009-10-20 | 2016-08-23 | Vishay-Siliconix | Structures of and methods of fabricating split gate MIS devices |
US9419129B2 (en) | 2009-10-21 | 2016-08-16 | Vishay-Siliconix | Split gate semiconductor device with curved gate oxide profile |
US9577089B2 (en) | 2010-03-02 | 2017-02-21 | Vishay-Siliconix | Structures and methods of fabricating dual gate devices |
KR101619580B1 (ko) | 2011-05-18 | 2016-05-10 | 비쉐이-실리코닉스 | 반도체 장치 |
JP6290526B2 (ja) | 2011-08-24 | 2018-03-07 | ローム株式会社 | 半導体装置およびその製造方法 |
JP6524279B2 (ja) * | 2011-08-24 | 2019-06-05 | ローム株式会社 | 半導体装置およびその製造方法 |
JP6219140B2 (ja) | 2013-11-22 | 2017-10-25 | ルネサスエレクトロニクス株式会社 | 半導体装置 |
CN115483211A (zh) | 2014-08-19 | 2022-12-16 | 维西埃-硅化物公司 | 电子电路 |
US11217541B2 (en) | 2019-05-08 | 2022-01-04 | Vishay-Siliconix, LLC | Transistors with electrically active chip seal ring and methods of manufacture |
US11218144B2 (en) | 2019-09-12 | 2022-01-04 | Vishay-Siliconix, LLC | Semiconductor device with multiple independent gates |
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CN1279620C (zh) | 2006-10-11 |
EP2267786A3 (en) | 2011-01-12 |
WO2001065607A3 (en) | 2002-05-30 |
EP2267786A2 (en) | 2010-12-29 |
EP1266406A2 (en) | 2002-12-18 |
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EP1266406B1 (en) | 2011-11-30 |
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