TW409366B - Ferroelectric memory cell and method of making the same - Google Patents
Ferroelectric memory cell and method of making the same Download PDFInfo
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經濟部中央標準扃員工消費合作社印製 ~_409366 五、發明説明(1 ) 發明背景 1 ·發明領域 本案係有關用於非易失性記憶體之鐵電薄膜,特別係有 關金屬-鐵電-金屬-氧化物_碎半導,體。 : 2·相關技術之説明 本案係有關用於非易失性記憶體之鐵電薄膜,及特別係 有關金屬-鐵電;金屬-矽半導體(或淺接面金屬-鐵電-金屬 •碎半導體)。已知鐵電隨機存取記憶體(FRAM )係以一個 電晶體(1T )及一個電容器(1C )構成。電拜器通常係經由 夾置鐵電薄膜於兩個導電電極間製造,該—電極通常爲鉑 製成。此型記憶體之電路構型及讀/寫順序類似習知動態 隨機存取記憶體(DRAM),但FRAM無需資料更新。已知 FRAM有疲勞問題,於鐵電電容器觀察得疲勞問題,此乃 限制此種記憶體之商業用途的—大障礙。疲勞係由於隨著 又換週期數目增加,可交換偏極化下降(儲存的非易失性 電‘荷減少)。用於本例,「交換週期」.表示記憶體之讀與 寫脈衝總和。 鐵電薄膜用於記憶體應用之另—種已知用途係經由直接 沉積鐵電薄膜於FET閘區上形成鐵電閘控場效電晶體 (FET)。此種鐵電閘控裝置已知一}吃間及包括稱做金屬 -鐵電-石夕(MFS) FET之裝,置。合併MFS FET結構之F R A Μ ’、有兩大優於電晶體-電容器構型的優點:.(1) Mps fet佔 據表面積較少,及(2)提供非破壞性讀出(NDR)。後述特 性可使MFS FET裝置讀取數千遍而未交換鐵電偏極化。因 —™ 本紙張尺度適财關家縣(CNS ) A4規格(.2]Qx297公楚) < ---X3水— (婧先閱讀背面之注意事項再填^本瓦) 訂 A7 B7 五、發明説明(2 ) 此使用MFS FET裝置時疲勞不成問題。可構成各型MFS FET結構,例如金屬鐵電絕緣體矽(MFIS) FET,金屬鐵電 金屬矽(MFMS) FET及金屬鐵電金屬氧化物矽(MFMOS) FET 0 ;ι 欲製造有效MFS FET裝置必須克服多種問題。第一個問 題爲難以於矽上直接形成可接受的結晶性鐵電薄膜。此種 結構適於美國專利第3,832,700號。此外,極難以於鐵電材 料與矽間具有^淨介面。又有一個問題係有關鐵電材料之 適當電荷。閘區上之FEM結構顯示於美國淨利第5,303,182 號,其強調金屬離子移轉至閘區乃非期望^。類似結構顯 示於美國專利第5,416,735號。 本發明之目的係克服前_述問題。 本發明之目的係提供一種可提供非破壞性讀出之MFS FET裝置。 本發明之另一目的係提供佔據相對較小表面積之MFS FET裝置。 本發明之另一目的係提供一種需要相對低程式规劃電壓 之MFS FET裝置。 經濟部中央標準局員工消費合作社印製 (請先閱讀背面之注意事項再填寫本頁) 本發明之另一目的係提供一種具有極低漏電流之FEM記 憶單元。 . 本發明之另一目的係提供一種包括MOS電晶體上方鋪設 / FEM單元之MFS FET裝置。 本發明之另一目的係提供一種鋪置於淺接面ϊΓ層上之 FEM閘單元,該ρ·層延伸超出FEM閘單元邊緣。 _ 5 _ ,, V-1 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) 409366 A7 B7 五、發明説明(3 ) '" 本發明气另一目的係提供一種其中含有容易形成的擴散 障層之FEM單元。 本發明1之另一目的係提供一種包括汲極電極其接觸n+及 P導電面之FEM單元。 ( 本發明之另一目的係提供一種佔據相對小表面積且需要 相對低程式规劃電壓之FEM裝置。 本發明之另二目的係提供一種具有非對稱鐵電偏極化之 FEM閘單元。〆 發明概述- ?1 本發明之形成FEM單元半導體結構之方_包括對矽基板 上的鐵電記憶體FEM閘單元形成一個裝置區。適當雜質植 入裝置區形成導電通路供用作源極接面區,閘極接面區及 汲極接面區。FEM單元包括形成於基板上的FEM閘單元。 閘極接面區對FEM閘單元裝置區上的FEM閘單元形成於源 極接面區與汲極接面區間,該FEM閘單元包括下金屬層, 鐵電(FE)層及上金屬層•蕭^(Sch〇tt:y)障層或極淺接面 層形成於FEM閘單元與閘極接面區間作爲另—導電通路。 FEM閘單元與源極區及閘極區隔開。依據其它建立於基板 上裝置而定’及依據各種構造順序之效率而定,形成多種 導電通路可於多個製造嘴段進行。 FEM單元半導體結構包,括一個基板其可爲本體♦基板或 SOI型基板’第一及第二型導電通路形成於基板上,—個 FEM閘單元形成於閘極區上,其中該]pem閘單元包括—層 下金屬層’一層FE層及一層上金屬層,,及其中—條第二 -6 - : 说尺度適財關家轉(CNS ) A视格(21GX297公楚) "~1" ^-~~~—-- (請先閱讀背面之注意事項再填寫本頁) 衣. 訂 -d. 經濟部中央標準局員工消費合作社印製. 經濟部中央標準局員工消资合作社印製 噠 0ί)366 五、發明説明(4 〉 ' 型導電通路形成於FEM閘單元與閘極區間/ FEM單元可與 習知MOS電晶體串聯構造。 本發明形成兩種電晶體半導體結構之方法包括於矽基板 上形成MOS電晶體及鐵電記憶體(FEM)閘單:元之裝置區。 適當雜質植入裝置區形成導電通路供用作源極接面區,閘 極接面區及汲極接面區。習知M〇s電晶體形成於基板 上。FEM單元包括—個形成於基板上的FEM閘單元’可位 於MOS電晶體上方或沿其旁側。閘極接面區形成於fem 閘單元之源極接面區與汲極接面區闓,該gEM閘單元包括 下金屬層’鐵電(FE)層及上金屬層。FEM:閘單元與源極 區及汲極區隔開,如同FEM閘單元與閘極接面區間的導電 通路般。依據建立於基板上的其它裝置而定及依據多種構 造順序之效率而定,形成多條導電通路可於多個製造階段 進行。 二電晶體半導體結構包含矽基板,其可爲本體矽基板或 SOI型基板"三類型導電通路皆位於基板上方。FEM閘單 元·位於閘極區上方,可於習知MOS電晶體上方或沿其旁 侧,其中該FEM閘單元包括下金屬層,fe層及上金屬 層〇 . 本發明之形成FEM單牟半導體結構之方法包括於矽基板 上形成鐵電記憶體FEM閘,單元之裝置區。適當雜質植入裝 置區形成導電通路,供用作源極接面區,閘極接面區及没 極接面區。FEM單元包括一個形成於基板上的FEM閘單 元。對FEM閘單元裝置區上FEM閘單元形成—個閘極接面 本紙乐尺度適用中國國家標準(CNS ) A4規格(2丨OX 297公釐) ^ ,4 Bn ,--------ο农---------IT------0 (請先閲讀背面之注意事項再填寫本莧) 經濟部中央標準局負工消費合作社印製 409366 A7 —---_; 67__ 五、發明説明(s ) 區介於源極接面區與没極接面區間,該FEM閘單元包括下 金屬層’鐵電(FE)層及上金屬層。淺接面區形成於fem 閘單元與閘極接面區間作爲另一導電通路。如同介於fem 閑單元與閘極接面區間的導電通路般,fem,閉單元與源極 區及没極區隔開。依據其它建立於基板上的裝置而定及依 據各種構造順序之效率而定,形成多姻導電通路可於各製 造階段進行。 FEM單元半 < 體結構包括一個基板其可爲本體矽基板或 s〇i型基板。第一及第二型導電通路位於拳板上方。 閘單元位於通路區上方,其中jtem閘單元包括下金屬層, FE層及上金屬層β第三型導電通路位於fEM閘單元與通 路區間。FEM單元可與習知M0S電晶體串聯構成。 本發明之形成FEM單元半導體結構之方法包括於矽基板 上形成鐵電記憶體FEM閘單元之裝置區。適當雜質植入該 裝置形成導電通路供用作源極接面區,閘極接面區及汲極 接面區。:FEM單元包括一個FEM閘單元形成於基板上。對 FEiM閘單元裝置區上的FEM閘單元形成一個閘極接面區介 於源極接面區與汲極接面區間,該FEM閘單元包括下金屬 層’鐵電(FE)層及上金屬層。淺接面層形成於fem閘單 元與閘極接面區間作爲乃一導電通_路二其延伸入汲極接面 區内。如同FEM閘單元产閘極接面區間的導電通路般, FEM閘單元係與源極區及汲極區隔開。依據基板上建立何 種其它裝置而定及依據各種構成順序之效率而定,多條導 電通路之形成可於多個製造階段進行。 -8 - 本紙張尺度適用中國國家標準(CNS ) A4規格(21〇X297公楚) (請先閱讀背面之注意事項再填寫本頁) 訂 i. 409B66 B7 五、發明説明(6 ) FEM單元半導體結構包括矽基板,其可爲本體矽基板或 SOI型基板。兩型導電通路位於基板上方。FEM閘單元位 於閘極區上方,其中FEM閘單元包括下金屬層,FE層及 上金屬層。另一第三型導電通路位於FEM附單元與通路區 間及延伸入汲極區。FEM單元可與習知MOS電晶體串聯 構成。 於矽基板上形成半導體記憶體装置之方法包括植入第一 類型攙雜雜質i矽基板而形成第一型導電通路供用作閘極 區;於第一型導電通路上形成MOS電容If ;沉積FEM電 容器於MOS電容器上,包括沉積下金屬層FE層及上金 屬層,因此形成堆疊閘單元;於閘極區任一侧上植入第二 類型攙雜雜質於矽基板而形成第二型導電通路供用作源極 接面區及汲極接面區;及沉積絕緣結構包圍FEM閘單元周 園。. 經濟部中央標準局負工消費合作社印製 (諳先閲讀背面之注意事項再填"本頁)Central Standard of the Ministry of Economic Affairs 印 Printed by Employee Consumer Cooperatives ~ _409366 V. Description of the Invention (1) Background of the Invention 1 · Field of the Invention This case relates to ferroelectric thin films used for non-volatile memory, especially to metal-ferroelectric-metal -Oxide_fragmented semiconducting, body. : 2 · Description of related technology This case is about ferroelectric thin film for non-volatile memory, and especially about metal-ferroelectric; metal-silicon semiconductor (or shallow junction metal-ferroelectric-metal · broken semiconductor) ). It is known that a ferroelectric random access memory (FRAM) is composed of a transistor (1T) and a capacitor (1C). An electric worshipper is usually made between two conductive electrodes by sandwiching a ferroelectric film. The electrode is usually made of platinum. The circuit configuration and read / write sequence of this type of memory are similar to the conventional dynamic random access memory (DRAM), but FRAM does not require data update. FRAM is known to have fatigue problems, and fatigue problems observed in ferroelectric capacitors are a major obstacle limiting the commercial use of such memory. Fatigue is due to the increase in the number of cycles, and the exchangeable polarization decreases (the stored non-volatile charge decreases). For this example, the "swap cycle" means the sum of the read and write pulses of the memory. Another known use of ferroelectric thin films for memory applications is to form ferroelectric gated field effect transistors (FETs) on the FET gate region by directly depositing the ferroelectric thin film. This type of ferroelectric gate control device is known as a cabinet and includes a device called a metal-ferroelectric-stone evening (MFS) FET. Merging the F R A M 'of the MFS FET structure has two major advantages over the transistor-capacitor configuration: (1) Mps fet occupies less surface area, and (2) provides non-destructive readout (NDR). The features described below enable MFS FET devices to read thousands of times without exchanging ferroelectric polarization. Because — ™ This paper is suitable for Guancai County (CNS) A4 size (.2) Qx297 Gongchu < --- X3 water — (Jing first read the notes on the back before filling ^ this tile) Order A7 B7 5 2. Description of the invention (2) When using the MFS FET device, fatigue is not a problem. Can form various types of MFS FET structures, such as metal ferroelectric insulator silicon (MFIS) FET, metal ferroelectric metal silicon (MFMS) FET and metal ferroelectric metal oxide silicon (MFMOS) FET 0; ι To make an effective MFS FET device must Overcoming multiple problems. The first problem is that it is difficult to form an acceptable crystalline ferroelectric thin film directly on silicon. This structure is suitable for U.S. Patent No. 3,832,700. In addition, it is extremely difficult to have a clean interface between ferroelectric materials and silicon. Another issue concerns the proper charge of ferroelectric materials. The FEM structure on the gate is shown in US Net Profit No. 5,303,182, which emphasizes that the transfer of metal ions to the gate is not expected ^. A similar structure is shown in U.S. Patent No. 5,416,735. The object of the present invention is to overcome the aforementioned problems. An object of the present invention is to provide an MFS FET device capable of providing non-destructive readout. Another object of the present invention is to provide an MFS FET device occupying a relatively small surface area. Another object of the present invention is to provide an MFS FET device requiring a relatively low programming voltage. Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs (please read the notes on the back before filling out this page) Another object of the present invention is to provide a FEM memory unit with extremely low leakage current. Another object of the present invention is to provide an MFS FET device including a MOS transistor / FEM unit. Another object of the present invention is to provide a FEM gate unit which is laid on the 接 Γ layer of the shallow junction, and the p · layer extends beyond the edge of the FEM gate unit. _ 5 _ ,, V-1 This paper size is in accordance with Chinese National Standard (CNS) A4 specification (210X297 mm) 409366 A7 B7 V. Description of the invention (3) '" Another object of the invention is to provide an FEM unit of the formed diffusion barrier. Another object of the present invention is to provide a FEM unit including a drain electrode in contact with the n + and P conductive surfaces. (Another object of the present invention is to provide a FEM device occupying a relatively small surface area and requiring a relatively low program voltage. Another object of the present invention is to provide a FEM gate unit with asymmetric ferroelectric polarization. 〆 Summary of the invention -? 1 The method for forming a semiconductor structure of the FEM unit of the present invention includes forming a device region for a ferroelectric memory FEM gate unit on a silicon substrate. Appropriate impurities are implanted into the device region to form a conductive path for use as a source junction region, The electrode junction area and the drain junction area. The FEM unit includes a FEM gate unit formed on the substrate. The gate junction area is opposite the FEM gate unit on the FEM gate unit device area and is formed at the source junction area and the drain junction. Area, the FEM gate unit includes a lower metal layer, a ferroelectric (FE) layer, and an upper metal layer. (Schott: y) barrier layer or very shallow contact layer is formed at the interface between the FEM gate unit and the gate. The interval serves as another conductive path. The FEM gate unit is separated from the source region and the gate region. It depends on other devices built on the substrate 'and on the efficiency of various structural sequences. Forming multiple conductive paths can be manufactured in multiple Mouth section. FE The M-unit semiconductor structure includes a substrate, which can be a body. The substrate or an SOI substrate is formed by the first and second conductive paths, and a FEM gate unit is formed on the gate region. The unit includes-a lower metal layer, a FE layer, and an upper metal layer, and among them, the second-6-: said that the scale is suitable for wealth and family (CNS) A view grid (21GX297), " ~ 1 " ^-~~~ --- (Please read the notes on the back before filling out this page) Clothing. Order -d. Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs. Printed by the Consumers Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs Da 0) 366 V. Description of the invention (4>) The "type" conductive path is formed in the FEM gate unit and the gate interval / FEM unit can be connected in series with the conventional MOS transistor. The method of the present invention for forming two transistor semiconductor structures includes A MOS transistor and a ferroelectric memory (FEM) gate: a device region are formed on a silicon substrate. Appropriate impurities are implanted into the device region to form a conductive path for use as a source junction region, a gate junction region, and a drain junction. Area. The conventional Mos transistor is formed on the substrate. FEM single It includes a FEM gate unit formed on the substrate, which can be located above or along the MOS transistor. The gate junction area is formed at the source junction area and the drain junction area of the fem gate unit. The gEM The gate unit includes a lower metal layer, a ferroelectric (FE) layer, and an upper metal layer. FEM: The gate unit is separated from the source region and the drain region, as is the conductive path between the FEM gate unit and the gate interface. Depending on the other devices on the substrate and the efficiency of various construction sequences, the formation of multiple conductive paths can be performed at multiple manufacturing stages. The two-transistor semiconductor structure includes a silicon substrate, which can be a bulk silicon substrate or an SOI-type substrate " Three types of conductive paths are located above the substrate. The FEM gate unit is located above the gate region, and can be above or along the side of the conventional MOS transistor. The FEM gate unit includes a lower metal layer, a fe layer, and an upper metal layer. The structure method includes forming a ferroelectric memory FEM gate on a silicon substrate, and a device area of the unit. Appropriate impurity implantation device regions form conductive paths for use as source contact areas, gate contact areas, and non-contact contact areas. The FEM unit includes a FEM gate unit formed on a substrate. For the formation of the FEM gate unit on the FEM gate unit installation area, a paper gate scale is applicable to the Chinese National Standard (CNS) A4 specification (2 丨 OX 297 mm) ^, 4 Bn, -------- οAgriculture --------- IT ------ 0 (Please read the notes on the back before filling in this 苋) Printed by the Consumers Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs 409366 A7 ------- 67__ 5. Description of the invention (s) The region is between the source junction region and the non-electrode junction region. The FEM gate unit includes a lower metal layer, a ferroelectric (FE) layer, and an upper metal layer. The shallow junction area is formed in the interval between the fem gate unit and the gate electrode as another conductive path. Just like the conductive path between the fem free cell and the gate interface, the fem, closed cell is separated from the source and non-electrode regions. Depending on the other devices built on the substrate and the efficiency of various construction sequences, forming multiple conductive paths can be performed at various manufacturing stages. The FEM unit half < body structure includes a substrate which can be a bulk silicon substrate or a soi-type substrate. The first and second conductive paths are located above the fist. The gate unit is located above the passage area. The jtem gate unit includes a lower metal layer, an FE layer and an upper metal layer. The third type conductive path is located between the fEM gate unit and the passage. The FEM unit can be formed in series with a conventional MOS transistor. The method for forming a semiconductor structure of an FEM unit of the present invention includes forming a device region of a ferroelectric memory FEM gate unit on a silicon substrate. Appropriate impurities are implanted into the device to form a conductive path for use as a source junction area, a gate junction area, and a drain junction area. : The FEM unit includes a FEM gate unit formed on the substrate. A gate junction area is formed between the source junction area and the drain junction area of the FEM gate unit on the FEIM gate unit device area. The FEM gate unit includes a lower metal layer, a ferroelectric (FE) layer, and an upper metal. Floor. The shallow junction layer is formed in the interval between the fem gate unit and the gate electrode as a conductive pathway, which extends into the drain junction region. The FEM gate unit is separated from the source region and the drain region just like the conductive path in the gate contact area of the FEM gate unit. Depending on what other devices are built on the substrate and the efficiency of various constituent sequences, the formation of multiple conductive paths can be performed at multiple manufacturing stages. -8-This paper size applies to Chinese National Standard (CNS) A4 specification (21 × 297). (Please read the precautions on the back before filling this page.) Order i. 409B66 B7 V. Description of the invention (6) FEM unit semiconductor The structure includes a silicon substrate, which can be a bulk silicon substrate or an SOI type substrate. Two types of conductive paths are located above the substrate. The FEM gate unit is located above the gate region. The FEM gate unit includes a lower metal layer, an FE layer and an upper metal layer. Another third type of conductive via is located between the FEM attachment unit and the via region and extends into the drain region. The FEM unit can be formed in series with a conventional MOS transistor. A method for forming a semiconductor memory device on a silicon substrate includes implanting a first type doped impurity silicon substrate to form a first type conductive path for use as a gate region; forming a MOS capacitor If on the first type conductive path; and depositing a FEM capacitor On MOS capacitors, a lower metal layer FE layer and an upper metal layer are deposited to form a stacked gate unit; a second type of doped impurity is implanted on a silicon substrate on either side of the gate region to form a second type conductive path for use as The source junction region and the drain junction region; and the deposited insulation structure surrounds the FEM gate unit perimeter. Printed by the Consumers' Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs (谙 Please read the notes on the back before filling in " this page)
根據本發明構成之鐵電記憶體(FEM )單元包括一片矽基 板;一個閘極區位於該基板,經攙雜而形成第一型導電通 路:;一個源極接面區及一個汲極接面區位於基板之閘極區 之任一側上,經攙雜而形成一對第二型導電通路;一個 MOS電容器包括一層氧化物層及第三型導電層位於閘極 接面區上,其中MOS電多器具有預定表面積;一個FEM 電容器包括下金屬層,:FE層及上金屬層;其中該FEM電 / 容器堆疊於及鋪置於MOS電容器之至少部分上,因此與 MOS電容器形成一個堆疊閘單元;一層絕緣層具有上表 面鋪置於接面區、堆疊閘單元及基板上;及一個源極電極 -9- 本紙張尺度適用中國國家標牟(CNS ) A4規格(210X297公釐)A ferroelectric memory (FEM) unit constructed according to the present invention includes a silicon substrate; a gate region is located on the substrate, and a first type conductive path is formed by doping: a source junction region and a drain junction region It is located on either side of the gate region of the substrate and is doped to form a pair of second-type conductive paths. A MOS capacitor includes an oxide layer and a third-type conductive layer on the gate junction area. The device has a predetermined surface area; a FEM capacitor includes a lower metal layer: an FE layer and an upper metal layer; wherein the FEM capacitor / container is stacked on and laid on at least part of the MOS capacitor, and thus forms a stacked gate unit with the MOS capacitor; An insulating layer has an upper surface laid on the interface area, the stack gate unit and the substrate; and a source electrode-9- This paper size is applicable to China National Standards (CNS) A4 specifications (210X297 mm)
經濟部中央標準馬員工消費合作杜印製 409366 A7 B7 五、發明説明(7 ) ‘ 及—個没極電極各自位於絕緣層之上表面上及延伸貫穿絕 緣層而與其個別接面區做電接觸;及一個閘極電極位於絕 緣層上表面上及延伸貫穿絕緣層而與堆疊閘單元之上金屬 層做電接觸。 本發明之此等及其它目的及優點經由連同附圖研讀後文 説明將更完整明瞭。 圖式之簡單説明 圖1及圖2闡明形成用於本發明之FEM單元之基板之循 序步踩範例。 圖3闡明於基板上構成的FEM閘單元。 圖4闡明本‘發明之FEM單元之具體例,其含有一層矽層 形成於FEM閘單元下方 圖5闡明用於本發明之另—具體例之基板之製備。 圖6闡明形成於p導電層上之本發明之FEM.閘單元之另 二本發明之FEM單元之電流流動。 t本發明之MFSFET裝置之基本作業原理。 發明之FEM閘單元之ID相對於之線圖,Department of Economics, Central Standard, Malaysia, Consumer Cooperation, Du Printed 409366 A7 B7 V. Description of Invention (7) 'and a non-polar electrode are located on the surface of the insulation layer and extend through the insulation layer to make electrical contact with its individual interface area And a gate electrode is located on the upper surface of the insulating layer and extends through the insulating layer to make electrical contact with the metal layer above the stacked gate unit. These and other objects and advantages of the present invention will become more complete and clear by studying the following description in conjunction with the accompanying drawings. Brief Description of the Drawings Figures 1 and 2 illustrate examples of sequential steps for forming a substrate for a FEM unit of the present invention. Figure 3 illustrates a FEM gate unit constructed on a substrate. Fig. 4 illustrates a specific example of the FEM unit of the present invention, which includes a silicon layer formed under the FEM gate unit. Fig. 5 illustrates the preparation of a substrate for another specific example of the present invention. Fig. 6 illustrates the current flow of another FEM unit of the FEM. Gate unit of the present invention formed on a p-conductive layer. tThe basic operating principle of the MFSFET device of the present invention. Line diagram of the ID of the invented FEM gate unit,
圖10-13闡明用於本發明之FEM單元製備基板及形成活 性區之循序階段P 圖1 4闡明如於本體矽声板上構成的完整二電晶體記憶 單元。 圖15闡月於SOI基板上構成的完整二電晶體記憶單元。 圖1 6闡明於SOI基板上構成的完整二電晶體記憶單元之 -10 本紙張尺賴财_家榡^TCNS )八4了見格(2I0X297公幻 f (諳先閲讀背面之注意事項再填寫本頁)Figures 10-13 illustrate the sequential stages P of the FEM unit preparation substrate and active area formation used in the present invention. Figure 14 illustrates the complete two-transistor memory cell as constructed on a bulk silicon acoustic board. FIG. 15 illustrates a complete two-transistor memory cell formed on an SOI substrate. Figure 16 illustrates a complete two-transistor memory cell constructed on an SOI substrate. -10 paper rule Lai Choi_ 家 榡 ^ TCNS (This page)
4093G6 A7 B7 五、發明説明(8 ) 另一具體例。4093G6 A7 B7 V. Description of the invention (8) Another specific example.
經濟部中央標準局員工消費合作社印裝 本發明之記憶單元之4 X 4陣列。 證本發明之MFSFET装置之基本作業原理。 發明之FEM閘單元之ID相對於尤線圖。 圖20闡明用於本發明之FEM單元之基板及浩性區。 圖2 1闡明其上形成有FEM閘單元之基板。 圖22闡明於基板上構成且由絕緣區包圍之FEM閘單 元。 圖2 3闡明本發明之FEM閘單元於基板上附有形成源 極、閘極及没極區。 圖24闡明本發明之;ρΕΜ單元具有淺接面層形成於FEM 閘單元下方。 _ 圖2 5激ΐ!月本發明之完整FEM單元,也闡明流過其中之 電流 圖本發明之MFS FET裝置之基本作業原理 -圖發明之FEM閘單元之ID相對於VGt線圖。 :圖28-3:0闡明用於本發明之ϊέμ單元製備基板及形成活 性區之循序階段& 圖3 1闡明構成於基板上且由絕緣區包圍的FEM閘單 元。 圖32闡明本發明之FEM閛單元於基板上附有形成源 t 極、閘極及汲極區。 圖33闡明本發明之FEM單元具有淺接面層形成於FEM 閘單元下方。 11 本纸張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) (請先閱讀背面之注意事項再填Ϊ?本頁) hi 五·、發明説明(9 409366 A7 B7 圖34闡明本發明之完整FEM單元及亦闡明流經其中的 _電流。 圖35闡明於本體♦基板上形成的FEM單元之替代具_ 例。 ' 圖3^^1^於301基板上形成的FEM單元之替代具體例。 圖本發明之MFSFET裝置之基本作業原理。 圖發明之FEM閘單元之ID相對於VG之線圖a 圖39闡明一 ^矽基板其已經製妥而有助於構成本發明 之FEM單元。 _ , 圖論聞明根據本發明構成之單一電晶體“偏位堆疊閘單 码-圖4^〇;名圏 一闡朗根據采發朋構成之堆疊電晶體閘極構造之Printed by the Consumer Standards Cooperative of the Central Bureau of Standards of the Ministry of Economic Affairs of the present invention, a 4 X 4 array of memory cells. Prove the basic operation principle of the MFSFET device of the present invention. The ID of the invented FEM gate unit is relative to the graph. FIG. 20 illustrates a substrate and a fertile region for a FEM unit of the present invention. FIG. 21 illustrates a substrate on which a FEM gate unit is formed. Fig. 22 illustrates a FEM gate unit formed on a substrate and surrounded by an insulating region. FIG. 23 illustrates that the FEM gate unit of the present invention has a source electrode, a gate electrode, and a non-electrode region attached to a substrate. Figure 24 illustrates the present invention; the pEM unit has a shallow junction layer formed below the FEM gate unit. _ Figure 25: The complete FEM unit of the present invention also clarifies the current flowing through it. The basic operating principle of the MFS FET device of the present invention-The ID of the FEM gate unit of the invention is compared to the VGT line diagram. : Figures 28-3: 0 illustrate the sequential stages of preparing substrates and forming active regions for the hand-mu cells used in the present invention & Figure 31 illustrates the FEM gate units formed on the substrate and surrounded by insulating regions. FIG. 32 illustrates that the FEM unit of the present invention has a source t-gate, a gate, and a drain region formed on a substrate. FIG. 33 illustrates that the FEM unit of the present invention has a shallow junction layer formed under the FEM gate unit. 11 This paper size applies Chinese National Standard (CNS) A4 specification (210X297 mm) (Please read the notes on the back before filling out this page) hi V. Description of the invention (9 409366 A7 B7 Figure 34 illustrates the invention The complete FEM unit and the current flowing through it are also illustrated. Figure 35 illustrates an example of the replacement of the FEM unit formed on the main body substrate. 'Figure 3 ^^ 1 ^ The specific replacement of the FEM unit formed on the 301 substrate For example, the basic operating principle of the MFSFET device of the present invention is shown. Figure of the ID of the FEM gate unit of the invention vs. VG. _, Picture theory, the single transistor formed according to the present invention "offset stack gate single code-Figure 4 ^ 〇; Ming Yi explained the structure of the stacked transistor gate structure based on mining
1—··-1 Λ -I I: -- ^^1 1^1 1^1 (Λ-^fe^—r. I {請先閱讀背面之注意事項再填寫本頁} r」ii 、1 經濟部中央標準局員工消費合作社印製 圖46-49闡明構成根據本發明組成之單一電晶體堆叠閘 單元之變化例之循序步骤。 ‘圖5〇_^]於本發明之FE之Ρ-Ε磁滯迴線圖。 圖sijg^jsib分別爲本發明裝置於「0 J態及「i」態之電荷彳 圖岁發明之FEM閘單元之ID相對於VG之線圖 圖5 根據本發明構成之FEMj $。 ,發明之FEM,單元之ID相對於VG之線圖 多種FEM閘單元之P-E磁滯迴線。 本發明之MFS FET裝置之基本作業原理 圖57闡明根據本發明構成之記憶體陣列。1— ·· -1 Λ -II:-^^ 1 1 ^ 1 1 ^ 1 (Λ- ^ fe ^ —r. I {Please read the precautions on the back before filling this page} r ”ii, 1 Economy Figures 46-49 printed by the Ministry of Standards and Staff's Consumer Cooperatives illustrate the sequential steps of a variation example of a single transistor stacked gate unit composed according to the present invention. 'Figure 5〇_ ^] The P-E magnetic field of the FE of the present invention Hysteresis diagram. Figure sijg ^ jsib is the charge of the device in the "0 J state" and "i" state of the device according to the invention. Figure 5 shows the ID of the FEM gate unit versus the VG of the invention. Figure 5 FEMj constructed according to the invention $. The invented FEM, the unit ID is relative to the VG, and the PE hysteresis loops of various FEM gate units. Basic operating principle of the MFS FET device of the present invention Figure 57 illustrates a memory array constructed according to the present invention.
-12- 表紙張尺度適用中國國家標準(CNS ) Μ規格(2】0X297公釐) ό 經濟部中央標準局員工消費合作社印裝 409366 at ‘ B7 五、發明説明(10 ) ‘ 較佳具體例之説明 (實例1) 本實例之鐵電記憶體(FEM)單元可於s〇I (SiM〇x)基板 上形成,或可形成於本體矽基板其中形成7個〆阱。初步 説月术中在於SIMOX基板上形成fem閘單元。須了解fem 閘單元之若干具體例中,M〇s電晶體係藉業界人士眾所 周知的習知手,與鐵電記憶單元同時製造。如此爲求清晰 起見,附圖未闡明MOS電晶體的形成^ 現在參照圖1,SIMOX基板闡明於3 〇 ^ _佳具體例中基 板3 0係由二氧化矽形成且爲單晶基极β如_ j闡明,基板 30已經可以部分蝕刻成闡明的構型,及部分基板已經輕 度攙雜而形成一個活性區或裝置區32,其提供所需背景 極性’本例中知;供η區之背景極性β如業界人士眾所周 知’多個此種區形成於一片矽晶圓表面上。用於本發明之 FEM閘單元,單元排列於垂直格柵而形成一個記憶體陣 列。 初步説明基板之概略形成及製備方法,j?EM閘單元將鋪 置於基板上,最終結果形成FEM記憶單元。活性區3 2邊 緣包圍非活性區或絕緣區30a,30b,其爲基板3 〇之向上 延伸部。基板一區形成溝渠,概亨闡明於34,36,溝渠 區最終以絕緣材料通常爲/二氧化矽填補。 現在參照圖2,可見活性區3 2已經修改成源極區3 8, 閘極區4 0及汲極區4 2 。此等區係經由施用光阻跨越活 性區32遮蔽,最終將變成閘極區40之區及將適當離子 -13- 未紙張尺度適用中國國家梯举·( cns )Λ4規格(2ΐ〇χ.297公t)-12- The paper size of the table applies the Chinese National Standard (CNS) M specification (2) 0X297 mm) ό Printed by the Consumer Cooperatives of the Central Bureau of Standards of the Ministry of Economic Affairs 409366 at 'B7 V. Description of the invention (10)' Explanation (Example 1) The ferroelectric memory (FEM) unit of this example can be formed on a SOI (SiMOx) substrate, or it can be formed on a bulk silicon substrate to form 7 counterbores. It is said that the fem gate unit is formed on the SIMOX substrate during the moon operation. It should be understood that in some specific examples of fem gate units, the MOS transistor system is manufactured at the same time as the ferroelectric memory unit by well-known hands in the industry. So for the sake of clarity, the drawing does not clarify the formation of MOS transistors. ^ Now referring to FIG. 1, the SIMOX substrate is illustrated at 3 ^ ^ In a specific example, the substrate 30 is formed of silicon dioxide and is a single crystal base β. As stated by _j, the substrate 30 can already be partially etched into the clarified configuration, and part of the substrate has been slightly doped to form an active region or device region 32, which provides the required background polarity, 'known in this example; for the n region The background polarity β is well known in the art. 'A plurality of such regions are formed on the surface of a silicon wafer. The FEM gate unit used in the present invention is arranged in a vertical grid to form a memory array. The rough formation and preparation method of the substrate will be explained initially. The j? EM gate unit will be laid on the substrate, and the final result will form a FEM memory unit. The edges of the active region 32 surround the inactive or insulating regions 30a, 30b, which are upward extensions of the substrate 30. A trench was formed in the first area of the substrate, which was explained at 34, 36. The trench area was finally filled with insulating material, usually silicon dioxide. Referring now to FIG. 2, it can be seen that the active region 32 has been modified into a source region 38, a gate region 40 and a drain region 4 2. These areas are shielded by applying photoresistance across the active area 32, and will eventually become the area of the gate area 40 and the appropriate ions will be applied to the Chinese National Elevation Standard (cns) Λ4 (2ΐ〇χ.297) T)
(請先閱讀背面之注意事項再填筠本頁;I(Please read the notes on the back before filling out this page; I
經濟部中央標準局員工消費合作社印製 —------409308 Β7 五、發明説明(11 ) 植入活性區32其餘部分形成兩層η+層,此處也稱做第一 型導電通路,將作爲源極區38及汲極區42形成。本例 义適當離子植入可於較佳能量約5〇 keV植入砷離子,但 植入40 keV至70 keV之範圍可接受,及劑量係於〜切, 平方厘来至5x1015/平方厘米之範圍。另外,磷離子可於 相同劑量範圍以30 keV-60 keV之能量範圍植入。然後晶 圓加為處理而激發及擴散植入的離子。加熱處理之溫度範 圍爲 5〇〇6c 至 lloo X:。 此時可開始形成FEM閘單元。現在參照\圓3 , FEM閘單 元概略標示於44及包括下電極46,鐵電(F;E)材料48及上 電極5 0。FEM閘單元4 4之構成始於沉積下電極於閘極區 40上,此處也稱做第二型導電通路。下電極46可由銘或 銥,鉑/銥合金或其它適當導電材料製成。金屬厚度爲2〇 毫微米至1〇〇毫微米。 其次,FE材料藉化學蒸氣沉積(CVD)沉積。FE材料可 爲下列任一者:Pb(Zr,Ti)03 (PZT),SrBi2Ta209 (SBT), PhGesOn,BaTi〇3,或LiNb〇3。較佳化合物之較佳順序爲 PbsGesOu ’ SBT及PZT。FEM閘單元領域的大半實驗工作 係對PZT化合物進行a fe材枓48沉積至1〇〇毫微米至4〇〇 毫微米厚度。 · 然後上電極50形成於gE材料上。上電極可由下電極的 相同材料形成至20毫微米至200毫微米厚度。導電通路前 驅物標示於52 ^此種前.驅物最終藉著金屬離子由下電極 46擴散入閘極區40變成金屬矽化物層。 __ -14- 二 ____· 本紙張尺度制中觸家縣(CNS ) A视格(2!GX297讀) :—~ ~~--- f靖先閱锖背面之注意事項再填寫本頁j -訂_ -JU. A7 B7 409366 五、發明説明(12 ) 光阻施用於FEM閘單元上,然後單元蝕刻成適當構形及 尺寸°須了解三層FEM閘單元如所示無需準確對正,原因 爲其形狀可經由施加光阻及以具有不同幾何的阻罩蝕刻形 成。但爲清晰起見,FEM閘單元闡明爲具有:鄰接對正側壁 的結構。 現在參照圖4,FEM閘單元4 4闡明爲FEM記憶單元5 3之 部件,其包括FEM閘單元4 4及下方源極區、通路區及没 極區,該具體例包括一層形成於FEM閘單元4 4下方之;5夕 化物薄層54,導電通路前驅物52位於此砗。如本發明方 法之第二具體例所述,砂化物層5 4可於沉積FEM閘單元 44各組件前形成;或假定下電極46係由鉑(pt)或其合金 製成’可Ί吏鉑擴散入閘極區4 0上部,形成淺矽化物層其 作爲蕭隄障層,於此處稱做第三型導電通路。 氧化鈦5 6或其它適當障層絕緣材料層係藉CVD形成俾 保護FEM閘單元。氧化鈦經蝕刻形成閘極電極之侧壁絕緣 層°光阻經施用及適當n+及P+區藉離子植入形成。氧化物 層係藉CVD形成或應用其它適當鈍化絕緣。結構體於5〇〇 C至1000X:加熱處理而使植入的離子鈍化及擴散。欲完整 説明FEM單元53 ,於氧化物層58及源極電極6〇、閘極電 極62及汲極電極64形成搪孔且連^至多個別组件。 圖4闡明之具體例表示产發明結構‘最簡單μ。結構爲 鐵電閉極耗盡她S電晶體。於〇閘極電壓,刪閉單元 下万η通路之電荷完全耗盡。因此漏電流極小。欲維持小 的漏“ u下電極46接觸η砂之任何邊緣該點與η+源極區 Μ民張尺度適用家標準(CNS ) (锖先閱請背面之注意事項再填寫本1)Printed by the Consumer Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs ------- 409308 B7 V. Description of the Invention (11) The rest of the active area 32 is implanted to form two layers of η + layers, which is also called the first type conductive path here , Will be formed as the source region 38 and the drain region 42. In this example, the appropriate ion implantation can implant arsenic ions at a preferred energy of about 50 keV, but the range of implantation from 40 keV to 70 keV is acceptable, and the dose is from ~ cut, square centimeter to 5x1015 / cm2. range. In addition, phosphorus ions can be implanted in the same dose range with an energy range of 30 keV-60 keV. The wafers then excite and diffuse the implanted ions for processing. The temperature range of the heat treatment is 506c to lloo X :. At this point, the formation of the FEM gate unit can begin. Now referring to \ circle 3, the FEM gate unit is roughly indicated at 44 and includes a lower electrode 46, a ferroelectric (F; E) material 48 and an upper electrode 50. The structure of the FEM gate unit 44 begins by depositing a lower electrode on the gate region 40, which is also referred to herein as a second type conductive path. The lower electrode 46 may be made of Mg or iridium, platinum / iridium alloy or other suitable conductive material. The metal thickness is between 20 nm and 100 nm. Second, FE materials are deposited by chemical vapor deposition (CVD). The FE material can be any of the following: Pb (Zr, Ti) 03 (PZT), SrBi2Ta209 (SBT), PhGesOn, BaTi03, or LiNb03. The preferred order of the preferred compounds is PbsGesOu 'SBT and PZT. Most of the experimental work in the field of the FEM gate unit is to deposit PZT compounds to a thickness of 100 nm to 400 nm. · The upper electrode 50 is then formed on the gE material. The upper electrode may be formed from the same material as the lower electrode to a thickness of 20 nm to 200 nm. The precursor of the conductive path is indicated at 52. This precursor is finally diffused into the gate region 40 by the lower electrode 46 through the metal ions to become a metal silicide layer. __ -14- Two ____ · Touch home county (CNS) A in this paper scale system (2! GX297 reading): — ~ ~~ --- fjing read the precautions on the back before filling in this page j -Order_ -JU. A7 B7 409366 V. Description of the invention (12) Photoresist is applied to the FEM gate unit, and then the unit is etched into a proper configuration and size. It is necessary to understand that the three-layer FEM gate unit does not need to be accurately aligned as shown, The reason is that its shape can be formed by applying photoresist and etching with a mask having a different geometry. However, for clarity, the FEM gate unit is illustrated as having a structure adjacent to the facing sidewalls. Referring now to FIG. 4, the FEM gate unit 44 is illustrated as a component of the FEM memory unit 53, which includes the FEM gate unit 44 and the lower source region, the passage region and the non-electrode region. The specific example includes a layer formed in the FEM gate unit. Below the 4; a thin layer 54 of the compound, the conductive path precursor 52 is located here. As described in the second specific example of the method of the present invention, the sanding layer 54 may be formed before the components of the FEM gate unit 44 are deposited; or it is assumed that the lower electrode 46 is made of platinum (pt) or its alloy. Diffusion into the upper part of the gate region 40, forming a shallow silicide layer as a Xiaodi barrier layer, which is referred to herein as a third type conductive path. A layer of titanium oxide 56 or other appropriate barrier insulating material is formed by CVD to protect the FEM gate unit. Titanium oxide is etched to form the sidewall insulation layer of the gate electrode. The photoresist is formed by application and appropriate n + and P + regions by ion implantation. The oxide layer is formed by CVD or other suitable passivation insulation. Structure at 500 C to 1000X: heat treatment to passivate and diffuse the implanted ions. For a complete description of the FEM unit 53, a hole is formed in the oxide layer 58 and the source electrode 60, the gate electrode 62 and the drain electrode 64 and connected to a plurality of other components. The specific example illustrated in FIG. 4 shows the invention structure ‘simplest μ. The structure is a ferroelectric closed electrode depleting her S transistor. At the gate voltage of 0, the charge of the 10,000 n path under the closed cell is completely depleted. Therefore, the leakage current is extremely small. To maintain a small leakage, u The lower electrode 46 contacts any edge of the η sand, and this point is related to the η + source region. The standard of the household scale (CNS) applies (锖 Please read the notes on the back before filling in this 1)
、1T d. 經濟部中央標準局員工消费合作社印掣 -15 A7 B7 經濟部中央標準局員工消費合作社印製 409SS6 五、發明説明(13 或n+汲極區邊緣間距以「D」表示, I ^ ^ # 〜至少5 0毫微米俾 保持小的漏電流。但隨著];)的增加,記、 矸 ,匕厲早兀I串聯雷阻 也曰加。因此較佳D不大於3〇〇毫微米1 舶至η型梦祕障層接觸及姑至鐵電材料接觸決定。= 流爲閘極電流由極小至中等場強度。鉑與η_型矽間的電位 障層爲0.9 eV。此種大小的電位障層使"秒通路於鐵電 材料未偏極化,,或鐵電材料下電極以負電荷偏極化時 完全被耗盡。當鐵電材料於下電極以正電荷偏極化時,記 憶體電晶體之閾電壓小v此等記憶體電荷牿質及改變程式 規劃單元所需電壓量之技術容後詳述。1T d. Printed by the Consumers 'Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs -15 A7 B7 Printed by the Consumers' Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs 409SS6 5. Description of the invention ^ # ~ At least 50 nm 俾 keep a small leakage current. But with the increase of];), remember, 矸, 厉, 兀, and 串联 series lightning resistance is also increased. Therefore, it is preferable that D is not greater than 300 nanometers. The contact between the ship-to-n-type dream barrier layer and the ferroelectric material is determined. = Current is the minimum to medium field strength of the gate current. The potential barrier between platinum and η-type silicon is 0.9 eV. A potential barrier of this size makes the "second channel unpolarized in the ferroelectric material, or the electrode under the ferroelectric material is completely depleted when it is polarized with a negative charge. When the ferroelectric material is polarized with a positive charge at the lower electrode, the threshold voltage of the memory transistor is small. The quality of these memory charges and the technique of changing the amount of voltage required by the programming unit will be described in detail later.
本發明之MFSFET之另一具體例中,參照圖5,p•層7〇 可於閘極通路區40形成作爲導電通路前驅物。基板3〇及 活性區32係如圖1及2所述形成β p-層可藉植入;6或3][72離 子形成,或由FEM閘單元擴散金屬離子形成。硼離子可於 3 keV至10 keV能量植入,而bF2離子可以15 keV至5〇 keV 之能量植入》二例之離子濃度係於1χ1〇η/平方厘米至 lxlO15/平方厘米之範圍。 使用本體CMOS基板作範例來説明製造過程,第一步驟 係製造η·陆及p-阱結構,分離此等結構,及植入適當離子 而提供電晶體之閾電壓調整。光阻用於遮蔽晶圓之CMOS 區段。其次磷離子以,能量3〇 keV至120 keV,劑量 l.OxlO12/平方厘米至5.〇χ1〇15/平方厘米植入ρ·阱,此處將 構成FEM閘單元。需要多次植入步驟及/或熱擴散來獲得 ιΓ層之最佳供給者分布。光阻被剝脱去除。植入的η •型矽 -16 本紙張尺度適用中國國家標準(CMS〉Α4規格(210Χ29:?公绝) ( (請先閱讀背面之注意事項再填寫本瓦〕In another specific example of the MFSFET of the present invention, referring to FIG. 5, the p • layer 70 can be formed in the gate via region 40 as a conductive path precursor. The substrate 30 and the active region 32 are formed as a β p-layer as described in FIGS. 1 and 2 and can be formed by implantation; 6 or 3] [72 ions, or formed by diffusion of metal ions by a FEM gate unit. Boron ions can be implanted at an energy of 3 keV to 10 keV, while bF2 ions can be implanted at an energy of 15 keV to 50 keV. The ion concentration of the two cases is in the range of 1 × 10 η / cm 2 to 1 × 10 15 / cm 2. The bulk CMOS substrate is used as an example to explain the manufacturing process. The first step is to manufacture η · land and p-well structures, separate these structures, and implant the appropriate ions to provide the threshold voltage adjustment of the transistor. Photoresist is used to mask the CMOS section of the wafer. Secondly, the phosphorus ion is implanted into the p · well with an energy of 30 keV to 120 keV and a dose of 1.0 × 10 12 / cm 2 to 5.0 × 10 15 / cm 2, where a FEM gate unit will be formed. Multiple implantation steps and / or thermal diffusion are required to obtain the optimal donor distribution of the ιΓ layer. The photoresist is peeled off. Implanted η-type silicon -16 This paper is in accordance with the Chinese national standard (CMS〉 Α4 size (210 × 29 :?)) ((Please read the precautions on the back before filling in this tile)
409366 A7 B7 經濟部中央標準局負工消費合作社印製 五、發明説明(14 ) 層也可以厚度lp〇毫微米至1 〇〇〇毫微米之選擇性外延晶膜 增長矽替代。硼(3 keV至5 keV)或BF2 (30 keV至50 keV) 離子植入具有劑量爲yOMOl2/平方厘米至1 〇χ1〇Ι3/平方厘 米。離子經熱激發。 , 現在參照圖6 ’現在如前述藉沉積銘或其它適當材料形 成下電極46而構成FEM閛單元。此種金屬厚度爲2〇毫微 米至100¾微米。可植入膨或BF2離子。fe材料48沉積至 1〇〇毫微米至4“毫微米厚度,及上.電極5〇係經由沉積鉑 或其它適當電極材料之2 〇毫微米至_2〇0毫學米厚度形成。 光阻經施用,及上及下電極及FE經蝕刻而如前述提供距 離源極區及汲極區的適當間隔「D」。然後光阻由結構上 剝脱去除。如於圖4説明」氧化鈦(5 6 )或另一種適當障壁 絕緣層藉CVD沉積而保護鐵電材料。氧化鈦經蝕刻而於閘 極電極形成侧壁絕緣層。其它氧化物可用於此步驟。再度 施用光阻,及植入離子。光阻FEM剥脱去除及氧化物或 另’一種適當鈍化絕緣層藉CVD施用。結構體經加熱處理而 密化鈍化絕緣層及激活植入的離子。再度施用光阻,接觸 孔經银刻,製成係以業界人士眾所周知之方法完成。 至於用於形成蕭隄障層54或淺接面層7〇乏方法,障層 結構用來提供本發明之巧£]^單元之有$交換機制。 .另外若鐵電材料無法号續高溫加熱;^理,則.源極/汲極 離子植入及退火可於下閘極電極沉積前完成。 作業: 根據本發明構成的結構體特別有效,原因爲位於閉極區 (請先閲讀背面之注意事項再填寫本瓦) ^---- - -409366 A7 B7 Printed by the Consumers' Cooperative of the Central Bureau of Standards of the Ministry of Economic Affairs 5. The description of the invention (14) The layer can also be a selective epitaxial film with a thickness of lpnm to 1000nm and grown silicon instead. Boron (3 keV to 5 keV) or BF2 (30 keV to 50 keV) ion implantation has a dose of yOMOl2 / cm2 to 100x103 / cm2. Ions are thermally excited. Referring now to FIG. 6 ′, the FEM (R) unit is now formed by forming the lower electrode 46 by depositing inscriptions or other suitable materials as described above. This metal has a thickness of 20 nanometers to 100 ¾ micrometers. Can be implanted with puff or BF2 ions. The fe material 48 is deposited to a thickness of 100 nanometers to 4 "nanometers, and the upper electrode 50 is formed by depositing a thickness of 20 nanometers to 200 nanometers from platinum or other suitable electrode materials. Photoresist Upon application, and the upper and lower electrodes and FE are etched to provide the appropriate distance "D" from the source and drain regions as previously described. The photoresist is then removed by structural exfoliation. As illustrated in Figure 4, "Titanium oxide (56)" or another suitable barrier insulating layer is deposited by CVD to protect the ferroelectric material. Titanium oxide is etched to form a sidewall insulating layer on the gate electrode. Other oxides can be used in this step. Photoresist was applied again, and ions were implanted. Photoresist FEM exfoliation and oxide or another appropriate passivation insulating layer is applied by CVD. The structure is heated to densify the passivation insulating layer and activate the implanted ions. Photoresist was applied again, and the contact holes were engraved with silver. As for the method for forming the Xiaodi barrier layer 54 or the shallow junction layer, the barrier structure is used to provide the ingenuity of the present invention. In addition, if the ferroelectric material cannot be heated at high temperature, the source / drain ion implantation and annealing can be completed before the lower gate electrode is deposited. Assignment: The structure constructed according to the present invention is particularly effective because it is located in the closed pole area (please read the precautions on the back before filling in this tile) ^ ------
'1T'1T
409366 A7 B7 五、發明説明(15 ) 之導電通路上方的FEM閘單元.可移動閘極區極性,而可獲 得有效電流由源極流經閘極至汲極β結構體於「闕」狀^ 時提供幾乎完全電荷耗盡,及於「開」狀態時提供電流之 有效低傳熱。圖7爲本發明之FEM.單元之放.大視圖其闡明 虚線7 2表示之典型先前技術電流流動,其中流經閘極區 40之電流僅位於FEM閘單元正下方。原因爲已知之fem 單元構型無法完全容許電流流經閘極區。此種構造可視爲 半「開」的開I。實線74闡明本發明之全「關」開關, 此處電流可流經障層結構7 0下方的整個閘;声.區。 根據本發明構成之記憶早元可置於記憶單元陣列,因而 閘極線垂直汲極線β欲寫入FEM閘單元4 4 ’ +Vpl施加至 全部閘極電極,而έ己憶單元之源極電極及汲極電極處於接 地電位。如此偏極化FE 48,因此正電荷位於下電極46及 負电何位於上電極50 (參照圖8b)。如此使FEM閘單元4 4 呈高導電態。 當負電壓-Vp0施加至閘極電極(程式規劃線)及正電壓 +VpC施加至汲極,及源極接地且此處丨Vpl|>|Vp〇丨時,^係 以下電極46的負電荷偏極化。如此使feM閘單元4 4處於 低導電態(參照圖8 a)。窝過程可使記憶體陣列中各個記 憶體電晶體與陣列中的其它記憶單一元今關被寫入,而未造 成或無來自陣列其它記,單元之閾電壓的干擾。 FEM閘單元44之閾電壓決定如下:對大型陣列而言,於 「1 J態之閾電壓必須爲正値亦即0,4 V至0.8 V。Γ 〇」態 之閾電壓必須大於供應電壓亦即3.3 V。η-通路層被p-型基 -18 - 本紙張尺度適用中國國家標準(CNS ) Λ4規格(210‘<297公茇) f J ^ — (請先閱讀背面之注意事項再填寫本頁) -56 d 經濟部中央標準局員工消费合作社印製 409360 A7 B7 五、發明説明(16 ) 板接面以及被下電極蕭隄障層,或極淺的p-表面層及閘極 偏壓所耗盡。可將記憶體視窗顯示爲等於:409366 A7 B7 V. FEM gate unit above the conductive path of the invention description (15). The polarity of the gate region can be moved, and the effective current can be obtained from the source flowing through the gate to the drain β structure in a "阙" shape ^ Provides almost complete charge depletion at all times and provides effective low heat transfer in the "on" state. Fig. 7 is an enlarged view of the FEM cell of the present invention and its explanation. A typical prior art current flow indicated by a dashed line 72, in which the current flowing through the gate region 40 is located just below the FEM gate unit. The reason is that the known fem cell configuration cannot fully allow current to flow through the gate region. This structure can be regarded as a semi-open "I". The solid line 74 illustrates the all-off switch of the present invention, where current can flow through the entire gate below the barrier structure 70; the acoustic zone. The memory early element formed according to the present invention can be placed in a memory cell array, so the gate line vertical drain line β is to be written into the FEM gate unit 4 4 ′ + Vpl is applied to all gate electrodes, and the source of the memory cell The electrode and the drain electrode are at a ground potential. The FE 48 is thus polarized so that the positive charge is located at the lower electrode 46 and the negative charge is located at the upper electrode 50 (see Fig. 8b). This makes the FEM gate unit 4 4 highly conductive. When the negative voltage -Vp0 is applied to the gate electrode (programming line) and the positive voltage + VpC is applied to the drain, and the source is grounded and here 丨 Vpl | > | Vp〇 丨, ^ is negative to the following electrode 46 The charge is polarized. This causes the feM gate unit 44 to be in a low conductivity state (see Fig. 8a). The nest process enables each memory transistor in the memory array to be written to other memory cells in the array without any interference from the threshold voltage of other memory cells in the array. The threshold voltage of the FEM gate unit 44 is determined as follows: For large arrays, the threshold voltage in the "1 J state must be positive, that is, 0,4 V to 0.8 V. The threshold voltage in the Γ 〇" state must be greater than the supply voltage. That is 3.3 V. η-pass layer is p-type base-18-This paper size applies Chinese National Standard (CNS) Λ4 specification (210 '< 297 cm) f J ^ — (Please read the precautions on the back before filling this page) -56 d Printed by the Consumer Cooperatives of the Central Bureau of Standards of the Ministry of Economic Affairs 409360 A7 B7 V. Description of the invention (16) The board junction and the low-electrode Xiaodi barrier layer, or the very shallow p-surface layer and gate bias are consumed Exhausted. The memory window can be displayed as:
CPE 此處Qfe爲剩餘電荷及CFE爲閘單元之鐵電電容。 讀取作業過程中,不大於矯頑電壓(亦即記憶體内容可 改變的電壓)之電壓Va施於閘極電極及汲極電極。因當任 何電極以\^加偏壓時,記憶單元内容未受干擾,故讀取作 業將不會干擾任何記憶單元的記憶内容。因此可獲得長期 電荷保有性。 - 單一電晶體記憶單元: MFMOS FET之一般ID相對於VG之作圖闡明於圖9。圖9a 闡明附有高通路攙雜ND之FEM單元之ID相對於VG特性。當 FEM閘單元未帶電時,中線爲ID相對於V〇曲線。當FEM單 元程式規劃之「1」態時,FEM單元之閾電壓爲負。如此 大汲極電流流經通路區,即使VG = 0 V。此種裝置不適合 大,型陣列應用。 經濟部中央標準局負工消費合作社印製 (請先閱讀背面之注意事項再填寫衣頁) ⑴ ΔΥ, 圖9 b闡明附有低通路攙雜之FE Μ單元之ID相對於VG 特性。FEM單元之閾電壓當程式規劃至Γ 1』態時爲正。 當閘極位於地電位時,並無電流流經裝置。此種裝置之大 型記憶體陣列將有極小的備用漏電_說厂故無需頻頻更新。 MFMOS應用之鐵電Pb5G&Ou薄膜: 顯示較低鐵電電容導致較高記憶體視窗及較低程式規劃 電壓。較厚膜及較mer材料可獲得較低鐵電電容;但若鐵 19- 本紙張尺度適用中國國家榡準(CNS ) A4規格(210X 297公釐) 409366 A7 B7 五 '發明説明(17 ) " 電交換場經過明確界定,則前一種選擇可增高程式规劃電 壓°常見氧化物鐵電材料具有較高〜及τ。,而非氧化物鐵 電材料具有較低erAT。》氧化物PbgGesOu薄膜具有極低sr 及中等丁。(178°C )。表1比較!^^03裝置之:纪憶體視窗與 PbsGesOn,pZT及SrBi2Ta2〇9薄膜之鐵電閘極。即使 膜之穩態偏極化遠比薄膜更 低,由於低er$,經PbsGhOu閘極控制的MFMOS裝置的 §己憶體视窗大於其相對視窗。 表1 :具有各種鐵電材料之MFM0S裝羣之記憶體視窗 (請先閲讀背面之注意事項再填筇本頁) sr鐵電 Pr(pC/cm2) Pb(Zr,Tn〇 3__SrBi2T&2〇9__PbsGe3〇i ιCPE Here Qfe is the residual charge and CFE is the ferroelectric capacitance of the gate unit. During the reading operation, a voltage Va that is not greater than the coercive voltage (that is, the voltage that can be changed in the memory content) is applied to the gate electrode and the drain electrode. As any electrode is biased with \ ^, the content of the memory cell is not disturbed, so the reading operation will not interfere with the memory content of any memory cell. Therefore, long-term charge retention can be obtained. -Single transistor memory cell: The general ID of MFMOS FET vs. VG is illustrated in Figure 9. Figure 9a illustrates the ID vs. VG characteristics of a FEM unit with a high-path doped ND. When the FEM gate unit is not charged, the center line is the ID vs. V0 curve. When the "1" state of the FEM unit program is planned, the threshold voltage of the FEM unit is negative. Such a large drain current flows through the path region, even if VG = 0 V. This device is not suitable for large and large array applications. Printed by the Central Laboratories of the Ministry of Economic Affairs and Consumer Cooperatives (please read the precautions on the back before filling in the clothing page) ⑴ ΔΥ, Figure 9b illustrates the ID vs. VG characteristics of the FEM unit with a low-pass doping. The threshold voltage of the FEM unit is positive when the program is planned to the Γ 1 ′ state. When the gate is at ground potential, no current flows through the device. The large memory array of such a device will have minimal standby leakage. Ferroelectric Pb5G & Ou film for MFMOS application: Displaying lower ferroelectric capacitance results in higher memory window and lower programming voltage. Thicker films and more mer materials can get lower ferroelectric capacitance; but if iron 19- this paper size is applicable to China National Standard (CNS) A4 specification (210X 297 mm) 409366 A7 B7 Five 'invention description (17) The electric exchange field is clearly defined, the former option can increase the programming voltage. Common oxide ferroelectric materials have higher ~ and τ. Non-oxide ferroelectric materials have a lower erAT. 》 Oxide PbgGesOu film has extremely low sr and medium D. (178 ° C). Table 1 comparison! ^^ 03 device: Ji Yi body window and PbsGesOn, pZT and SrBi2Ta209 thin film ferroelectric gate. Even though the steady-state polarization of the film is much lower than that of the thin film, due to the low er $, the §memory window of the MFMOS device controlled by the PbsGhOu gate is larger than its relative window. Table 1: Memory window of MFM0S package with various ferroelectric materials (please read the precautions on the back before filling this page) 〇i ι
Pr* (^C/cm2) 當 Vdep=〇.5V 記:隐體视窗 |2 Pr* /CFR(V) 0.8 0.25 訂 1,08 1.29 3.23Pr * (^ C / cm2) when Vdep = 0.5V Note: hidden window2 Pr * / CFR (V) 0.8 0.25 order 1,08 1.29 3.23
經濟部中央標準局員工消費合作社印製Printed by the Consumer Cooperatives of the Central Bureau of Standards of the Ministry of Economic Affairs
穩態Vdep假定爲0.5 V 如此。揭示FEM記憶單元及其構成—方洽。FEM閘單元可構 造爲單一電晶體裝置,/或可與相關M〇s電晶體一起構 造。雖然已經揭示本發明之較佳具體例,但須了解可未背 離如隨附之中請專利_界定之本發明之範㈣其構造及 方法做出進一步改變。 ___- 20 - · ν' 本紙瘅尺度適用中國國家標準(--:~~ ( 經濟部中央標準局員工消費合作社印製 409366 五、發明説明(18 ) (實例2 ) 本例之鐵電記憶體(FEM)單元可於s〇l (SIMOX)基板上 形成或可於本體矽基板上形成β此處説明集中於本體矽基 板上形成FEM閘單元’但如此處使用「矽基板」表示S0I 基板或本體矽基板。須了解M〇S電晶體及fem閘單元可 順序或同時製造俾形成本發明之雙電晶體結構。完成的結 構可提供具有成本效益的極小型記憶單元,具有簡單電路 構型’提供非易失性記憶體及具有極低漏電流β 現在參照圖1 0,矽基板闡明於^丰;具體例中基板 210爲單晶基板及由本體矽製成β如圖1 〇免明,基板21〇 已經修改成闡明的構型,及部分基板輕度攙雜而形成活性 區或裝置區212,其提供_所需背景極性,本例爲η-區之背 景極性,後文稱做第一型導電通路《磷離子於此處也稱做 第一型攙雜雜質,經以30 keV至120 keV之能量, l.OxlO12/平方厘米至5.0χ1013/平方厘米之劑量植入待構成 FEM閘單元之p-阱而形成第一型導電通路。需要多個植入 步驟及/或熱擴散來於η·層獲得最佳给予者分布。植入的n-型矽層也可以厚1 〇〇毫微米至1000毫微米的選擇性外延晶 膜增長梦替代°活性區212被絕緣區214包崮,絕緣區係 藉熱氧化法或藉化學蒸氣沉積(CV^ )由二氧化矽製成,而 形成裝置間的LOCOS 或/inesa隔離。如業界人士眾所周 知,多個活性區於矽晶圓表面上形成。至於本發明之雙電 晶體s己憶單元’活性區係成垂直格拇排列而形成記憶體陣 列(容後詳述)。 -21 - 本紙張尺度適用中國國家標準(CNS ) A4規格(2IOX297公釐) r (請先閲锖背面之注意Ϋ頃再填寫本頁)The steady-state Vdep is assumed to be 0.5 V. Reveal FEM memory unit and its composition-Fang Qia. The FEM gate unit can be constructed as a single transistor device, and / or can be constructed with the associated Mos transistor. Although the preferred specific examples of the present invention have been disclosed, it should be understood that the structure and method of the present invention may be further changed without departing from the scope of the present invention, as defined in the appended patents. ___- 20-· ν 'The size of this paper is applicable to Chinese national standards (-: ~~ (Printed by the Staff Consumer Cooperative of the Central Bureau of Standards of the Ministry of Economic Affairs 409366) 5. Description of the invention (18) (Example 2) Ferroelectric memory of this example (FEM) unit can be formed on a sol (SIMOX) substrate or can be formed on a bulk silicon substrate β The description here focuses on forming a FEM gate unit on the bulk silicon substrate ', but as used herein, "silicon substrate" means a S0I substrate or The body silicon substrate. It must be understood that the MOS transistor and the fem gate unit can be sequentially or simultaneously manufactured to form the double transistor structure of the present invention. The completed structure can provide a cost-effective extremely small memory unit with a simple circuit configuration. Provide non-volatile memory and have extremely low leakage current β. Referring now to FIG. 10, the silicon substrate is illustrated in ^ Feng; in the specific example, the substrate 210 is a single crystal substrate and is made of bulk silicon. The substrate 21 has been modified into a clarified configuration, and some substrates are slightly doped to form an active region or a device region 212, which provides the required background polarity. This example is the background polarity of the η-region, which is hereinafter referred to as the first Conductive path It is also referred to herein as the first type of doped impurity, and is formed by implanting a p-well to form a FEM gate unit with an energy of 30 keV to 120 keV at a dose of 1.0x1012 / cm2 to 5.0x1013 / cm2. Type I conductive pathways. Multiple implantation steps and / or thermal diffusion are required to obtain optimal donor distribution in the η · layer. The implanted n-type silicon layer can also be 100 nm to 1000 nm thick. The selective epitaxial film growth dream replaces the active region 212 with an insulating region 214. The insulating region is made of silicon dioxide by thermal oxidation or chemical vapor deposition (CV ^) to form a LOCOS between devices or / Inesa isolation. As is well known in the industry, multiple active regions are formed on the surface of the silicon wafer. As for the dual-electrode s memory cell 'active region of the present invention, they are arranged in a vertical grid to form a memory array (detailed later) ). -21-This paper size applies to Chinese National Standard (CNS) A4 (2IOX297 mm) r (Please read ΫNotes on the back before filling this page)
鯉濟部中央標準局員工消費合作社印製 Α7 409366 Β7 五、發明説明(19 ) 現在參照圖11,可知本發明之半導體裝置之構造進展 至MOS電晶體215已經於基板上形成該點。活性區212已 被修改而包括p-阱216,係藉遮蔽活性區212及離子植入完 成。卩層可經由植入B或BFi離子(.此處稱做:第二型攙雜雜 質)於活性層212形成。硼離子可於3 keV至10 keV之能量 植入’ JBF2離子係以15 keV至50 keV之能量植入。二例之 離子濃度係於5χ10η/平方厘米至ιχ1〇ΐ5/平方厘米之範 圍。離子藉退;熱激發。植入離子擴..散Αη-活性區而形成 ρη層’此處稱做第二型導電通路人退火聲於5〇〇。〇至11〇〇 c之溫度進行。第一型導電通路之通路區七18保留於ρ-阱 216之任一侧上。 活性區212之外侧部經遮蔽’一層二氧化矽層22〇藉cvd 於plf 216及部分通路區218上形成。一層η+多晶矽再度藉 CVD沉積其上。一層矽化物層224可藉cVD形成於η—多晶 秒上及作爲MOS電晶體之部件,其雖然於附圖中闡明, 但爲本發明方法及結構的選擇性部分。另一層二氧化矽層 226於此處也稱做電晶體絕緣層藉cvd鋪設。 另外二氧化妙層可沉積於ρ-阱216之非遮蔽區及通路區 218 ’二氧化矽層經蝕刻而形成侧壁,η+多晶.麥層222及層 224沉積其中。頂層二氧·化矽層沉積於_側壁及層224上。Printed by the Consumer Standards Cooperative of the Central Bureau of Standards of the Ministry of Civil Engineering A7 409366 B7 V. Description of the Invention (19) Now referring to FIG. 11, it can be seen that the structure of the semiconductor device of the present invention has progressed to the point that the MOS transistor 215 has been formed on the substrate. The active region 212 has been modified to include a p-well 216 by masking the active region 212 and ion implantation. The hafnium layer can be formed on the active layer 212 by implanting B or BFi ions (herein referred to as: a second type of dopant impurity). Boron ions can be implanted at an energy of 3 keV to 10 keV ’JBF2 ions are implanted at an energy of 15 keV to 50 keV. The ion concentration in the two cases ranged from 5x10η / cm2 to ιχ100.5 / cm2. Ion loan; thermal excitation. The implanted ion is diffused to form the Δη-active region to form a ρη layer ', which is referred to herein as a second type of conductive path. It is carried out at a temperature of 0 to 1100 c. The via region 718 of the first type conductive via remains on either side of the p-well 216. The outer side of the active region 212 is formed by masking a silicon dioxide layer 22 through the cvd on the plf 216 and a part of the via region 218. A layer of η + polycrystalline silicon was deposited thereon again by CVD. A silicide layer 224 may be formed on the η-poly second by cVD and as a component of a MOS transistor. Although illustrated in the drawings, it is an optional part of the method and structure of the present invention. Another silicon dioxide layer 226 is also referred to herein as a transistor insulation layer and is laid by cvd. In addition, a fine dioxide layer can be deposited in the non-shielded region and the via region 218 'of the p-well 216. The silicon dioxide layer is etched to form a sidewall, and η + polycrystalline. Wheat layer 222 and layer 224 are deposited therein. A top silicon dioxide layer is deposited on the sidewall and layer 224.
M〇S電晶體以光阻22^覆蓋,光阻覆蓋FEM閘單元之 MOS電晶體215及通路區218。然後其餘裝置區212藉坤離 子植入處理形成!!+矽源極g23〇&n+矽汲極區232,此處稱 做第二型導電通路。本例之適當離子植入可爲於約50 keV 22- (請先閲讀背面之注意事項再填寫本頁)The MOS transistor is covered with a photoresist 22 ^, which covers the MOS transistor 215 and the via region 218 of the FEM gate unit. Then, the remaining device region 212 is formed by the ion implantation process! + Silicon source g23 and n + silicon drain region 232, which is referred to herein as a second type conductive path. Appropriate ion implantation in this example is about 50 keV 22- (Please read the precautions on the back before filling this page)
毕 S - 、 VBi S-, V
S N 格 規 t r 經濟部中央標準局貝工消費合作社印掣 409366 A7 ----- - B7 五、發明説明(20 ) ^ 之較佳能量進行砷離子植入,但40 keV至70 keV之植入亦 可接受’及劑量係於lxl0i5/平方厘米至5χ1〇15/平方厘米 I耗圍。另外磷離子可以相同劑量範圍於3〇 keV_6〇 keV 之能量範圍植入。任一種情況下,於此構成步驟植入的材 料於此處稱做第三型挽雜雜質。 光阻被剝脱去除。現在參照圖1 2,製造FEM閘單元 234。閉單元包括下電極236,fE層238及上電核 240 FEM閘早元23 4之構造始於沉.積下電極於二氧化矽 層226上二氧化♦層部分延伸於通路區jig上。下電接 236~T由箱或銀,一氧化敏或舶/绞合金或其它適當導電材 料製成。也可使用其它適當導電障層β較佳具體例之電極 23 6厚度爲20毫微米至ΐα〇毫微米。 其次藉CVD沉積FE材料238。FE材料可爲下列任— 者:Pb(Zr5 Ti)03 (ΡΖΤ),SrBi2Ta2〇9 (SBT),Pb5Ge3〇u,SN standard tr 410366 A7 ------B7 printed by the Central Bureau of Standards of the Ministry of Economic Affairs of the Bayer Consumer Cooperative V. Description of the invention (20) ^ The better energy for arsenic ion implantation, but the planting of 40 keV to 70 keV It is also acceptable and the dosage ranges from 1 × 10 5 / cm 2 to 5 × 10 15 / cm 2. In addition, phosphorus ions can be implanted at the same dose range from 30 keV to 60 keV. In either case, the material implanted in this constituent step is referred to herein as a type III dopant impurity. The photoresist is peeled off. Referring now to FIG. 12, a FEM gate unit 234 is manufactured. The closed cell includes the lower electrode 236, the fE layer 238, and the power core 240 FEM gate early element 234. The structure starts from sinking. The lower electrode is deposited on the silicon dioxide layer 226, and the dioxide layer partially extends on the via area jig. The power-down contacts 236 ~ T are made of box or silver, monoxide-sensitive or ship / stranded alloy or other suitable conductive materials. Electrodes of other preferred embodiments of the appropriate conductive barrier layer β can also be used. The thickness is 20 nm to ΐα0 nm. The FE material 238 is then deposited by CVD. The FE material can be any of the following: Pb (Zr5 Ti) 03 (PNZT), SrBi2Ta209 (SBT), Pb5Ge3〇u,
BaTi〇3 ’或LiNbO广以較佳順序排列,較佳化合物爲 PhGesOn,SBT及PZT。FEM閑單元領域之大半實驗工作 係於PZT化合物進行。ρ E材料23 8沉積至5 0亳微米至4〇〇 毫微米厚度》 然後於FE材料上形成上電極240。上電極寸由下電極之 相同材料製成至厚度爲2.0毫微米吳_1 〇〇_毫微米。 光阻施用於FEM閘單元,上’然後單元蚀刻至適當構型及 尺寸°須了解FEM閘單元的三層無需如所示準確對正,原 因爲其形狀係藉施用光阻及也具有不同幾何的阻罩兹刻形 成。但爲清晰起見’ FEM閘單元闡明爲具有鄰接對正侧壁 -23- ·;: 本紙張尺度適用中國國家標準(CNS ) Λ4規格(2ΪΟΧ 297公釐) { ί請先閲讀背面之注意事項耳填寫本頁jBaTi03 'or LiNbO are arranged in a preferred order, and the preferred compounds are PhGesOn, SBT and PZT. Most of the experimental work in the field of FEM idle units is performed on PZT compounds. The p E material 23 8 is deposited to a thickness of 50 μm to 400 nm. Then, an upper electrode 240 is formed on the FE material. The upper electrode is made of the same material as the lower electrode to a thickness of 2.0 nm. The photoresist is applied to the FEM gate unit, and then the unit is etched to an appropriate configuration and size. It must be understood that the three layers of the FEM gate unit do not need to be exactly aligned as shown, because the shape is based on the application of photoresist and has different geometries. The mask is formed momentarily. But for the sake of clarity, the FEM gate unit is clarified as having adjacent facing sidewalls-23- · :: This paper size applies the Chinese National Standard (CNS) Λ4 specification (2Ϊ〇 × 297 mm) {PLEASE read the precautions on the back first Ear fill in this page j
、1T d 4093G6 A7 B7 五、發明説明(21 ) 的結構。 (請先閲讀背面之注意事頃再填寫大t頁) 現在參照圖1 3,光阻由FEM閘單元剝脱去除,一層TiOx 242,Si3Ny^其它適當介電材料藉CVD沉積而隔離鐵電材 料與二氧化矽。 ’ 如圖1 4所示,該結構係經由沉積二氧化矽層244,覆蓋 絕緣層於結構體之延伸部上,及研磨及插置设極電極 246,閘極電極248及源極電極250完成。 現在參照圖ί 5,本發明之結構關明爲於SOI基板上形 成,其包括標示以圖1 4具體例之相同參_編號的大體全 - 4 :4 部相同组件,但基板係由二氧化矽252製成而非圖1 4具體 例使用的本體矽。 現在參照圖1 6,記愎單元之替代具體例概略闡明於 260。本具體例中,使用本體矽作爲基板262,形成活性 區264及隨後修改成f阱266,ιΓ區268,270其分別作爲 M0S電晶體272及FEM單元274之閘極區。如同η+源極區 278,形成n+汲極區276。氧化物區279旁出於活性區264 及係藉熱氧化或CVD形成。M0S電晶體272及FEM閘單元 274二者之材料依序鋪設,至於M0S電晶體272之各層爲 二氧化矽層280,n+多晶矽層282及選擇性矽北物層284。 經濟部中央標準局員工消f合作社印製 FEM閘單元274係經由沉.積底電極286,FE材料288及頂電 極290形成。其次,藉CVD沉積TiOx,Si3N4或其它適當絕 / 緣層292,及亦藉CVD沉積一層二氧化矽層294。經由妾 裝汲極電極296,閘極電極298及源極電椏2100而完成製 造過程。M0S電晶體與FEM以TiOpt Si3N4層陽離。本具 -24· 本紙張尺度適用中国國家標準(CNS ) A4規格(210X297公茇) ’ 4093(56 .A 7 B7 五、發明説明(22 ) 體例中層292作爲電晶體絕緣層,而層294作爲覆蓋絕緣 層。 (請先閲讀背面之注意事項再填寫本頁} 如此業已顯示毗鄰MOS電晶體形成MFS電晶體組合之若 干具體例。如此處使用「毗鄰」表示沿兩:侧形成雙電晶 體,或一個電晶體疊置於另一電晶體之上。1T d 4093G6 A7 B7 V. The structure of invention description (21). (Please read the notes on the back before filling in the large page.) Now referring to Figure 13, the photoresist is peeled off by the FEM gate unit, and a layer of TiOx 242, Si3Ny ^ other suitable dielectric materials are isolated by CVD to isolate the ferroelectric materials. With silicon dioxide. 'As shown in Figure 14, this structure is completed by depositing a silicon dioxide layer 244, covering the insulating layer on the extension of the structure, and grinding and inserting the electrode 246, the gate electrode 248, and the source electrode 250. . Referring now to FIG. 5, the structure of the present invention is shown to be formed on an SOI substrate, which includes substantially all of the same parameters _ numbered with the specific example of FIG. 14-4: 4 identical components, but the substrate is made of dioxide Silicon 252 is made of bulk silicon instead of the bulk silicon used in the specific example of FIG. 14. Referring now to FIG. 16, an alternative specific example of the recording unit is schematically illustrated at 260. In this specific example, bulk silicon is used as the substrate 262 to form an active region 264 and subsequently modified into f-wells 266, ιΓ regions 268, 270, which serve as gate regions of the MOS transistor 272 and the FEM unit 274, respectively. Like the n + source region 278, an n + drain region 276 is formed. The oxide region 279 is formed next to the active region 264 and is formed by thermal oxidation or CVD. The materials of both the MOS transistor 272 and the FEM gate unit 274 are laid in order. As for each layer of the MOS transistor 272, a silicon dioxide layer 280, an n + polycrystalline silicon layer 282, and a selective silicon layer 284 are formed. The FEM gate unit 274, printed by the staff of the Central Standards Bureau of the Ministry of Economic Affairs, is formed through the bottom electrode 286, the FE material 288, and the top electrode 290. Next, TiOx, Si3N4, or other appropriate insulating / insulating layer 292 is deposited by CVD, and a silicon dioxide layer 294 is also deposited by CVD. The manufacturing process is completed by mounting the drain electrode 296, the gate electrode 298, and the source electrode 2100. The MOS transistor and FEM were ionized with TiOpt Si3N4 layer. This tool-24 · This paper size applies Chinese National Standard (CNS) A4 specification (210X297 cm) '4093 (56 .A 7 B7 V. Description of the invention (22) In the system, layer 292 is used as the transistor insulation layer, and layer 294 is used as the Cover the insulating layer. (Please read the precautions on the back before filling out this page} This has shown some specific examples of MFS transistor combinations formed next to MOS transistors. If "adjacent" is used here to indicate the formation of a double transistor along two sides: Or one transistor is stacked on top of the other.
圖1 4,1 5及1 6闡明之具體例表示鐵電閘極耗盡型MIS 電晶體組合習知MOS電晶體。當FE於底電極介面238a以Specific examples illustrated in Figs. 14, 15 and 16 show a conventional MOS transistor of a ferroelectric gate depletion type MIS transistor combination. When FE is at the bottom electrode interface 238a
正電荷偏極化^,MFS電晶體之閾.電.壓可爲負値。當FE 以於底電極介面23 8a之負電荷偏極化時,^FS電晶體之閾 電壓極大。於零閘極電壓時,MOS電晶體''不導電。故即 使MFS電晶體之閾電壓爲負値,亦無電流流經裝置。 當閘極電壓等於工作電:壓時,MOS電晶體極爲導電。裝 置電流係由MFS電晶體之電流流動控制。當MFS電晶體處 於.「0」態時,亦即閾電壓大於工作電整時,並無電流流 經裝置。欲於「0 _!態維持小漏電流,下電極236及2 8 6任 一緣與n+源極區及n+汲極區任一緣間距以「D」表示,須 至少爲5 0毫微米。但隨著D的加大,記憶單元之串聯電阻 也增高。因此較佳D不大於300毫微米。當MFS.電晶體處 於「1」態時,亦即閾電壓極低或具有負値時,MOS電晶 經濟部中央標準局員工消費合作社印製 體及MFS電晶體皆導電。.因此大電jfL峰經裝置。如此即使 MFS電晶體之「1」態閾電壓爲負値,裝置仍可用於大型 / 記憶體陣列。 作業: 根據本發明構成之記憶單元可置於記憶單元陣列,而閘 -25- ;: 本紙張尺度適用中国國家標準(CMS ) A4規格(2丨0:'、297公攰) ' 409366 A7 B7 五、發明説明(23 ) 極線垂直没極線,如圖1 7所示。現.在參照圖1 4,1 7及 1 8,欲窝入FEM閘單元234,+Vpl施加至全部間極電極 248 (Y1,Y2,Y3及Y4),而記憶單元之源極電極25〇及 汲極電極246 (XI,X2,X3及X4)位於地·,電位a如此偏 極化FE 238,故正電荷位於下電極介面238a及負電荷位於 上電極介面238b (參見圖18b)。如此使FEM閘單元234變 成高導電態。 當負電壓- Vp0施加於閘極電極248..'(程式规劃線)時,例 如爲Y 2 ’正電壓+ VPQ施加於ί及極23 2,例.,如爲X 3,及源 極230接地及此處丨Vpi丨>.j Vp〇丨’ F Ε例如210立,X 3,Υ 2以 於下電極介面23 8a之負電荷偏極化。如此使'FEM閉單元 234處於低導電態(參見圖i8a)。窝過程可使記憶體陣列之 各個記憶體電晶體與陣列中的其它記憶單元互不相干地窝 入,而不干擾陣列的其它記憶單元。 圖1 4及1 6所示FEM閘單元215,274之閾電壓測定如 下:用於大型陣列,於Γ 1」態之閾電壓可爲負値或小正 電塵。「〇」態之閾電壓必須大於供應電壓亦即33 V。 經濟部中央標準局負工消費合作社印製 若if區之攙雜密度爲约ΐ,Οχίο!6/立方厘米,則pt_n發障 層之ιΓ區之間隔寬度爲約〇.3微米。閾電壓可藉改變n-通路 區之攙雜密度及厚度,尽鐵電電容—氣$電容率及剩餘電荷 調整。 f 讀取作業中,不大於矯頑電壓(亦即可改變記憶體内容 之電壓)之電壓Va施加於閘極電極及汲極電極。因當任何 電極以va加偏壓時,記憶單元内容不受干擾,故讀取作業 -26- 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公验〉 409366 A7 B7 經濟部中央標準局貝工消費合作社印製 五、發明説明(24 將不會干擾任何記_簞开^ u早疋的圯憶内容。因此獲得長時間電 荷保有性。 MFMOS.FET之lD相對於v&略㈣m卜目⑼㈣ 具:高通路攙雜ND之脑單元之。相對於讀性The positive charge is polarized ^, and the threshold, voltage, and voltage of the MFS transistor can be negative. When FE is polarized with the negative charge of the bottom electrode interface 23 8a, the threshold voltage of the FS transistor is extremely large. At zero gate voltage, the MOS transistor "is not conductive. Therefore, even if the threshold voltage of the MFS transistor is negative, no current flows through the device. When the gate voltage is equal to the working voltage: the MOS transistor is extremely conductive. The device current is controlled by the current flow of the MFS transistor. When the MFS transistor is in the "0" state, that is, when the threshold voltage is greater than the operating voltage, no current flows through the device. To maintain a small leakage current in the "0_!" State, the distance between any edge of the lower electrodes 236 and 268 and any edge of the n + source region and the n + drain region is represented by "D", which must be at least 50 nm. However, as D increases, the series resistance of the memory cell also increases. Therefore, D is preferably not more than 300 nm. When the MFS. Transistor is in the "1" state, that is, when the threshold voltage is extremely low or has a negative voltage, the printed body of the MOS transistor's Central Standards Bureau employee consumer cooperative and the MFS transistor are conductive. Therefore, the large electric jfL peak passes through the device. This allows the device to be used in large / memory arrays even if the "1" state threshold voltage of the MFS transistor is negative. Operation: The memory unit constructed according to the present invention can be placed in the memory unit array, and the gate-25- ;: This paper size is applicable to China National Standard (CMS) A4 specifications (2 丨 0: ', 297 cm)' 409366 A7 B7 5. Description of the invention (23) The epipolar line is perpendicular to the non-polar line, as shown in FIG. Now, referring to FIG. 14, 17, 7 and 18, if the FEM gate unit 234 is to be nested, + Vpl is applied to all the inter electrode 248 (Y1, Y2, Y3, and Y4), and the source electrode of the memory cell is 25. The drain electrode 246 (XI, X2, X3, and X4) is located at ground. The potential a is so polarized as FE 238, so the positive charge is located at the lower electrode interface 238a and the negative charge is located at the upper electrode interface 238b (see FIG. 18b). This causes the FEM gate unit 234 to become highly conductive. When negative voltage-Vp0 is applied to the gate electrode 248 .. '(programming line), for example, Y 2' Positive voltage + VPQ is applied to ί and electrode 23 2, for example, if it is X 3, and source 230 ground and here 丨 Vpi 丨 > .j Vp〇 丨 'F E such as 210 stand, X 3, Υ 2 with the negative charge polarization of the lower electrode interface 23 8a. This puts the 'FEM closed cell 234 in a low conductivity state (see Fig. I8a). The nesting process allows each memory transistor of the memory array to be nested incoherently with other memory cells in the array without interfering with other memory cells in the array. The threshold voltages of the FEM gate units 215 and 274 shown in Figures 14 and 16 are as follows: For large arrays, the threshold voltage in the Γ 1 ″ state can be negative 値 or small positive dust. The threshold voltage of the "0" state must be greater than the supply voltage, which is 33 V. Printed by the Consumers' Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs If the impurity density of the if area is about ΐ, Οχίο! 6 / cm3, the interval width of the ιΓ area of the pt_n barrier layer is about 0.3 microns. The threshold voltage can be adjusted by changing the doping density and thickness of the n-channel region to make the ferroelectric capacitance-gas $ permittivity and residual charge. f During the reading operation, a voltage Va that is not greater than the coercive voltage (that is, the voltage that changes the memory content) is applied to the gate electrode and the drain electrode. As any electrode is biased with va, the content of the memory cell is not disturbed, so the reading operation is -26- This paper size applies to China National Standard (CNS) A4 specification (210X297 public inspection) 409366 A7 B7 Central Standards Bureau of the Ministry of Economic Affairs Printed by Pui Gong Consumer Cooperative Co., Ltd. 5. Description of the invention (24 will not interfere with any memory content of _ 记 开 ^ u 早 疋. Therefore, long-term charge retention is obtained. Compared with v & Objective: The brain unit of ND mixed with high pathway. Relative to readability
。當 FEM 閘單元未夢私時,中線21〇4爲^相對於V。曲線。當FEM單 元%式规劃爲「1」態(線21G6 )時’ fem單元之閾電壓爲 負▲ FEM單,程式規割爲「〇」態(線2⑽)時,feM單 元之闕電壓爲正。如此於「1」態,..即使VG = 0V,大没 極呢咖可流Ik通路區。單獨此種裝置不填合大型陣列應 用。 、+ 圖19b闡明本發明裝置之1〇相對於特性。線J 2鬧明 田FEM閘單元不帶電時之Id相對於ν〇曲線。當單元程 式规劃爲「1」態(線211〇)時,FEM單元之閾電壓爲負。 當FEM單元程式规劃爲「〇」態(線2114)時,阳%單元之 閾電壓爲正。當MOS電晶體之閾電壓(虛線2116)程式規 劃局「1J態時,將裝置閾電壓限於小正値。當閘極處於 地電位時,並無電流流經裝置。此種裝置之大型記憶體陣 列將有極小的備用漏電流。 如此已經揭示包括MOS電晶體及FEM閘單元之雙電晶體 記憶單元及其構成方法。·雖然已經^揭$本發明之較佳具體 例及其變化例,但須了气可未背離如随附之申請專利範圍 界定之本發明之範圍對構造及方法做出進一步改變。 (實例3 ) 本實例之鐵電記憶體(FEM)單元可於SOI (SIMOX)基板 27 - - · 本紙張尺度適用中國國家標华(CNS ) M規格(210X29*7公釐) r (諳先聞锖背面之注意事項再填寫本頁). When the FEM gate unit is not dreaming, the center line 2104 is ^ relative to V. curve. When the FEM unit's% formula is set to the “1” state (line 21G6), the threshold voltage of the fem unit is negative ▲ FEM unit, and when the program is set to the “0” state (line 2⑽), the fem unit voltage is positive. This is in the "1" state .. Even if VG = 0V, it is possible to flow the Ik channel area. Such a device alone does not fill a large array application. Figure 19b illustrates the relative characteristics of the device according to the invention. The Id vs. ν curve of line J 2 Nameitian FEM gate unit when it is not charged. When the cell programming is in the "1" state (line 2110), the threshold voltage of the FEM cell is negative. When the FEM cell program is planned to be “0” (line 2114), the threshold voltage of the positive% cell is positive. When the threshold voltage of the MOS transistor (dotted line 2116) is “1J state, the device threshold voltage is limited to the small positive voltage. When the gate is at ground potential, no current flows through the device. The large memory of this device The array will have a very small standby leakage current. In this way, a dual-transistor memory cell including a MOS transistor and a FEM gate unit and a method for constructing the same have been disclosed. The structure and method have been further changed without departing from the scope of the present invention as defined in the accompanying patent application. (Example 3) The ferroelectric memory (FEM) unit of this example can be mounted on a SOI (SIMOX) substrate. 27--· This paper size is applicable to China National Standards (CNS) M specification (210X29 * 7mm) r (Please read the notes on the back of this page before filling out this page)
409366 經濟部中央椋準局員工消費合作社印製 五、發明説明(25 ) — 上形成,或可於本體矽基板形成。此處説明集中於本體矽 基板上形成FEM閘單元。須了解FEM閘單元之若干具體例 中’ MOS電晶體係藉業界人士眾所周知的習知手段=鐵 電記憶單元同時製造。如此爲求清晰起見,,附圖未闡明 MOS電晶體的形成〇 現在參考圖20,矽基板闡明於310。較佳具體例中基板 310爲單晶基;^其係由本體矽製成。其它具體例可於soi 基板上形成β如此處使用「矽基板丄一詞表示本體矽基板 或soi基板或任何其它適當基於矽的基板&如圖2 〇闡明, 基板310已經部分蝕刻至闡明的構型,及^分基板已經輕 度攙雜而形成活性區或裝置區312,其提供所嚅背景極 性,本例爲n-區極性,於此處稱做第一型導電通路。活性 區312由一氣化秒製成的絕緣區包園。如業界人士眾 所周知,多個此種區於矽晶圓表面上形成。用於本發明之 FEM閘單7L,單元係呈垂直袼柵設置而形成記憶體陣列。 .使用本體CMOS基板作範例來解釋製程,最初步驟係製 造η阱及p阱結構,隔離此等結構,及植入適當離子提供 電晶體之閾電壓調整。光阻用來遮蔽晶圓區段。其次磷離 子(此處亦稱做第一型攙雜雜質)於3〇 keV至‘12〇 keV能量 以l.OxlO12/平方厘米至5,0χ1〇13/平米劑量植入,將構 成FEM閘單冗的p_阱。雩要多個植入步驟及/或熱擴散來 於η層獲得最佳給予者分布。光阻被剝脱去除。植入型 矽層也可以厚100毫微米至〗〇〇〇毫微米之矽選擇性外延晶 膜增長替代。 '•II-' (請先閲請背面之注意事項再填寫本頁) -» d 山 -28 ” 冬...民張尺度適用中國國尽標準(CNS ) 規格.(2IGx 297公楚) 409366 A7 __. B7 五、發明説明(26 ) 此時開始形成FEM閘單元ώ現在參照圖2 1,F E Μ閘單 元概略標示於316,包括下金屬層或電極318,鐵電(FE) 材料320及上金屬層或電極322。FEM閘單元316之構成始 於沉積下電極於活性區312上》下電極318;可由Pt,Ir, 或Pt/Ir合金或其它適當導電材料製成。較佳具體例中金屬 厚度爲20毫微米至100亳微米。 最終可於FEM閘單元316與閘極接面區間形成p-層。p-層 可經由將B或BF2離子植入第一型導...電.通路表面或下電極 318形成。棚離子可於3 keV至10 keV能章;植入,而3?2離 子係於15 keV至50. keV能量植入。兩種情浼之離子濃度皆 於lxlO11/平方厘米至lxl〇15/平方厘米之範園。退火步驟 中(容後詳述)’植入離子擴散入η-閘極接面區形成p_層, 此處稱做第三型導電通路。 其次於適當遮蔽後,FE材料藉化學蒸氣沉積(CVD)沉 積。?丑材料可爲下列任一者:Pb(Zr,Ti)03 (PZT), SrBi2Ta209 (SBT) ’ Pb5Ge3On,BaTi03,或 LiNb03。較佳 經濟部中央標準局員工消費合作社印製 (請先閱讀背面之注意事項再填释本頁} ηΊ 化合物以較佳順序排列分別爲PbsGegOn,SBT及PZT。大 半FEM閘單元領域之實驗工作係對ΡΖΤ化合物進行。 F Ε 材料320沉積至50毫微米至400毫微米厚度。- 然後於FE材料上形成·上電極322 ―。上電極可由下電極之 相同材料製成至20毫微f至200毫微米厚度。光阻施用於 FEM閘單元上,然後單元蚀刻至.適當構型及尺寸。須了解 如所示三層FEM閘單元無需準確對正,原因爲其形狀可能 經由施用光阻及以具有不同幾何的阻罩蝕刻形成。但爲求 «29- r 本纸張尺度適用中國國家標準(CNS ) A4規枱(210X297公麓) ~ Γ~ ^--- 409366 A7 __B7 -- ----—η ...________ ____ 五、發明説明(27 ) 一' 明瞭,FEM閘單元闡明爲具有鄰接對正侧壁的結構。409366 Printed by the Consumers' Cooperative of the Central Bureau of Standards and Assistance of the Ministry of Economic Affairs of the People's Republic of China 5. Invention Description (25) — can be formed on the silicon substrate. The description here focuses on forming a FEM gate unit on a bulk silicon substrate. It must be understood that in some specific examples of FEM gate units, the MOS transistor system is manufactured at the same time by a well-known means known to those in the industry = ferroelectric memory cells. As such, for the sake of clarity, the formation of MOS transistors is not illustrated in the drawings. Referring now to FIG. 20, the silicon substrate is illustrated at 310. In a preferred embodiment, the substrate 310 is a single crystal substrate; it is made of bulk silicon. Other specific examples can be formed on the soi substrate. For example, the term "silicon substrate" is used herein to refer to the bulk silicon substrate or soi substrate or any other appropriate silicon-based substrate. As shown in Figure 2, substrate 310 has been partially etched to the The configuration and the sub-substrate have been slightly doped to form an active region or device region 312, which provides the background polarity. In this example, the n-region polarity is referred to herein as the first type of conductive path. The active region 312 consists of One gasification second insulation zone package garden. As is well known in the industry, multiple such areas are formed on the surface of a silicon wafer. The FEM gate sheet 7L used in the present invention has a vertical grid structure to form a memory. Arrays. The bulk CMOS substrate is used as an example to explain the process. The initial steps are to manufacture n-well and p-well structures, isolate these structures, and implant the appropriate ion to provide the threshold voltage adjustment of the transistor. Photoresist is used to shield the wafer area Secondly, phosphorus ions (herein referred to as the first type doped impurities) are implanted at an energy of 30 keV to '12 keV at a dose of 1.0x1012 / cm2 to 5,0χ1013 / m2, which will constitute a FEM gate. Single redundant p_well. 雩Multiple implantation steps and / or thermal diffusion are required to obtain the optimal donor distribution in the η layer. The photoresist is stripped and removed. The implantable silicon layer can also be silicon with a thickness of 100 nm to 〇00 nm Growth epitaxial film growth alternative. '• II-' (Please read the notes on the back before filling this page)-»d-28-28” Winter ... Min Zhang standards are applicable to China National Standards (CNS) specifications. (2IGx 297) 409366 A7 __. B7 V. Description of the invention (26) At this time, the FEM gate unit is formed. Now refer to Figure 21 1. The FE gate unit is generally labeled at 316, including the lower metal layer or electrode 318, iron Electrical (FE) material 320 and an upper metal layer or electrode 322. The composition of the FEM gate unit 316 starts by depositing a lower electrode on the active region 312, and a lower electrode 318; it can be made of Pt, Ir, or Pt / Ir alloy or other suitable conductive materials. In a preferred embodiment, the metal has a thickness of 20 nm to 100 亳 m. Finally, a p-layer can be formed at the interface between the FEM gate unit 316 and the gate. The p-layer may be formed by implanting B or BF2 ions into the first type conductive surface or the lower electrode 318. Shelf ions can be implanted at 3 keV to 10 keV energy, and 3? 2 ions are implanted at 15 keV to 50. keV energy. The ion concentration of the two kinds of emotions is in the range of lxlO11 / cm2 to lxlO15 / cm2. In the annealing step (to be detailed later), the implanted ions diffuse into the η-gate junction area to form a p_ layer, which is referred to herein as a third type conductive path. Secondly, after proper shielding, the FE material is deposited by chemical vapor deposition (CVD). ? The ugly material can be any of the following: Pb (Zr, Ti) 03 (PZT), SrBi2Ta209 (SBT) 'Pb5Ge3On, BaTi03, or LiNb03. Printed by the Consumer Cooperative of the Central Standards Bureau of the Ministry of Better Economy (please read the notes on the back before filling out this page) ηΊ The compounds are arranged in a better order as PbsGegOn, SBT and PZT. Most of the experimental work in the field of FEM gate units The PZT compound is performed. The FE material 320 is deposited to a thickness of 50 nm to 400 nm.-Then is formed on the FE material. The upper electrode 322 is made from the same material of the lower electrode to 20 nm f to 200. Nanometer thickness. The photoresist is applied to the FEM gate unit, and the unit is etched to the appropriate configuration and size. It must be understood that the three-layer FEM gate unit as shown does not need to be accurately aligned, because its shape may be applied by photoresist and Masks with different geometries are etched. But for the purpose of «29- r, this paper size applies the Chinese National Standard (CNS) A4 gauge (210X297 feet) ~ Γ ~ ^ --- 409366 A7 __B7---- -—Η ... ________ ____ V. Description of the invention (27) a 'It is clear that the FEM gate unit is clarified as having a structure adjacent to the opposite side wall.
Ti〇x,si#4或其它適當障壁絕緣材料層324,如囷22所 示,係藉CVD形成而保護FEM閘單元❶障壁絕緣材料經蝕 刻而形成閘極電極的側壁絕緣層。. . 現在參照圖23,可見活性區312已經修改成源極區 326 ,閘極區328及汲極區330。各區係經由將適當離子 (此處亦稱做第< 二型攙雜雜質)植入活性區312其餘部分形 成兩層層(此處亦稱做第二型導電.通路),其將作爲源極 區326及ί及極區330形成。本例之適當離贫植入可於較佳 能量約50 keV植入崎離子進行,但可接受'於4〇 kev至7〇 keV範園之植入及使用lxl0〖V平方厘米至5xl015/平方厘米 之劑量。另外,磷離子可於30 keV至60 keV之能量範圍以 相同劑量範園植入。 經濟部中央標準局貝工消費合作社印製 (請先閱讀背面之注$項再填苑本頁) 現在參照圖2 4,晶圓經加熱處理而激發及擴散植入離 子包括源極區及汉極區之離子及下電極之離子。下電極 318植入之離子擴散導致於FEM閘單元316下方形成淺接 面332 ’此乃第三型導電通路。加熱處理之溫度範圍爲5〇〇 °C至110(TC而純化及擴散植入離子。然後藉cVD於結構體 上方形成二氧化矽層334,或可施用其它適當‘鈍化絕緣。 現在參照圖2 5,FEM.閘單元31$闡J月爲FEM記憶單元 336之一部分,FEM記憶;單元包括FEM閘單元316及下方 源極、通路及汲極區,該具體例包括薄的淺接面區332其 爲p層形成於FEM閘單元316下方。 欲完成FEM單元336之説明,於氧化物層334形成搪孔而 -30- 本紙張尺度適用中國國家標準(CNS ) Λ4規格(210X 297公釐) 4093G6 A7 B7 五、發明説明(28 ) 經濟部中央標準局員工消費合作社印製 谷納源極電極338,閘極電極340及汲極電極342其連結至 其個別組件。 圖25闡明之具體例代表鐵電閘極耗盡型銜1§電晶體。於 零閘極電壓’ FEM閘單元下方之η-通路的電:荷完全耗盡。 如此漏奄流極小。欲維持小的漏電流,下電極3 α 8任一邊 緣與η·源極區或n_汲極區之邊緣間距以「^」表示必須至 少5 0毫微米俾維持小的漏電流。但随著d的加大,記憶單 元之舉聯電阻也增高。因此較佳D不..大於3〇〇毫微米。閘 極漏電流藉ρ·型矽淺接面332及鉑至鐵電付料接觸決定。 鉑與H-型矽間之電位障層爲〇9 eV。第三型·ρ-導電層332與 第一型ιΓ導電層328間之電位障層亦約〇_9 ev。此種大小之 電位障層造成鐵電材料未被偏極化時,η·型矽通路完全被 耗盡。當鐵電材料於下電極介面348以正電荷偏極化時, 閾電壓小。當鐵電材料於下電極介面348以負電荷偏極化 時’ s己憶體電晶體之閾電壓極大。此種記憶體電荷性質及 改變程式規劃·單元之電壓需要量之技術容後詳述。 植入的Β或BF2離子擴散入閘極接面區係經由維持淺接 面層332任何邊緣與源極區及汲極區間距「c」控制6較 佳具體例中「C」爲約〇毫微米至300毫微米。淺接面結構 用來於閘極區328與導電通路間提^兔漏電流可靠的電位 障層及提供本發明之FE]^單元之有效交換機制。 另外若鐵電材料無法維持高溫加熱處理,則可於下問極 電極沉積前完成源極/汲極離子植入及退火。 作業: Γ (請先Μ讀背面之注意事項再填寫本頁) -έ. 訂 d -31 - 經濟部中央榡準局貝工消费合作社印製 409366 A7 __ B7 五、發明説明(29 ) 根據本發明構成之結構特別有效,原因爲位於閘極區之 導電通路上方FEM閘單元可移轉閘極區極性,因此許可有 效電流由源極流經通路至汲極。當處於「關」狀態時結構 提供冗全電荷耗盡。圖2 5亦闡明典型先前技術電流流 動,以虛線344表示,其中流經閘極區328之電流僅流經 FEM閘單元正下方。原因爲已知FEM單元構型爲表面·顚 倒型結構,而此處揭示的裝置屬於耗盡型。耗盡型裝置之 作業理論類似接面FET之作業理論.〇一實線346闡明流經本 發明裝置之電流,電流可流過接面332下孝整個閘極區。 根據本發明構成之记憶早元可設置於記憶:單元陣列,使 閘極線垂直汲極線。於負電壓時,-乂一施加至閘極電極 340 (程式規劃線)’及於正電壓時+Vp。施加至汲極33〇, 及源極3:Z6接地及此處|Vpll>|Vp〇丨時,FE以於下電極介面 348的負電荷偏極化。如此使FEM閘單元316處於低導電 態(參照圖26a)。寫過程可使記憶體陣列中各個記憶體電 晶‘體與陣列中其它記憶單元獨立被窝入,而不干擾陣列其 它記憶單元。 欲寫入FEM問早元316 ’ +Vpi施加至全部閉極電極340, 而記憶單元之源極電極338及汲極電極342‘皆處於地電 位。如此偏極化FE 320 :可使正電荷位於下電極介面34‘8 及負電荷位於上電極介,面35〇 (參照圖20b)。如此可使 FEM閘單元316呈高導電態。 FEM閘單元316之閾電壓決定如下:對大型陣列而言, 於「1」態之閾電壓必須爲小正値亦即0.4 V至〇.8 V。 -32- 本纸悵尺度適用中國國家標準(CNS ) Α4規格( (請先閲讀背面之注意事項再填寫本頁}TiOx, si # 4 or other appropriate barrier insulating material layer 324, as shown in Figure 22, is formed by CVD to protect the FEM gate unit. The barrier insulating material is etched to form the sidewall insulating layer of the gate electrode. .. Now referring to FIG. 23, it can be seen that the active region 312 has been modified into a source region 326, a gate region 328 and a drain region 330. Each region forms a two-layer layer (also referred to herein as a second-type conductive pathway) by implanting appropriate ions (also referred to herein as < type II doped impurities) into the rest of the active region 312, which will be referred to as a source here A polar region 326 and a polar region 330 are formed. The appropriate depleted implantation in this example can be performed at a preferred energy of about 50 keV implantation of osmium ions, but can be implanted in the range of 40kev to 70keV Fanyuan and used lxl0 [V cm2 to 5xl015 / m2 Dose in centimeters. In addition, phosphorus ions can be implanted in the energy range of 30 keV to 60 keV at the same dose range. Printed by the Shell Standard Consumer Cooperative of the Central Bureau of Standards of the Ministry of Economic Affairs (please read the note on the back and fill in this page) Now referring to Figure 24, the wafer is heated and excited to diffuse and implant the implanted ions including the source region and the Han Ions in the polar region and ions in the lower electrode. The diffusion of the implanted ions of the lower electrode 318 results in the formation of a shallow interface 332 'under the FEM gate unit 316. This is a third type conductive path. The temperature range of the heat treatment is 500 ° C to 110 ° C to purify and diffuse the implanted ions. Then cVD is used to form a silicon dioxide layer 334 over the structure, or other appropriate 'passivation insulation can be applied. Now refer to FIG. 2 5, FEM. Gate unit 31 $ Explanation: JEM is a part of FEM memory unit 336, FEM memory; the unit includes FEM gate unit 316 and the source, path, and drain regions below. This specific example includes a thin shallow junction area 332 It is a p-layer formed below the FEM gate unit 316. To complete the description of the FEM unit 336, a boring hole is formed in the oxide layer 334 and -30- This paper size applies the Chinese National Standard (CNS) Λ4 specification (210X 297 mm) 4093G6 A7 B7 V. Description of the invention (28) The employee cooperative of the Central Bureau of Standards of the Ministry of Economic Affairs printed the Gona source electrode 338, the gate electrode 340 and the drain electrode 342 which are connected to their individual components. The specific example illustrated in Figure 25 represents Ferroelectric gate depletion type 1 § Transistor. The charge in the η-channel under the zero-gate voltage 'FEM gate unit: the charge is completely depleted. This leakage current is very small. To maintain a small leakage current, the lower electrode 3 α 8 Any edge and η · source region The edge spacing of the n_drain region is indicated by "^". It must be at least 50 nm. It must maintain a small leakage current. However, as d increases, the resistance of the memory cell also increases. Therefore, the preferred D is not .. More than 300 nanometers. Gate leakage current is determined by ρ · type silicon shallow junction 332 and platinum to ferroelectric materials. The potential barrier between platinum and H-type silicon is 〇9 eV. Type III · The potential barrier between the ρ-conductive layer 332 and the first type ΓΓ conductive layer 328 is also about 0-9 ev. When a potential barrier of this size causes the ferroelectric material to not be polarized, the η-type silicon path is completely Depletion. The threshold voltage is small when the ferroelectric material is polarized with a positive charge on the lower electrode interface 348. When the ferroelectric material is polarized with a negative charge on the lower electrode interface 348, the threshold voltage of the transistor This kind of memory charge property and the technique of changing the programming and unit voltage requirements will be described in detail later. The implanted B or BF2 ions diffuse into the gate junction area by maintaining any edge of the shallow junction layer 332 and The distance between the source region and the drain region "c" controls 6. In a preferred embodiment, "C" is about 0 nm to 300 nm. Shallow The surface structure is used to increase the potential barrier layer with reliable leakage current between the gate region 328 and the conductive path and to provide an effective exchange mechanism of the FE] unit of the present invention. In addition, if the ferroelectric material cannot maintain high temperature heating treatment, it can be Complete source / drain ion implantation and annealing before lower electrode deposition. Assignment: Γ (Please read the precautions on the back before filling out this page)-.. Order d -31-Central Bureau of Standards, Ministry of Economic Affairs Printed by Pui Gong Consumer Cooperative 409366 A7 __ B7 V. Description of the Invention (29) The structure constructed according to the present invention is particularly effective because the FEM gate unit located above the conductive path in the gate region can transfer the polarity of the gate region, so the license is valid Current flows from the source through the path to the drain. The structure provides redundant full charge depletion when in the "off" state. Figure 25 also illustrates a typical prior art current flow, indicated by the dashed line 344, where the current flowing through the gate region 328 flows only directly below the FEM gate unit. The reason is that the known FEM unit configuration is a surface- 表面 inverted structure, and the device disclosed here is of the depletion type. The operating theory of the depletion device is similar to that of the junction FET. A solid line 346 illustrates the current flowing through the device of the present invention, and the current can flow through the junction 332 to the entire gate region. The memory early element formed according to the present invention can be arranged in a memory: cell array so that the gate line is perpendicular to the drain line. At a negative voltage,-乂 is applied to the gate electrode 340 (programming line) 'and at a positive voltage + Vp. When applied to the drain electrode 33o and the source 3: Z6 to ground and here | Vpll> | Vp0 丨, the FE is polarized with the negative charge of the lower electrode interface 348. This places the FEM gate unit 316 in a low conductivity state (see Fig. 26a). The writing process allows each memory transistor in the memory array to be nested independently of other memory cells in the array without disturbing other memory cells in the array. To write the FEM, the early element 316 '+ Vpi is applied to all the closed electrode 340, and the source electrode 338 and the drain electrode 342' of the memory cell are both at the ground potential. FE 320 is thus polarized in such a way that positive charges are located at the lower electrode interface 34′8 and negative charges are located at the upper electrode interface, surface 35 (see FIG. 20b). This makes the FEM gate unit 316 highly conductive. The threshold voltage of the FEM gate unit 316 is determined as follows: For a large array, the threshold voltage in the "1" state must be a small positive voltage, that is, 0.4 V to 0.8 V. -32- The standard of this paper is applicable to China National Standard (CNS) Α4 specification ((Please read the precautions on the back before filling in this page)
A7 409366 B7 五、發明説明(3〇 ) 「0」態之閾電壓必須大於供應電壓亦即3.3 V。η'通路層 藉Ρ—型基板接面耗盡以及藉極淺ρ·表層及閘極偏壓耗盡。 (請先閲讀背面之注意事項再填寫本頁) 可顯示爲記憶體視窗等於: 20 △VT=-^ (2)A7 409366 B7 V. Description of the invention (30) The threshold voltage of the "0" state must be greater than the supply voltage, that is, 3.3 V. The η ′ path layer is depleted by the P-type substrate and depleted by the extremely shallow ρ · surface layer and the gate bias. (Please read the precautions on the back before filling in this page) Can be displayed as a memory window equal to: 20 △ VT =-^ (2)
^FE 此處QfE爲剩餘電荷及爲閑單元之鐵電電容。 讀取作業中,不大於矯頭電壓(亦即記憶體内容可改變 的電壓)之電歷<Va施加至閘極電極及汲極電極。因當任何 電極以VaM偏壓時,記憶單元内容不受干擾,故讀取作業 不會干擾記憶單元之記憶内容。因―此可長邊間保有電荷。 單一電晶體記憶單元: MFMS FET之一般ID相對於Vg作圖闡明於圖27。圖27a 闡明含高通路攙雜ND之FEM單元之ID相對於VG特性。當 FEM閘單元未帶電時,中線爲ID相對於V〇曲線。當FEM單 元被程式規劃爲「1」態時,FEM單元之閾電壓爲負。如 此.即使V〇 = 〇 V大31極電流可流經通路區。此種裝置不適 合..大型陣列應用。 經濟部中央標準局員工消費合作社印製 圖27b闡明含低通路攙雜ND之FEM單元之ID相對於VG特 性。FEM單元當程式規劃爲「1」態時,閾電壓爲正。當 閘極位於地電位時,並無電流流經裝置。此種裝置之大型 記憶體陣列具有極小備用漏電流。—一 MFMS應用之鐵電Pb5Ge30n薄膜: 顯然較低鐵電電容導致較高記憶體視窗及較低程式規劃 電壓。較厚膜及較低心材料可導致較低鐵電電容;但前者 -33- 本紙張尺度適用中國國家標隼((:!'«:)六4規格(210><297公1) 409366 a? _____B7 五、發明説明(31 ) " 選擇可提高程式規劃電壓。氧化物Pb5Ge3〇li薄膜具有極 低er及中等Tc (178°C )。即使Pb5Ge3〇u薄膜之穩態偏極化 遠低於PZT及SrBi2Ta2〇9膜之偏極化,但因前者之&低, 故PbsGesOu閉極控制之MFMS裝置之記憶.體視窗大於後 二者之記憶體視窗。 如此已經揭示FEM記憶單元及其構成方法。fem閘單元 可構成爲單一電晶體裝置’或可構成爲結合M〇s電晶 體°雖然已經揭不本發明之較佳具體..例.,但須了解可未背 離如随附之申請專利範園界定之本發明之释園,而對架構 及方法做出進一步改變。 (實例4) 本實例之鐵電記憶體(ΙΈΜ)單元可形成於SOI (SIMOX) 基板上,或可形成於本體矽基板内。此處説明將集中於本 體石夕基板形成FEM閘單元,但如此處使用,「衫基板」表 示SOI基板或本體矽基板。須了解Fem閘單元之若干具體 例·中,M0S電晶體係藉業界人士眾所周知的習知手段與 鐵·電記憶單元同時製造。如此爲求清晰起見,附圖不闡明 M0S電晶體》 經濟部中央橾準局ί工消費合作社印掣 現在參照圖2 8,珍基板闡明於410。.本具‘謹例之基板 410爲單晶基极且由本體矽製成。如圖28闡明,基板41〇 已經部分蝕刻爲闡明的;^型,部分基板輕度攙雜而形成活 性區或裝置區412,其提供所需背景極性,本例爲n-區之 背景極性,此處稱做第一型導電通路。活性區412周園a包 園著二氧化矽形成的絕緣區414。如業界人士眾所周知, -34 - k 本紙張尺度適用中國國家標準(CNS ) Λ4規格(210Χ 297公赴) 經濟部中央標準局員工消費合作社印製 409366 A7 _______B7 五、發明説明(32 ) ~~~~'— 多區於珍晶®表面上形心至於本發明之觀閘單元,單 元係以垂直格柵排列而形成記憶體陣列。 使用本體CMOS基板作範例來解釋製法,最初步驟爲製 造η·阱及P-醉結構,隔.開此等結構.,及植入:通當離子而對 電晶體提供閾電壓調整。本具體例之基板41〇已經 Ρ-砂或Ρ—醉。光阻用來遮蔽晶圓區段,其次,磷離子此處 也稱做第一 ^攙雜雜質於30 keV至keV能量以 l.Pxio12/平方i米至5.0xl0,平方厘.米劑量植入p_阱,此 處將構成FEM閘單元。需要多個植入步蟬尋/或熱擴散來 獲得n_層之最佳給予者分布。光阻被剥脱姜除。植入的 型矽層也可以選擇性外延晶膜增長矽至1〇〇毫微米至1〇〇〇 毫微米厚度替代。 _ 現在參照圖2 9,其次於活性區412上形成p-·層1 6 D p--層 可藉植入B或BF2離子(此處稱做第二型換雜雜質)至活性 區412形成。棚離子可於3 keV至10 keV能量植入,而BF2 離子可於15 keV至50 keV能量植入。二例之離子泼度係於 5xl〇u/平方厘米至ΐχΐ〇15/平方厘米之範園。.離子藉退火 而熱激發。植入的離子將擴散入n-活性區而形成p-n層, 此處稱做第二型導電通路。退火係於5〇〇。〇皇丨〗00。〇之溫 度進行·。 _ 此時可開始形成FEM〒單元。現在參照圖3 〇,FEM閘 單元概略標示於418及包括下金屬層或電極42〇,鐵電(FE) 材料422及上金屬層或電極424。FEM閘單元41 8之構造始 於沉積下電極於p-層416。下電極420可由Pt或Ir,Ir02或 -35 本紙張尺度適用中國國家標準(CNS } Λ4規格(210X297公發) Γ^ FE Here QfE is the residual charge and the ferroelectric capacitance of the free cell. During the reading operation, an electric calendar < Va which is not greater than the voltage of the head (that is, a voltage that can be changed in the memory content) is applied to the gate electrode and the drain electrode. As any electrode is biased with VaM, the contents of the memory unit are not disturbed, so the reading operation will not interfere with the memory contents of the memory unit. Because of this-there can be a charge between the long sides. Single transistor memory cell: The general ID of MFMS FET vs. Vg is illustrated in Figure 27. Figure 27a illustrates the ID vs. VG characteristics of a FEM unit with high-path doped ND. When the FEM gate unit is not charged, the center line is the ID vs. V0 curve. When the FEM unit is programmed to the "1" state, the threshold voltage of the FEM unit is negative. This is so even if V0 = 〇 V, a large 31-pole current can flow through the path area. This type of device is not suitable for large array applications. Printed by the Employees' Cooperative of the Central Bureau of Standards, Ministry of Economic Affairs Figure 27b illustrates the ID vs. VG characteristics of the FEM unit with low-channel doped ND. When the FEM unit is programmed to the "1" state, the threshold voltage is positive. When the gate is at ground potential, no current flows through the device. The large memory array of such a device has minimal standby leakage current. —A ferroelectric Pb5Ge30n film for MFMS application: Obviously lower ferroelectric capacitance results in higher memory window and lower programming voltage. Thicker films and lower core materials can result in lower ferroelectric capacitance; but the former -33- This paper size applies to the Chinese national standard ((:! '«:) six 4 specifications (210 > < 297 male 1) 409366 a? _____B7 V. Description of the invention (31) " Selection can increase the programming voltage. The oxide Pb5Ge3〇li film has extremely low er and medium Tc (178 ° C). Even the steady-state polarization of Pb5Ge3〇u film is far away. The polarization of PZT and SrBi2Ta209 films is lower than that of the PZT and SrBi2Ta2O9 films. However, the memory of the MFMS device controlled by PbsGesOu is closed. The body window is larger than the memory window of the latter two. Thus, the FEM memory unit and Its construction method. The fem gate unit can be constituted as a single transistor device or it can be constituted as a combination of Mos transistors. Although the present invention has not been disclosed as a specific example, it must be understood that it may not deviate from it as attached According to the patent application park of the invention, the structure and method of the invention are further modified. (Example 4) The ferroelectric memory (ΙΜΜ) unit of this example can be formed on a SOI (SIMOX) substrate, or Formed in the body silicon substrate. The description here will focus on the body Even though the FEM gate unit is formed on the substrate, but if used here, "shirt substrate" means an SOI substrate or a bulk silicon substrate. Some specific examples of Fem gate units must be understood. · Electric memory units are manufactured at the same time. So for the sake of clarity, the drawings do not explain the M0S transistor. "The Central Government Standards Bureau of the Ministry of Economic Affairs of the Industrial and Commercial Cooperatives Co., Ltd. Now refer to FIG. The example substrate 410 is a single crystal base and is made of bulk silicon. As illustrated in Figure 28, the substrate 41 has been partially etched as illustrated; ^ type, and some substrates are slightly doped to form an active region or device region 412. Provide the required background polarity. This example is the background polarity of the n-region, which is called the first type of conductive path. The active region 412 contains a silicon dioxide insulating region 414. As the industry knows well,- 34-k This paper size is in accordance with Chinese National Standard (CNS) Λ4 specification (210 × 297 public trips) Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs 409366 A7 _______B7 V. Description of the invention (32) As for the gate unit of the present invention, the cell is arranged in a vertical grid to form a memory array. The bulk CMOS substrate is used as an example to explain the manufacturing method. The initial steps are to manufacture η-well and P-dross structures. Separate these structures, and implant: provide threshold voltage adjustment to the transistor through ions. The substrate 41 of this specific example has been P-sand or P-dip. Photoresist is used to shield the wafer section, Secondly, the phosphorus ion is also referred to here as the first impurity doped at 30 keV to keV and implanted into the p_well at a dose of l.Pxio12 / sq. . Multiple implantation steps and / or thermal diffusion are required to obtain the optimal donor distribution for the n_layer. Photoresist was removed by stripping ginger. The implanted silicon layer can also be replaced by a selective epitaxial film that grows silicon to a thickness of 100 nm to 10,000 nm. _ Now refer to FIG. 29, followed by the formation of a p- · layer 1 6 D p-on the active region 412. The layer can be formed by implanting B or BF2 ions (herein referred to as a second type impurity replacement impurity) to the active region 412. . Shelf ions can be implanted at 3 keV to 10 keV, while BF2 ions can be implanted at 15 keV to 50 keV. In two cases, the ionic titers ranged from 5x10u / cm2 to ΐχΐ15 / cm2. Ions are thermally excited by annealing. The implanted ions will diffuse into the n-active region to form a p-n layer, which is referred to herein as a second type conductive path. The annealing is at 500. 〇 皇 丨〗 00. 〇 的 温度 进行 ·。 Temperature. _ At this point, the formation of FEM〒 units can begin. Referring now to FIG. 30, the FEM gate unit is generally indicated at 418 and includes a lower metal layer or electrode 42, a ferroelectric (FE) material 422, and an upper metal layer or electrode 424. The construction of the FEM gate unit 418 begins by depositing a lower electrode on the p-layer 416. The lower electrode 420 can be made of Pt or Ir, Ir02 or -35. The paper size is applicable to the Chinese national standard (CNS) Λ4 specification (210X297). Γ
U (請先閲讀背面之注意事項再填寫本頁) 訂U (Please read the notes on the back before filling this page) Order
•1J 經濟部中央標準局員工消費合作社印製 A7 --—87 —- —__ 五、發明説明(33 ) ~• 1J Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs A7 --- 87 --- --__ V. Description of Invention (33) ~
Pt/Ir合金或其它適當導電材料製成。也可使用其它適當導 電障層材料。較佳具體例中電極420厚度爲20毫微米至 100毫微米。 其次’ F E材料藉化學蒸氣沉積(C VD )沉積。]p E材料可 爲下列备一者:Pb(Zr Ti)〇3 (pzT),SrBi2Ta2〇9 (SBT),Made of Pt / Ir alloy or other suitable conductive material. Other suitable conductive barrier materials may also be used. In a preferred embodiment, the thickness of the electrode 420 is 20 nm to 100 nm. Next, the 'FE material is deposited by chemical vapor deposition (CVD). ] p E materials can be prepared for one of the following: Pb (Zr Ti) 〇3 (pzT), SrBi2Ta209 (SBT),
Pb5Ge3〇ii ’ BaTi03 ’或LiNb03。較佳化合物以較佳順序拆 列分別爲PbsGeWn,SBT及ΡΖΤ。FEM閘單元領域之大半 實驗工作係對ίζτ化合物進行。FE材料422沉積至100毫 微米至400毫微米厚度。 _ / r ^ — * 然後於FE材料上方形成上電極424 »上查極可由下電極 之相同材料製成至20毫微米至200毫微米厚度。 光阻施用於FEM閘單元上,然後單元蝕刻至適當構形及 尺寸。須了解如所示FEM閘單元之三層無需準確對正,原 因爲其形狀可能經由施用光阻及以具有不同幾何的阻罩钱 刻形成。但爲求请晰起見,FEM閘單元闡明爲具有鄰接對 正側壁的結構。 如圖3 1所示,1^(^層426或其它適當障壁絕緣材料係藉 CVD形成而保護FEM閘單元。TiOx經蚀刻而形成閘極電植 之側壁絕緣層。 現在參照圖3 2,可見.活性區412已經被修改成源極區 428,閘極區430,汲極學432。各區係經由施加光阻跨越 活性區412,ρ·層416及FEM閘單元418而遮蔽最終將變成 閘極區430之區域及將適當離子,此處也稱做第三型攙雜 雜質,植入活性區412之其餘部分而形成兩層n+層,此處 _ -36- 一 本紙張尺度適用中國國家標準(CNS > Λ4現格(2iOX*^7公漦) : 一~~ f請先閱讀背面之注意事項再填苑本頁} 訂Pb5Ge3〇ii 'BaTi03' or LiNb03. The preferred compounds are listed in a preferred order as PbsGeWn, SBT, and PKT. Most of the experimental work in the field of FEM gate units is performed on ζ compounds. The FE material 422 is deposited to a thickness of 100 nm to 400 nm. _ / r ^ — * Then an upper electrode 424 is formed over the FE material »The upper electrode can be made of the same material as the lower electrode to a thickness of 20 nm to 200 nm. A photoresist is applied to the FEM gate unit, and the unit is etched to the appropriate configuration and size. It must be understood that the three layers of the FEM gate unit as shown need not be precisely aligned, as its shape may be formed by applying photoresist and engraving with masks with different geometries. However, for the sake of clarity, the FEM gate unit is illustrated as having a structure that adjoins the facing sidewalls. As shown in FIG. 31, the 1 ^ (^ layer 426 or other appropriate barrier insulation material is formed by CVD to protect the FEM gate unit. TiOx is etched to form a sidewall insulation layer of the gate electrode plant. Now referring to FIG. 32, it can be seen The active region 412 has been modified into a source region 428, a gate region 430, and a drain electrode 432. Each region is shielded by applying a photoresist across the active region 412, the p · layer 416, and the FEM gate unit 418. The region of the polar region 430 and the appropriate ion, also referred to as the third type doped impurity, are implanted in the rest of the active region 412 to form two n + layers. Here _ -36- a paper size applies Chinese national standards (CNS > Λ4 is now grid (2iOX * ^ 7 公 漦): 1 ~~ f Please read the notes on the back before filling in this page} Order
I A7 B7 409366 五、發明説明(34 ) (請先閲讀背面之注意事項再填寫本頁) 稱做第三型導電通路,其將作爲源極區428及汲極區 432 〇須注意p層416延伸於閘極接面區430上及部分延伸 於汲極接面區432上。此種情沉下,適當離子植入可於較 佳能量約50 keV,但40 keV至70 keV也可接受,及ΐχΐ〇15/ 平方厘米至5xl015/平方厘米之劑量植入砷離子。另外, 磷離子可於30 keV - 60 keV之能量範圍以相同劑量範圍植 入0 現在參照圖3 3 ’晶圓藉加熱處理..而激發及擴散植入離 子,包括源極區,汲極區及下電極—。植八^|416iB*BF2 離子擴散導致形成FEM閘單元41S下方的淺p-n接面,此乃 第二型導電通路。加熱處理溫度範園係於5〇〇°C至11〇(rc (範圍可使植入離子鈍化及擴散。然後藉CVD於結構體上 方形成二氧化矽層434,或施用其它鈍化絕緣。 現在參照圖3 4,FEM閘單元418闡明爲FEM記憶單元 436之一部分,FEM記憶單元包括FEM閘單元418及下方 源極、通路及没極區,該具體例包括形成於FEm閘單元 418下方的薄淺接面區416,其爲p-n層。 經濟部中央標準局負工消費合作社印製 欲冗整説明FEM單元436,於氧化物層434形成搪孔而接 纳源極電極43 8,閘極電極440及ί及極電極44Ϊ2其連接至個 別组件。汲極電極442可.連接至汲箜區—432及ρ·η接面416。 圖3 3闡明之具體例表专鐵電閘極耗盡型MIS電晶體β於 零閘極電壓時’ FEM閘單元下方之η-通路的電荷完全被耗 _盡。如此漏電流極小。欲維持小的漏電流,下電極42〇任 何邊緣與η+源極或η+汲極區之邊緣間距以「D」表示,必 -37- 表紙張又度適用中國國家標準(CNS ) Α4規格(210XW7公釐) 經濟部中央標準局員工消贤合作社印製 409366 a? -------- ' B7 五、發明説明(35 ) " 須至少爲50毫微米俾維持小的漏電流。但隨著乃的加大, 記憶單元之串聯電阻也增高。因此較佳D不太於300毫微 米閘極漏電流係由鉑與p'型矽淺接面432之接觸及鉑與 鐵電材料之接觸決定^漏電流爲於極小至中等場強度之閘 極電施。〆層與η·型梦間之電位障壁爲〇 8 eV至i 〇…。此 種大]之%位障壁可使鐵電材料未偏極化時,或鐵電材料 以下電極的正,荷偏極化時,n-型矽通路被完全耗盡。當 鐵電材料以於+電極之負電荷偏極化時,記憶體電晶體之 閾书壓小。此種記憶體電荷性質及改變程率规劃單元需要 電壓量之技術容後詳述β __ 另外’若鐵電材料無法維持高溫加熱處理,則源極/汲 極離子植入及退火可於沉積下閘極電極前完成。 現在參照圖3 5,闡明FEM單元之替代具體例,該具體 例包括兩層矽化物層444,446形成於源極及汲極接面 區。秒化物層係於沉積絕緣層434前藉CVE>形成。此種結 構及優點爲對源極區及汲極區具有較低電阻。如此提高記 憶早元之ί及極電流£> 於SOI基板448上形成之FEM單元之具體例闡明於圖 3 6° 作業: 根據本發明構成之結構,特別有故,原因爲位於閘極區的 導電通路上方之FEM閘單元可改變閘極區極性,許可有效 電流由源極流經通路至汲極,當於「關」態時,此種結構 提供電荷完全耗盡。當於「開」態時,電流流經整個通路 -38 " ” 1' 本紙張尺度適用中國國家標準(CMS ) A4規格(2丨0·〆2?7公釐) f請先閲讀背面之注意事項再填窍本頁) -訂I A7 B7 409366 V. Description of the invention (34) (Please read the notes on the back before filling this page) It is called the third type conductive path, which will be used as the source region 428 and the drain region 432. Note the p-layer 416 Extending on the gate junction region 430 and partially on the drain junction region 432. In this case, suitable ion implantation can be performed at a better energy of about 50 keV, but 40 keV to 70 keV is acceptable, and arsenic ions are implanted at a dose of ΐχΐ015 / cm2 to 5xl015 / cm2. In addition, phosphorus ions can be implanted in the same dose range within the energy range of 30 keV-60 keV. Now refer to Figure 3 3 'Wafer by heat treatment ... and stimulate and diffuse the implanted ions, including the source region and the drain region And the lower electrode—. Plant ^ | 416iB * BF2 ion diffusion leads to the formation of a shallow p-n junction under the FEM gate unit 41S, which is a second type conductive path. The heat treatment temperature range is from 500 ° C to 110 ° C (range can passivate and diffuse the implanted ions. Then CVD forms a silicon dioxide layer 434 over the structure, or applies other passivation insulation. Now refer to In Figure 34, the FEM gate unit 418 is illustrated as a part of the FEM memory unit 436. The FEM memory unit includes the FEM gate unit 418 and the lower source, pathway, and non-electrode regions. The specific example includes a shallow layer formed under the Fem gate unit 418. The interface area 416 is a pn layer. The Central Standards Bureau of the Ministry of Economic Affairs has printed a FEM unit 436 for redundancy description, forming boring holes in the oxide layer 434 to receive the source electrode 43 8 and the gate electrode 440 and The anode electrode 44Ϊ2 is connected to an individual component. The drain electrode 442 may be connected to the drain area—432 and the ρ · η junction 416. Figure 3 3 illustrates a specific example of a special ferroelectric gate depletion type MIS transistor. When β is at zero gate voltage, the charge of the η-channel under the FEM gate unit is completely consumed. So the leakage current is very small. To maintain a small leakage current, any edge of the lower electrode 42 and the η + source or η + The distance between the edges of the drain region is indicated by "D". The paper is again applicable to the Chinese National Standard (CNS) A4 specification (210XW7 mm) printed by the Consumers ’Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs 409366 a? -------- 'B7 V. Description of Invention (35) " Must be at least 50 nanometers to maintain a small leakage current. But with the increase, the series resistance of the memory cell also increases. Therefore, it is preferred that D is not less than 300 nanometers. Gate leakage current is made of platinum and p 'type. The contact of the silicon shallow junction 432 and the contact of platinum and ferroelectric materials determine the leakage current to be the gate electricity application at a very small to medium field strength. The potential barrier between the 〆 layer and the η-type dream is 0 8 eV to i 〇 …. This kind of large]% barrier barrier can make the ferroelectric material unpolarized, or the positive electrode of the ferroelectric material below the polarized charge, the n-type silicon path is completely depleted. When the ferroelectric material Because the negative charge of the + electrode is polarized, the threshold voltage of the memory transistor is small. This kind of memory charge property and the voltage change technology required by the programming unit will be described in detail later. The material cannot sustain high-temperature heat treatment, so source / drain ion implantation and annealing can deposit the gate under The electrode is completed. Now referring to FIGS. 3 and 5, an alternative specific example of the FEM unit is illustrated. The specific example includes two silicide layers 444 and 446 formed at the source and drain junction regions. The second compound layer is deposited on the insulating layer 434. Formed by CVE >. This structure and advantages are lower resistance to the source and drain regions. This increases the early memory and electrode currents. ≫ Specific examples of FEM cells formed on SOI substrate 448 Illustrated in Figure 3 6 ° Operation: The structure constructed according to the present invention is particularly important because the FEM gate unit located above the conductive path in the gate region can change the polarity of the gate region, allowing the effective current to flow from the source through the path to The drain, when in the "off" state, this structure provides a complete depletion of charge. When in the "on" state, the current flows through the entire path -38 " "1" This paper size applies to China National Standard (CMS) A4 specifications (2 丨 0 · 〆2? 7mm) f Please read the back Note refill this page)-Order
A 409366 A7 B7 五、發明説明(36 ) 區。 根據本發明構成之記憶單元可置於記憶單元陣列,使閘 極線垂直汲極線。欲窝入;FEM閘單元418,十丫^施加至全 部閘極電極,而記憶單元之源極及汲極電極處於地電位。 如此偏極化FE 422,故負電荷位於下電極420及正電荷位 於上電極424 (參照圖1 〇b )。如此使FEM閘單元418變成高 導電態。 ®負電壓-VP4加至閘極電極(程式..規劃線),及正電壓 +vpQ施加至汲極,及源極接地及此處時,FE& — ί 於下電極420之正電荷偏極化。如此使feM閘單元418變 成低導電態(參照圖37a)。寫入過程可使記憶體陣列之各 個記憶體電晶體與陣列中-的其它記憶單元獨立窝入,並未 干擾陣列中其它記憶單元的程式規劃。 FEM閘早元418之閾電壓決定如下:對大型陣列而女, 於「1」態之閾電壓須爲正値亦即〇 4 V至0.8 V。Γ 〇」雜 之閣電壓須大於供應電壓亦即3.3 V。if通路層被p-型基板 接面以及被極淺p-表層及閘極偏壓耗盡。 記憶體视窗顯示爲等於: 2么 經濟部中央標準局貝工消费合作社印製 ΔΥ- (3)A 409366 A7 B7 V. Description of invention (36) area. The memory cell constructed according to the present invention can be placed in a memory cell array such that the gate line is perpendicular to the drain line. FEM gate unit 418, Shi Ya ^ is applied to all gate electrodes, while the source and drain electrodes of the memory unit are at ground potential. The FE 422 is thus polarized, so that the negative charge is located on the lower electrode 420 and the positive charge is located on the upper electrode 424 (see FIG. 10b). This causes the FEM gate unit 418 to become highly conductive. ® Negative voltage-VP4 is applied to the gate electrode (program .. planning line), and positive voltage + vpQ is applied to the drain, and the source is grounded and here, FE & — + Positive charge bias on the lower electrode 420 Into. This causes the feM gate unit 418 to become low-conducting (see FIG. 37a). The writing process allows each memory transistor of the memory array to be nested independently of the other memory cells in the array without disturbing the programming of other memory cells in the array. The threshold voltage of the FEM gate early element 418 is determined as follows: For large arrays, the threshold voltage in the "1" state must be positive, that is, 0 4 V to 0.8 V. The voltage of Γ 〇 ″ must be greater than the supply voltage, which is 3.3 V. The if-via layer is depleted by the p-type substrate junction and by the very shallow p-surface and gate bias. The memory window shows that it is equal to: 2? Printed by the Shellfish Consumer Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs ΔΥ- (3)
CPS 此處Qpe爲剩餘電荷及CFE爲閘單元K食電容。 P+M接面之ιΓ區之空間免度於n-區攙雜密度爲i 〇xi〇1S/立 方厘米時,約爲0.3微米。顯然若n_通路層的厚度小及挽 雜少,則「1」態閾電壓可爲正値。閾電壓可藉通路層 39 本纸張尺度適用中國國家標準{ CNS ) Λ4規格(210 X 297公疫) r 409366 A7 五、發明説明(37 ) 及p'表層之攙雜密度及厚度,電容率及鐵電電容器之剩餘 電荷調整。 讀取作業中,不大於矯頑電壓(亦即可改變記憶體内容 的電壓)之電壓乂3施加至閘極電極'及汲極電:極。因當電極 以VJu偏壓時,記憶單无内容未受干擾,故讀取作業不會 干擾記憶單元之記憶内容。因此可保有長期電荷。 單一電晶體記憶單元: MFMOS FETi —般ID相對於VG作圖.閣明於圖3 8。圖38a 闡明含高通路攙雜ND之FEM單元之10相嘴於VG特性。當 FEM閘單元未帶電時,中線爲ID相對於V〇妬線。當FEM單 元程式規劃爲「1」態時,FEM單元之閾電壓爲負値。如 此即使V G = 0,大设極電流流經通路區a此種裝置不適合 大型陣列用途。 圖3 8b闡明含低通路攙雜ND之FEM單元之ID相對於VG特 性.。FEM單元當程式规劃爲Γ 1」態時,閾電壓爲正。當 閘·極處於地電位時,並無電流流經裝置。此種裝置之大型 記:憶體陣列具有極小備用漏電流,且無需經常更新。 MFMOS用途之鐵電Pb5Ge3Ou薄膜: 經濟部中央標準局員工消費合作社印製 (請先閱讀背面之注意事項再填寫本頁} 顯然較低鐵電電容導致較高記憶體視窗及竣低程式規劃 電壓。較厚膜及較低er材料可導致鐵電電容;但若明 確界定鐵電交換域,則前一種選擇可提高程式規劃電壓。 t 常見氧化物鐵電材料具有較高er及T。。氧化物?135(^3011薄 膜具有極低er及中等T。(178°C )。表2比較MFMOS裝置之 記憶體視窗與Pb5Ge30„,PZT及SrBi2Ta209薄膜之鐵電閘 -40 - ^' 本纸張尺度適用中國國家標準(CNS ) Λ4規格(210X297公釐} 409366 A7 B7 五、發明説明(38 ) 極。即使Pb5Ge3On薄膜之穩態偏極化遠低於PZT及 SrBi2Ta209薄膜之穩態偏極化,藉Pb5Ge3On閘極控制的 MFMOS裝置之記憶體視窗仍大於它者,原因爲其低之 故。 ' 表2 :具有各種鐵電材料之MFMOS裝置之記憶體視窗 鐵電 Pb(Zr,Ti)03 SrBi2Ta2〇9 Pbs Ge3 011 ΡΓ (μϋ/οηι2) X 15 7 3.5 1000 280 35 dFerir。(埃) 2000 2Θ00 2000 vdeo (V) 3.14 4.39 6.87 Pr* (μΟ/οιη2) 當 Vd0p=O.5V 2.4 0.8 0.25 記憶體視窗 2 ?rVC^(V) 1.08 ' 1.29 3.23CPS Here Qpe is the residual charge and CFE is the K capacitor of the gate unit. The spatial avoidance of the ιΓ region of the P + M junction is about 0.3 microns when the impurity density of the n-region is i 0xi〇1S / cm3. Obviously, if the thickness of the n_channel layer is small and the interference is small, the threshold voltage of the “1” state can be positive. Threshold voltage can be obtained through the passage layer 39 This paper size is applicable to the Chinese national standard {CNS) Λ4 specification (210 X 297 public epidemic) r 409366 A7 V. Description of the invention (37) and the impurity density and thickness of p 'surface layer, permittivity and Adjustment of the residual charge of the ferroelectric capacitor. During the reading operation, a voltage not greater than the coercive voltage (that is, the voltage that changes the memory content) is applied to the gate electrode 'and the drain electrode: electrode. When the electrode is biased by VJu, the memory list has no content and is not disturbed, so the reading operation will not disturb the memory content of the memory unit. Therefore, long-term charge can be maintained. Single transistor memory cell: MFMOS FETi-general ID vs. VG mapping. Figure 38a illustrates the VG characteristics of the 10-phase mouth of a FEM unit with a high-channel doped ND. When the FEM gate unit is not charged, the center line is ID relative to the V o line. When the program of the FEM unit is “1”, the threshold voltage of the FEM unit is negative. Therefore, even if V G = 0, a large set current flows through the path areaa. This device is not suitable for large array applications. Figure 38b illustrates the ID vs. VG characteristics of a FEM unit with low-channel doped ND. When the FEM unit is programmed to the Γ 1 ″ state, the threshold voltage is positive. When the gate electrode is at ground potential, no current flows through the device. The large scale of such devices: Memories arrays have minimal standby leakage currents and do not need to be updated frequently. Ferroelectric Pb5Ge3Ou film for MFMOS: Printed by the Consumer Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs (please read the precautions on the back before filling out this page). Obviously lower ferroelectric capacitance results in higher memory window and lower program voltage. Thicker films and lower er materials can lead to ferroelectric capacitance; but if the ferroelectric exchange domain is clearly defined, the former option can increase the programming voltage. T Common oxide ferroelectric materials have higher er and T ... oxides 135 (^ 3011 film has extremely low er and medium T. (178 ° C). Table 2 compares the memory window of MFMOS device with Pb5Ge30 „, ferroelectric gate of PZT and SrBi2Ta209 film-40-^ 'This paper size is applicable Chinese National Standard (CNS) Λ4 specification (210X297 mm) 409366 A7 B7 V. Description of invention (38) pole. Even though the steady-state polarization of Pb5Ge3On film is much lower than the steady-state polarization of PZT and SrBi2Ta209 film, Pb5Ge3On The memory window of the gate-controlled MFMOS device is still larger than the others, because it is low. 'Table 2: Memory window of MFMOS devices with various ferroelectric materials Ferroelectric Pb (Zr, Ti) 03 SrBi2Ta209 Pbs Ge3 011 Γ (μϋ / οηι2) X 15 7 3.5 1000 280 35 dFerir. (Angstrom) 2000 2Θ00 2000 vdeo (V) 3.14 4.39 6.87 Pr * (μΟ / οιη2) When Vd0p = O.5V 2.4 0.8 0.25 Memory window 2? RVC ^ (V) 1.08 '1.29 3.23
竞I態Vde“叚定爲0.5V 經濟部中央標準局員工消費合作社印製 (請先閲讀背面之注意事項再坑寫本頁) 如此揭示FEM記憶單元及其構成方法。FEM閘單元可構 成爲單一電晶體裝置,或可與相關MOS電晶體構成。雖 然已經揭示本發明之較佳具體例,但須了解可未背離如隨 附之申請專利範圍界定之本發明之範圍對架_及方法做出 進一步改變。 (實例 5) ' —-- 如前述,本發明爲一種MFMOS記憶單元之製法, MFMOS記憶單元包括鐵電(FE )電容器或FEM閘單元位於 MOS電容器頂上,兩種裝置於此處合稱堆疊閘單元。本 發明之具體例中,MOS電容器面積大於鐵電電容器面 * 41 · 本紙張尺度適用中國國家標準(CNS ) A4規格(2I〇X 297公楚) ’ 經濟部中央標準局員工消费合作社印製 409366 A7 --------. B7 五、發明説明(39 ) ^ ~ ' 積,如此提高耦合效率及降低裝置的程式规劃電壓。敘述 f 一具體例其中沿堆疊M〇s &FE電容器旁側形成第二電 W體,及包括設置鐵電電容器於M〇s電容器頂上·,其中 ?電電容器及MOS電容器具有相同剖面。:此種構型可獲 # 型單兀及比較不同尺寸結構(也稱做偏位閘極鐵電記 元)更高的程式規劃電壓。又另一具體例包括1^〇3電 奋灸堆疊於FE電容器上,其中兩種電容器之大小足跡相同。 〆 本發明之堆疊鐵電記憶體閘單元―可於spj 基枝 上形成,或可於其中形成p-阱的本體矽基g形成。如此處 使用,「矽基板J表示SOI基板,本體矽基板或任何其它 類型含碎作爲一種成分且適用於本發明之基板。 使用本體基板時,基板爲n‘型。最初步驟係製造n-阱及 ρ阱…構,隔離兩種結構,及植入適當離子而對電晶體做 閾電壓調整》當使用S〇I基板時,無需形成n_阱或ρ·阱。 -現在參照圖39,矽基板闡明於51〇。較佳具體例中,基 板510爲單晶基板,係由本體矽製成。如圖39所示,基板 510係由η·矽製成。p-阱512可藉將B或BF2離子植入基板表 面,接著於95(TC至120(TC進行熱擴散步驟歷·1至4小時形 成。硼離子可於3 keV至;10 keV之g量,入,而BF2離子可 於I5 keV至5〇 keV之能,量植入。—二例之離子濃度係於 ixio12/平方厘米至lxio14/平方厘米之範園。 欲隔離裝置,二氧化矽形成的絕緣區514係於〆阱512形 成前於基板上增長。如業界人士眾所.周知,多個此區形成 "42 - - (請先閲讀背面之注意事項再填寫本頁) 1ϋ t衣--- 訂 本紙伕尺度適用中國國家標準(CNS ) Λ4規格(210X 297公费)The competition state Vde "is set to 0.5V printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs (please read the precautions on the back before writing this page). This reveals the FEM memory unit and its composition method. The FEM gate unit can be composed as A single transistor device may be formed with the related MOS transistor. Although the preferred specific examples of the present invention have been disclosed, it must be understood that the scope of the present invention and the method can be made without departing from the scope of the invention as defined by the accompanying patent application. (Example 5) As mentioned above, the present invention is a method for manufacturing an MFMOS memory unit. The MFMOS memory unit includes a ferroelectric (FE) capacitor or a FEM gate unit on top of the MOS capacitor. The two devices are here Collectively referred to as a stacking gate unit. In the specific example of the present invention, the area of the MOS capacitor is larger than the surface of the ferroelectric capacitor * 41 · This paper size applies to the Chinese National Standard (CNS) A4 specification (2IO × 297 Gongchu) '' Central Bureau of Standards, Ministry of Economic Affairs Printed by the employee consumer cooperative 409366 A7 --------. B7 V. Description of the invention (39) ^ ~ 'product, so as to improve the coupling efficiency and reduce the programming voltage of the device. Narration f a In the system, a second electric body is formed along the side of the stacked Mos & FE capacitor, and it includes a ferroelectric capacitor on top of the Mos capacitor. Among them, the electric capacitor and the MOS capacitor have the same cross section .: This configuration You can obtain # -type single-units and compare higher programming voltages of different size structures (also known as off-position gate ferroelectric cells). Another specific example includes 1 ^ 〇3 electric moxibustion stacked on FE capacitors, The two types of capacitors have the same size footprint. 堆叠 The stacked ferroelectric memory gate unit of the present invention can be formed on the spj base, or the bulk silicon base g can be formed in the p-well. As used herein, "silicon The substrate J represents an SOI substrate, a bulk silicon substrate, or any other type of substrate that contains debris as a component and is suitable for use in the present invention. When a bulk substrate is used, the substrate is an n 'type. The initial steps are to manufacture n-wells and p-wells ... Isolate the two structures and implant the appropriate ions to adjust the threshold voltage of the transistor. "When using a SOI substrate, there is no need to form an n-well or a p-well.-Referring now to Figure 39, the silicon substrate is illustrated at 51 °. In a preferred embodiment, the substrate 5 10 is a single crystal substrate, which is made of bulk silicon. As shown in Figure 39, the substrate 510 is made of η · silicon. The p-well 512 can be implanted with B or BF2 ions on the surface of the substrate, and then at 95 (TC The thermal diffusion step is performed to 120 ° C for 1 to 4 hours to form. Boron ions can be implanted in amounts of 3 keV to 10 keV, and BF2 ions can be implanted in amounts of 1 keV to 50 keV. —The ion concentration of the two cases is in the range of ixio12 / cm2 to lxio14 / cm2. To isolate the device, the insulating region 514 formed by silicon dioxide is grown on the substrate before the well 512 is formed. As everyone in the industry knows, many of this area are formed " 42--(Please read the precautions on the back before filling this page) 1ϋ t-shirt --- The size of the paper is applicable to the Chinese National Standard (CNS) Λ4 specifications (210X 297 at public expense)
I 經濟部中央標準局買工消費合作社印製 ^09366 A7 B7 五、發明説明(4〇 ) 於矽晶圓表面上。對本發明之結構而言,單元係以閘極2 對汲極及ρ·阱垂直格柵而形成記憶體陣列a 現在參照圖40 ’説明本發明之單—電晶體記憶單元。 如圖40所示,活性區512修改而含有兩個以區^石及518, 其特別最終作爲記憶單元之源極及汲極。於-味通路區52〇 此處稱做第一型導電通路仍留在基板51〇上。源極區516 及汲極區518係藉植入適當離子(此處稱做第二型攙雜雜質) 至活性區512形成兩個區,此處亦...稱做第二型導電通路 形成。此種情況下’適當離子植入可爲於1约5 〇 keV之較佳 能量,但40keV至80keV之植入可接受平方厘米 至5xl015/平方厘米之劑量範圍植入砷離子。另外,磷離 子可於20 keV- 50 keV之能量範圍以相同劑量範圍植入。 MOS電容器522係藉於適當遮蔽後增長熱氧化物524薄層 於p_通路520形成。較佳具體例中,層524之厚度爲3毫微 米至1 0毫微米。選擇性n+多晶矽層524其藉CVD形成爲 100毫微米至300毫微米厚度而完成MOS電容器522。n+多 晶矽作爲緩衝層而解除FEM電容器下電極與下方氧化物間 之應力。 此時開始形成FEM電容器閘單元。FEM閘草元528包括 下金屬層或電極53〇,鐵電(FE) 料I32及上金屬層或電 極534。FEM閘單元528 構成始於沉積下電極於m〇S電 容器522上。 下電極530可由Pt,Ir,Ir〇2或Pt/Ir合金或其它適當導 電材料製成。金屬厚度於較佳具體例爲20毫微米至100毫 -43 .. 本紙張尺度適用中國國家標华(CNS ) Μ規格(210X297公釐} f '---1 1^—J^ I ^^^1 F:· - . ^-n (請先閱讀背面之注意事項再填寫本頁)I Printed by the Central Bureau of Standards, Ministry of Economic Affairs, Consumer Cooperatives ^ 09366 A7 B7 V. Description of the invention (40) on the surface of the silicon wafer. For the structure of the present invention, the unit is a memory array formed by a gate 2 pair of drain and a ρ · well vertical grid. Now, a single-transistor memory cell of the present invention will be described with reference to FIG. 40 '. As shown in FIG. 40, the active region 512 is modified to include two regions 518 and 518, which are particularly used as the source and drain of the memory cell. The Yu-wei via region 52o, referred to herein as the first type conductive via, remains on the substrate 51o. The source region 516 and the drain region 518 are formed by implanting appropriate ions (herein referred to as a second-type doped impurity) into the active region 512 to form two regions, and are also referred to herein as second-type conductive path formation. In this case, a proper ion implantation may be a preferred energy of about 50 keV, but implantation of 40 keV to 80 keV can accept arsenic ions in a dose range of 5 cm / cm to 5 x 1015 / cm2. In addition, phosphorus ions can be implanted in the same dose range from 20 keV to 50 keV. The MOS capacitor 522 is formed by growing a thin layer of thermal oxide 524 on the p_channel 520 after being appropriately shielded. In a preferred embodiment, the thickness of the layer 524 is 3 nm to 10 nm. The selective n + polycrystalline silicon layer 524 is formed by CVD to a thickness of 100 nm to 300 nm to complete the MOS capacitor 522. n + polycrystalline silicon acts as a buffer layer to relieve the stress between the lower electrode of the FEM capacitor and the underlying oxide. At this time, the formation of the FEM capacitor gate unit is started. The FEM gate element 528 includes a lower metal layer or electrode 53, a ferroelectric (FE) material I32, and an upper metal layer or electrode 534. The FEM gate unit 528 is formed by depositing a lower electrode on the MOS capacitor 522. The lower electrode 530 may be made of Pt, Ir, Ir02 or Pt / Ir alloy or other suitable conductive materials. In the preferred embodiment, the thickness of the metal is 20 nm to 100 nm-43. The paper size is applicable to China National Standards (CNS) M specifications (210X297 mm) f '--- 1 1 ^ —J ^ I ^^ ^ 1 F: ·-. ^ -N (Please read the notes on the back before filling this page)
,1T A7 409366 B7 五、發明説明(41 ) 微米。下電極530及n+多晶矽層當使用時構成MOS電容器 522之上電極。 (請先閲讀背面之注意事項再填寫本頁) 其次,FE材料藉化學蒸氣沉積(CVD)沉積。FE材料可 爲下列任一者:Pb(Zr,Ti)03 (PZT),SrBi2Ta209 (SBT), PbsGegOu,BaTi03,LiNb03或其它適當鐵電材料。較佳化 合物以較佳順序排列爲Pb5Ge3On,SBT及PZT。FEM閘單 元領域之大半實驗工作係對PZT化合物進行。FE材料532 沉積至50毫微米至400毫微米厚度。..一 然後於FE材料上形成上電極534 2上電極可由下電極之 r 相同材料製成至20毫微米至200毫微米厚皮,形成堆疊閘 單元包括FEM閘單元528及MOS電容器522。此特定具體 例表現徧位FEM閘單元之特點,其中FEM閘'單元遮蓋面積 比MOS電容器之全表面積更小。 圖4 0結構係經由沉積適當絕緣材料如TiOx,Si3N4或其 它適當障壁絕緣材料於記憶單元上完成。形成厚層階層間 介電材料,獲得源極區、閘極區與汲極區間的適當接觸。 經濟部中央標準局員工消費合作社印製 覌在參照圖41 a及41 b,説明具有堆疊閘單元之兩種電晶 體記憶單元之構成及結構。本例中,結構係於其上方已經 形成有氧化物層542的秒基板540上形成。瑭極、汲極及 閘極區可於方法之此步驟形成或於_^彳务形成。總而言之, 較佳藉CVD沉積n+多晶梦,層544,其連同氧化物層542形成 MOS電容器546。然後如前述於n+多晶矽層,544上形成下金 屬層或電極548。下金屬層548之頂視平面圖闡明於圖 41b 0 -44- 本紙張尺度適用中國國家標华(CNS ) Λ4規格(210乂297公犮〉 ' 經濟部中央標準局員工消費合作社印製 409366 A7 _________· B7 五、發明説明(42 ) 次一步驟中’如就單一電晶體具體例説明,鐵電材料 550沉積於下電極5 48上,然後形成上金屬層5 52。下金屬 層548及上金屬層552之頂視平面圖閣明於圖42b。上及下 金屬層及FE材料構成FEM閘單无554。 光阻經施加及下電極548及η+多晶矽層544經蝕刻結果獲 得圖43所示構型。圖43所示結構包括第二電晶體556其包 括部分氧化物層542 ; η+多晶矽層544,及下金屬層548,, 該等組件以「撇號」標示。先前施加..的.光阻被剝脱去除, 施加新光阻’如前述植入第二型雜質而形吟圖44閫明之η+ 區558 ’ 560 ’ 562,於此處稱做第二型導電''通路。 現在參照圖4 5,剝脱去除原有光阻,晶圓以適當絕緣 層鈍化,施加新光阻至開放的接觸孔及界定第一互連金 屬’結果導致上金屬層552電接合至金屬層548,。 此種構型具有低漏電流的優點。裝置漏電流係由M0S電 晶體電流限制。 ‘本發明之次一具體例再度始於前述矽基板。參照圖 4 6,p_阱570上方形成氧化物層572。額外各層循序沉積 其上,包括n+多晶矽層574,下金屬層576,FE層5 78及上 金屬層580。 光阻經施加及結構經蝕刻,結是獲多圖47所示構型其 包括MOS電容器582及FPM閘單元或電容器584形成爲堆 疊閘單元585。此時一層絕緣材料如丁丨〇3£或其它適當絕緣 材料可施加俾保護鐵'電。然後,植入n+離子形成n+源極區 5 86及n+汲極區5 88。其餘ρΓ材料闡明於590提供閘通路。 ___-45-_,_ 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公疫) : ’ r (請先閲讀背面之注意事項再填两本I') 、-=θ1T A7 409366 B7 V. Description of the invention (41) Micron. The lower electrode 530 and the n + polycrystalline silicon layer constitute an upper electrode of the MOS capacitor 522 when used. (Please read the notes on the back before filling out this page.) Second, FE materials are deposited by chemical vapor deposition (CVD). The FE material can be any of the following: Pb (Zr, Ti) 03 (PZT), SrBi2Ta209 (SBT), PbsGegOu, BaTi03, LiNb03, or other suitable ferroelectric materials. The preferred compounds are arranged in a preferred order as Pb5Ge3On, SBT and PZT. Most of the experimental work in the field of FEM brake units is performed on PZT compounds. FE material 532 is deposited to a thickness of 50 nm to 400 nm. .. An upper electrode 534 is then formed on the FE material. The upper electrode can be made of the same material as the lower electrode to a thickness of 20 nm to 200 nm. A stacked gate unit includes a FEM gate unit 528 and a MOS capacitor 522. This specific example shows the characteristics of an over-position FEM gate unit, where the FEM gate 'unit covers a smaller area than the full surface area of the MOS capacitor. The 40 structure is completed by depositing a suitable insulating material such as TiOx, Si3N4 or other appropriate barrier insulating materials on the memory cell. A thick layer of interlayer dielectric material is formed to obtain proper contact between the source region, the gate region, and the drain region. Printed by the Consumers' Cooperative of the Central Standards Bureau of the Ministry of Economics 覌 Referring to Figures 41a and 41b, the structure and structure of two types of transistor memory units with stacked gate units will be described. In this example, the structure is formed on the second substrate 540 on which the oxide layer 542 has been formed. The cathode, drain, and gate regions can be formed at this step of the method or formed at the ^^ service. All in all, it is preferable to deposit the n + polycrystalline silicon layer 544 by CVD, which together with the oxide layer 542 forms the MOS capacitor 546. A lower metal layer or electrode 548 is then formed on the n + polycrystalline silicon layer, 544, as previously described. The top plan view of the lower metal layer 548 is illustrated in Figure 41b. 0 -44- This paper size is applicable to the Chinese National Standard (CNS) Λ4 specification (210 乂 297 public 犮) '' Printed by the Consumers' Cooperative of the Central Standards Bureau of the Ministry of Economy 409366 A7 _________ · B7 V. Description of the invention (42) In the next step, as described in the specific example of a single transistor, a ferroelectric material 550 is deposited on the lower electrode 5 48, and then an upper metal layer 5 52 is formed. The lower metal layer 548 and the upper metal The top plan view of layer 552 is shown in Figure 42b. The upper and lower metal layers and the FE material constitute the FEM gate 554. The photoresist is applied and the lower electrode 548 and the η + polycrystalline silicon layer 544 are etched to obtain the structure shown in Figure 43 The structure shown in FIG. 43 includes a second transistor 556 which includes a portion of the oxide layer 542; an η + polycrystalline silicon layer 544, and a lower metal layer 548. These components are marked with an "apostrophe". Previously applied .. The photoresist is stripped and removed, and a new photoresist is applied. As described above, the second type of impurities are implanted and the shape of the η + region 558 '560' 562 shown in Figure 44 is referred to herein as the second type of conductive `` path. Now refer to Figure 4 5. The original photoresist is peeled off, and the wafer is properly insulated. Layer passivation, applying new photoresistance to open contact holes and defining the first interconnecting metal 'results in the upper metal layer 552 being electrically bonded to the metal layer 548. This configuration has the advantage of low leakage current. The device leakage current is controlled by M0S Transistor current limitation. 'The next specific example of the present invention starts again from the aforementioned silicon substrate. Referring to Figure 46, an oxide layer 572 is formed above the p-well 570. Additional layers are sequentially deposited thereon, including the n + polycrystalline silicon layer 574, below Metal layer 576, FE layer 5 78 and upper metal layer 580. The photoresist is applied and the structure is etched. The structure shown in Figure 47 is obtained. It includes a MOS capacitor 582 and an FPM gate unit or a capacitor 584 formed as a stacked gate unit. 585. At this time, a layer of insulating material such as Ding O 3 £ or other appropriate insulating material can be applied with a protective iron. Then, n + ions are implanted to form n + source region 5 86 and n + drain region 5 88. The remaining ρΓ material It is stated that the gate access is provided at 590. ___- 45 -_, _ This paper size is applicable to the Chinese National Standard (CNS) A4 specification (210X297 public epidemic): 'r (Please read the precautions on the back before filling in two I'), -= θ
-JJ 409366 A7 B7 五、發明説明(43 ) 現在參照圖4 9,敘述最終結構且有絕緣層592安置定位 其包括源極電極594,閘極電椏596及汲極電極598。 此特定具體例提供極小型單元《該裝置格外適用於VLSI 記憶體用途。 程式規劃至高閾電壓態: 圖5 0闡明用於此處記憶單元之鐵電材料的P-E磁滞迴 線。P r爲鐵電材料之偏極化值。Pr〇爲負極性飽和偏極 化。Pr00爲裝置已經程式規劃至高閾-電.壓態後鬆他裝置後 鐵電村料之偏極化。Pr!爲正極性飽-和偏極;化.Pr10爲裝置 — · 已經程式規劃至低閾電壓態後於裝置鬆弛破之鐵電材料之 偏極化。 根據本發明構成之裝置之電何分布闡明於圖5 1,其中 圖51a闡明裝置程式规劃爲「〇」態之電荷分布。及圖51b 闡明裝置程式規劃爲「1」態時之電荷分布。欲對大的正 閾電壓程式規劃記憶體電晶體至Γ 〇」態時,裝置於正常 工作電壓不導電,負電壓施加至控制閘,結果獲得圖5 j a 所示之電荷分布□波森(poison)方程式爲: (請先閱讀背面之注意事項再填寫本頁) * JL. --- ά'Ϋ 經濟部中央標準局貝工消費合作社印製 ctc: ε〇χ —[c(x)c(x = Τοχ) ] + c(x = Tax) ε〇χ εη (4) 積分兩次獲得-JJ 409366 A7 B7 V. Description of the Invention (43) Now referring to FIG. 49, the final structure will be described with an insulating layer 592 for positioning. It includes a source electrode 594, a gate electrode 596, and a drain electrode 598. This specific example provides a very small unit "This device is particularly suitable for VLSI memory applications. Programming to a high threshold voltage state: Figure 50 illustrates the P-E hysteresis loop of the ferroelectric material used for the memory cell here. P r is the polarization value of the ferroelectric material. Pr0 is a negative polarity saturation polarization. Pr00 is the polarization of the ferroelectric material after the device has been programmed to a high threshold-electricity. After the pressure is released, the device is released. Pr! Is positive-polarity and partial-polarity; and Pr10 is the device — · The polarization of the ferroelectric material that has been loosened and broken in the device after it has been programmed to a low threshold voltage state. The electrical distribution of the device constructed according to the present invention is illustrated in Fig. 51, where Fig. 51a illustrates the charge distribution of the device program planned to the "0" state. And Fig. 51b illustrates the charge distribution when the device program is planned to be "1". When you want to program a large positive threshold voltage to program the memory transistor to the Γ ″ state, the device is not conductive at normal operating voltage, and a negative voltage is applied to the control gate. As a result, the charge distribution shown in Figure 5ja is shown. Poson (poison ) The formula is: (Please read the notes on the back before filling this page) * JL. --- ά'Ϋ Printed by the Shellfish Consumer Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs ctc: ε〇χ — [c (x) c ( x = Τοχ)] + c (x = Tax) ε〇χ εη (4) points obtained twice
Pr〇qp si Cfe (5) -46 本紙張尺度適用中國國家標隼(CNS ) A4規狢(2丨OX 297公釐) 409366 A7 B7 五、發明説明(44 此處PrQ顚示於圖5 0。跨越鐵電電容器之塵降爲:Pr〇qp si Cfe (5) -46 The paper size is applicable to Chinese National Standard (CNS) A4 (2 丨 OX 297 mm) 409366 A7 B7 V. Description of the invention (44 PrQ is shown here in Figure 5 0 Dust across ferroelectric capacitors is:
FF
Pr〇qp Cf£ (6) 因此程式规劃電壓爲: ⑺ 程式规劃後之閾*壓爲:Pr〇qp Cf £ (6) So the programming voltage is: 阈 The threshold * pressure after programming is:
Vw = Vfs + Hf〆 ^<r>FP£Stcl^ ^ . + Pr〇〇 C〇.xVw = Vfs + Hf〆 ^ < r > FP £ Stcl ^ ^. + Pr〇〇 C〇.x
Cfe (8) 此處Pr00爲由程式規劃裝置至高閾電壓鬆弛後之鐵電材料 之偏極化。 程式规劃至低閾電壓態: •欲程式规劃記憶體爲低閾電壓亦即「1」態,正電壓v 施加至閘極及負電壓VD1施加至没極及p-阱。當襞置係於 SOI基板上製造時’無需p-阱。源極爲地電位。電荷分布 作圖於圖51be波森方程式爲: - j--------—— (請先閲讀背面之注意事項再填寫本頁) -5 經濟部中央標準局貝工消費合作社印製 —--qN^[U(x)U(^v)]^ ~A^qn [c(x = W)c(x = W^T〇x)]^ [S^^qn]PrL 的=·^ )内) dx: es/ 積分式(9)兩次獲得:Cfe (8) Here Pr00 is the polarization of the ferroelectric material after the program planning device is relaxed to a high threshold voltage. Program to Low Threshold Voltage State: • To program the memory to a low threshold voltage, which is the "1" state, a positive voltage v is applied to the gate and a negative voltage VD1 is applied to the non-pole and p-well. When fabricated on a SOI substrate, a p-well is not required. The source is at ground potential. The charge distribution is plotted in Figure 51be. The Posen equation is:-j --------—— (Please read the precautions on the back before filling this page) -5 Printed by the Shellfish Consumer Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs --- qN ^ [U (x) U (^ v)] ^ ~ A ^ qn [c (x = W) c (x = W ^ T〇x)] ^ [S ^^ qn] of PrL = · ^)) Dx: es / integral formula (9) obtained twice:
〜+ 2 4 + ί^,^^Ζη y〇i C〇x CfE (10) 47- 表紙張尺度適用中國國家標準(CNS ) Λ4規格(210X297公釐) r 409366 五、發明説明(45 ) 式(10)改寫爲: A7 B7 yn=vFB+2<pf ί-f^ Sr, :v7fyr ^ ^ (v -fq gy Νλ φΡ„ + qrt] Pr,~ + 2 4 + ί ^, ^^ Zη y〇i C〇x CfE (10) 47- The paper size is applicable to the Chinese National Standard (CNS) Λ4 specification (210X297 mm) r 409366 5. Description of the invention (45) Formula (10) Rewritten as: A7 B7 yn = vFB + 2 < pf ί-f ^ Sr,: v7fyr ^ ^ (v -fq gy Νλ φΡ „+ qrt] Pr,
Cf£ Ύ ( H ) 由表面顚倒成至鐵電電容器頂電極之壓降爲: ε<;, , s:si Ν ^φ^Λ-qn] Pr,Cf £ Ύ (H) The voltage drop from the surface 顚 to the top electrode of the ferroelectric capacitor is: ε <;,, s: si Ν ^ φ ^ Λ-qn] Pr,
CoxCox
C η (12) 鐵電電容之壓降爲 y fe 因此供應電壓爲:C η (12) The voltage drop of the ferroelectric capacitor is y fe so the supply voltage is:
Cfb (13) f請先闼請背面之注意事項耳嗔寫本頁} V^V0,-VF8^-V^1^ (14) .丁 閾電壓爲: ,[4〇7^~J7f .和。H Pr,〇 νΤί^ν^2φ^ —^ F£ (15) 經濟部中央標準局I工消費合作社印製 此處由程式规劃至低閾電壓•遙鬆他後.’ PrlQ爲偏輕化電 荷β如此經由(1 )提高通路攙雜密! N>. ’( 2 )經由選擇較 低介電常數材料及/或增,加鐵電膜厚度而減少鐵電電容, 及(3 )經由使用較薄的熱氧化物層增加閘極氧化物電容 Cox,裝置於「0」態之閾電壓可大於0.〇V。此乃單一電 晶體RAM VLSI陣列的必要條件。結果顯然指示當氧化物 48 - 本紙張尺交適用中國國家標準(CNS ) Λ4規格(2IOX297公釐) 4093G6 經濟部中央標準局員工消費合作社印製 A7 B7 五、發明説明(46 ) " — 電容増高時,程式規劃電壓變小。 於多種偏極化條件下,裝置之程式规劃電壓及閾電壓可 由上式算出.及顯示於表3,此處程式規劃電壓及通路攙雜 密度調整而獲得「1」態閾電壓爲Vt/= 〇6, v。程式規劃 期間偏極化電荷假定爲比穩態偏極化高36%。.進一步假定 鐵電材料厚度爲300毫微米及電容爲2·9χ10-7 F/cm2。程式 規劃期間跨越鐵電材料之壓降爲3 V。兩種閘極氧化物厚 度亦即5毫微米及6毫微米已經評估.記憶體視窗△▽^顯 示於表3末欄及示例説明於圖5 2 / _ 表3 ^ 丁 ox = T〇x = 6nm prc〇 = Prt 攙雜 Vp[ •vP〇 攙雜 I VP| Vp〇 AVth 0.50 5,70 -4.70 1.23 I 5.23 -3.53 ^ 05 0,75 6.00 5.95 -4.4-5 5.22 '5.71 -3.09 ;78 1.00 13.59 6.20 -4-.20 11.97 6.15 -2.65 '50 1.25 24.50 6.45 -3.95 21.48 6.59 -2.21 c 73 1.50 38.44 6,70 ‘3.70 33.76 7.03 -1.78 V 95 1,75 55,50 6.95 -3.45 48.79 7Λ6 -1.34 *、68 2.00 75,69 7.20 -3.20 66.59 7.90 -0.90 I 2.25 99.00 7.45 1 -2.95 ' B7.U 8.34 -0.46 1 . 13— 2.50 125.44 7.70 1 -2.70 no. 8.78 -0.03 I -'S5 現在參照圖52a,闡明先前技術裝置之ID# VG作圖。線 5100表示Vtl小於零而Vt0爲正値之,沉^。具有此種特性之 結構需要至少兩種裝置(,一種記憶體電晶體及一種普通電 晶體)用於RAM陣列,作用於單一電晶體RAM陣列將需要 相當高的程式規劃電壓。 圖52b闡明根據本發明方法形成之裝置之Γ 1」閾電壓以 _-49- ] . 本纸張尺度適用中國國家標孪(CNS ) A4規格(210X297公逄) (請先閲讀背面之注意事項再填寫本頁)Cfb (13) f, please read the notes on the back first. Please write this page} V ^ V0, -VF8 ^ -V ^ 1 ^ (14). The threshold voltage is:, [4〇7 ^ ~ J7f. And . H Pr, 〇νΤί ^ ν ^ 2φ ^ — ^ F £ (15) Printed by the I-Consumer Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs. The program is planned to a low threshold voltage. • After easing him. PrlQ is a lighter charge. In this way, β increases the density of the passage through (1)! N >. '(2) reducing ferroelectric capacitance by selecting lower dielectric constant materials and / or increasing ferroelectric film thickness, and (3) increasing gate oxide capacitance by using thinner thermal oxide layer Cox, the threshold voltage of the device in the "0" state can be greater than 0.0V. This is a necessary condition for a single transistor RAM VLSI array. The results clearly indicate that when the oxide 48-this paper rule is applied to the Chinese National Standard (CNS) Λ4 specification (2IOX297 mm) 4093G6 Printed by the Consumer Standards Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs A7 B7 V. Invention Description (46) " — Capacitor When it is high, the programming voltage becomes smaller. Under a variety of polarization conditions, the programmed voltage and threshold voltage of the device can be calculated by the above formula. It is shown in Table 3. Here, the programmed voltage and the channel impurity density are adjusted to obtain the “1” state threshold voltage as Vt / = 〇 6, v. During the programming period, the polarization charge is assumed to be 36% higher than the steady-state polarization. It is further assumed that the thickness of the ferroelectric material is 300 nm and the capacitance is 2.9 × 10-7 F / cm2. The voltage drop across the ferroelectric material during programming was 3 V. The thicknesses of the two gate oxides, 5 nm and 6 nm, have been evaluated. The memory window △ ▽ ^ is shown in the bottom column of Table 3 and an example is shown in Figure 5 2 / _ Table 3 ^ ox = T〇x = 6nm prc〇 = Prt doped Vp [• vP〇 doped I VP | Vp〇AVth 0.50 5,70 -4.70 1.23 I 5.23 -3.53 ^ 05 0,75 6.00 5.95 -4.4-5 5.22 '5.71 -3.09; 78 1.00 13.59 6.20 -4-.20 11.97 6.15 -2.65 '50 1.25 24.50 6.45 -3.95 21.48 6.59 -2.21 c 73 1.50 38.44 6,70 '3.70 33.76 7.03 -1.78 V 95 1,75 55,50 6.95 -3.45 48.79 7Λ6 -1.34 *, 68 2.00 75,69 7.20 -3.20 66.59 7.90 -0.90 I 2.25 99.00 7.45 1 -2.95 'B7.U 8.34 -0.46 1. 13— 2.50 125.44 7.70 1 -2.70 no. 8.78 -0.03 I -'S5 Referring now to Figure 52a, Illustrate ID # VG mapping of prior art devices. Line 5100 indicates that Vtl is less than zero and Vt0 is positive, which is Shen. A structure with this characteristic requires at least two devices (a memory transistor and a common transistor) for the RAM array, and acting on a single transistor RAM array will require a relatively high programming voltage. Figure 52b illustrates the Γ 1 ″ threshold voltage of the device formed according to the method of the present invention is _-49-]. This paper size is applicable to the Chinese National Standard (CNS) A4 specification (210X297 cm) (Please read the precautions on the back first) (Fill in this page again)
經濟部中央標準局員工消贽合作社印製 409366 A7 _______ B7_ 五、發明説明(47 ) 線5104表示’及「〇」閾電壓以線51〇6表示。 如此揭示FEM記憶單元及其構成方法。雖然已經揭示本 發明之較佳具體例,但須了解未背離如隨附之申請專利範 圍界定之本發明之範園可對架構及方法做出,進一步改變。 (實例6 ) _ 本實例之鐵電圮憶體(FEM)單元係於SOI (SIMOX)基板 上形成,或可巧成於本體矽基板。此處説明將集中於本體 矽基板形成的/em閘單元。 現在參照圖5 3 ’矽基板闡明於61〇。較缚具體例中,基 板610爲單晶基板且由本體矽製成。其它真體例可於s〇i 基板上形成。如此處.使用「矽基板」表示本體矽基板或 SOI基板或任何其它適當-以矽爲主的基板。如圖5 3閣明, p基板610含有第一型攙雜雜質,其爲硼或硼化合物,濃 度爲約l.OxlO15/立方厘米至50M015/立方厘米。 淺ιΓ型層612 (阱結構)此處亦稱做第二型導電通路,其 含有第二型攙雜雜質隨後藉磷或砷植入而於閘極區下方形 成。離子能爲10 keV至50 keV及劑量爲ΐ.οχίο!2/平方厘米 至l.OxlO13/平方厘米。 p型硬之極淺層i 4 (次阱結構)形成於淺n_型層1 2且含有 第三型攙雜雜▼以BF2植入n-型第土導!層頂上。能係 於10 keV至4〇 keV之範p及劑量爲5 〇χ1〇11/平方厘米至 5.0x10 /平方厘米之範圍。此層於此處稱做第三型導電通 路。 此時可開始形成FEM閘單元。FEM閘單元概略標示爲 "50 - 银尺度適用巾ϋ 準(CNS ) Λ峨格(2似297公髮〉 -——--- t - - ^^1· - - — (請先聞靖背面之注意事項再填寫本頁)Printed by the Consumer Standards Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs 409366 A7 _______ B7_ V. Description of the Invention (47) Line 5104 indicates ’and“ 〇 ”threshold voltage is indicated by line 5106. In this way, the FEM memory unit and its constitution method are revealed. Although the preferred specific examples of the present invention have been disclosed, it must be understood that the structure and method of the present invention can be further changed without departing from the scope of the present invention as defined in the appended patent application scope. (Example 6) _ The ferroelectric memory (FEM) unit of this example is formed on a SOI (SIMOX) substrate, or it may be formed on a bulk silicon substrate. The description here will focus on the / em gate unit formed by the bulk silicon substrate. Referring now to Fig. 5 3 'silicon substrate is illustrated at 61 °. In a more specific example, the substrate 610 is a single crystal substrate and is made of bulk silicon. Other real examples can be formed on the soi substrate. As used herein, "silicon substrate" means the bulk silicon substrate or SOI substrate or any other suitable-silicon-based substrate. As shown in FIG. 5A, the p-substrate 610 contains a first-type doped impurity, which is boron or a boron compound, and has a concentration of about 1.0 × 10 15 / cm 3 to 50 M015 / cm 3. The shallow Γ-type layer 612 (well structure) is also referred to herein as a second-type conductive path, which contains a second-type doped impurity and is then formed in a square shape under the gate region by implanting phosphorus or arsenic. The ion energy is 10 keV to 50 keV and the dose is ΐ.οχίο! 2 / cm 2 to l.OxlO13 / cm 2. The p-type hard extremely shallow layer i 4 (sub-well structure) is formed in the shallow n_-type layer 12 and contains the third type dopant ▼ The n-type soil guide is implanted with BF2! Layer on top. It can range from 10 keV to 40 keV and the dose is in the range of 50 × 1010 / cm2 to 5.0 × 10 / cm2. This layer is referred to herein as a third type conductive path. At this point, the formation of the FEM gate unit can begin. The FEM brake unit is roughly labeled as "50-Silver Standard Applicable Standard (CNS) ΛEG (2 similar to 297 public hair)-------t--^^ 1 ·---(please first hear Jing (Notes on the back then fill out this page)
I 丁 、-'° 409366 A7 B7 五、發明説明(48 ) 616及包括下金屬層或電極618,鐵電(FE)材料620及上金 屬層或電極622。FEM閘單元616之構成始於沉積下電極 618與ρ·層614上。下電極618可由Ir或Ir/Ir02合金或Pt/Ir合 金或其它適當導電材料製成。較佳具體例中:,,金屬厚度爲 20毫微来至100毫微米。 其次,於適當遮蔽後,:FE材料藉化學蒸氣沉積(CVD) 沉積。FE材料可爲下列任一者·· Pb(Zr,Ti)03 (PZT), SrBi2Ta209 (SBT),Pb5Ge3On,BaTi03,或 LiNb03。以較 佳順序表示,較佳化合物爲Pb5Ge30„,SgT及PZT。FEM 閘單元領域之大半實驗工作係對PZT化合私進行。FE材 料620沉積至5 0毫微米至400毫微米厚度。 然後,於FE材料上形,成上電極622。上電極可由Pt, Pt/Ir合金,Pt/Ir02合金或其它適當材料製成至20毫微米至 200毫微米厚度。 光阻施用於FEM閘單元上,然後單元蝕刻成適當構形及 尺寸。須了解如所示FEM閘單元之三層無需準確對正,原 因爲其形狀可經由施加光阻及以具有不同幾何的阻罩蝕刻 形成。但爲求清晰起見,FEM閘單元闡明爲具有鄰接對正 側壁的結構。 現在〆基板610藉植入.適當離子#處亦稱做第四型攙雜 雜質而形成兩層n+層,此.處亦稱做第四型導電通路,其作 / 爲源極區624及ί及極區626。此種情況下,適當離子植入 可爲於約50 keV之較佳能,但40 keV至70 keV亦可接受及 以lxlO15/平方厘米至5x1015/平方厘米劑量植入砷離子。 •*51 - 本紙張尺度適用中國國家標隼(CNS ) A4規格(2〗0X297公楚:〉 ‘ ( 11^ - > - I / 1/ -1 ^^1 ^ϋ> n (請先閲读背面之注意事項再填寫本頁) -1° 經濟部中央標準局貝工消費合作社印製 409366 ^ ------ --^_____ 五、發明説明(49 ) · 另外可以相同劑量範園於30 keV- 60 keV之能量範園植入 磷離子。 晶圓經加熱處理而激發及擴散源極區及汲極區的植入離 子°加熱處理之溫度範圍爲500Ό至1100β〇而使植入離子 激發及擴散。I Ding,-'° 409366 A7 B7 V. Description of the invention (48) 616 and includes a lower metal layer or electrode 618, a ferroelectric (FE) material 620 and an upper metal layer or electrode 622. The composition of the FEM gate unit 616 begins by depositing the lower electrode 618 and the p · layer 614. The lower electrode 618 may be made of Ir or Ir / Ir02 alloy or Pt / Ir alloy or other suitable conductive material. In a preferred embodiment, the thickness of the metal is 20 nanometers to 100 nanometers. Secondly, after proper masking, the FE material is deposited by chemical vapor deposition (CVD). The FE material can be any of the following: Pb (Zr, Ti) 03 (PZT), SrBi2Ta209 (SBT), Pb5Ge3On, BaTi03, or LiNb03. In a preferred order, the preferred compounds are Pb5Ge30, SgT, and PZT. Most of the experimental work in the field of FEM gate units is performed on PZT compounds. FE material 620 is deposited to a thickness of 50 nm to 400 nm. Then, in The FE material is shaped to form an upper electrode 622. The upper electrode may be made of Pt, Pt / Ir alloy, Pt / Ir02 alloy or other suitable material to a thickness of 20 nm to 200 nm. A photoresist is applied to the FEM gate unit, and then The unit is etched into a proper configuration and size. It must be understood that the three layers of the FEM gate unit as shown do not need to be precisely aligned, because the shape can be formed by applying photoresist and etching with masks with different geometries. But for clarity See, the FEM gate unit is illustrated as having a structure adjacent to the opposite side wall. Now the 〆 substrate 610 is implanted. The appropriate ion # is also called a fourth type doped impurity to form two n + layers, which is also called the fourth. Type conductive paths, which are / are source regions 624 and ί and pole regions 626. In this case, appropriate ion implantation may be better than about 50 keV, but 40 keV to 70 keV is also acceptable and lxlO15 / Cm2 to 5x1015 / cm2 Implantation of arsenic ions. * 51-This paper size is applicable to China National Standard (CNS) A4 specification (2〗 0X297):> '(11 ^->-I / 1 / -1 ^^ 1 ^ ϋ > n (Please read the notes on the back before filling this page) -1 ° Printed by the Shellfish Consumer Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs 409366 ^ -------^ _____ V. Description of the Invention (49) · In addition Phosphorus ions can be implanted at the same dosage range in the energy range of 30 keV- 60 keV. The wafer is heated to excite and diffuse the implanted ions in the source and drain regions. The temperature range of the heat treatment is 500Ό to 1100β. 〇 Excitation and diffusion of implanted ions.
TiOx ’ Si3N4或其它適當障壁絕緣材料層630係藉CVD形 成而保護FEM閘單元,結果導致形成FE記憶單元632。 欲完成FEM單元632之説明,於絕.綠層630形成搪孔而容 納字線(WL)(閘極)電極634及位元線(BL ),電極636其連接 至其個別組件。源極624接地640。 經濟部中央標準局員工消費合作社印製 (諳先閱讀背面之注意事項再填寫本頁) 圖5 3闡明之具體例表示鐵電閘極耗盡型MFMS電晶體。 於零閘極電壓時’於FEM閘單元下方n_通路之電荷完全耗 盡。如此漏電流極小。欲維持小的漏電流,介於下電椏 618任一邊緣與n+源極區及n+汲極區626乏邊緣間距以 「D J表示必須至少爲5 〇毫微米俾維持小的漏電流。但隨 著D的加大,記憶單元之串聯電阻也增加。因此較佳〇不 大於3〇0毫微米。第三型p-導電層14與第二型^導電層612 間之電位障層約〇9 eV。此種大小的電位障層可使n-型發 通路於鐵電材料未偏極化時完全被耗盡。當·鐵電材料62〇 以毗鄰下電極618之正電荷偏極化^,閾電壓小。當鐵電 材料620以础鄰下電極6丨8之負電荷偏極化時,記憶體電 晶體之闞電壓極大,此種記憶體電荷本質及改變程式規劃 單元所需電壓量技術容後詳述。 另外若鐵電材料無法忍受高溫加熱處理,則源極/汲極 -52 - 本纸張尺度適用中國國家榇準(CNS ) A4規格(2!0X297公垃) 409366 A7 經濟部中央標準局員工消費合作社印製 . B7五、發明説明(5〇 ) 離子植入及退火可於沉.積下閘極電極前完成。作業: 根據本發明構成之結構特別有效,原因爲位於閘極區之 導電通路上方的ΪΈΜ閘單元可改變閘極區極性。許可有效 電流由源極流經通路至汲極。於「關」條件時結構提供全 部電荷耗盡。耗盡型裝置之作業理論類似接面FET。 IMFMS ΪΈΤ之概略1〇對VG作圖闡明於圖5 4。圖54a説明 對稱FEM單元ilD,VG特性。當FEM.間單元未帶電時,中 線爲Id相對於V〇曲線,此處Pr=0。當FEM單元程式規劃爲 「1」態時,FEM單元之閾電壓爲負。如此即使VG = 0V,大的汲極電流可流經通路區。此種裝置不適合大型 陣列應用。 - 圖54b説明本發明之非對稱FEM單元之。對VG特性。當 程式規劃爲「1」態時,FEM單元之閾電壓爲正。當閘極 處於地電位時,並無電流流經裝置。此種裝置之大型記憶 體陣列可有極小的備用漏電流。 本發明之非對稱偏極化鐵電記憶體電晶體單元可應用至 MFMS單元及MFMOS單元提供低漏電流、高速、極大型 記憶體陣列。低漏電流可對「1」態及「0」‘態獲得正閾 電壓達成。經由提高驅動電流及降_低|置之通路電容可達 成高速讀及寫。因電子$動性比較孔隙移動性遠更高,故 ιΓ通路記憶體裝置用於高速作業較佳。 現在參照圖5 5,Jiang等「高密度非易失性鐵電 SrBi2Ta20“i憶體之新穎技術」,1996年VLSI技術研討 « 53 ** 本纸張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) — ·々 r !0 ^ - - - I- - J A I (讀先閱讀背而之注意事項再填寫本瓦)TiOx'Si3N4 or other appropriate barrier insulating material layer 630 is formed by CVD to protect the FEM gate unit, resulting in the formation of an FE memory unit 632. To complete the description of the FEM unit 632, a hole is formed in the green layer 630 to accommodate the word line (WL) (gate) electrode 634 and bit line (BL), and the electrode 636 is connected to its individual component. The source 624 is grounded 640. Printed by the Consumer Cooperatives of the Central Bureau of Standards of the Ministry of Economic Affairs (please read the precautions on the back before filling this page). Figure 5 3 illustrates a specific example of a ferroelectric gate depleted MFMS transistor. At zero gate voltage, the charge in the n_ path below the FEM gate unit is completely depleted. Thus, the leakage current is extremely small. To maintain a small leakage current, the distance between any edge of the power down 618 and the n + source and n + drain regions 626 has a marginal margin of "626. The DJ indicates that it must be at least 50 nm. However, the small leakage current is maintained. With the increase of D, the series resistance of the memory cell also increases. Therefore, it is preferably 0 or less than 300 nm. The potential barrier layer between the third type p-conductive layer 14 and the second type ^ conductive layer 612 is about 0.9 eV. A potential barrier of this size can completely deplete the n-type hair path when the ferroelectric material is not polarized. When the ferroelectric material 62 ° is polarized with a positive charge adjacent to the lower electrode 618 ^, The threshold voltage is small. When the ferroelectric material 620 is polarized with the negative charge of the lower electrode 6 丨 8, the threshold voltage of the memory transistor is extremely large. The nature of the charge of this memory and the amount of voltage required to change the programming unit In addition, if the ferroelectric material cannot tolerate high temperature heat treatment, the source / drain -52-this paper size applies to China National Standard (CNS) A4 specification (2! 0X297 public waste) 409366 A7 Ministry of Economy Printed by the Consumer Standards Cooperative of the Central Bureau of Standards. B7 V. Invention Description (50) Ion Implantation The annealing and annealing can be completed before the gate electrode is deposited. Operation: The structure constructed according to the present invention is particularly effective, because the MG gate unit located above the conductive path in the gate region can change the polarity of the gate region. The source flows through the path to the drain. The structure provides full charge depletion in the "off" condition. Depletion devices operate similarly to interface FETs. The outline of the IMFMS VT 10 vs. VG is illustrated in Figure 54. Figure 54a illustrates the symmetric FEM cell ilD, VG characteristics. When the FEM unit is not charged, the center line is the curve of Id versus V0, where Pr = 0. When the FEM unit program is planned to be "1", the threshold voltage of the FEM unit is negative. Thus, even if VG = 0V, a large drain current can flow through the path region. This device is not suitable for large array applications. -Figure 54b illustrates one of the asymmetric FEM units of the present invention. For VG characteristics. When the program plan is "1", the threshold voltage of the FEM unit is positive. When the gate is at ground potential, no current flows through the device. The large memory array of such a device can have minimal standby leakage current. The asymmetrically polarized ferroelectric memory transistor unit of the present invention can be applied to MFMS units and MFMOS units to provide low leakage current, high speed, and very large memory arrays. Low leakage current can be achieved for the "1" state and the "0" 'state' for a positive threshold voltage. High-speed read and write can be achieved by increasing the driving current and reducing the path capacitance. Because the electron mobility is much higher than the pore mobility, ιΓ channel memory devices are better for high-speed operations. Referring now to Fig. 5, Jiang et al. "High-density non-volatile ferroelectric SrBi2Ta20" innovative technology of i-memory body ", 1996 VLSI Technology Seminar« 53 ** This paper size applies the Chinese National Standard (CNS) A4 specification ( 210X297 mm) — · 々r! 0 ^---I--JAI (Read the precautions before reading and then fill out the tile)
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J 409366 B7__ 五、發明説明(S1 ) 會,檀香山1996年6月11-1 3日26頁,敘述以銦替代鉑作 爲鐵電記憶體電容器之下電極可獲得改良性能。如圖5 5 闡明,敘述對具有不同下電極之SrBi2Ta209 (SBT)電容器 對100 kHz單擊脈層測得之磁滯迴線。圖55a之下電極 爲Pt/Ti〇2 ;圖551>之下電極爲ir〇2 ;及圖55c之下電極爲純 Ir。電容器被寫入後1 〇秒測量剩餘偏極化ρΝν。如圖55c 所示,Pt/SBT/Ir電容器於正偏極化顯示極大去偏極化電 荷,而負偏極化電容器之去偏極化極小_。 欲獲得正値「1」態(高導電態)閾電壓裝置必須於下 鐵電/電極介面具有小的正偏極化電荷,如細56a所示。欲 維持大的記憶體視窗,也需於下鐵電/電極介面有大的偏 極化負電荷,如圖56b所-示。此可以Pt/SBT/Ir半導體結構 達成。'穩態「1 J態偏極化電荷爲約10 μ(:/£;ιη2,而穩態 「0 J ,禮偏極化電荷爲約-2 pC/cin2 〇對具介電常數280之 0.3微米SBT薄膜而言,對應閾電壓遷移分別爲12」v及· 2/42 V。經由調整通路攙雜密度而於〇鐵電偏極化達成閾 電壓約3 V ’可獲得VT1及VT〇分別爲約〇. 6伏及1 5伏,如圖 54b所示。 經濟部中央標準局員工消费合作社印" (請先聞讀背面之注意事項再填寫本頁) 此種鐵電記憶體裝置可用於低電壓、高奢度及高速用 途。記憶單元鋪置於p-阱610如圖5—7所—示。圖5 7闡明九單 元記憶禮陣列’其中字鱗標示爲WL1,WL2及WL3,位元 線或汲極線標示爲BLI,BL2及BL3。全部電晶體之源極 區及基板皆接地。源極、字線及位元線獨立連接至周邊電 路,如圖5 7所示。記憶體陣列經由施加Vpp正電壓至字線 -54 ** ·* 本紙張尺度適用中國國家橒準(<:呢)如说格(210\297公釐) 經濟部中夫摞準扃負工消费合作社印製 409366 A7 ' B7 五、發明説明(52 ) (閘椏)而位元線接地而被區塊程式規劃爲「〗」(高導電) 態。欲程式規劃個別記憶單元爲「〇」(低導電)態。負程 式規劃電壓-Vpp施加至字線而正程式規劃電壓Vpp施加至 位元線。如此導致僅有一個單元具有偏壓於閘極爲^^及 於汲極爲+Vpp。此種記憶單元爲整個陣列中唯一將被窝成 「〇」態的單元。 許多電極組气可觀察得非對稱偏極化鬆弛。此外可於任 一種鐵電薄膜及任一種鐵電閘極結構觀.察得。非對稱性偏 極化鬆弛機制對處理條件既複雜且敏感。命此要求於本發 明之較佳具體例中’非對稱偏極化鬆弛技褚用來製造鐵電 閘極控制的單一電晶體記憶單元。 ΪΈΜ閘單元616之閾電塵決定如下:對大型陣列而言, 於「1 J態之閾電壓必須爲小正値亦即04 V至〇 8 V。 「〇」態之閾電壓須大於供應電壓亦即3.3 v a n-通路層被 p型基板接面以及被極淺p-表層及閘極偏壓耗盡。 記憶體視窗顯示爲等於: ΔΥί 此處Qfe爲剩餘電荷及Cfe爲閘單元之鐵電電容。 讀取作業期間,不大於矯頭電壓(亦即可改變記憶體内 容之電壓)之電壓Va施加至閘極電雇支汲極電極。極 以VaM偏壓時,記憶單天;内容未受干擾,故讀取作業不會 干擾任何記憶單元之記憶内容。因此可獲得長時間保有杏 荷。 租 -55 本紙張疋度適用中國國家標準(CNS ) A4規格(21〇><297公楚 (請先閲讀背面之注意事項弃填蒋本頁)J 409366 B7__ V. Introduction to the Invention (S1), Honolulu, June 11-1, 1996, page 26, describes the use of indium instead of platinum as the lower electrode of ferroelectric memory capacitors to achieve improved performance. As illustrated in Figure 5-5, the hysteresis loop measured for a 100 kHz single-click pulse layer on a SrBi2Ta209 (SBT) capacitor with different lower electrodes is described. The lower electrode in Fig. 55a is Pt / Ti〇2; the lower electrode in Fig. 551> is irO2; and the lower electrode in Fig. 55c is pure Ir. The residual polarization ρNν was measured 10 seconds after the capacitor was written. As shown in Figure 55c, the Pt / SBT / Ir capacitor shows a great depolarization charge in the positive polarization, and the depolarization of the negative polarization capacitor is extremely small. In order to obtain the positive 11 state (highly conductive state) threshold voltage device, it must have a small positively polarized charge at the lower ferroelectric / electrode interface, as shown in Figure 56a. To maintain a large memory window, a large polarized negative charge is also required at the lower ferroelectric / electrode interface, as shown in Figure 56b. This can be achieved with a Pt / SBT / Ir semiconductor structure. The "steady state" 1 J state has a polarized charge of about 10 μ (: / £; ιη2, while the steady state "0 J, the politely polarized charge is about -2 pC / cin2 〇 to 0.3 with a dielectric constant of 280 For micron SBT films, the corresponding threshold voltage migration is 12 ″ v and 2/42 V. By adjusting the channel doping density, the threshold voltage is reached at about 3 V at 0 ferroelectric polarization, and VT1 and VT can be obtained respectively. Approximately 0.6 volts and 15 volts, as shown in Figure 54b. Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs (please read the precautions on the back before filling out this page) This ferroelectric memory device can be used for Low voltage, high luxury and high-speed applications. The memory cell is placed in the p-well 610 as shown in Figure 5-7. Figure 57 illustrates the nine-cell memory array. The word scales are labeled WL1, WL2, and WL3. The element line or drain line is marked as BLI, BL2 and BL3. The source area and substrate of all transistors are grounded. The source, word line, and bit line are independently connected to peripheral circuits, as shown in Figure 5-7. Memory The array is applied with a positive voltage of Vpp to the word line -54 ** · * This paper size is applicable to the Chinese national standard (<:?) Such as said (210 \ 297 mm Printed by 409366 A7 'B7 of the Ministry of Economic Affairs, Zhunxun Cooperative Consumer Cooperative V. Invention Description (52) (Gate) and the bit line is grounded and planned by the block program as "" (highly conductive). Individual memory cells in the program plan are in the "0" (low conductivity) state. The negative program plan voltage -Vpp is applied to the word line and the positive program plan voltage Vpp is applied to the bit line. This results in that only one cell has a bias voltage at the gate terminal ^ ^ And Yu Jiji + Vpp. This memory cell is the only cell in the entire array that will be nested in the "0" state. Many electrode groups can be observed to relax asymmetric polarization polarization. In addition, it can be used in any kind of ferroelectric film and Observation of any kind of ferroelectric gate structure. Observed. The asymmetry polarization relaxation mechanism is both complex and sensitive to the processing conditions. Therefore, it is required in the preferred embodiment of the present invention that the 'asymmetry polarization relaxation technique is used. Manufacture of a single transistor memory cell controlled by a ferroelectric gate. The threshold electric dust of the MM gate unit 616 is determined as follows: For a large array, the threshold voltage in the "1 J state must be small positive, that is, 04 V to 08 V The threshold of "〇" state The pressure must be greater than the supply voltage, that is, the 3.3 va n-channel layer is depleted by the p-type substrate junction and depleted by the extremely shallow p-surface layer and gate. The memory window is displayed as: ΔΥί Here Qfe is the residual charge and Cfe It is the ferroelectric capacitance of the gate unit. During the reading operation, a voltage Va that is not greater than the voltage of the head (that is, the voltage that changes the content of the memory) is applied to the gate electrode of the gate electrode. When the pole is biased by VaM, Memory for a single day; the content is not disturbed, so the reading operation will not interfere with the memory content of any memory unit. Therefore, it is possible to obtain a long-term retention of Xinghe. Rent -55 This paper is compatible with Chinese National Standard (CNS) A4 specifications (21〇 > < 297 Gongchu (Please read the precautions on the back first and discard this page)
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US08/812,579 US5731608A (en) | 1997-03-07 | 1997-03-07 | One transistor ferroelectric memory cell and method of making the same |
US08/834,499 US6018171A (en) | 1997-03-07 | 1997-04-04 | Shallow junction ferroelectric memory cell having a laterally extending p-n junction and method of making the same |
US08/869,534 US5942776A (en) | 1997-03-07 | 1997-06-06 | Shallow junction ferroelectric memory cell and method of making the same |
US08/870,161 US5932904A (en) | 1997-03-07 | 1997-06-06 | Two transistor ferroelectric memory cell |
US08/870,375 US6048738A (en) | 1997-03-07 | 1997-06-06 | Method of making ferroelectric memory cell for VLSI RAM array |
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CN111081761A (en) * | 2019-12-16 | 2020-04-28 | 电子科技大学 | Low-power-consumption transistor device with anti-radiation reinforcing structure and preparation method thereof |
CN111081761B (en) * | 2019-12-16 | 2022-05-03 | 电子科技大学 | Low-power-consumption transistor device with anti-radiation reinforcing structure and preparation method thereof |
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