TW293150B - - Google Patents
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- Publication number
- TW293150B TW293150B TW085102998A TW85102998A TW293150B TW 293150 B TW293150 B TW 293150B TW 085102998 A TW085102998 A TW 085102998A TW 85102998 A TW85102998 A TW 85102998A TW 293150 B TW293150 B TW 293150B
- Authority
- TW
- Taiwan
- Prior art keywords
- polycrystalline silicon
- gate
- bridge
- conductive material
- layer
- Prior art date
Links
- 229910021420 polycrystalline silicon Inorganic materials 0.000 claims description 36
- 238000000034 method Methods 0.000 claims description 22
- 238000001020 plasma etching Methods 0.000 claims description 22
- 239000004065 semiconductor Substances 0.000 claims description 16
- 238000004519 manufacturing process Methods 0.000 claims description 14
- 229920005591 polysilicon Polymers 0.000 claims description 8
- 239000004020 conductor Substances 0.000 claims description 6
- 229910052751 metal Inorganic materials 0.000 claims description 6
- 239000002184 metal Substances 0.000 claims description 6
- 239000004576 sand Substances 0.000 claims description 5
- 238000005381 potential energy Methods 0.000 claims 1
- 238000005530 etching Methods 0.000 description 12
- 230000015556 catabolic process Effects 0.000 description 10
- 239000000758 substrate Substances 0.000 description 9
- 150000002500 ions Chemical class 0.000 description 8
- 238000009825 accumulation Methods 0.000 description 7
- 238000006731 degradation reaction Methods 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 230000008901 benefit Effects 0.000 description 2
- 239000013078 crystal Substances 0.000 description 2
- 238000006073 displacement reaction Methods 0.000 description 2
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 2
- 239000010931 gold Substances 0.000 description 2
- 229910052737 gold Inorganic materials 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- WQJQOUPTWCFRMM-UHFFFAOYSA-N tungsten disilicide Chemical compound [Si]#[W]#[Si] WQJQOUPTWCFRMM-UHFFFAOYSA-N 0.000 description 2
- 229910021342 tungsten silicide Inorganic materials 0.000 description 2
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical group [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 230000008030 elimination Effects 0.000 description 1
- 238000003379 elimination reaction Methods 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 229910044991 metal oxide Inorganic materials 0.000 description 1
- 150000004706 metal oxides Chemical class 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012261 overproduction Methods 0.000 description 1
- 229920002120 photoresistant polymer Polymers 0.000 description 1
Classifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor 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
- H01L29/40—Electrodes ; Multistep manufacturing processes therefor
- H01L29/41—Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions
- 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
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L27/00—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate
- H01L27/02—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components specially adapted for rectifying, oscillating, amplifying or switching and having potential barriers; including integrated passive circuit elements having potential barriers
- H01L27/04—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components specially adapted for rectifying, oscillating, amplifying or switching and having potential barriers; including integrated passive circuit elements having potential barriers the substrate being a semiconductor body
- H01L27/06—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components specially adapted for rectifying, oscillating, amplifying or switching and having potential barriers; including integrated passive circuit elements having potential barriers the substrate being a semiconductor body including a plurality of individual components in a non-repetitive configuration
- H01L27/0611—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components specially adapted for rectifying, oscillating, amplifying or switching and having potential barriers; including integrated passive circuit elements having potential barriers the substrate being a semiconductor body including a plurality of individual components in a non-repetitive configuration integrated circuits having a two-dimensional layout of components without a common active region
- H01L27/0617—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components specially adapted for rectifying, oscillating, amplifying or switching and having potential barriers; including integrated passive circuit elements having potential barriers the substrate being a semiconductor body including a plurality of individual components in a non-repetitive configuration integrated circuits having a two-dimensional layout of components without a common active region comprising components of the field-effect type
- H01L27/0629—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components specially adapted for rectifying, oscillating, amplifying or switching and having potential barriers; including integrated passive circuit elements having potential barriers the substrate being a semiconductor body including a plurality of individual components in a non-repetitive configuration integrated circuits having a two-dimensional layout of components without a common active region comprising components of the field-effect type in combination with diodes, or resistors, or capacitors
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- 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
- H01L21/30—Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26
- H01L21/31—Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26 to form insulating layers thereon, e.g. for masking or by using photolithographic techniques; After treatment of these layers; Selection of materials for these layers
- H01L21/3205—Deposition of non-insulating-, e.g. conductive- or resistive-, layers on insulating layers; After-treatment of these layers
- H01L21/321—After treatment
- H01L21/3213—Physical or chemical etching of the layers, e.g. to produce a patterned layer from a pre-deposited extensive layer
- H01L21/32133—Physical or chemical etching of the layers, e.g. to produce a patterned layer from a pre-deposited extensive layer by chemical means only
- H01L21/32135—Physical or chemical etching of the layers, e.g. to produce a patterned layer from a pre-deposited extensive layer by chemical means only by vapour etching only
- H01L21/32136—Physical or chemical etching of the layers, e.g. to produce a patterned layer from a pre-deposited extensive layer by chemical means only by vapour etching only using plasmas
- H01L21/32137—Physical or chemical etching of the layers, e.g. to produce a patterned layer from a pre-deposited extensive layer by chemical means only by vapour etching only using plasmas of silicon-containing layers
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L27/00—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate
- H01L27/02—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components specially adapted for rectifying, oscillating, amplifying or switching and having potential barriers; including integrated passive circuit elements having potential barriers
- H01L27/0203—Particular design considerations for integrated circuits
- H01L27/0248—Particular design considerations for integrated circuits for electrical or thermal protection, e.g. electrostatic discharge [ESD] protection
- H01L27/0251—Particular design considerations for integrated circuits for electrical or thermal protection, e.g. electrostatic discharge [ESD] protection for MOS devices
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Computer Hardware Design (AREA)
- Plasma & Fusion (AREA)
- Ceramic Engineering (AREA)
- Chemical & Material Sciences (AREA)
- Chemical Kinetics & Catalysis (AREA)
- General Chemical & Material Sciences (AREA)
- Manufacturing & Machinery (AREA)
- Insulated Gate Type Field-Effect Transistor (AREA)
- Electrodes Of Semiconductors (AREA)
- Semiconductor Memories (AREA)
- Drying Of Semiconductors (AREA)
- Non-Volatile Memory (AREA)
Description
經濟部中央標準局員工消費合作社印製 A7 B7 — — 五、發明説明(1 ) 發明背景 本發明係關於一種半導體記憶裝置製造方法,尤指一 種降低以離子化氣體加諸於複晶矽層之電漿蝕刻過程中所 必然產生的電荷累積。 通常,在半導體裝置的製造過程中需要一些蝕刻步 驟。此外,使用離子化氣體的電漿蝕刻過程廣泛地在半導 體裝置的製造中使用。在電漿處理過程中,用於電漿蝕刻 的離子以及被蝕刻的裝置離子結合在一起,因而在被蝕刻 的裝置中收集了不需要的離子。該等累積的離子降低了裝 置中所產生的應力電流(stress current),所以可會g 在MOS電晶體內鄰近複晶矽層之薄氧化層之處產生崩潰 (breakdown) 〇也就是說,在形成MOS電晶體之閘極的 圖案的情況中,在爲形成閘極所爲之電漿蝕刻期間所產生 的電荷累積於被蝕刻的裝置中。以這種方式所累積的離子 導致了流經閘極與基體間之閘極氧化層的號勒-諾得海 (Fowler-Nordheim)電流,且因此電荷被捕捉於閘極 氧化層內。此外,被捕捉於閘極氧化層內的電荷降低閘極 氧化層的崩潰電壓,因而引發M0S電晶體之閘極氧化層的 崩潰。另外,以半導體裝置的高積體化及低溫,電晶體的 薄氧化層有變薄的傾向。既然閘極氧化層對於因電漿蝕刻 過程所產生的電荷累積所致之應力變得比較敏感,由於該 2 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) ----------^------1T'|_一_----^ (請先閲讀背面之注意事項再填寫本頁) 經濟部中央橾準局貝工消費合作社印製 A7 B7 五、發明説明(2 ) 應力的閘極氧化層的退化即行產生,並導致了產品品質的 惡化。 圖1A係習知NMOS電晶體在金屬蝕刻過程中的截面 圖,而圖1B表示了圖1A的等效電路》以圖ΙΑ,ΙΒ來解釋 消除金靥蝕刻過程期間的電漿蝕刻所導致之損壞的程序* 在電漿蝕刻過程期間,在晶圓材料上反應的材料大部份是 正離子,而該正離子經由金屜或複晶矽直接或間接地與電 晶體的閘極連接》因此,離子引發了對電晶體閘極的正方 向性電壓。 在本發明之複晶矽閘極NMOS電晶體結構中,η型雜質 110形成於一 Ρ型基體100之二側,而一閘極氧化層150形 成於基體100上。因此,由於施加於閘極130之正電荷所 形成的電場,Fowler-Nordheim電流在鬧極150內產 生。當負電荷由於該F-N電流而於電晶體的閘極氧化層內 增加時,臨界電壓(threshold voltage)增加。所 以,增加的臨界電壓導致了閛極氧化層內的崩潰。 分析上述臨界電壓的偏移(shift)現象,二極體120 連接於閘極130與基體100之間,所以連接至電晶體閘極 130的電荷可能放電於基體100之內。也就是說,爲了防 止F-N電流所造成之導致臨界電壓位移的崩潰*二極體 120被形成於半導體基體100之上,隨後形成金屬天線 140以便連接閘極電極130與二極體120,藉此將收集於 閘極130的電荷經由二極體120放電至半導體基體100 內。然而,在如前所述的NM0S電晶體內,二極體係與半導 3 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) ----------^------ΐτ--:----^ (請先閲讀背面之注意事項再填寫本頁) 經濟部中央標準局貝工消費合作社印製 A7 B7 五、發明説明(3 ) 體基體成反向偏壓關係,而因此難以使連接至閘極130的 電荷放電。此外還有因電荷被收集於閘極內所產生之閘極 氧化層1 5 0加速退化的問題。 爲解決圖一所產生的問題,圖二電晶體形成了如下的 結構。取代圖一的二極體,一雙載子接面電晶體BJT200 連接於閘極130與基體100之間。因此,如果BJT200藉由 電漿蝕刻過程中所產生的電荷而導通,閘極130與基體自 動互相連接,而與閘極13 0連接的電荷放電至基體內。藉 此防止閘極氧化層的退化。因此,經由上述的方法可以防 止在金屬蝕刻過程中所產之由電槳引發的電荷所造成的損 壞,但仍有一個由在複晶矽蝕刻過程中之電漿蝕刻所產生 的嚴重問題極待解決。 發明綜合說明 因此,本發明之一目的在於提供一種半導體記憶裝置 製造方法,能夠使以離子化氣體施加於複晶矽層之電漿触 刻過程中所累積於一氧化層內的電荷降至最少》 本發明之另一目的在提供一種半導體記憶裝置製造方 法,使在使用電漿形成複晶矽閘極圖案時所產生的電荷累 積減至最少,而能夠降低對複晶閘極與基體間之氧化層造 成影響的應力(stress)。 4 本紙張尺度適用中國國家標準(CNS ) A4说格(210X297公釐) 裝17線 (請先閲讀背面之注意事項再填寫本頁) S〇3i5〇 A7 B7 五、 發明説明(4 本發明之次一目的在提供一種半導體記憶裝置製造方 法,可以使造成閘極氧化層退化之電漿蝕刻所致之電荷累 積降至最小而保護了閘極氧化層。 本發明之又一目的在供一種半導體記憶裝置製造方 法,可以使複晶矽蝕刻過程中造成閘極氧化層退化之電漿 蝕刻所致之電荷累積降至最小而防止裝置的崩潰,並且解 決因電荷累積所造成之電晶體臨界電壓的位移現象。 爲達成上述及其它目的,在依據本發明原理之半導體 記憶裝置之製造方法中包括一電漿蝕刻步驟用以形成一複 晶矽閘極,爲了降低氧化層內的累積電荷所致之損壞,複 晶砂閘極被分爲形成於一主動區域(active region)中 之閘極複晶矽以及形成於一非主動區域(inactive r e g i ο η )中用以蝕刻的橋複晶矽。 圖式簡要說明 經濟部中央標準局貝工消費合作杜印製 本發明得藉下列圖式及詳細說明俾得一深入了解,其 中相同的標號指示相同或相似的部份,其中: 圖1Α :係用以解釋習知金屬蝕刻步驟之NM0S截面 rcrt ·圖, 圖1 B :係圖1 A之等效電路; 圖2A :係用以解釋金屬蝕刻步驟之另一 NU0S截面 nsrt · 圖, 圖2B :係圖2A之等效電路; 本紙張尺度逋用中國國家標準(CNS ) A4規格(210X297公釐) ----------餐------IT'—-----線- (請先閱讀背面之注意事項再填寫本頁) 經濟部中央標準局貝工消費合作社印製 A7 B7 五、發明説明(5) 圖3 :係解釋習知複晶矽閘極製造過程之示圖; 圖4 :表示在蝕刻過程後即將被蝕刻之一裝置的截面 結構,用以解釋習知複晶矽閘極的製造過程; 圖5 :表示圖4即將被蝕刻之裝置的平面圖; 圖6 :表示一將被蝕刻之裝置的平面圖,用以解釋依 據本發明原理之半導體記憶裝置之製造方法》 較佳實施例詳細說明 以下將參照所附之圖3,4, 5而解釋本發明較佳實施例 之結構及運作細節。此外,足以混淆本發明之功能及結構 的事物將不予以描述。 參照圖3,爲解釋複晶矽閘極製造過成,一複晶矽間 極330分佈於一場氧化層320及一形成於一 p型基體的薄氧 化層360之上,而一鶴的砂化物340(tungsten silicide)形成於複晶政之上。 圖4表示在蝕刻過程後將被蝕刻之一裝置的截面結構 圖,用以解釋包括使用含數百瓦特能量的電漿370的蝕刻 步驟的複晶矽閘極製造過程。在圖4,由於複晶閘極330, 鎢的矽化物340及光阻350收集的電荷,應力(stress) 施加於電晶體的閘極氧化層360,因而導致了閘極氧化層 3 6 0的退化。 圖5表示MOS電晶體的平面結構,包括複晶矽閘極 540,一源極530連接至一接地線550,以及一汲極510連 6 本紙張尺度適用中國國家梂準(CNS ) A4規格(210X297公釐) ---------裝-------——^----線. (請先閱讀背面之注意事項再填寫本頁) 經濟部中央標率局員工消費合作社印製 A7 ,__ B7i、發明説明(6 ) 接至其它電晶體530的閘極。在圖5,一栓鎖區域570代表 該處被加上了複晶矽矽蝕刻過程中所產生的損壞。此時, 電漿蝕刻損壞施加應力至閘極氧化層,因而導致了閘極氧 化層的損壞。 圖6表示將被蝕刻之裝置的平面結構圖,用來解釋依 據本發明原理之半導體記憶裝置之製造方法。以圖6解釋 降低被電漿蝕刻損壞所影響之栓鎖區域570中所收集的電 荷。在圖6中,爲了藉由降低電漿蝕刻時受影響的複晶矽 區域而使電漿蝕刻的損壞降至最小,栓鎖區域570被分爲 一閘極複晶矽部份610以及一橋複晶矽部份620。 另一方面,如果希望縮小電晶體的複晶閘極570的區 域而降低在閘極氧化層內所產生的應力,電漿蝕刻損壞可 以減小。此時,形成於主動區域(active region)內的 閘極複晶矽部份610與和該部份610分開的橋複晶矽部份 620的長度比大約是1比10。此外,閘極複晶矽部份610 及和該部份610分開的橋複晶矽部份620係由導電材料 6 0 0連接,如金靥之類。 在如前所述之本發明中,藉由降低在使用電漿蝕刻的 過程中所產生的電荷累積而存在著降低電漿蝕刻所產生之 損壞的益處。此外,閘極氧化層的退化可以被防止,且因 此消除了 Fowler-Nordheim電流所造成的臨界電壓篇移 現象。因此具有防止閘極氧化層崩潰的益處。 當本發明係參照特定實施例而爲描述時,所有的描述 僅爲舉例之用而非用以限制本發明。熟悉本技藝之人士於 (請先閱讀背面之注意事項再填寫本頁) .裝. 訏 線 7 本紙張尺度逋用中國國家標準(CNS ) A4規格(210 X 25>7公釐) A7 B7 五、發明説明(7 ) 不悖離本發明申請專利範圍所定義之眞實精神及範圍的情 況下可有不同修飾。 ---------裝------ΐτΓί.:----線· (請先閱讀背面之注意事項再填寫本頁) 經濟部中央標準局員工消費合作社印策 本紙張尺度適用中國國家標準(CNS ) Α4規格(210X297公釐)
Claims (1)
- 經濟部中央標準局員工消费合作杜印製 293150 ll ___ D8 ☆、申請專利範圍 1. —種使用電漿蝕刻步驟之半導體記憶裝置製造方法,包 括下列步驟: 形成該半導體記憶裝置之相互分離之一閘極複晶砂層 及一橋複晶矽層,其中該閘極複晶矽層係分佈於一主動區 域(active region)內而該橋複晶矽層係分佈於一非主 動區域(inactive region)內; 以一導電材料連接於該閘極複晶矽層與該橋複晶矽層 之間。 2. 如申請專利範圍第1項之方法,其中該電漿蝕刻步驟使 用數百瓦特電位能量的離子化氣體。 3. 如申請專利範圍第1項之方法,其中該導電材料從該閘 極複晶矽至該橋複晶矽層具有不同的導電度。 4. 如申請專利範圍第3項之方法,其中該導電材料係金 屬。 5. 如申請專利範圍第1項之方法,其中該閘極複晶矽與該 橋複晶矽之長度比爲1比1 0或更多。 6. —種半導體記憶裝置之複晶矽閘極,包括一第一複晶砂 層形成於一主動區域(active region),一第二複晶砂 形成於一非主動區域(inactive region),以及一導 電材料連接於該相互分離的第一與第二複晶矽,該導電材 料從該等複晶矽層具有不同的導電度。 9 本紙張尺度適用中國國家梯準(CNS〉A4規格(210 X 297公釐〉 In 1VH J^i tl^^i f^i— i m'- ^ I n^i flun n ϋκ i V~-J^1/1 ^^^^1 nt ^^^^1 - 务 .% J 备 (請先間讀背面之注意事項再填寫本頁)
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KR1019950010174A KR0142118B1 (ko) | 1995-04-27 | 1995-04-27 | 반도체 메모리 소자 제조방법 |
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TW293150B true TW293150B (zh) | 1996-12-11 |
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US (1) | US5736772A (zh) |
JP (1) | JP3108365B2 (zh) |
KR (1) | KR0142118B1 (zh) |
TW (1) | TW293150B (zh) |
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JP3683398B2 (ja) | 1997-12-22 | 2005-08-17 | 株式会社ルネサステクノロジ | 半導体集積回路及びその製造方法 |
JP3461443B2 (ja) | 1998-04-07 | 2003-10-27 | 松下電器産業株式会社 | 半導体装置、半導体装置の設計方法、記録媒体および半導体装置の設計支援装置 |
KR100349348B1 (ko) * | 2000-08-17 | 2002-08-21 | 주식회사 하이닉스반도체 | 반도체 장치의 실리콘층 식각 방법 |
KR101660162B1 (ko) | 2015-03-05 | 2016-10-04 | 고려대학교 산학협력단 | 자율 주행 기반 무인 운반차 시스템 및 이의 제어 방법 |
KR101695557B1 (ko) | 2015-07-17 | 2017-01-24 | 고려대학교 산학협력단 | 자율 주행 기반 무인 운반차 시스템 및 이의 제어 방법 |
KR102425529B1 (ko) | 2020-12-08 | 2022-07-25 | 한남대학교 산학협력단 | 카메라를 이용한 자율주행 지게차 |
KR102437266B1 (ko) | 2021-01-15 | 2022-08-26 | 한남대학교 산학협력단 | 카메라부를 활용한 중장비의 자율주행 네비게이션 시스템 |
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DE3732611A1 (de) * | 1987-09-28 | 1989-04-06 | Siemens Ag | Verfahren zur herstellung eines implantierten source-/drain-anschlusses fuer einen kurzkanal-mos-transistor |
JPH01276762A (ja) * | 1988-04-28 | 1989-11-07 | Seiko Epson Corp | 半導体装置 |
US5581105A (en) * | 1994-07-14 | 1996-12-03 | Vlsi Technology, Inc. | CMOS input buffer with NMOS gate coupled to VSS through undoped gate poly resistor |
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1995
- 1995-04-27 KR KR1019950010174A patent/KR0142118B1/ko not_active IP Right Cessation
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1996
- 1996-03-12 TW TW085102998A patent/TW293150B/zh active
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JPH08306922A (ja) | 1996-11-22 |
US5736772A (en) | 1998-04-07 |
JP3108365B2 (ja) | 2000-11-13 |
KR0142118B1 (ko) | 1998-06-01 |
KR960039379A (ko) | 1996-11-25 |
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