TW200950059A - Semiconductor device - Google Patents
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- TW200950059A TW200950059A TW98101257A TW98101257A TW200950059A TW 200950059 A TW200950059 A TW 200950059A TW 98101257 A TW98101257 A TW 98101257A TW 98101257 A TW98101257 A TW 98101257A TW 200950059 A TW200950059 A TW 200950059A
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Abstract
Description
200950059 六、發明說明: 【發明所屬之技術領域】 本發明係有關於-種半導體裝置,尤其係有關於一種適 用於形成有三層構造之井,即所謂三重井構造之半導體裝 置,前述三重井構造係於第丨導電型之基板内具有與第工導 電型不同之第2導電型之深井,進而於該深井内具有第】導 電型之淺井。 【先前技術】 例如於日本專利特開2〇〇6_3〇3753號公報(專利文獻1) 中’記載有-種具有所謂三重井構造之半導體積體電路裝 置之邏輯電路及I/〇(Input/〇utput,輸人輸出)電路,上述 三重井構造係指於p型半導體基板上形成較深之〇井並2 其上形成用於構成p型MISFETi 11井以及用於構刑 MISFET之p井。 1 又’於日本專利特開平u_9756〇號公報(專利文獻2)中揭 示有-種如下述之技術,即,於半導體基板上具有浮 極與控制閘極電極之非揮發性半導體記憶裳置中,藉 P型半導體基板上形成n井,於n井内形成#,於 成η型之防止帶電用之擴散層,並將該防止帶電用之= 層與控制閘極電極電性連接’從而防止於蝕刻配: 帶電導致之絕緣膜之可靠性降低或者絕緣破壞。…因 又,於日本專利特開2〇〇5_34〇548號公報(專利文 揭不有-種技術,即,藉由將浮動配線連接於箝 體,使洋動配線中流動之電荷逸向箝位二極體,從而防止 137166.doc 200950059 浮動配線與鄰接於該浮動配線之接地線之間之短路。 又’於日本專利特開2001_358143號公報(專利文獻4)中 揭示有一種技術,即,具備至少一層配線層及最上層之配 線層’上述至少一層配線層包含與複數個閘極電極分別電 性連接之複數個中繼插腳,而上述最上層之配線層包含與 複數個中繼插腳分別電性連接之複數個配線圖案,使用最 上層之配線圖案進行閘極電極之配線,藉此防止蝕刻加工 ❹200950059 VI. Description of the Invention: [Technical Field] The present invention relates to a semiconductor device, and more particularly to a semiconductor device suitable for forming a well having a three-layer structure, that is, a so-called triple well structure, the aforementioned triple well structure A deep well having a second conductivity type different from the first conductivity type in the substrate of the second conductivity type, and further having a shallow conductivity of the first conductivity type in the deep well. [Prior Art] A logic circuit and I/〇 (Input/) of a semiconductor integrated circuit device having a so-called triple well structure are described in Japanese Patent Laid-Open Publication No. Hei. No. Hei. The 三utput, input output circuit, the above-mentioned triple well structure means that a deep well is formed on the p-type semiconductor substrate and 2 wells for forming the p-type MISFETi 11 well and for constructing the MISFET are formed thereon. A technique disclosed in Japanese Laid-Open Patent Publication No. Hei 9-725-6 (Patent Document 2) is a technique in which a nonvolatile semiconductor memory having a floating electrode and a control gate electrode on a semiconductor substrate is used. Forming n wells on the P-type semiconductor substrate, forming # in the n-well, forming an n-type diffusion layer for preventing electrification, and electrically connecting the anti-charged layer to the control gate electrode to prevent Etching: The reliability of the insulating film caused by charging is reduced or the dielectric is broken. In addition, in Japanese Patent Laid-Open Publication No. Hei. No. 5-34-548 (the patent publication does not have a technique, that is, by connecting a floating wiring to a caliper body, the electric charge flowing in the marine wiring is slid into the tongs. a diode, thereby preventing a short circuit between the floating wiring and the ground line adjacent to the floating wiring. Further, a technique is disclosed in Japanese Patent Laid-Open Publication No. 2001-358143 (Patent Document 4), that is, a wiring layer having at least one wiring layer and an uppermost layer, wherein the at least one wiring layer includes a plurality of relay pins electrically connected to the plurality of gate electrodes, and the wiring layer of the uppermost layer includes a plurality of relay pins respectively Electrically connecting a plurality of wiring patterns, and wiring the gate electrodes using the wiring pattern of the uppermost layer, thereby preventing etching processing
配線層時之帶電電荷逃逸至閘極電極以外之區域而導致閘 極絕緣膜劣化。 [專利文獻1]日本專利特開2006-303753號公報 [專利文獻2]日本專利特開平丨號公報 [專利文獻3]曰本專利特開2005 — 340548號公報 [專利文獻4]曰本專利特開2〇〇1 _358 143號公報 【發明内容】 [發明所欲解決之問題] 於曰曰片上系統(System On Chip : SOC)產品中,為減少 待機時之功耗等目的而使用有具有三重井構造之半導體裝 置。然而’具有三重井構造之半導體裝置存在以下說明之 各種技術問題。 一般而言,於不同之三重井區域中分別形成之場效電晶 體之間’以及於三重井區域巾形成之場效電晶體與基板之 間,係為交換信號而視需要來電性連接、然而,本發明者 等人於研究後發現,於特定之電路中,會產生因三重井構 造引起之場效電晶體之閘極絕緣膜的絕緣破壞。作為防止 137166.doc 200950059 如此之絕緣破壞之一個有效方法 |yj如0丁考慮經由位準移 位電路而將不同之三重井區域中 汴L_次甲刀別形成之場效電晶體之 間加以電性連接之方法。然而 诅早移位電路原本係為了 將電源電壓彼此不同之區域之間連結起來而設計者,若將 其設置於電源電壓彼此相同之區域間 僅設計會變得煩雜,而且位準移位電路會伯=裝: 之-部分區域,因此會產生半導體裝置變大,#而產品之 製造成本變高等問題。 本發明之目的在於提供—種於具有三重井構造之半導體 裝置中可提高製造良率及產品可靠性之技術。 本發明之上述及其他目的以及新賴之特徵當可根據本說 明書之敍述及附圖而加以明瞭。 [解決問題之技術手段] 對本申請案所才馬示之㈣中之代表十生發明之一實施形態 進行簡單說明如下。 本實施形態係一種半導體裝置,其包含、型基板;不 與基板接線之深η型井;淺p型井與淺11型井其等形成於 冰η型井内之彼此不同之區域中;以及反相器電路其由 形成於上述淺ρ型井中in通道型場效電晶體及形成於上述 淺η型井中之p通道型場效電晶體構成。上述淺p型井係使 用第1層配線與基板接線,13通道型場效電晶體之閘極電極 及η通道型場效電晶體之閘極電極係於閘極電極形成之同 時或者於配線步驟之較早階段相互接線,並且使用最上層 之配線而直接或者間接地與基板、具有基板電位之部位、 137166.doc 200950059 深η型井、淺P型井、淺η型井或電路動作上之特定部位接 線。 ❹ 又,另-實施形態係-種半導體裝置,其包含:ρ型基 板·,不與基板接線之駐型井;淺?型井,其形成於基板内 之深η型井以外之區域中:淺,型井,其形成於上述深㈣ 井内;以及反相器電路,其由形成於上述淺ρ型井内之η通 道型場效電晶體及形成於上述淺η型井内之?通道型場效電 晶體構成。Ρ通道型場效電晶體之閘極電極及η通道型場效 電晶體之閘極電極係於閘極電極形成之同時或者於配線步 驟之較早階段相互接線,並且使用最上層之配線而直接或 者間接地與基板、具有基板電位之部位、深η型井、淺ρ型 井、淺η型井或者電路動作上之特定部位接線。 又,另一實施形態係一種半導體装置,其包含:ρ型美 板;不與基板接線之深η型井;^㈣,其形成於深^ 井内;淺Ρ型井,其形成於深η型井内之淺η型井以外之區 域中,且不與基板接線;以及反相器電路,其由形成於上 述淺Ρ型井内之η通道型場效電晶體及形成於上述淺η型井 内之Ρ通道型場效電晶體構成。ρ通道型場效電晶體之間極 電極及η通道型場效電晶體之閘極電極係於閘極電極形成 之同時或者於配線步驟之較早階段相互接線,並且使用最 配線而直接或者間接地與基板、具有基板電位之部 '衣11型井、淺ρ型井、淺η型井或者電路動作上之特定 部位接線。 又另—實施形態係一種半導體裝置,其包含:ρ型基 137166.doc 200950059 板;深η型井;淺p型井與淺11型井,其等形成於深〇型井内 之彼此不同之區域中;以及反相器電路,其由形成於上述 淺P型井内之η通道型場效電晶體及形成於上述淺η型井内 之Ρ通道型場效電晶體構成。ρ通道型場效電晶體之閘極電 極及η通道型場效電晶體之閘極電極係使用最上層之配線 而直接或者間接地與基板、具有基板電位之部位或者具有 電源電位之部位接線。 八刀一 •*17肪:农直,兵包含:1)型基 板;心型井;以及淺Ρ型井與淺„型井’其等形成於深η型 井内之彼此不同之區域中。上述深„型井、上述&型井及 上述淺η型井中之至少一者係使用最上層之配線而直接或 者間接地與基板或者具有基板電位之部位接線。 又’另-實施形態係-種半導體裝置,其包含:ρ型基 板in型井;以及淺ρ型井與淺„型井,其等形成於深^ 井内之彼此不同之區域中。上述淺η型井内之部位與美 板、基板區域中形成之淺㈣井内之部位或者具有基板電 位之淺Ρ型井内之部位之間之接線中之至少_者係使 上層之配線而直接或者間接地進行。 、 又,另—實施形態係-種半導體裝置,其包含、型其 型井;以及淺ρ型井與淺η型井,其等形成於深η; 井内之彼此不同之區域中。上述淺Ρ型井與基板、具有基 内井、上述深11型井及上述淺η型井均不連接。上 ,井内之部位與上述㈣井内之部位、基板區域中 形成之淺η型井内之部位或者基板之間之接線令之至少— J37166.doc 200950059 者係使用最上層之配線而直接或者間接地進行。The charged charge at the time of the wiring layer escapes to a region other than the gate electrode, resulting in deterioration of the gate insulating film. [Patent Document 1] Japanese Patent Laid-Open Publication No. Hei. No. 2006-303753 [Patent Document 2] Japanese Patent Laid-Open Publication No. Publication No. Hei No. 2005-340548 [Patent Document 4] 。 〇〇 143 143 143 143 143 143 143 143 143 143 143 143 143 143 143 143 143 143 143 143 143 143 143 143 143 System System System System System System System System System System System System System System System System System System System System System System System System A semiconductor device of well construction. However, the semiconductor device having the triple well structure has various technical problems described below. In general, between the field effect transistors formed in the different triple well regions and between the field effect transistors formed in the triple well region and the substrate, the signals are exchanged as needed, but are required to be electrically connected. The inventors of the present invention found that in a specific circuit, insulation breakdown of a gate insulating film of a field effect transistor due to a triple well structure occurs. As an effective method to prevent the insulation damage of 137166.doc 200950059, yj, such as 0, considers the field effect transistor formed by 汴L_次甲刀 in the different triple well regions via the level shifting circuit. The method of electrical connection. However, the early shift circuit was originally designed to connect the regions where the power supply voltages are different from each other. It is cumbersome to design them only between the regions where the power supply voltages are the same, and the level shift circuit will In the case of a partial area, there is a problem that the semiconductor device becomes large, and the manufacturing cost of the product becomes high. SUMMARY OF THE INVENTION An object of the present invention is to provide a technique for improving manufacturing yield and product reliability in a semiconductor device having a triple well structure. The above and other objects and features of the present invention will become apparent from the description and appended claims. [Technical means for solving the problem] An embodiment of the representative ten inventions in (4) of the present application is briefly described as follows. The present embodiment is a semiconductor device comprising: a type substrate; a deep n-type well not connected to the substrate; a shallow p-type well and a shallow 11-type well formed in different regions of the ice n-type well; and The phaser circuit is composed of an in-channel type field effect transistor formed in the shallow p-type well and a p-channel type field effect transistor formed in the shallow n-type well. The shallow p-type well system uses the first layer wiring and the substrate wiring, and the gate electrode of the 13-channel type field effect transistor and the gate electrode of the n-channel type field effect transistor are formed at the same time as the gate electrode or in the wiring step. Interconnected at an earlier stage, and directly or indirectly connected to the substrate, the portion having the substrate potential, the 137166.doc 200950059 deep n-type well, the shallow P-type well, the shallow n-type well or the circuit action using the uppermost wiring Wiring at a specific location. Further, another embodiment is a semiconductor device comprising: a p-type substrate, a standing well not connected to the substrate; shallow? a well formed in a region other than a deep n-type well in the substrate: a shallow, well formed in the deep (four) well; and an inverter circuit formed by the n-channel type formed in the shallow p-type well Field effect transistor and formed in the above shallow n-type well? Channel type field effect transistor. The gate electrode of the Ρ channel type field effect transistor and the gate electrode of the η channel type field effect transistor are connected to each other at the same time as the gate electrode formation or at an earlier stage of the wiring step, and are directly used by the wiring of the uppermost layer. Or indirectly connected to a substrate, a portion having a substrate potential, a deep n-type well, a shallow p-type well, a shallow n-type well, or a specific portion of the circuit operation. Further, another embodiment is a semiconductor device comprising: a p-type US plate; a deep n-type well not connected to the substrate; ^ (4) formed in the deep well; and a shallow well type formed in the deep n-type In the region other than the shallow n-type well in the well, and not connected to the substrate; and an inverter circuit, which is formed by the n-channel type field effect transistor formed in the shallow well type and formed in the shallow n-type well Channel type field effect transistor. The gate electrode between the ρ channel type field effect transistor and the gate electrode of the η channel type field effect transistor are connected to each other at the same time as the gate electrode formation or at an earlier stage of the wiring step, and are directly or indirectly using the most wiring. The ground is connected to the substrate, the portion having the substrate potential, the clothing type 11 well, the shallow p type well, the shallow n type well, or a specific part of the circuit operation. Still another embodiment is a semiconductor device comprising: a p-type 137166.doc 200950059 plate; a deep n-type well; a shallow p-type well and a shallow 11-type well, which are formed in different regions of the deep well type well And an inverter circuit comprising: an n-channel type field effect transistor formed in the shallow P-type well; and a meandering channel type field effect transistor formed in the shallow n-type well. The gate electrode of the ρ channel type field effect transistor and the gate electrode of the η channel type field effect transistor are directly or indirectly connected to the substrate, the portion having the substrate potential, or the portion having the power supply potential, using the wiring of the uppermost layer. Eight knives and one *16 fat: Nongzhi, the soldiers include: 1) type substrate; heart type well; and shallow Ρ type well and shallow „type well' are formed in different areas of the deep η type well. At least one of the deep well, the above-mentioned & well and the shallow n-type well is directly or indirectly connected to the substrate or the portion having the substrate potential using the wiring of the uppermost layer. Further, an embodiment-type semiconductor device includes: a p-type substrate in-type well; and a shallow p-type well and a shallow-type well, which are formed in different regions in the deep well. The wiring between the portion in the well and the portion in the shallow (four) well formed in the substrate, the substrate region, or the portion in the shallow well having the substrate potential is directly or indirectly performed by wiring the upper layer. Further, an embodiment is a semiconductor device including a type well; and a shallow p-type well and a shallow n-type well are formed in a deep η; different regions in the well. The well is not connected to the substrate, the inner well, the deep type 11 well, and the shallow n-type well. The upper part of the well and the part in the above (4) well, the part of the shallow n-type well formed in the substrate area or the substrate At least the wiring order between the two - J37166.doc 200950059 is directly or indirectly using the uppermost wiring.
又,另一實施形態係一種半導體裝置,其包含:p型基 板;深η型井,其形成於基板内;淺卩型井與淺n型井,其 等形成於深井内之彼此不同之區域中;以及η通道型場效 電晶體,其形成於淺ρ型井内。場效電晶體之汲極與淺η型 井接線,淺Ρ型井與接地電位接線,場效電晶體之閘極電 極與淺η型井直接或者間接地接線,場效電晶體對應於淺打 型井令蓄積之電荷量而成為導通狀態或者斷開狀態。 人,为一實施形 ,,似你且,升巴含:ρ型基 板’深η型井,其形成於基板内;淺㈣井與淺η型井,其 等形成於深井内之彼此不同 . 、 雷曰_ ^ L坟中,以及η通道型場效 日日體’其形成於淺Ρ型井内。場效 , 軍日日體之及極與淺η型 井接線,淺ρ型井與接地電位接 接線%效電晶體之閘極電 極與汙動狀態之配線接線, 配線之中間……“電曰曰體根據該浮動狀態之 中間電位而成為導通狀態或者斷開狀態。 [發明之效果] ’糟由防止三重井區 之絕緣破壞,可提高 '於具有三重井構造之半導體裝置中 域中形成之場效電晶體之閘極絕緣膜 製造良率及產品可靠性。 【實施方式】 時為方便起見而分成複數個部 仁除了特別明示之情形以外,該 於以下之實施形態中 分或實施形態進行說明 137166.doc 200950059 等部分或實施形態並非彼此無關,而是存在一方係另一方 之部分或全部變形例、詳細、補充說明等之關係。 又’於以下之實施形態中,當言及要素之數等(包括個 數、數值、量、範圍等)時,除了特別明示之情形以及原 理上明確限定於特定數之情形等以外,並不限定於該特定 數既了為特疋數以上亦可為特定數以下。進而,於以下 之實施形態中’其構成要素(亦包括要素步驟等)當然未必 為必需,除了特別明示之情形以及於原理上明確認為係必 需之情形等以外。同樣地,於以下之實施形態中,當言及 構成要素等之形狀、位置關係等時,除了特別明示之情形 以及於原理上明確認為並非如此之情形等以外,包括實質 上近似或類似於該形狀等之要素。該說明對於上述數值及 範圍亦同樣適用。 又’於以下之實施形態中所用之圖式中,即使為平面 圖’有時為使圖式容易觀察,亦會局部地標註陰影。又, 於以下之實施形態中’將代表場效電晶體之MISFET(MetalStill another embodiment is a semiconductor device comprising: a p-type substrate; a deep n-type well formed in the substrate; a shallow-type well and a shallow n-type well, which are formed in different regions in the deep well And an n-channel field effect transistor formed in a shallow p-type well. The gate of the field effect transistor is connected with the shallow n-type well, the shallow well type is connected with the ground potential, the gate electrode of the field effect transistor is directly or indirectly connected with the shallow n-type well, and the field effect transistor corresponds to the shallow hit The well is made to be in an on state or an off state by accumulating the amount of charge. People, for an implementation, like you, Shengba contains: p-type substrate 'deep η-type well, which is formed in the substrate; shallow (four) well and shallow η-type well, which are formed in deep wells. , Thunder _ ^ L grave, and η channel type field effect day body 'is formed in shallow well type well. Field effect, military and Japanese body and pole and shallow n-type well wiring, shallow p-type well and grounding potential connection wiring of the gate electrode of the % effect transistor and the dirty state wiring, the middle of the wiring... "Electricity The body is turned on or off according to the intermediate potential of the floating state. [Effects of the Invention] 'When the insulation damage of the triple well region is prevented, the formation of the semiconductor device in the middle of the semiconductor device having the triple well structure can be improved. The manufacturing efficiency of the gate insulating film of the field effect transistor and the reliability of the product. [Embodiment] For the sake of convenience, it is divided into a plurality of parts, except for the case where it is specifically indicated, in the following embodiments. In the following description, 137166.doc 200950059 or the like is not related to each other, but there is a relationship between some or all of the other modifications, detailed descriptions, supplementary explanations, etc. In the following embodiments, When the number, such as the number, the numerical value, the quantity, the range, etc., are specifically indicated, and the case is clearly limited to a specific number in principle, etc. The specific number is not limited to a specific number or more, and may be a specific number or less. Further, in the following embodiments, the constituent elements (including the element steps and the like) are of course not necessarily required, except for the case where it is specifically indicated. In addition, in the following embodiments, when the shape, the positional relationship, and the like of the constituent elements and the like are recited, the case is specifically indicated, and it is clearly not the case in principle. Other than the case, it includes elements that are substantially similar or similar to the shape, etc. The same applies to the above numerical values and ranges. Further, in the drawings used in the following embodiments, even a plan view is sometimes used. The pattern is easy to observe, and the shadow is also partially marked. In addition, in the following embodiment, 'the MISFET (Metal) which will represent the field effect transistor
Insulator Semiconductor Field Effect Transistor)略寫成 MIS, 將p通道型MISFET略寫成pMIS,並將n通道型MISFET略寫 成nMIS。又,於以下之實施形態中,當言及晶圓時,係以 Si(Silicon ’碎)單晶晶圓為主,但不僅為此,亦指 SOI(Silicon On Insulator,絕緣體上矽)晶圓、用於在其上 形成積體電路之絕緣膜基板等。其形狀亦不僅為圓形或者 大致圓形,亦包括正方形、長方形等。 又,於以下之實施形態中,於表達構成三重井構造之井 137166.doc •10- 200950059 時使用了深井及淺井,此處之深、淺係指自基板之主面至 基板厚度方向之深度,相對地大體上分成兩種,即深井和 淺井。因此’複數個深井之深度未必為固定,有時亦會彼 此不同,同樣,複數個淺井之深度未必為固定,有時亦會 彼此不同,但複數個深井之深度必然形成為大於複數個淺 井之/木度。又,淺井係形成於基板内或者深井内,有時亦 會於未形成深井之基板内之彼此不同之區域或者深井内之 彼此不同之區域中形成複數個淺井。 再者,在用於說明以下實施形態之所有圖中,具有相同 功能之部分原則上標註相同之符號,並省略重複說明。以 下,根據圖式詳細說明本發明之實施形態。 首先,為了使本發明之實施形態之半導體裝置更加明 確’對本發明者等人所發現之三重井區域中形成之刪之 閘極絕緣膜之絕緣破壞之原因加以說明。 本發明者等人進行了研究之結果發現,當於下層配線盘The Insulator Semiconductor Field Effect Transistor is abbreviated as MIS, the p-channel type MISFET is abbreviated as pMIS, and the n-channel type MISFET is abbreviated as nMIS. Further, in the following embodiments, when a wafer is referred to, a Si (Silicon 'sprayed) single crystal wafer is mainly used, but not only for this, but also an SOI (Silicon On Insulator) wafer, An insulating film substrate or the like for forming an integrated circuit thereon. The shape is not only circular or substantially circular, but also includes squares, rectangles, and the like. Further, in the following embodiments, deep wells and shallow wells are used in expressing the wells constituting the triple well structure 137166.doc •10-200950059, where the deep and shallow portions refer to the depth from the main surface of the substrate to the thickness direction of the substrate. Relatively roughly divided into two types, namely deep wells and shallow wells. Therefore, the depth of a plurality of deep wells may not be fixed and sometimes different from each other. Similarly, the depth of a plurality of shallow wells may not be fixed and sometimes different from each other, but the depth of a plurality of deep wells must be formed to be larger than a plurality of shallow wells. / Woodiness. Further, the shallow well system is formed in the substrate or in the deep well, and a plurality of shallow wells are sometimes formed in regions different from each other in the substrate in which the deep well is not formed or in regions different from each other in the deep well. In the drawings, the same functions are denoted by the same reference numerals, and the description thereof will not be repeated. Hereinafter, embodiments of the present invention will be described in detail based on the drawings. First, in order to make the semiconductor device according to the embodiment of the present invention more clear, the reason for the dielectric breakdown of the gate insulating film formed in the triple well region discovered by the inventors of the present invention will be described. The inventors of the present invention conducted research and found that when the lower wiring panel
上層配線之間形成之絕緣膜上形成用於連接下層配線與: 層配線之連接孔時,=重并F敁 —董开區域中形成之ΜIS之閘極絕緣 膜會產生絕緣破壞。本發明去望A ,a丨 ^ +赞明者羊人推測,由於該連接孔之 形成係藉由使用電漿放雷之兹益irt、+ + €之乾式蝕刻法來進行,因此因電 漿放電引起之帶電導致了靜雷 . 電破壤之產生。進而亦明確 了.構成三重井區域之深井因 电策孜电而帶電,從而導致 介於深井至基板之路徑中 ^ 甲之MIS之閘極絕緣膜產生絕緣破 壞。特別係當深井之面積較大砵 _ 大。再者,關於因電漿放電 頻羊杈 W起之▼電而導致場效電晶體 137166.doc 200950059 之閘極絕緣膜產生絕緣破壞之機構’例如於Cheung著之 「高級VLSI技術中之電漿充電破壞」,1998年,IEDM短期 課程(C. Cheung, "Plasma Charging Damage in Advanced VLSI Technology", 1998 IEDM Short Course)以及 McVittie 著之「電漿電流、電壓和充電」,1997年,關於電漿處理 引起之破壞之第二屆國際研討會,講座(J. McVittie,"Plasma Currents, Voltages and Charging", 1997 2nd International Symposium on Plasma Process-Induced Damage,Tutorial)中有詳細之敘 述。 使用圖1〜圖8’對本發明者等人獲得之三重井區域中形 成之MIS之閘極絕緣膜之絕緣破壞之分析結果進行具體說 明。圖1係本發明者等人用於分析之聲音圖像處理裝置之 構成圖’圖2係表示構成圖1之聲音圖像處理裝置之1/〇(輸 入輸出)電路部及邏輯電路部之一例之電路圖,圖3係用於 說明深井中蓄積有正電荷時之第良產生機構之電路元 件之剖面不意圖’圖4(a)及圖4(1?)係用於說明反相器電路 中之電荷流動之不意圖,圖5係用於說明深井中蓄積有正 電荷時之第2不良產生機構之電路元件之剖面示意圖,圖6 係表不構成圖1之聲音圖像處理裝置之1/〇(輸入輪出)電路 部及邏輯電路部之其他例之電路圖,圖7係用於說明形成 於深井内且具有與基板相同之導電性之淺井中蓄積有負電 荷時之第3不良產生機構之電路元件之剖面示意圖,圖8係 用於說明形成於深井内且具有與基板相同之導電性之淺井 中蓄積有負電荷時之第4不良產生機構之電路元件之剖面 137166.doc 200950059 不意圖。 如圖1所不,聲音圖像處理裝置LSI係由圖像處理電路、 通^制電路及聲音控制電路等複數個電路構成,該等電 路大:各自设有I/O電路部,經由該1/〇電路部,將電路動 作所而之電壓作為信號而間歇地供給至邏輯電路部。圖1 • 中僅於通k控制電路中例示了 I/O電路部1〇,而省略了設 於/、他電路中之1/〇電路,但其他電路大多亦同樣設有I/O 電路部。 ❹ 如圖2所示,於邏輯電路部中,於P型基板1内之彼此不 同之區域中形成有深η型井200、300。由於用於供給電源 电壓之電路設計上之必要性,深η型井2〇〇、3〇〇並不與基 板1電性連接。再者,於邏輯電路部中除了該等深η型井 200、300以外還形成有複數個深η型井,但此處省略了圖 示。 本發明者等人於製造具有三重井構造之半導體裝置(例 φ 如上述之聲音圖像處理裝置LSI)並進行功能檢查後確認: 於深井之内部與外部之間,當MIS之閘極電極與MIS之汲 極接線時,發現MIS之閘極絕緣膜產生絕緣破壞之第丨不良 - 產生機構及第3不良產生機構,以及於同一深井之内部, • 當MIS之閘極電極與MIS之没極接線時,發現MIS之閘極絕 緣膜產生絕緣破壞之第2不良產生機構及第4不良產生機 構。第1及第2不良產生機構係因正電荷之放電引起之機 構’第3及第4不良產生機構係因負電荷之放電引起之機 構。以下,對該等第1〜第4不良產生機構進行說明。所謂 137166.doc •13- 200950059 反相器電路,係指由一組pMIS及nMIS構成,且兩者 < 間 極電極相連接並且兩者之汲極相連接,進而pMIS之源極與 形成有pMIS之η型井連接,nMIS之源極與形成有nMIS夕When a connection hole for connecting the lower layer wiring and the layer wiring is formed on the insulating film formed between the upper wirings, the gate insulating film formed by the 重IS formed in the Dongkai region may cause dielectric breakdown. The present invention goes to A, a丨^ + the sage of the sheep, speculating that since the formation of the connection hole is performed by dry etching using the plasma thunder, i ir, + + €, The electrification caused by the discharge led to the static mine. Furthermore, it has been clarified that the deep wells constituting the triple well area are charged by the electric power, which causes the insulation of the gate insulating film of the MIS in the path from the deep well to the substrate to be broken. Especially when the area of the deep well is larger 砵 _ large. Furthermore, the mechanism for causing dielectric breakdown of the gate insulating film of the field effect transistor 137166.doc 200950059 due to the electric discharge of the plasma discharge frequency is, for example, the plasma of the advanced VLSI technology by Cheung. Charging Destruction, 1998, IEDM short course (C. Cheung, "Plasma Charging Damage in Advanced VLSI Technology", 1998 IEDM Short Course) and McVittie's "plasma current, voltage and charging", 1997, on electricity The second international seminar on pulp damage (J. McVittie, "Plasma Currents, Voltages and Charging", 1997 2nd International Symposium on Plasma Process-Induced Damage, Tutorial) is described in detail. The analysis results of the insulation breakdown of the gate insulating film of the MIS formed in the triple well region obtained by the inventors of the present invention will be specifically described with reference to Figs. 1 to 8'. 1 is a configuration diagram of an audio image processing apparatus used for analysis by the inventors of the present invention. FIG. 2 is a view showing an example of a 1/〇 (input and output) circuit unit and a logic circuit unit constituting the audio image processing apparatus of FIG. FIG. 3 is a schematic diagram for explaining a circuit component of a first good generating mechanism in a deep well in which a positive charge is accumulated. FIG. 4(a) and FIG. 4(1?) are for explaining an inverter circuit. FIG. 5 is a schematic cross-sectional view showing a circuit element of a second defective generating mechanism in which a positive charge is accumulated in a deep well, and FIG. 6 is a schematic diagram of the sound image processing apparatus of FIG. FIG. 7 is a circuit diagram for explaining another example of the circuit portion and the logic circuit portion of the 输入 (input rotation), and FIG. 7 is a third defect generation mechanism for explaining that a negative charge is accumulated in a shallow well having the same conductivity as that of the substrate. FIG. 8 is a cross-sectional view showing a circuit component of a fourth circuit in which a negative charge is accumulated in a shallow well having the same conductivity as that of the substrate. 137166.doc 200950059 . As shown in Fig. 1, the audio image processing device LSI is composed of a plurality of circuits such as an image processing circuit, a communication circuit, and a sound control circuit, and these circuits are large: each of which is provided with an I/O circuit unit. The /〇 circuit unit intermittently supplies the voltage of the circuit operation to the logic circuit unit as a signal. Fig. 1 • The I/O circuit unit 1 is exemplified in the control circuit of the pass k, and the 1/〇 circuit provided in the / circuit is omitted, but most of the other circuits are also provided with the I/O circuit unit. . As shown in Fig. 2, in the logic circuit portion, deep n-type wells 200, 300 are formed in regions different from each other in the P-type substrate 1. Due to the necessity of designing the circuit for supplying the power supply voltage, the deep n-type wells 2, 3, and 3 are not electrically connected to the substrate 1. Further, a plurality of deep n-type wells are formed in the logic circuit portion in addition to the deep n-type wells 200, 300, but the illustration is omitted here. The inventors of the present invention have manufactured a semiconductor device having a triple well structure (for example, φ such as the above-described sound image processing device LSI) and performed a function check to confirm that: between the inside and the outside of the deep well, when the gate electrode of the MIS is When the gate of MIS is connected, it is found that the gate insulating film of MIS has the third defect of dielectric breakdown - the generating mechanism and the third defective generating mechanism, and the inside of the same deep well, • When the gate electrode of MIS and the MIS are not extremely At the time of wiring, the second defective generating mechanism and the fourth defective generating mechanism which caused the dielectric breakdown of the gate insulating film of MIS were found. The first and second defective generating means are mechanisms caused by the discharge of the positive electric charge. The third and fourth defective generating mechanisms are mechanisms caused by the discharge of the negative electric charge. Hereinafter, the first to fourth defective generation mechanisms will be described. The so-called 137166.doc •13- 200950059 inverter circuit is composed of a set of pMIS and nMIS, and the two electrodes are connected and the drains of the two are connected, and then the source and formation of pMIS are The pMIS n-type well connection, the source of nMIS and the formation of nMIS
又P 型井連接之電路。 首先說明於深井之内部與外部之間,當MIS之閘極電板 與MIS之汲極電極接線時,MIS之閘極絕緣膜因正帶電而 產生絕緣破壞之第1不良產生機構,以及於同一深井之内 部,當MIS之閘極電極與MIS之汲極電極接線時,MIS之閉 極絕緣膜因正帶電而產生絕緣破壞之第2不良產生機構。 I.第1不良產生機構(深井之内部與外部之間當MIS之閉 極電極與MIS之汲極電極接線時因深井之正帶電引起之絕 緣破壞)。 如上述之圖2所示,於深n型井200内之彼此不同之區域 中形成有淺η型井201及淺ρ型井202,進而,於淺η型井201 中形成有pMIS 203ρ,於淺ρ型井202中形成有nMIS 203η。 由該等pMIS 203ρ及nMIS 203η構成反相器電路,藉由本發 明者等人之功能檢查可確認pMIS 203ρ之閘極絕緣膜或者 nMIS 203η之閘極絕緣膜產生了絕緣破壞。pMIS 203ρ之閘 極電極及nMIS 203η之閘極電極係使用第3層配線2(Μ3)而 與深η型井200之外部區域、例如I/O電路部上形成之pMIS 103p之汲極及nMIS 103η之汲極電性連接。 又,於深η型井200内形成有以nMIS 207η為構成要素之 反相器電路,上述nMIS 207η形成於藉由第1層配線 206(Μ1)而與基板1電性連接之淺Ρ型井205中,其閘極電極 137166.doc -14 - 200950059 藉由第3層配線208(M3)而與特定部分接線。 其次,使用圖3及圖4,對反相器電路之pMIS 203p之閘 極絕緣膜或者nMIS 203η之閘極絕緣膜產生絕緣破壞之機 構進行說明。圖3係表示由於在形成於第3層配線上之層間 絕緣膜上形成連接孔(經由第1層、第2層及第3層配線而到 達淺η型井20 1及淺ρ型井202)時之乾式蝕刻法之電漿放 電,而造成製造中途之半導體裝置之深η型井200正帶電之 示意圖。若正電荷自連接孔流入深η型井200内形成之淺η 型井201及淺ρ型井202中,則由於深η型井200不與基板1電 性連接,因此流入之正電荷會蓄積於深η型井200内。另一 方面,即便正電荷流入未形成於深η型井200内而係形成於 基板1上之淺ρ型井102中,由於淺ρ型井102之導電型與基 板1相同,因此流入之正電荷會朝基板1放電。 但一般認為,於由形成於基板1上之淺η型井1 0 1中形成 之pMIS(未圖示)與淺ρ型井102中形成之nMIS(未圖示)構成 之反相器電路中,當pMIS與nMIS之閘極電極相互接線且 存在處於浮動狀態者時,彼此不同之區域中形成之淺η型 井101與淺ρ型井102之間會成為低電阻之導通狀態。對於 此現象可作如下說明。首先,如圖4(a)所示,當對構成具 有上述特徵之反相器電路之pMIS之源極施加電壓Vcc時, 於pMIS之閘極電極G與通道之間以及nMIS之閘極電極G與 通道之間分別形成電容C。結果,pMIS之閘極電極G及 nMIS之閘極電極G上分別被施加電壓Vcc/2,從而使得 pMIS及nMIS成為導通狀態。當pMIS及nMIS成為導通狀態 137166.doc -15- 200950059 時,如圖4(b)所示,正電荷自η型井n-well中形成之pMIS之 源極S流向没極D,進而自p型井p-well中形成之nMIS之汲 極D流向源極S,進而流向形成有nMIS之ρ型井p-well、基 板p-sub 〇 如此,無論nMIS 1 03η之閘極電極之接線狀況如何,淺η 型井101與淺ρ型井102之間均會經由反相器電路而成為低 電阻之導通狀態,且正電荷會經由淺η型井101及淺ρ型井 102而自配線朝基板1放電(圖3之路徑I)。因此,由pMIS 203p及nMIS 203η構成之反相器電路之閘極電極之電位變 得與基板1之電位(〇 V)相等,施加於閘極絕緣膜上之電壓 會變大,從而導致絕緣破壞之產生。 又,即便於淺η型井1 01與淺ρ型井1 02中形成之反相器電 路之閘極電極全部接線之情形時,當nMIS 103η之閘極電 極之連接目的地正帶電時,nMIS 103η亦會成為導通狀 態,且正電荷會自配線朝nMIS 1 03η之汲極、源極、淺ρ型 井102、基板1放電(圖3之路徑II)。因此,由pMIS 203ρ及 nMIS 203η構成之反相器電路之閘極電極之電位變得與基 板之電位(〇 V)相等,而施加於閘極絕緣膜上之電壓變大, 從而導致絕緣破壞之產生。然而,一般認為nMIS 103η之 閘極電極之連接目的地是否正帶電係受偶然性支配,其概 率依存於電路構成及電路構成要素之形狀等。因此,大量 製造之半導體裝置係偶然產生絕緣破壞。再者,當深η型 井200之面積例如為1 mm2以上時,深η型井200中蓄積之電 荷量會變多,從而容易產生絕緣破壞。 137166.doc •16· 200950059 Π.第2不良產生機構(於同一深井之内部當mis之閘極電 極與MIS之沒極電極接線時因深井之正帶電引起之絕緣破 壞)。 如上述之圖2所示,於深n型井3〇〇内之彼此不同之區域 . 巾形成有淺_井则及淺ρ型井3〇4,進而於&型井3〇4内 , 形成有nMIS 308。淺Ρ型井304由於電路設計上之需要而藉 由第1層配線3〇5(M1)與基板1電性連接。又,於深 ❹ 300内,在與淺η型井303及淺p型井304不同之區域中,以 彼此不同之區域形成有淺η型井3〇1及淺ρ型井3〇2,進而於 淺η型井3〇1内形成有_3 3〇7ρ,於淺ρ型井搬内形成有 nMIS 3G7n。由該等pMIS 3Q7p及nMIS 3()7η構成反相器電 路,反相II電路之輸出段與形成於淺p型井3〇4中之n_ 3 〇 8之閘極電極係、使用第7層i線3 i(m 7)而電性連接。 又,於由淺η型井303中形成之pMIS 3〇9p及淺ρ型井3〇4中 形成之nMIS 3〇9n構成之反相器電路之輸出段,反相器電 〇 路之PMIS 3〇7?之閘極電極及爾IS 307n之閘極電極使用第 7層配線31G(M7)而電性連接,但省略了圖示。如由州π 3〇9p及nMIS 3〇9n構成之反相器電路之間極電極般,以淺ρ 型井304中形成之nMls為構成要素之反相器電路之間極電 . 極全部藉由第7層配線或者第7層以前之層之配線312等而 與電路動作上所需之特定部位電性連接。 其次,使用圖5,對在同一深井之内部進行接線之祕以 308之閘極絕緣膜產生絕緣破壞之機構進行說明。圖$係表 示由於在形成於第7層配線上之層間絕緣膜上形成連接孔 137166.doc 17 200950059 時之乾式蝕刻法之電漿放電,而導致製造中途之半導體裝 置之深η型井3〇〇正帶電之示意圖。於該階段中,以淺p型 井3 04中形成之11河18為構成要素之反相器電路之閘極電極 全部與特定部位接線。因此,淺Ρ型井304與淺η型井3〇3或 珠η型井300構成二極體,經由淺卩型井3〇2、淺η型井^、 3〇3而流入深11型井3〇〇中之正電荷不放電而蓄積。可推 測,配線310(M7)之連接目的地於深n型井3〇〇帶電時處於 與基板1相同之電位(0 V),此時,pMIS 3〇7p成為導通狀 態。結果形成自深!1型井300到達淺n型井3〇1、淺η型井3〇1 中形成之pMIS 307ρ之源極、汲極、配線3u(M7)以及 riMIS 308之閘極電極之連接路徑。藉此可推測,由於在 nMIS 308中形成與基板!為等電位之反轉層,因此其閘極 絕緣膜上被施加較大電壓,從而導致絕緣破壞之產生。 此時,由於在pMIS 307p之閘極絕緣膜上亦產生電位 差,因此該閘極絕緣膜亦可能會產生絕緣破壞,但於本發 明者等人進行之功能檢查中並未產生絕緣破壞。推測其原 因在於,於nMIS 308之絕緣破壞部位存在有被稱為脆弱點 之構造缺陷,而與此相對地,於pMls 3〇7p之閘極絕緣膜 中並不存在脆弱點。 至^此,對深η型井200、300正帶電時之不良產生機構(第 1及第2不良產生機構)進行了敍述,但根據產品之不同, 有時深η型井200、300内形成之淺ρ型井亦會負帶電,有時 亦可推測係由於淺ρ型井負帶t而導致⑽之閘極絕緣膜產 生絕緣破壞。特別係於圖6所示之淺?型井2〇2、3〇2之面積 137166.doc -18- 200950059 較大時此情形較為顯著。 其次’對在深井之内部與外部之間,當MIS之閘極電極 與MIS之汲極電極接線時因MIS之閘極絕緣膜負帶電而產 生絕緣破壞之第3不良產生機構、以及在同一深井之内部 當MIS之閘極電極與MIS之汲極電極接線時因MIS之閘極絕 緣膜負帶電而產生絕緣破壞之第4不良產生機構進行說 明。 ❹The circuit of the P-well connection. First, when the gate electrode of MIS and the gate electrode of MIS are connected between the inside and the outside of the deep well, the first defective generating mechanism of the gate insulating film of MIS due to positive charging is destroyed, and the same In the inside of the deep well, when the gate electrode of the MIS is connected to the drain electrode of the MIS, the second defective generating mechanism of the MIS closed-electrode insulating film is damaged by the positive charging. I. The first defect-producing mechanism (the insulation between the inside and the outside of the deep well when the MIS's closed electrode and the MIS's drain electrode are connected due to the positive charge of the deep well). As shown in FIG. 2 above, shallow n-type wells 201 and shallow p-type wells 202 are formed in regions different from each other in the deep n-type well 200, and further, pMIS 203p is formed in the shallow n-type well 201, An nMIS 203η is formed in the shallow p well 202. The inverter circuit is constituted by the pMIS 203p and the nMIS 203n, and it is confirmed by the function check of the present inventors that the gate insulating film of the pMIS 203p or the gate insulating film of the nMIS 203n is insulated. The gate electrode of pMIS 203ρ and the gate electrode of nMIS 203η use the third layer wiring 2 (Μ3) and the outer region of the deep n-type well 200, for example, the pMIS 103p bungee and nMIS formed on the I/O circuit portion. The 103η is electrically connected. Further, an inverter circuit having nMIS 207n as a constituent element is formed in the deep n-type well 200, and the nMIS 207n is formed in a shallow well type electrically connected to the substrate 1 via the first layer wiring 206 (Μ1). In 205, the gate electrode 137166.doc -14 - 200950059 is wired to the specific portion by the third layer wiring 208 (M3). Next, a mechanism for causing dielectric breakdown of the gate insulating film of the pMIS 203p or the gate insulating film of the nMIS 203n of the inverter circuit will be described with reference to Figs. 3 and 4 . 3 is a view showing formation of a connection hole in the interlayer insulating film formed on the third layer wiring (to reach the shallow n-type well 20 1 and the shallow p-type well 202 via the first layer, the second layer, and the third layer wiring) The plasma discharge of the dry etching method causes a positive charging of the deep n-type well 200 of the semiconductor device in the middle of manufacturing. If a positive charge flows from the connection hole into the shallow n-type well 201 and the shallow p-type well 202 formed in the deep n-type well 200, since the deep n-type well 200 is not electrically connected to the substrate 1, the positive charge flowing in will accumulate. In the deep η type well 200. On the other hand, even if the positive electric charge flows into the shallow p-type well 102 which is not formed in the deep n-type well 200 and is formed on the substrate 1, since the conductivity type of the shallow p-type well 102 is the same as that of the substrate 1, the inflow is positive. The charge will discharge toward the substrate 1. However, it is considered to be in an inverter circuit composed of a pMIS (not shown) formed in the shallow n-type well 1 0 1 formed on the substrate 1 and an nMIS (not shown) formed in the shallow p-type well 102. When the gate electrodes of the pMIS and the nMIS are connected to each other and there is a floating state, the shallow n-type well 101 formed in the different regions from each other and the shallow p-type well 102 become a low-resistance conduction state. This phenomenon can be explained as follows. First, as shown in FIG. 4(a), when a voltage Vcc is applied to the source of the pMIS constituting the inverter circuit having the above characteristics, between the gate electrode G of the pMIS and the channel and the gate electrode G of the nMIS A capacitor C is formed between the channel and the channel. As a result, a voltage Vcc/2 is applied to the gate electrode G of the pMIS and the gate electrode G of the nMIS, respectively, so that pMIS and nMIS are turned on. When pMIS and nMIS become the conduction state 137166.doc -15- 200950059, as shown in Fig. 4(b), the positive charge flows from the source S of the pMIS formed in the n-well n-well to the immersion D, and further from p The drain D of the nMIS formed in the p-well of the well flows to the source S, and then flows to the p-well of the p-well formed with the nMIS, and the substrate p-sub 〇, regardless of the wiring state of the gate electrode of nMIS 1 03η The shallow n-type well 101 and the shallow p-type well 102 are both turned into a low-resistance conduction state via the inverter circuit, and the positive electric charge is self-wiring toward the substrate via the shallow n-type well 101 and the shallow p-type well 102. 1 discharge (path I of Figure 3). Therefore, the potential of the gate electrode of the inverter circuit composed of the pMIS 203p and the nMIS 203n becomes equal to the potential (〇V) of the substrate 1, and the voltage applied to the gate insulating film becomes large, thereby causing dielectric breakdown. Produced. Moreover, even when the gate electrodes of the inverter circuit formed in the shallow n-type well 01 and the shallow p-type well 102 are all connected, when the connection destination of the gate electrode of the nMIS 103n is positively charged, nMIS The 103n also becomes in an on state, and the positive electric charge is discharged from the wiring toward the drain of the nMIS 101n, the source, the shallow p-type well 102, and the substrate 1 (path II of FIG. 3). Therefore, the potential of the gate electrode of the inverter circuit composed of pMIS 203ρ and nMIS 203η becomes equal to the potential of the substrate (〇V), and the voltage applied to the gate insulating film becomes large, thereby causing dielectric breakdown. produce. However, it is considered that whether or not the connection destination of the gate electrode of the nMIS 103n is continually dominated by the positive charging system depends on the circuit configuration and the shape of the circuit constituent elements. Therefore, a semiconductor device manufactured in large quantities accidentally causes dielectric breakdown. Further, when the area of the deep n-type well 200 is, for example, 1 mm 2 or more, the amount of charge accumulated in the deep n-type well 200 is increased, and insulation breakdown is likely to occur. 137166.doc •16· 200950059 Π. The second bad-producing mechanism (in the same deep well, when the gate electrode of mis is connected to the electrode of the MIS, the insulation is broken due to the positive charge of the deep well). As shown in Fig. 2 above, in the deep n-type well 3 彼此 different regions. The towel is formed with shallow _ well and shallow ρ-type well 3 〇 4, and then within the & type well 3 〇 4, An nMIS 308 is formed. The shallow well 304 is electrically connected to the substrate 1 by the first layer wiring 3〇5 (M1) due to the circuit design. Further, in the squat 300, in a region different from the shallow n-type well 303 and the shallow p-type well 304, shallow n-type wells 3〇1 and shallow p-type wells 3〇2 are formed in regions different from each other, and further _3 3〇7ρ is formed in the shallow η type well 3〇1, and nMIS 3G7n is formed in the shallow ρ type well. The inverter circuit is constituted by the pMIS 3Q7p and the nMIS 3() 7η, and the output section of the inverted II circuit and the gate electrode system of n_3 〇8 formed in the shallow p-type well 3〇4, using the seventh layer The i line 3 i (m 7) is electrically connected. Further, the output section of the inverter circuit formed by the nMIS 3〇9n formed in the pMIS 3〇9p and the shallow p type well 3〇4 formed in the shallow n-type well 303, and the PMIS 3 of the inverter electric circuit The gate electrode of 〇7? and the gate electrode of IS 307n are electrically connected using the seventh layer wiring 31G (M7), but the illustration is omitted. Like the pole electrode between the inverter circuits composed of the state π 3〇9p and nMIS 3〇9n, the nMls formed in the shallow ρ-well 304 are the poles of the inverter circuits. The seventh layer wiring or the wiring 312 of the layer before the seventh layer is electrically connected to a specific portion required for the operation of the circuit. Next, a mechanism for causing insulation breakdown of the gate insulating film of 308 by wiring the inside of the same deep well will be described with reference to Fig. 5 . Fig. $ is a diagram showing the deep η-type well of the semiconductor device in the middle of manufacturing due to the plasma discharge of the dry etching method in the case where the connection hole 137166.doc 17 200950059 is formed on the interlayer insulating film formed on the wiring of the seventh layer. 〇 is a schematic diagram of charging. At this stage, all of the gate electrodes of the inverter circuit in which the 11 river 18 formed in the shallow p-type well 309 is a component are wired to a specific portion. Therefore, the shallow well type 304 and the shallow η type well 3〇3 or the bead type η type well 300 constitute a diode, and flow into the deep type 11 well through the shallow 卩 type well 3〇2, the shallow η type well ^, 3〇3 The positive charge in 3〇〇 does not discharge and accumulates. It can be inferred that the connection destination of the wiring 310 (M7) is at the same potential (0 V) as that of the substrate 1 when the deep n-type well 3 is charged, and at this time, the pMIS 3〇7p is turned on. The result is formed from the deep! Type 1 well 300 to the shallow n-type well 3〇1, the shallow η-type well 3〇1 formed in the pMIS 307ρ source, the drain, the wiring 3u (M7) and the riMIS 308 gate electrode Connection path. From this, it can be inferred that the substrate is formed in the nMIS 308! It is an inversion layer of equipotential, and therefore a large voltage is applied to the gate insulating film, resulting in insulation breakdown. At this time, since the potential difference is also generated on the gate insulating film of the pMIS 307p, the gate insulating film may also cause dielectric breakdown, but no dielectric breakdown occurs in the functional inspection performed by the present inventors. It is presumed that the reason is that there is a structural defect called a weak point in the dielectric breakdown portion of nMIS 308, and in contrast, there is no weak point in the gate insulating film of pMls 3〇7p. In this case, the defective generating mechanism (the first and second defective generating mechanisms) when the deep n-type wells 200 and 300 are positively charged is described. However, depending on the product, the deep n-type wells 200 and 300 may be formed. The shallow p-type well is also negatively charged, and it is also speculated that the gate insulating film of (10) is insulated and damaged due to the negative p-band of the shallow p-type well. Specifically, it is shallow as shown in Figure 6. The area of the well 2〇2, 3〇2 137166.doc -18- 200950059 This situation is more significant when it is larger. Secondly, the third defective generating mechanism that causes dielectric breakdown due to the negative charging of the gate insulating film of MIS when the gate electrode of MIS is connected to the drain electrode of MIS between the inside and the outside of the deep well, and in the same deep well In the inside, when the gate electrode of the MIS is connected to the drain electrode of the MIS, the fourth defect generation mechanism that causes dielectric breakdown due to the negative charge of the gate insulating film of the MIS will be described. ❹
ΙΠ.第3不良產生機構(於深井之内部與外部之間當Mis 之閘極電極與MIS之汲極電極接線時因深井之負帶電引起 之絕緣破壞)β 使用圖7對反相器電路ipMIS 2〇3ρ之閘極絕緣膜或者 nMIS 203η之閘極絕緣膜產生絕緣破壞之機構進行說明。 圖7係表示由於在形成於第3層配線上之層間絕緣膜上形成 連接孔時之乾式蝕刻法之電漿放電,而導致製造中途之半 ¥體裝置之深η型井200内形成之淺ρ型井2〇2負帶電之示意 圖。當負電荷自連接孔流入深η型井2〇〇内形成之淺ρ型井 202中時,由於淺ρ型井2〇2形成於深η型井2〇〇内且不與基 板1電性連接’因此流入之負電荷會蓄積於淺ρ型井逝 内。另一方面’即便電荷流入未形成於深η型井200内而係 形成於基板丨内之淺ρ型井1〇2中,由於 型與基板〗相同,因此流入之電荷亦會朝基二電^電 對於配線聊)中存在之負電荷而言,由於自連接於配線 2(Μ3)之nMIS 1G3n之沒極朝向淺Ρ型井102之方向係順方 向’因此負電荷會經由淺P型井1〇2而朝基W放電。因 137166.doc •19- 200950059 此,由pMIS 203p及nMlS 2〇3!!槿点夕g 士日势中Λ wn稱成之反相窃電路之閘極電 極之電位會變得與基板i之電位Μ 〜电伹(υ v)相專,施加於閘極絕 緣膜上之電壓變大,結果會導致絕緣破壞之產生。 IV.第4不良產生機構(於同一深井之内部當刪之間極 電極與MIS之汲極電極接線時因深井之負帶電引起之絕緣 破壞)。 ' 使用圖8對在同一深井之内部進行接線之nMis 3〇8之閘 極絕緣膜產生絕緣破壞之機構進行說明。圖8係表示由於 在形成於第7層配線上之層間絕緣膜上形成連接孔時之乾 式蝕刻法之電漿放電,而導致製造中途之半導體装置之深 η型井300内之淺p型井302負帶電之示意圖。於該階段中, 以淺Ρ型井302内形成之11河18為構成要素之反相器電路之閘 極電極全部與特定部位接線。因此,淺ρ型井3〇2與淺η型 井301或者深η型井3〇〇構成二極體,流入淺ρ型井3〇2中之 負電荷不放電而蓄積。可推測,配線3丨〇(Μ7)之連接目的 地於淺ρ型井302帶電時處於與基板1相同之電位,此時, nMIS 307η成為導通狀態。結果,自淺ρ型井3〇MinMIS 3〇7η 之源極、汲極、配線311以及nMIS 3〇8之閘極電極施加負 電位。由於形成有nMIS 308之淺p型井3〇4係藉由第1層配 線305(M1)而與基板】電性連接’因此於nMIS 308之間極絕 緣膜上產生電位差,結果導致絕緣破壞之產生。 根據以上所述之分析結果,為防止MIS之閘極絕緣膜之 絕緣破壞,可使用以下之(1)或(2)中之任一方法或者併用 該等方法,即:(1)第!方法:(1-1)防止深井帶電(針對上述 137166.doc -20- 200950059 第1及第2不良產生機構之解決方法)或者(1_2)防止形成於 深井内且具有與基板相同導電性之淺井帶電(針對上述第3 及第4不良產生機構之解決方法);或者⑺&方法:阻斷 自深井或者深井内形成之淺井經由MIS之閘極絕緣膜到達 基板或者具有基板電位之部位之配線路徑(針對上述第1〜 1 第4不良產生機構之解決方法)。 其次’詳細說明上述第1方法及第2方法。 (1)第1方法: ❹ (1-1)防止深井帶電。 於深井内形成具有與基板相同導電型之淺井,於一連串 配線步驟之較早階段將該淺井連接於基板並且於該淺井内 形成Mls,於-連串配線步驟之較早階段構築以此為構成 要素之反相器電路,直至配線步驟結束為止,將該mis之 閘極電極維持為浮動狀態而不與其他部分接線。此處,作 為將構成反相器電路之MIS之閘極電極與基板或淺井最後 © 接線之配線,較好的是如下所述之配線,該配線係構成多 層配線中之一層之配線,且該配線正上方之絕緣膜上所形 成之連接孔之數量小於下層配線之正上方之絕緣膜上所形 • 成之連接孔之數量。若有可能,較理想的是藉由最上層之 . 配線來進行上述接線。 再者,本實施形態中所說明之最上層之配線,係指與成 為焊墊之配線層為同層之配線層。焊墊係指於之後之步驟 中,接合線或凸塊電極等外部連接用導體所連接之區域。 此處,以具有與基板相同之導電型之淺井及該淺井内形 137166.doc 21 200950059 =IS為構成要素之反相器電路係為了防止帶電之目的 而I作,對於電路動作並無貢獻。於可使用電的 來進行上述接線之情形砗 成要素 上述接亦可使用電路構成要素來進行 接線。此時,只要於產品完成階段避免㈣之閑極電 極成為洋動狀態之情形即可,因此MIS之㈣電極可連接 於電路構成上所需之任意部位…具有與基 7型之淺井與基板之間之連接亦可不直接進行,而係經^ 連接於基板之淺井來間接地進行。 (1-2)防止形成於深井内且具有與基板相同導電性 井帶電。 / 當形成於深井内且具有與基板相同導電性之淺井與基板 連接時’藉由於-連串配線步驟之較早階段進行該連^, 可防止帶電。 當於電路構成上’無法將形成於深井内且具有與基板相 同導電性之淺井與基板連接時,不將㈣井與基板連接而 係於其内部形成MIS,於一連串配線步驟之較早階段構築 以此為構成要素之反相器電路,並且直至配線步驟結束為 止,將該MIS之閘極電極維持為浮動狀態而不與其他部分 接線。此處,作為將構成反相器電路之MIS之閘極電極與 基板或者淺井最後接線之配線,較好的是如下所述之配 線,該配線係構成多層配線中之一層之配線,且該配線正 上方之絕緣膜上所形成之連接孔之數量小於下層配線之正 上方之絕緣膜上所形成之連接孔之數量。若有可能,較理 想的是藉由最上層之配線來進行上述接線。 137166.doc -22- 200950059 此處,以具有與基板相同之導電型之淺井及該㈣内形 成之刪為構成要素之反相器電路係為了防止帶電之目的 而製作,對於電路動作並無貢獻。於可使用電路構成要素 來進仃上述接線之情形時,亦可使用電路構成要素來進行 上述接線。此時,只要於產品完成階段避免峨之閑極電 極成為浮動狀態之情形即可,因此MIS之閘極電極可連接 於電路構成上所需之任意部位。 ⑺第2方法··阻斷自深井、或者深井内形成之淺井經 由順之閘極絕緣膜到達基板或者具有基板電位之部位之 配線路徑。 使用如下所述之配絲進行三㈣區域與三重井區域以 外之區域之間之電性連接之至少—部分,上述配線係構成 多層配線中之-層之配線,且該配線正上方之絕緣膜上所 形成之連接孔之數量小於下層配線之正上方之絕緣膜上所 形成之連接孔之數量。若有可能,較理想的是使用最上層 之配線來進行上述接線。 又,不同之三重彳區域之間t電性$接亦可藉由上述之 配線而同樣地進行。該方法特別係於針對其中一個三重井 區域適用第1方法而針對另一個三重井區域並不適用第^方 法之情形時有效。 又,於同一二重井區域之内部,具有與基板相同之導電 型且與基板直接或者間接地連接之淺井之内部與外部之間 之電性連接亦可藉由上述配線而同樣地進行。 又,於三重井區域中,具有與基板相同之導電型且不與 137166.doc -23- 200950059 之電性連接亦可藉由上 基板連接之淺井之内部與外部之間 述配線而同樣地進行。 ⑨電路5又§十上必須與基板連接之深η型井及深n型 一内形成之淺井與基板之間之電性連接之至少一部分亦可 藉由上述配線而同樣地進行。 ’、對藉由第1方法及第2方法防止mis之閘極絕緣膜 之絕緣破壞之機構進行說明。此處,係'對基板為p型之情第. Third bad-producing mechanism (insulation breakdown caused by negative charging of deep wells when the gate electrode of Mis is connected to the drain electrode of MIS between the internal and external parts of the deep well) β Use the Figure 7 for the inverter circuit ipMIS A mechanism for insulating damage caused by a gate insulating film of 2 〇 3 ρ or a gate insulating film of nMIS 203 η will be described. Fig. 7 is a view showing the plasma discharge in the dry etching method in the case where the connection holes are formed in the interlayer insulating film formed on the third layer wiring, which results in the formation of the deep n-type well 200 in the middle half of the manufacturing apparatus. Schematic diagram of the negative charging of the p-type well 2〇2. When a negative charge flows from the connection hole into the shallow p-type well 202 formed in the deep n-type well 2, the shallow p-type well 2〇2 is formed in the deep n-type well 2〇〇 and is not electrically connected to the substrate 1. The connection 'so the negative charge flowing in will accumulate in the shallow p-type well. On the other hand, even if the charge inflow is not formed in the deep n-type well 200 and is formed in the shallow p-type well 1〇2 in the substrate crucible, since the type is the same as the substrate, the inflow charge will also be directed toward the base two. In the negative charge that exists in the wiring, since the nMIS 1G3n connected to the wiring 2 (Μ3) is oriented in the direction of the shallow well 102, the negative charge will pass through the shallow P-well 1 〇 2 and discharge toward the base W. 137166.doc •19- 200950059 Therefore, by pMIS 203p and nMlS 2〇3!! 槿 夕 g 士 士 士 势 wn wn wn wn wn 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒 倒The potential Μ ~ 伹 () v) phase is dedicated, and the voltage applied to the gate insulating film becomes large, resulting in insulation breakdown. IV. The fourth defect-producing mechanism (in the same deep well, the insulation between the pole electrode and the MIS electrode is broken due to the negative charging of the deep well). The mechanism for causing insulation breakdown of the gate insulating film of nMis 3〇8 which is wired inside the same deep well will be described with reference to FIG. Fig. 8 is a view showing a shallow p-type well in a deep n-type well 300 of a semiconductor device in the middle of manufacturing due to plasma discharge of a dry etching method when a connection hole is formed on an interlayer insulating film formed on a seventh layer wiring. 302 is a schematic diagram of negative charging. At this stage, all of the gate electrodes of the inverter circuit in which the 11 river 18 formed in the shallow well 302 is a component are connected to a specific portion. Therefore, the shallow p-type well 3〇2 and the shallow n-type well 301 or the deep n-type well 3〇〇 constitute a diode, and the negative electric charge flowing into the shallow p-type well 3〇2 does not discharge and accumulates. It is presumed that the connection of the wiring 3丨〇(Μ7) is at the same potential as that of the substrate 1 when the shallow p-type well 302 is charged, and at this time, the nMIS 307η is turned on. As a result, a negative potential is applied from the gate electrodes of the source, the drain, the wiring 311, and the nMIS 3〇8 of the shallow ρ-type well 3〇MinMIS 3〇7η. Since the shallow p-type well 3形成4 in which the nMIS 308 is formed is electrically connected to the substrate by the first layer wiring 305 (M1), a potential difference is generated between the insulating films between the nMISs 308, resulting in dielectric breakdown. produce. According to the analysis results described above, in order to prevent dielectric breakdown of the gate insulating film of MIS, any of the following methods (1) or (2) or a combination of the methods may be used, namely: (1) Method: (1-1) Prevention of deep well electrification (for the above-mentioned 137166.doc -20-200950059 solution for the first and second failure generating mechanisms) or (1_2) prevention of shallow wells formed in the deep well and having the same conductivity as the substrate Charge (for the third and fourth problems of the above-mentioned defective generation mechanism); or (7) & method: blocking the wiring path from the shallow well formed in the deep well or the deep well to the substrate or the portion having the substrate potential via the gate insulating film of the MIS (Remedy for the above 1st to 1st 4th defective generation mechanism). Next, the first method and the second method will be described in detail. (1) The first method: ❹ (1-1) Prevent deep wells from being charged. Forming a shallow well having the same conductivity type as the substrate in the deep well, connecting the shallow well to the substrate at an early stage of a series of wiring steps and forming Mls in the shallow well, constructing at an earlier stage of the series wiring step The inverter circuit of the element is maintained until the wiring step is completed, and the gate electrode of the mis is maintained in a floating state without being wired to other portions. Here, as the wiring for connecting the gate electrode of the MIS which constitutes the inverter circuit to the substrate or the shallow terminal, it is preferable to use a wiring which constitutes one of the layers of the multilayer wiring, and the wiring is The number of connection holes formed on the insulating film directly above the wiring is smaller than the number of connection holes formed on the insulating film directly above the lower wiring. If possible, it is desirable to perform the above wiring by wiring the top layer. In addition, the wiring of the uppermost layer described in the present embodiment means a wiring layer which is the same layer as the wiring layer which is a bonding pad. The pad is a region to which an external connection conductor such as a bonding wire or a bump electrode is connected in the subsequent step. Here, the inverter circuit having the same conductivity type as the substrate and the inverter internal circuit 137166.doc 21 200950059 = IS is used as a component to prevent charging, and does not contribute to circuit operation. In the case where the above wiring can be used by electricity, the above components can also be wired using circuit components. At this time, as long as the (4) idle electrode is in a state of eccentricity at the completion stage of the product, the (4) electrode of the MIS can be connected to any part required for the circuit configuration... having a shallow well and a substrate of the base type 7 The connection may not be made directly, but may be performed indirectly via a shallow well connected to the substrate. (1-2) Prevention of formation in a deep well and having the same conductivity as the substrate. / When a shallow well formed in a deep well and having the same conductivity as the substrate is connected to the substrate, the charging can be prevented by the earlier stage of the series-wiring step. When it is impossible to connect a shallow well formed in a deep well and having the same conductivity as the substrate to the substrate, the (4) well is not connected to the substrate and is formed inside the MIS, and is constructed at an early stage of a series of wiring steps. This is the inverter circuit of the constituent elements, and until the wiring step is completed, the gate electrode of the MIS is maintained in a floating state without being wired to other portions. Here, as the wiring for connecting the gate electrode of the MIS which constitutes the inverter circuit to the substrate or the shallow well, it is preferable to use a wiring which constitutes one of the layers of the multilayer wiring, and the wiring The number of the connection holes formed on the insulating film directly above is smaller than the number of the connection holes formed on the insulating film directly above the lower layer wiring. If possible, it is preferable to perform the above wiring by the wiring of the uppermost layer. 137166.doc -22- 200950059 Here, a shallow well having the same conductivity type as the substrate and an inverter circuit formed as the constituent element in the above (4) are produced for the purpose of preventing charging, and do not contribute to circuit operation. . In the case where the above-mentioned wiring can be used by using the circuit constituent elements, the above-mentioned wiring can also be performed using the circuit constituent elements. In this case, as long as the idle electrode of the crucible is prevented from being in a floating state at the completion stage of the product, the gate electrode of the MIS can be connected to any portion required for the circuit configuration. (7) The second method is to block the wiring path from the deep well or the shallow well formed in the deep well to the substrate or the portion having the substrate potential by the gate insulating film. At least a portion of the electrical connection between the three (four) region and the region other than the triple well region is performed by using a wire as described below, the wiring system constituting the wiring of the layer in the multilayer wiring, and the insulating film directly above the wiring The number of connection holes formed thereon is smaller than the number of connection holes formed on the insulating film directly above the lower layer wiring. If possible, it is desirable to use the uppermost wiring for the above wiring. Further, the electrical connection between the different triple-turn regions can be similarly performed by the wiring described above. This method is particularly effective when the first method is applied to one of the triple well regions and the second method is not applied to the other triple well region. Further, in the same double well region, the electrical connection between the inside and the outside of the shallow well having the same conductivity type as that of the substrate and directly or indirectly connected to the substrate can be similarly performed by the wiring. Moreover, in the triple well region, the same conductivity type as the substrate is used, and the electrical connection to the 137166.doc -23-200950059 is also performed in the same manner as the wiring between the inside and the outside of the shallow well connected by the upper substrate. . At least a part of the electrical connection between the deep n-type well and the deep n-type shallow well and the substrate which must be connected to the substrate in the circuit 5 and the circuit can be similarly performed by the wiring. The mechanism for preventing dielectric breakdown of the gate insulating film of mis by the first method and the second method will be described. Here, the relationship is 'p-type on the substrate.
$進仃說明’但於基板為n型之情形時,只要於下述說明 中將η型與p型替換即可。 (1)第1方法: 0-1)防止深井帶電。When the substrate is n-type, the n-type and p-type may be replaced in the following description. (1) Method 1: 0-1) Prevent deep wells from being charged.
田構成作為對象之深η型井内形成之反相器電路之pMis 及nMlS之閘極電極處於浮動狀態時,形成有p刪之淺打型 井與形成有壤18之淺Ρ料之間成為導通狀態(參照圖4⑷ ())因此若將具有與p型基板相同導電型之淺p型井連 ,;土板則不僅s亥淺p型井,而且内包該淺p型井之深〇 聖井及存在於深η型井内之淺η型井中流入之電荷均會朝基 板放電。因此,若藉由最初之配線層來連接淺ρ型井與基 板則’、要構成反相器電路之pMIS及nMIS之閘極電極處 於子動狀態,便可抑制;罙n型井之帶電,結果便就可防止 閘極絕緣膜之絕緣破壞。 於構成反相益電路之pMIS之閘極電極與nMISi閘極電 極之間’可將閘極電極自身作為配線而於形成問極電極之 同時進仃接線,於此情形時,無須藉由配線步驟來進行接 137166.doc -24· 200950059 線。 若構成反相器電路之pMIS及朗8之間極電極於產品完 成後仍處於浮動狀態,則相應之L型井與&型井之 間將成為導通狀態,結果會導致功耗增大,因而欠佳。因 , 此,將處於浮動狀態之構成反相器電路之pMIanMIk ‘ ^極電極於複數個配線步驟中之任—步驟中連接至特定要 ^。然而’於連接時會損及帶電抑制效果,因此較理想的 ❹ {上述連接儘可能於之後之步驟中進行。此時考慮到以下 方面可獲得更好之效果。 一般認為,當於層間絕緣膜上形成連接孔時,深n型井 中蓄積之正電荷大多會到達.型井及^型井,並自形成 有複數個之連接孔流入。該等連接孔係每當形成各層之層 間絕緣膜時,每次形成於大致相同之位置上藉此任一 配線層均能以低電阻而與淺p型井或者淺_井電性連接。 然而’於取上層之配線上所形成之絕緣膜中,主要係使與 〇 I導體裝置外部之連接部位開口’因此基本上不形成對淺 p型井或者淺n型井之連接孔。因此,即便沒有具有處於浮 動狀態之PMIS及nMIS之閘極電極之反相器電路,深n型井 亦基本上不帶電。因此,構成上述之反相器電路之p刪及 , nMIS之閘極電極與特定部位之連接較理想的是使用最上層 2配線來進行。‘然而,亦可視需要藉由於最上層之配線之 刖形成之配線來連接構成反相器電路之pMis&nMis之閘 極電^與特定部位,但效果會猶差。特別係於最上層之配 線之河形成之配線,當該配線上所形成之連接孔之數量小 137166.doc -25- 200950059 於該配線下層之配線上所形成之連接孔之數量時,若藉由 該配線來連接構成反相器電路之pMIS&nMIS之閘極電極 與特定部位,便可獲得接近藉由最上層之配線進行連接時 之效果。 U-2)防止形成於深井内且具有與基板相同導電性之淺 井帶電。 ' 當深η型井内之淺p型井與p型基板連接時,即便不進行 特別之操作,電荷亦會放電,因此並無問題。然而,當淺 P型井未與p型基板連接時,於配線步驟之較早階段構成以❹ 淺P型井内形成之nMIS為構成要素之反相器電路,並且將 其閘極電極維持為浮動狀態^藉此’與上述d — D防止深井 帶電之對策同樣地’形成有反相器電路之-組淺η型井與p 1井成為導通狀態’因此流入淺?型井之負電荷會經由淺打 型井及深η型井而朝基板放電。 此處’設想了使用構成反相器電路之要素之一部分,但 亦可不使用電路構成要素’而另外形成僅以防止深口型井 或者深η型井内之淺_井帶電為目的之反相器電路。此❹ 時亦可於其他電路要素以外,另行形成構成反相器電路 淺n^L井及庚ρ型井。無論如何,若於半導體裝置已完成 之狀態下MIS之閘極電極仍處於浮動狀態,則使用半導體· 裝置時淺η型井與&型井之間會流動較大電流而功耗冑, ,口此人仏。因此,與反相器電路係電路構成要素之情 =相同’較理想的是將閉極電極連接於適當之部位,例如 Ρ里井久η型井或者基板。當上述間極電極連接於淺ρ 137166.doc -26- 200950059 型井、淺η型井或者基板時閘極電位固, 因此不會有過 度之電流流動,功耗僅會略微增加。 亦可連接於除了 該等部位以外之部位,但閘極電極之電位會隨著電路動 而變動’從而會有過度之電流流動’因此功耗會稍許择 加。再者,以防止深η型井或者淺ρ型井帶電為目的而形^ 專用之反相器電路之方法’需要用於形成該反相器電路 區域’因而存在半導體晶片變大之缺點。另一方面,該方When the gate electrode of the pMis and nMlS in the inverter circuit formed in the deep n-type well is in a floating state, the field is formed between the shallow well formed with the p-cut and the shallow material formed with the soil 18. State (refer to Figure 4 (4) ()) Therefore, if a shallow p-type well with the same conductivity type as the p-type substrate is connected, the soil plate is not only the shallow p-type well, but also the deep p-well of the shallow p-type well The charge flowing into the shallow n-type well existing in the deep η well will discharge toward the substrate. Therefore, if the shallow p-type well and the substrate are connected by the first wiring layer, the gate electrodes of the pMIS and nMIS which constitute the inverter circuit are in a sub-moving state, and the charging of the 罙n-type well can be suppressed. As a result, insulation breakdown of the gate insulating film can be prevented. Between the gate electrode of the pMIS constituting the reverse phase benefit circuit and the nMISi gate electrode, the gate electrode itself can be used as a wiring to form a gate electrode while the wiring is formed. In this case, it is not necessary to use a wiring step. Come and pick up the line 137166.doc -24· 200950059. If the pole electrode between the pMIS and the Lang 8 forming the inverter circuit is still floating after the completion of the product, the corresponding L-well and the & well will become conductive, resulting in an increase in power consumption. Therefore, it is not good. Therefore, the pMIanMIk '^ electrode of the inverter circuit which is in a floating state is connected to the specific one in the step of the plurality of wiring steps. However, the charging suppression effect is impaired at the time of connection, so it is preferable that the above connection is made as far as possible in the subsequent steps. At this point, consider the following aspects for better results. It is considered that when a connection hole is formed on the interlayer insulating film, the positive charge accumulated in the deep n-type well mostly reaches the well and the well, and flows in from the plurality of connection holes formed. Each of the connection holes is formed at substantially the same position each time the interlayer insulating film of each layer is formed, whereby any of the wiring layers can be electrically connected to the shallow p-type well or the shallow-well with low resistance. However, in the insulating film formed on the wiring of the upper layer, the connection portion to the outside of the conductor device of the 〇I is mainly made to open, so that the connection hole to the shallow p-type well or the shallow n-type well is not substantially formed. Therefore, even without an inverter circuit having gate electrodes of PMIS and nMIS in a floating state, the deep n-type well is substantially uncharged. Therefore, it is preferable to use the uppermost layer 2 wiring for the connection of the above-described inverter circuit and the gate electrode of the nMIS to the specific portion. ‘However, it is also necessary to connect the gates of the pMis&nMis constituting the inverter circuit to a specific portion by wiring formed by the wiring of the uppermost layer, but the effect is not bad. In particular, when the number of connection holes formed on the wiring is small, the number of connection holes formed on the wiring is small, 137166.doc -25- 200950059, the number of connection holes formed on the wiring of the lower layer of the wiring By connecting the gate electrode and the specific portion of the pMIS&nMIS constituting the inverter circuit to the wiring, it is possible to obtain an effect when the connection is made by the wiring of the uppermost layer. U-2) Prevents shallow wells that are formed in deep wells and have the same conductivity as the substrate. When a shallow p-type well in a deep n-type well is connected to a p-type substrate, the charge is discharged even without special operation, so there is no problem. However, when the shallow P-type well is not connected to the p-type substrate, an inverter circuit having nMIS formed in the shallow P-type well as a constituent element is constructed at an early stage of the wiring step, and the gate electrode thereof is maintained floating. In the same state, the same as the above-mentioned countermeasures for preventing the deep well charging, the group shallow n-type well and the p 1 well are in an on state, so that the negative electric charge flowing into the shallow well is passed. The shallow well and the deep η well are discharged toward the substrate. Here, it is assumed that one of the elements constituting the inverter circuit is used, but it is also possible to form an inverter for the purpose of preventing shallow-well charging in deep-mouth wells or deep-n-type wells without using circuit components. Circuit. In this case, it is also possible to form a shallow n^L well and a G-p type well which constitute an inverter circuit in addition to other circuit elements. In any case, if the gate electrode of the MIS is still in a floating state in the state in which the semiconductor device has been completed, a large current flows between the shallow n-type well and the & type well when the semiconductor device is used, and the power consumption is reduced, This person is awkward. Therefore, it is preferable to be the same as the constituent elements of the inverter circuit system. It is preferable to connect the closed electrode to an appropriate portion, for example, a Ρ里井久 η-type well or a substrate. When the above-mentioned interpole electrode is connected to the shallow 127166.doc -26-200950059 well, shallow n-type well or substrate, the gate potential is solid, so there is no excessive current flow, and the power consumption is only slightly increased. It can also be connected to a part other than these parts, but the potential of the gate electrode fluctuates with the circuit's movement, and there is excessive current flow. Therefore, the power consumption is slightly increased. Furthermore, the method of forming a dedicated inverter circuit for the purpose of preventing the charging of a deep n-type well or a shallow p-type well is required to form the inverter circuit region, and thus there is a disadvantage that the semiconductor wafer becomes large. On the other hand, the party
法具有布局上不會產生制約之優點’特別係將淺型井與 淺Ρ型井設為專料’該優點顯著。因此,可視需要來選 擇是否形成專用之反相器電路。 ' ⑺第2方法:阻斷自深井、或者形成於深井内且具有與 基板相同導電性之淺井經由MIS之閘極絕緣膜到達基板或 者具有基板電位之部位之配線路徑。 該第2方法係於帶電顯著之製造步驟之期間,藉由阻斷 自深η型井經由MIS之雜絕緣膜料基板或者具有基板電 位之部位之電流路徑、或者自深n型井内之淺口型井經由 刪之閘極絕緣膜料基板或者具有基板電位之部位之電 流路徑mMISm㈣之絕緣破壞。當到達淺p 1井或者戋n型井之連接孔形成得較多時,深η型井或者深 η型井内形成之淺?型井之帶電顯著。因此,藉由使用正上 方之絶緣膜上形成之連接孔之數量相對較少之配線層來連 接冰η型井與基板或者具有基板電位之部位之間、或者深〇 里井内形成之淺ρ型井與基板或者具有基板電位之部位之 間,可使連接後之深η型井之帶電量或者深η型井内之 137166.doc •27· 200950059 型井之帶電量減少,從而可防止MIS之閘極絕緣膜之絕緣 破壞。此時,與上述第丨方法同樣,若使用最上層之配 線,則可獲得良好之結果。 (實施形態1) 使用圖9〜圖12,對本實施形態!之具有三重井構造之半 導體裝置進行說明。此處係說明針對正帶電實施第丨方法 之一例。圖9係表示本實施形態丨之構成上述圖聲音圖 像處理裝置之1/〇(輸入輸出)電路部及邏輯電路部之一例之 電路圖,圖10係本實施形態丨之包含構成適用上述第丨方法 之反相器電路之pMIS及nMIS之區域之主要部分剖面圖, 圖11係用於說明本實施形態丨之適用上述第丨方法之反相器 電路之電路元件之剖面示意圖,圖12係用於說明本實施形 態1之適用上述第丨方法之MIS之電路元件之剖面示意圖。 如圖9所示,於邏輯電路部中,於p型基板i内之彼此不 同之區域中形成有深η型井_、3⑽。由於用於供給電源 電壓之電路設計上之必要神,逛„袖#、Λ λ ____The method has the advantage that there is no restriction on the layout. In particular, the advantages of the shallow well and the shallow well are made special. Therefore, it is possible to select whether or not to form a dedicated inverter circuit as needed. (7) Second method: A wiring path from a deep well or a shallow well formed in a deep well and having the same conductivity as the substrate reaches the substrate or the portion having the substrate potential via the gate insulating film of the MIS. The second method is for blocking the current path from the deep η type well through the MIS impurity insulating film substrate or the portion having the substrate potential, or from the shallow mouth in the deep n-type well during the charging step of the significant charging process. The well is broken by the insulation of the gate insulating film substrate or the current path mMISm (4) of the portion having the substrate potential. When the connection holes reaching the shallow p 1 well or the 戋n-type well are formed more, is the shallow η-type well or the deep η-type well formed shallow? The wells are significantly charged. Therefore, the shallow p-type formed between the ice n-type well and the substrate or the portion having the substrate potential or the deep well is formed by using a wiring layer having a relatively small number of connection holes formed on the insulating film directly above. Between the well and the substrate or the portion having the substrate potential, the charge amount of the deep η-type well after the connection or the charge of the 137166.doc •27·200950059 well in the deep η-type well can be reduced, thereby preventing the MIS gate Insulation damage of the pole insulating film. At this time, similarly to the above-described third method, if the wiring of the uppermost layer is used, good results can be obtained. (Embodiment 1) This embodiment will be described with reference to Figs. 9 to 12! A semiconductor device having a triple well structure will be described. Here, an example of implementing the third method for positive charging will be described. Fig. 9 is a circuit diagram showing an example of a 1/〇 (input/output) circuit unit and a logic circuit unit of the audio image processing apparatus of the present embodiment, and Fig. 10 is a configuration of the present embodiment. FIG. 11 is a cross-sectional view showing a circuit component of an inverter circuit to which the above-described second method is applied, and FIG. 12 is a schematic diagram for explaining a main portion of a region of a pMIS and an nMIS of an inverter circuit of the present invention. A schematic cross-sectional view showing a circuit element of the MIS to which the above-described second method is applied in the first embodiment. As shown in Fig. 9, in the logic circuit portion, deep n-type wells _, 3 (10) are formed in regions different from each other in the p-type substrate i. Due to the necessity of designing the circuit for supplying power voltage, please visit “Sleeve #, Λ λ ____
pMIS 254ρ及nMIS 254η構成反相器電路出乂卜 254η。該等 。反相器電 137166.doc -28· 200950059 路INV1之pMIS 254p之閘極電極及nMIS 254η之閘極電極 係使用第8層配線255(Μ8)而與淺η型井251内形成之η型半 導體區域連接。用於構成反相器電路INV1之接線,除了 pMIS 254ρ之閘極電極及nMIS 254η之閘極電極以外,其他 係使用第1層配線來進行。pMIS 254ρ之閘極電極與nMIS 254η之閘極電極之間之接線係於形成閘極電極之同時進 行。淺ρ型井252係藉由第1層配線253(Μ1)而與基板1連 接。 圖10表示包含構成反相器電路INV1之pMIS 254ρ及nMIS 254η之區域之主要部分剖面圖。淺η型井251内形成之pMIS 254p之閘極電極例如係將添加有ρ型雜質之多晶矽膜503與 矽化物層505積層而成之構造,淺ρ型井252内形成之nMIS 254η之閘極電極例如係將添加有η型雜質之多晶矽膜504與 矽化物層505積層而成之構造,且pMIS 254ρ之閘極電極與 nMIS 254η之閘極電極藉由石夕化物層505而連接。又,pMIS 254p之閘極電極503及nMIS 254η之閘極電極504經由第1層 〜第8層配線Ml〜Μ8而與淺η型井251電性連接。又,淺ρ型 井252經由第1層配線253(Μ1)而與基板1電性連接。 又,於深η型井200内,形成有構成於電路動作中起特定 作用之反相器電路之pMIS 203ρ及nMIS 203η。反相器電路 之pMIS 203ρ之閘極電極及nMIS 203η之閘極電極係使用第 3層配線2(Μ3)而與深η型井200外部之區域,例如1/〇電路 部上形成之pMIS 103?之汲極及nMIS 10311之汲極連接。 又,於深η型井200内之彼此不同之區域中,形成有淺n 137166.doc -29- 200950059 型井204及淺p型井205,淺p型井205由於電路上之必要性 而藉由第1層配線206(M1)與基板1電性連接。淺η型井204 及淺Ρ型井205中包含由pMIS 207ρ及nMIS 207η構成之反相 器電路,且形成有複數個反相器電路,但其閘極電極均係 使用至第3層為止之配線中之任一條配線而與電路之特定 部分接線。因此,於形成第3層配線之步驟以後,對於淺ρ 型井205無法期望防止深η型井200帶電之功能。 於深η型井300中,亦形成有於電路動作中並不起任何作 用之反相器電路INV2。於深η型井300内之彼此不同之區域 中形成有淺η型井351與淺ρ型井352,進而於淺η型井351中 形成有卩1^18 3 54?,於淺?型井3 52中形成有11]^18 3 5411。由 該等pMIS 3 54p及nMIS 3 54n構成反相器電路INV2。反相 器電路INV2之pMIS 354ρ之閘極電極及nMIS 354η之閘極 電極係使用第8層配線355(Μ8)而與淺ρ型井352内形成之ρ 型半導體區域連接。用於構成反相器電路INV2之接線,除 了pMIS 3 54ρ之閘極電極及nMIS 3 54η之閘極電極以外,其 他係使用第1層配線來進行。又,pMIS 354ρ之閘極電極與 nMIS 354η之閘極電極之間之接線係於形成閘極電極之同 時進行。淺ρ型井352係藉由第1層配線353(Μ1)而與基板1 連接。 又,於深η型井300内形成之淺ρ型井304中形成有nMIS 3 08,nMIS 3 08之閘極電極係使用第3層配線311(M3)而與 由淺η型井301内形成之pMIS 307p及淺ρ型井302内形成之 nMIS 307η構成之反相器電路之輸出段連接。包含nMIS 308 137166.doc •30- 200950059 之淺P型井304由於電路上之必要性而藉由第i層配線 3 05(M1)與基板1電性連接。於淺p型井3〇4中包含以nMis 309η為構成要素之反相器電路’且形成有複數個反相器電 路,但其閘極電極均係使用至第3層為止之配線中之任一 • 絲線而與電路之特定部分連接。因此,於形成第3層配 . 線之步驟以後,對於淺Ρ型井304無法期望防止深η型井3〇〇 帶電之功能。 H 其次,使用圖11,對藉由本實施形態1之第1方法所獲得 之效果進行說明。圖丨〗係對在形成於第3層配線上之層間 絕緣膜上形成連接孔之步驟中,半導體裝置内之深η型井 200帶電之情形進行說明之剖面示意圖。 於該階段(在形成於第3層配線上之層間絕緣膜上形成連 接孔之步驟)中,構成反相器電路INV1之pMIS 254ρ之閘極 4極及nMIS 254η之閘極電極處於浮動狀態,因此因電衆 放電而流入深η型井2〇〇之正電荷會經由反相器電路^…及 〇 配線253(Μ1)而朝基板1放電。因此,於由深η型井200内形 成之pMIS 203ρ及nMIS 203η構成之反相器電路中,不管其 閘極電極疋否連接於基板1内形成之丨η之沒極,其 • 閘極絕緣膜上均不會產生電位差,因此不會產生絕緣破 . 壞。再者,隨著淺η型井1 〇 1之帶電,有時汲極之一部分會 正帶電’此時,於構成反相器電路之pMIS 2〇3ρ及nMls 2〇3n之閘極絕緣膜上產生電位差。然而,由於淺η型井ι〇1 之面積較小因此帶電量較少,達不到閘極絕緣膜產生絕緣 破壞之程度。對於其他電路構成要素,亦可按相同方式抑 137166.doc -31 · 200950059 制MIS之閘極絕緣膜之絕緣破壞。於上述之圖丨丨中,表示 了在形成於第3層配線上之層間絕緣膜上形成連接孔之步 驟中之帶電狀態,但直至在形成於第7層配線上之層間絕 緣膜上形成連接孔之步驟為止,流入深n型井2〇〇之電荷均 會放電,因此可抑制MIS之閘極絕緣膜之絕緣破壞。又, 在形成於第8層配線上之絕緣膜上形成連接孔之步驟中, 深η型井200之帶電量較少,因此MIS之閘極絕緣膜不會產 生絕緣破壞。 其次,使用圖12,對藉由本實施形態丨之第丨方法所獲得 之其他效果進行說明。圖12係對在形成於第3層配線上之 層間絕緣膜上形成連接孔之步驟中,半導體裝置内之深η 型井300帶電之情形進行說明之剖面示意圖。 於該階段(在形成於第3層配線上之層間絕緣膜上形成連 接孔之步驟)中,構成反相器電路INV22pMIS 354ρ之閘極 電極及nMIS 354η之閘極電極處於浮動狀態,因此因電漿 放電而流入深η型井300之正電荷會經由反相器電路跗¥2及 配線353(Μ1)而朝基板丨放電。藉此,可防止位於深η型井 3〇〇内之所有淺η型井及淺卩型井帶電。因此,於深η型井 3〇〇内形成之nMIS 308中,不管其間極電極是否連接於其 他淺P型井302内形成之nMIS 3〇7n之汲極,其閘極絕緣膜 均不會產生電位差,因此不會產生絕緣破壞。 (實施形態2) 使用圖13,對本實施形態2之具有三重井構造之半導體 裝置進行忒明。此處係說明針對正帶電實施與上述實施形 137I66.doc -32- 200950059 態1不同之第1方法之其他例。圖13係表示構成上述圖1之 聲音圖像處理裝置之本實施形態2之1/0(輸入輸出)電路部 及邏輯電路部之一例之電路圖。 如圖13所示,於深η型井200内,並未形成上述實施形態 1之半導體裝置中形成的對於電路動作並無貢獻之由pMIS 254p及nMIS 254η構成之反相器電路INV1、内包pMIS 254p之淺η型井251以及内包nMIS 254η之淺p型井252。取 而代之的是藉由第1層配線206(Μ1)來進行淺ρ型井205與基 板1之連接,並且藉由最上層之第8層配線209(Μ8)來進行 由pMIS 207ρ及nMIS 207η構成之反相器電路INV3之閘極 電極與電路之特定部分之連接,藉此使反相器電路INV3具 有防止深η型井200帶電之功能。 另一方面,於深η型井300内,並未形成上述實施形態1 之半導體裝置中形成的對於電路動作並無貢獻之由pMIS 354p與nMIS 354η構成之反相器電路INV2、内包pMIS 354p之淺η型井351以及内包nMI S 354η之淺ρ型井352。取 而代之的是藉由第1層配線305(Μ1)來進行淺ρ型井304與基 板之連接,並且藉由最上層之第8層配線313(Μ8)來進行由 pMIS 3 09ρ與nMIS 3 09η構成之反相器電路INV4之閘極電 極與電路之特定部分之連接。關於其他電路構成等與上述 實施形態1相同。 其次,對藉由本實施形態2所獲得之效果進行說明。The pMIS 254ρ and the nMIS 254η constitute an inverter circuit 254η. These are the same. Inverter power 137166.doc -28· 200950059 The gate electrode of pMIS 254p of INV1 and the gate electrode of nMIS 254η use the 8th layer wiring 255 (Μ8) and the n-type semiconductor formed in the shallow n-type well 251. Regional connection. The wiring for constituting the inverter circuit INV1 is performed using the first layer wiring except for the gate electrode of the pMIS 254p and the gate electrode of the nMIS 254n. The wiring between the gate electrode of pMIS 254p and the gate electrode of nMIS 254n is performed while forming the gate electrode. The shallow p-type well 252 is connected to the substrate 1 by the first layer wiring 253 (Μ1). Fig. 10 is a cross-sectional view showing the essential part of a region including pMIS 254p and nMIS 254n constituting the inverter circuit INV1. The gate electrode of the pMIS 254p formed in the shallow n-type well 251 is, for example, a structure in which a polycrystalline germanium film 503 to which a p-type impurity is added and a germanide layer 505 are laminated, and a gate of nMIS 254η formed in the shallow p-type well 252 is formed. The electrode is, for example, a structure in which a polycrystalline germanium film 504 to which an n-type impurity is added and a germanide layer 505 are laminated, and a gate electrode of the pMIS 254p and a gate electrode of the nMIS 254n are connected by a lithiation layer 505. Further, the gate electrode 503 of the pMIS 254p and the gate electrode 504 of the nMIS 254n are electrically connected to the shallow n-well 251 via the first to eighth wirings M1 to Μ8. Further, the shallow p-type well 252 is electrically connected to the substrate 1 via the first layer wiring 253 (Μ1). Further, in the deep n-type well 200, pMIS 203ρ and nMIS 203n which constitute an inverter circuit which plays a specific role in the operation of the circuit are formed. The gate electrode of the pMIS 203p and the gate electrode of the nMIS 203n of the inverter circuit are the regions outside the deep n-well 200 using the third layer wiring 2 (Μ3), for example, the pMIS 103 formed on the 1/〇 circuit portion. The bungee of the bungee and the nMIS 10311 are connected. Further, in the different regions of the deep η-type well 200, shallow n 137166.doc -29-200950059 type well 204 and shallow p-type well 205 are formed, and the shallow p-type well 205 is borrowed due to the necessity of circuit. The first layer wiring 206 (M1) is electrically connected to the substrate 1. The shallow n-well 204 and the shallow well 205 include an inverter circuit composed of pMIS 207ρ and nMIS 207η, and a plurality of inverter circuits are formed, but the gate electrodes are used until the third layer. Wire any of the wires to wire a specific part of the circuit. Therefore, after the step of forming the third layer wiring, the function of preventing the deep n-type well 200 from being charged is not expected for the shallow p-type well 205. In the deep n-well 300, an inverter circuit INV2 which does not function in the circuit operation is also formed. Shallow n-type wells 351 and shallow p-type wells 352 are formed in different regions of the deep n-type well 300, and 卩1^18 3 54? is formed in the shallow n-type well 351, which is shallow? The well 3 52 is formed with 11]^18 3 5411. The inverter circuit INV2 is constituted by the pMIS 3 54p and the nMIS 3 54n. The gate electrode of the pMIS 354p and the gate electrode of the nMIS 354n of the inverter circuit INV2 are connected to the p-type semiconductor region formed in the shallow p-well 352 by using the eighth layer wiring 355 (Μ8). The wiring for constituting the inverter circuit INV2 is performed using the first layer wiring except for the gate electrode of the pMIS 3 54p and the gate electrode of the nMIS 3 54n. Further, the wiring between the gate electrode of the pMIS 354p and the gate electrode of the nMIS 354n is performed while forming the gate electrode. The shallow p-type well 352 is connected to the substrate 1 by the first layer wiring 353 (Μ1). Further, nMIS 3 08 is formed in the shallow p-type well 304 formed in the deep n-type well 300, and the gate electrode of the nMIS 3 08 is formed by using the third layer wiring 311 (M3) and the shallow n-type well 301. The pMIS 307p and the output section of the inverter circuit formed by the nMIS 307n formed in the shallow p-type well 302 are connected. The shallow P-well 304 including nMIS 308 137166.doc • 30-200950059 is electrically connected to the substrate 1 by the ith layer wiring 3 05 (M1) due to the necessity of circuit. In the shallow p-type well 3〇4, an inverter circuit having nMis 309η as a constituent element is included and a plurality of inverter circuits are formed, but the gate electrodes are all used in the wiring up to the third layer. A wire is connected to a specific part of the circuit. Therefore, after the step of forming the third layer of the wiring, it is not desirable for the shallow well 304 to prevent the deep n-type well from being charged. H Next, the effect obtained by the first method of the first embodiment will be described with reference to Fig. 11 . Fig. 。 is a schematic cross-sectional view showing a case where a deep n-type well 200 in a semiconductor device is charged in a step of forming a connection hole in an interlayer insulating film formed on a wiring of a third layer. At this stage (the step of forming a connection hole on the interlayer insulating film formed on the wiring of the third layer), the gate 4 of the pMIS 254p and the gate electrode of the nMIS 254n which constitute the inverter circuit INV1 are in a floating state. Therefore, the positive electric charge that flows into the deep n-type well 2 due to the discharge of the electric power is discharged to the substrate 1 via the inverter circuit 〇 and the 〇 wiring 253 (Μ1). Therefore, in the inverter circuit composed of the pMIS 203ρ and the nMIS 203η formed in the deep η-type well 200, regardless of whether the gate electrode 连接 is connected to the 没η of the substrate 1, the gate is insulated. There is no potential difference on the film, so there is no insulation breakage. Furthermore, as the shallow n-type well 1 〇1 is charged, sometimes one of the drains is positively charged. At this time, on the gate insulating film of pMIS 2〇3ρ and nMls 2〇3n constituting the inverter circuit. A potential difference is generated. However, since the area of the shallow n-type well ι 〇 1 is small, the amount of charge is small, and the degree of insulation damage of the gate insulating film is not obtained. For other circuit components, the insulation damage of the gate insulating film of MIS can also be suppressed in the same way. In the above-mentioned figure, the charged state in the step of forming the connection hole in the interlayer insulating film formed on the wiring of the third layer is shown, but the connection is formed on the interlayer insulating film formed on the wiring of the seventh layer. At the step of the hole, the electric charge flowing into the deep n-type well is discharged, so that the insulation breakdown of the gate insulating film of MIS can be suppressed. Further, in the step of forming the connection holes formed in the insulating film formed on the eighth layer wiring, the deep n-type well 200 has a small amount of charge, so that the MIS gate insulating film does not cause dielectric breakdown. Next, another effect obtained by the second method of the present embodiment will be described with reference to Fig. 12 . Fig. 12 is a schematic cross-sectional view showing a state in which a deep n-type well 300 in a semiconductor device is charged in a step of forming a connection hole in an interlayer insulating film formed on a third layer wiring. In this stage (the step of forming a connection hole on the interlayer insulating film formed on the third layer wiring), the gate electrode constituting the inverter circuit INV22pMIS 354p and the gate electrode of the nMIS 354n are in a floating state, and thus The positive electric charge that flows into the deep n-type well 300 by the slurry discharge is discharged toward the substrate via the inverter circuit 跗¥2 and the wiring 353 (Μ1). Thereby, all shallow n-type wells and shallow wells located in the deep n-type well can be prevented from being charged. Therefore, in the nMIS 308 formed in the deep n-type well 3, regardless of whether the pole electrode is connected to the drain of the nMIS 3〇7n formed in the other shallow P-well 302, the gate insulating film is not generated. The potential difference is so that no dielectric breakdown occurs. (Embodiment 2) A semiconductor device having a triple well structure according to the second embodiment will be described with reference to Fig. 13 . Here, another example of the first method different from the first embodiment of the above-described embodiment 137I66.doc-32-200950059 will be described. Fig. 13 is a circuit diagram showing an example of a 1/0 (input/output) circuit unit and a logic circuit unit of the second embodiment which constitutes the audio image processing apparatus of Fig. 1 described above. As shown in FIG. 13, in the deep n-type well 200, the inverter circuit INV1 composed of the pMIS 254p and the nMIS 254n which does not contribute to the circuit operation formed in the semiconductor device of the first embodiment described above is not formed, and the pMIS is included. A shallow n-type well 251 of 254p and a shallow p-type well 252 containing nMIS 254η. Instead, the shallow p-well 205 is connected to the substrate 1 by the first layer wiring 206 (Μ1), and is composed of the pMIS 207ρ and the nMIS 207n by the eighth-layer wiring 209 (Μ8) of the uppermost layer. The gate electrode of the inverter circuit INV3 is connected to a specific portion of the circuit, whereby the inverter circuit INV3 has a function of preventing the deep n-well 200 from being charged. On the other hand, in the deep n-type well 300, the inverter circuit INV2 composed of the pMIS 354p and the nMIS 354n, which is formed in the semiconductor device of the first embodiment, which does not contribute to the circuit operation, is not formed, and the pMIS 354p is included. The shallow n-type well 351 and the shallow p-type well 352 enclosing the nMI S 354η. Instead, the shallow p-well 304 is connected to the substrate by the first layer wiring 305 (Μ1), and is composed of pMIS 3 09ρ and nMIS 3 09η by the eighth layer wiring 313 (Μ8) of the uppermost layer. The gate electrode of the inverter circuit INV4 is connected to a specific portion of the circuit. Other circuit configurations and the like are the same as those in the first embodiment described above. Next, the effects obtained by the second embodiment will be described.
於本實施形態2中,將由pMIS 207ρ與nMIS 207η構成之 反相器電路INV3之閘極電極以及由pMIS 309ρ與nMIS 137166.doc -33- 200950059 3 09η構成之反相器電路INV4之閘極電極均維持為浮動狀 態,直至將要進行最上層之第8層配線之形成步驟之前為 止,並且,包含構成反相器電路INV3之nMIS 207n之淺ρ型 井205以及包含構成反相器電路INV4之nMIS 309η之淺p型 井304分別使用第1層配線206(Μ1)、305(Μ1)而與基板1連 接。藉此,直至在形成於第7層配線上之層間絕緣膜上形 成連接孔之步驟為止,與上述實施形態1同樣地,流入深η 型井200、300之正電荷朝基板1放電。結果可抑制構成反 相器電路之pMIS 203ρ或者nMIS 203η上產生之閘極絕緣膜 之絕緣破壞、以及nMIS 308上產生之閘極絕緣膜之絕緣破壞。 (實施形態3) 使用圖14及圖15,對本實施形態3之具有三重井構造之 半導體裝置進行說明。此處係說明針對正帶電實施與上述 實施形態1及2不同之第1方法之其他例。圖14係表示構成 上述圖1之聲音圖像處理裝置之本實施形態3之1/0(輸入輸 出)電路部及邏輯電路部之一例之電路圖,圖1 5係本實施 形態3之包含構成適用上述第1方法之反相器電路之pMIS及 nMIS之區域之主要部分剖面圖。 如圖14所示,構成用於防止深η型井200帶電之反相器電 路 INV1 之 pMIS 254ρ 及 nMIS 254η 中,nMIS 254η 與上述實 施形態1不同,其形成於基板1内所形成之淺Ρ型井252内。 又,構成用於防止深η型井300帶電之反相器電路INV2之 pMIS 354ρ及nMIS 354η中,nMIS 354η與上述實施形態1不 同,其形成於基板1内所形成之淺Ρ型井352内。淺ρ型井 137166.doc • 34- 200950059 252、352係形成於基板1内,且自動與基板1電性連接,因 此無須藉由配線來進行與基板1之連接。其他電路構成等 與上述實施形態1相同。In the second embodiment, the gate electrode of the inverter circuit INV3 composed of pMIS 207ρ and nMIS 207n and the gate electrode of the inverter circuit INV4 composed of pMIS 309ρ and nMIS 137166.doc -33- 200950059 3 09η Both are maintained in a floating state until the formation step of the uppermost layer 8 wiring, and the shallow p well 205 including the nMIS 207n constituting the inverter circuit INV3 and the nMIS including the inverter circuit INV4 are included. The shallow p-type wells 309 η are connected to the substrate 1 using the first layer wirings 206 (Μ1) and 305 (Μ1), respectively. As a result, the positive electric charges flowing into the deep n-type wells 200 and 300 are discharged toward the substrate 1 in the same manner as in the first embodiment until the step of forming the connection holes in the interlayer insulating film formed on the seventh layer wiring. As a result, the dielectric breakdown of the gate insulating film generated on the pMIS 203p or nMIS 203n constituting the inverter circuit and the dielectric breakdown of the gate insulating film generated on the nMIS 308 can be suppressed. (Embodiment 3) A semiconductor device having a triple well structure according to Embodiment 3 will be described with reference to Figs. 14 and 15 . Here, another example of the first method different from the above-described first and second embodiments for positive charging will be described. Fig. 14 is a circuit diagram showing an example of a 1/0 (input/output) circuit unit and a logic circuit unit of the third embodiment which constitutes the audio image processing apparatus of Fig. 1, and Fig. 15 is a configuration including the configuration of the third embodiment. A cross-sectional view of a main portion of a region of pMIS and nMIS of the inverter circuit of the first method. As shown in FIG. 14, among the pMIS 254p and nMIS 254n constituting the inverter circuit INV1 for preventing the deep n-type well 200 from being charged, the nMIS 254n is different from that of the first embodiment, and is formed in the shallow layer formed in the substrate 1. Within the well 252. Further, among the pMIS 354 ρ and nMIS 354 η constituting the inverter circuit INV2 for preventing the deep n-type well 300 from being charged, the nMIS 354 η is formed in the shallow well 352 formed in the substrate 1 unlike the first embodiment. . Shallow p-type well 137166.doc • 34- 200950059 252, 352 are formed in the substrate 1 and are automatically electrically connected to the substrate 1, so that connection to the substrate 1 is not required by wiring. Other circuit configurations and the like are the same as in the first embodiment described above.
圖15表示包含構成反相器電路INV1之pMIS 254p及nMISFigure 15 shows the pMIS 254p and nMIS including the inverter circuit INV1.
254η之區域之主要部分剖面圖。淺η型井251内形成之pMIS 254p之閘極電極,例如係將添加有p型雜質之多晶矽膜503 與矽化物層505積層而成之構造,淺p型井252内形成之 nMIS 254η之閘極電極,例如係將添加有η型雜質之多晶石夕 ft w 膜504與矽化物層505積層而成之構造,pMIS 254p之閘極 電極與nMIS 254η之閘極電極藉由矽化物層505而連接。 又,pMIS 254ρ之閘極電極及nMIS 254η之閘極電極係藉由 第1層〜第8層配線Ml〜Μ8而與淺η型井251電性連接。又, 淺ρ型井252形成於ρ型基板1内,且與基板1電性連接。 (實施形態4) 使用圖16對本實施形態4之具有三重井構造之半導體裝 _ 置進行說明。此處係說明針對負帶電實施第1方法之一 例。圖16係表示構成上述圖1之聲音圖像處理裝置之本實 施形態4之電路之1/0(輸入輸出)電路部及邏輯電路部之一 - 例之電路圖。 如圖16所示,由於深η型井200内形成之淺ρ型井202及深 η型井300内形成之淺ρ型井302之面積較大,因此若置於淺 ρ型井202、302負帶電之狀況下,則其帶電量會變多,容 易產生MIS之絕緣破壞。因此,為防止淺ρ型井202、3 02負 帶電,於深η型井200内形成由pMIS 271p及nMIS 271η構成 137166.doc -35- 200950059 之反相器電路INV5,並於深η型井300内形成由pMIS 371p 及11]^118 3 7111構成之反相器電路11'^6。反相器電路1]^¥5 中,於對卩?418 271?之閘極電極與111^18 27111之閘極電極進 行加工之同時進行連接,並且將該等閘極電極與淺η型井 201藉由最上層之第8層配線272(Μ8)而進行連接。 同樣地,反相器電路INV6中,於對pMIS 371ρ之閘極電 極與nMIS 371 η之閘極電極進行加工之同時進行連接,並 且將該等閘極電極與淺η型井301藉由最上層之第8層配線 3 72(Μ8)而進行連接。用於構成反相器電路之其他接線係 藉由第1層配線來進行。其他電路構成等與上述實施形態3 相同。 其次,對藉由本實施形態4所獲得之效果進行說明。 於本實施形態4中,將由pMIS 271ρ及nMIS 271η構成之 反相器電路INV5之閘極電極維持為浮動狀態,直至將要進 行最上層之第8層配線之形成步驟之前為止,因此直至在 形成於第7層配線上之層間絕緣膜上形成連接孔之步驟為 止,淺Ρ型井202與深η型井200之間經由淺η型井201而維持 為導通狀態。結果,流入淺Ρ型井202之負電荷經由淺η型 井201及深η型井200而朝基板1放電。同樣地,將由pMIS 37 lp及nMIS 37 In構成之反相器電路INV6之閘極電極維持 為浮動狀態,直至將要進行最上層之第8層配線之形成步 驟之前為止,因此直至在形成於第7層配線上之層間絕緣 膜上形成連接孔之步驟為止,淺ρ型井302與深η型井300之 間經由淺η型井301而維持為導通狀態。結杲,流入淺ρ型 137166.doc -36- 200950059 井3 02之負電荷經由淺η型井3 01及深η型井3 00而朝基板1放 電。又,藉由與上述實施形態3相同,深η型井200、300之 正帶電亦得到防止。藉此,可抑制構成反相器電路之pMIS 203p或者nMIS 203η上產生之閘極絕緣膜之絕緣破壞、以 及nMIS 308上產生之閘極絕緣膜之絕緣破壞。 (實施形態5) 使用圖17〜圖19,對本實施形態5之具有三重井構造之半 導體裝置進行說明。此處係說明針對正帶電實施第2方法 之一例。圖17係表示構成本實施形態5之上述圖1之聲音圖 像處理裝置之1/〇(輸入輸出)電路部及邏輯電路部之一例之 電路圖,圖18係用於說明本實施形態5之適用上述第2方法 之反相器電路之電路元件之剖面示意圖,圖19係用於說明 本實施形態5之適用上述第2方法之MIS之電路元件之剖面 示意圖。 如圖17所示,於深η型井200中,與上述實施形態2同樣 地,並未形成對於電路動作無貢獻之由pMIS 254ρ及nMIS 254η構成之反相器電路INV1、内包pMIS 254p之淺η型井 251以及内包nMIS 254η之淺ρ型井252。代替防止帶電用反 相器電路之形成,為了即便於深η型井200帶電之情形時亦 能防止對構成反相器電路之pMIS 203ρ及nMIS 203η之閘極 絕緣膜施加電壓,藉由最上層之第8層配線3(Μ8)來進行構 成反相器電路之pMIS 203ρ及nMIS 203η之閘極電極、與 nMIS 103!1之汲極(淺ρ型井102内形成之η型半導體區域)之 連接。 137166.doc •37- 200950059 於深η型井300内,亦未形成對於電路動作無貢獻之由 PMIS 354ρ及nMIS 354η構成之反相器電路mv2、内包 PMIS 354P之淺η型井351以及内包nMls 354n之淺p型井 352。又,淺p型井304與基板丨之連接係藉由最上層之第8 層配線314(M8)來進行。關於其他電路構成等與上述實施 形態1相同。 其次,使用圖18對藉由本實施形態5之第2方法所獲得之 效果進行說明。圖18係對在形成於第7層配線上之層間絕 緣膜上形成連接孔之步驟中,半導體裝置因電漿放電而帶 電之情形進行說明之剖面示意圖。 於一連_製造步驟中之該階段(在形成於第7層配線上之 層間絕緣膜上形成連接孔之步驟)中,構成反相器電路之 pMIS 203p之閘極電極及nMIS 2〇311之閘極電極不與位於基 板1内之nMIS 103η之汲極連接,其閘極絕緣膜不會產生電 位差,因此不會產生絕緣破壞。於位於深η型井2〇〇内且必 須與基板1連接之其他電路構成要素中,亦係使用第8層配 線進行與基板1之接線,因此同樣可抑制MI s之閘極絕緣膜 之絕緣破壞。再者,在形成於第7層配線上之層間絕緣膜 上形成連接孔之步驟更前之步驟中,深n型井2〇〇與基板^ 之間亦不接線,因此可抑制MIS之閘極絕緣膜之絕緣破 壞。又,在形成於第8層配線上之絕緣膜上形成連接孔之 步驟中,深η型井200之帶電量較少,因此MIS之閘極絕緣 膜不會產生絕緣破壞。 其次,使用圖19,對藉由本實施形態5之第2方法所獲得 137166.doc •38· 200950059 〇他效果進行說明。圖19係對在形成於第7層配線上之 層間絕緣膜上形成連接孔之步驟中,深η型井300帶電之情 形進行說明之剖面示意圖。 於該階段(在形成於第7層配線上之層間絕緣膜上形成連 之乂驟)中,淺Ρ型井3〇4亦不與基板^連接,因此深η • 型井则整體帶電,結果,nMIS 3G8之閘極絕緣膜不會產 生電位差,從而不會產生絕緣破壞。於其他電路構成要素 φ 中,亦同樣可抑制MIS之閘極絕緣膜之絕緣破壞。再者, 在形成於第7層配線上之層間絕緣膜上形成連接孔之步驟 更前之步驟中,淺p型井304亦與基板丨絕緣,因此可抑制 MIS之閘極絕緣膜之絕緣破壞。又,與深n型井2〇〇同樣 地,在形成於第8層配線上之絕緣膜上形成連接孔之步驟 中’深η型井300之帶電量較少,因此MIS之閘極絕緣膜不 會產生絕緣破壞。 再者,本實施形態5中,例示了對於由pMIS 2〇外及 φ nMlS 203n構成之反相器電路之閘極電極與nMIS l〇3n之沒 極之連接適用第2方法之情形、以及對於形成有nMls 3〇8 之淺p型井304與基板1之連接適用第2方法之情形,但並不 限定於此。 . (實施形態6) 使用圖20,對本實施形態6之具有三重井構造之半導體 裝置進行說明。此處係說明針對正帶電實施與上述實施形 態1、2及3不同之第1方法之其他例。圖20係表示構成上述 圖1之聲音圖像處理裝置之本實施形態6之I/O(輸入輸出)電 137166.doc -39- 200950059 路部及邏輯電路部之一例之電路圖。 如圖20所示,構成用於防止深n型井2〇〇帶電之反相器電 路INV1之PMIS 254ρ及nMIS 254η中,形成有nMIS 25如之 淺P型井252與上述實施形態i不同,其係藉由第i層配線 256(M1)而與淺p型井205電性連接。淺p型井2〇5係藉由第1 層配線206(M1)而與基板1連接,因此淺卩型井252經由淺p 型井205而間接地與基板1連接。 又,構成用於防止深η型井300帶電之反相器電路inv2 之pMIS 354P及nMIS 354η中,形成#nMIS 354n之淺p型井 352與上述實施形態!不同,其係藉由第i層配線356(mi)而 與淺P型井304電性連接。淺p型井3〇4係藉由第1層配線 305(M1)而與基板1連接,因此淺p型井352係經由淺p型井 3 04而間接地與基板丨連接。關於其他電路構成等與上述實 施形態1相同。 (實施形態7) 對本實施形態7之具有三重井構造之半導體裝置進行說 明。於上述實施形態i、3或者6中,例如使用反相器電路 INV1,使因電漿放電而流入型井2〇〇、淺n型井“I或者 淺P型井202中之正電荷朝基板}放電,且例如使用反相器 電路INV2,使因電衆放電而流入深n型井则中之正電荷朝 基板1放電,但本實施形態7中對不使用反相器電路而能夠 獲得與上述實施形態1、3或者6同樣之效果之帶電應對電 路進行說明。以下,對帶電應對電路之第㈣〜第13例進行 說明’該等示例係對代表性之電路構成進行說明,當然於 137166.doc •40· 200950059 不脫離其主旨之範圍内可實施各種變更。 對本實施形態7之第1例之帶電應對電路進行說明。圖21 表示第1例之帶電應對電路之剖面示意圖。於深η型井200 内之彼此不同之區域中形成有淺η型井281與淺ρ型井282, 於淺η型井281内之彼此不同之區域中形成有η型半導體區 域284η與ρ型半導體區域284ρ,且於淺ρ型井282内形成有 nMIS 285η。進而,nMIS 285η之閘極電極與淺η型井281内 形成之Ρ型半導體區域284ρ藉由配線283a而接線,nMIS w 285η之汲極與淺η型井281内形成之η型半導體區域284η藉 由配線283b而接線,nMIS 285η之源極藉由配線283c並經 由淺ρ型井282内形成之ρ型半導體區域286而連接於接地電 位GND。對於該等配線283a、283b、283c使用第1層配 線。第1例之帶電應對電路係由該等形成於淺η型井281内 之η型半導體區域284η與ρ型半導體區域284ρ、以及淺ρ型 井282内形成之nMIS 285η等構成,於半導體裝置之電路動 0 作中不起任何作用。 例如於製造步驟中,當因電漿放電而導致深η型井200及 淺η型井281中蓄積有較多之正電荷時,藉由ρη接面電容來 • 使ρ型半導體區域284ρ之電位與淺η型井281之電位大致相 , 等。藉此,當對nMIS 285η之閘極電極施加大於臨限值電 壓之電位時,nMIS 285η成為導通狀態,流入深η型井200 及淺η型井281中之正電荷經由配線283b、nMIS 285η之通 道、配線283c及ρ型半導體區域286而朝接地電位GND放電。 對本實施形態7之第2例之帶電應對電路進行說明。圖22 137166.doc • 41 · 200950059 表示第2例之帶電應對電路之剖面示意圖。第2例之帶電應 對電路具有與上述第1例之帶電應對電路同樣之電路構 成,但與上述第1例之帶電應對電路之不同點在於,淺η型 井281内形成之ρ型半導體區域284ρ與淺ρ型井282内形成之 ρ型半導體區域286係藉由配線287來進行接線,該配線287 係於有可能會因電漿放電而導致閘極絕緣膜產生絕緣破壞 之步驟更後之步驟中所形成。該接線較理想的是藉由最上 層之配線來進行。如此,藉由將ρ型半導體區域284ρ固定 為接地電位GND,而於半導體裝置之電路動作時使nMIS 285η始終為斷開狀態,從而不會造成nMIS 285η向其他電 路漏電等不良影響。 對本實施形態7之第3例之帶電應對電路進行說明。第3 例之帶電應對電路例如具有與上述第1例或者第2例之帶電 應對電路同樣之電路構成,並且將nMIS 285η之閘極絕緣 膜之厚度設為1 〇 nm以上之厚度。例如亦可與1/0(輸入輸 出)電路部上形成之MISFET之閘極絕緣膜之厚度相同。藉 由使nMIS 285η之閘極絕緣膜形成得較厚,從而可減少漏 電而使其可靠地進行動作。 對本實施形態7之第4例之帶電應對電路進行說明。圖 23(a)及圖23(b)分別表示第4例之帶電應對電路之平面示意 圖及剖面示意圖。第4例之帶電應對電路具有與上述第1例 之帶電應對電路同樣之電路構成,但與上述第1例之帶電 應對電路之不同點在於,接線不使用配線283a、283b、 283c,而使用由與共用接點及閘極電極為同一層之導體膜 137166.doc •42- 200950059 (例如多晶矽膜與矽化物層之積層膜)構成之配線。 即,nMIS 285η之閘極電極與淺η型井281内形成之p型半 導體區域284ρ係藉由埋入於跨及兩者而形成之連接孔CNT 内部之插塞電極PLG來進行接線。又,nMIS 28 5η之汲極 與淺η型井281内形成之η型半導體區域284η,係於兩者之 間形成由與閘極電極為同一層之導體膜構成之配線288a, 並藉由埋入於跨及該配線288a與nMIS 285η之汲極而形成 之連接孔CNT内部之插塞電極PLG以及埋入於跨及該配線 288a與η型半導體區域284η而形成之連接孔CNT内部之插 塞電極PLG來進行接線。又,nMIS 285η之源極與淺ρ型井 282内形成之ρ型半導體區域286,係於兩者之間形成由與 閘極電極為同一層之導體膜構成之配線288b,並藉由埋入 於跨及該配線288b與nMIS 285η之源極而形成之連接孔 CNT内部之插塞電極PLG以及埋入於跨及該配線288b與ρ型 半導體區域286而形成之連接孔CNT内部之插塞電極PLG來 進行接線。 如此,例如即便於第1層配線中擔心因電漿放電引起之 帶電之情形時,由於帶電應對電路中並未使用由第1層配 線構成之配線283a、283b、283c,因此可防止帶電。 對本實施形態7之第5例之帶電應對電路進行說明。圖24 表示第5例之帶電應對電路之剖面示意圖。第5例之帶電應 對電路具有與上述第1例之帶電應對電路同樣之電路構 成,但與上述第1例之帶電應對電路之不同點在於,使用 淺η型井281上形成之電容元件CE來代替ρ型半導體區域 137166.doc -43- 200950059 284p。與上述第1例之帶電應對電路同樣,例如於製造步 驟中,當因電漿放電導致深η型井200及η型井281中蓄積有 較多正電荷時,利用電容元件CE之閘極電容,使電容元件 CE之閘極之電位與η型井28 1之電位大致相等。藉此,當對 nMIS 285η之閘極電極施加大於臨限值電壓之電位時, nMIS 285η成為導通狀態,流入深η型井200及淺η型井281 中之正電荷會經由配線283b、nMIS 285η之通道、配線 283c及ρ型半導體區域286而朝接地電位GND放電。電容元 件CE可由淺η型井281、與nMIS 285η之閘極絕緣膜為同一 層之絕緣膜、以及與nMIS 285η之閘極電極為同一層之導 體膜構成。 對本實施形態7之第6例之帶電應對電路進行說明。圖25 表示第6例之帶電應對電路之剖面示意圖。第6例之帶電應 對電路具有與上述第5例之帶電應對電路同樣之電路構 成,但與上述第5例之帶電應對電路之不同點在於,淺η型 井281上形成之電容元件CE之閘極與淺ρ型井282内形成之ρ 型半導體區域286係藉由配線287來進行接線,該配線287 係於有可能會因電漿放電而導致閘極絕緣膜產生絕緣破壞 之步驟更後之步驟中所形成。該接線較理想的是藉由最上 層之配線來進行。如此,藉由將電容元件CE之閘極固定為 接地電位GND,而於電路動作時使nMIS 285η始終為斷開 狀態,從而不會造成nMIS 28 5η向其他電路漏電等不良影 響。 對本實施形態7之第7例之帶電應對電路進行說明。圖 137166.doc • 44- 200950059 26(a)及圖26(b)分別表示第7例之帶電應對電路之剖面示意 圖及等效電路圖。第7例之帶電應對電路具有與上述第5例 之帶電應對電路同樣之電路構成,但與上述第5例之帶電 應對電路之不同點在於,電容元件CE之閘極電容Cc相對 於nMIS 285η之閘極電容Cg而設定得充分大,且nMIS 285η 之輸入電位(對閘極電極施加之電位)相對於淺η型井28 1之 電位(V(NW))可藉由耦合而追隨。 當電容元件CE之閘極電容Cc小於nMIS 285η之閘極電容 Cg時(Cc《Cg),將電容元件CE之閘極與nMIS 285η之閘極 電極接線之配線283a之電壓(V(node_x))接近接地電位 GND。相對於此,當電容元件CE之閘極電容Cc大於nMIS 285η之閘極電容Cg時(Cc》Cg),電容元件CE之閘極之電 位與η型井281之電位(V(NW))大致相等,淺η型井281之電 位(V(NW))經由配線283a而施加至nMIS 285η之閘極電極。 藉此,nMIS 285η容易成為導通狀態,從而使流入深η型井 200及淺η型井281中之正電荷經由配線283b、nMIS 285η之 通道、配線283c及ρ型半導體區域286而朝接地電位GND放 電。 對本實施形態7之第8例之帶電應對電路進行說明。圖 27(a)及圖27(b)分別表示第8例之帶電應對電路之剖面示意 圖及等效電路圖。第8例之帶電應對電路具有與上述第5例 之帶電應對電路同樣之電路構成,但與上述第5例之帶電 應對電路之不同點在於,為了補充因與電容元件CE相對向 之淺η型井281内形成之空乏層289而減少之電容元件CE之 137166.doc -45- 200950059 閘極電容Cc,而設計了將該減少量考慮在内之電容元件 CE。 即,當在與電容元件CE相對向之淺η型井281内形成空 乏層289時,由於空乏層289之電容Cx串聯連接於電容元件 CE之閘極電容Cc,因此實際之電容元件CE之閘極電容小 於根據電容元件CE之設計尺寸而獲得之閘極電容Cc。因 此,進行預先將因空乏層289之形成而導致之電容元件CE 之閘極電容Cc之減少量考慮在内之電容元件CE之設計。 對本實施形態7之第9例之帶電應對電路進行說明。圖 28(a)及圖28(b)分別表示第9例之帶電應對電路之剖面示意 圖及等效電路圖。又,29(a)及圖29(b)分別表示第9例之帶 電應對電路之變形例之剖面示意圖及等效電路圖。第9例 之帶電應對電路具有與上述第5例之帶電應對電路同樣之 電路構成,但與上述第5例之帶電應對電路之不同點在 於,為了防止因與電容元件CE相對向之淺η型井28 1内形成 之空乏層導致電容元件CE之閘極電容Cc減少,而於淺η型 井281之與電容元件CE相對向之位置上形成通道(反轉 層)。圖28表示於電容元件CE之閘極之單側側面下之η型井 281内形成有ρ型半導體區域290之帶電應對電路。圖29表 示於電容元件CE之閘極之兩側側面下之η型井28 1内形成有 ρ型半導體區域290之帶電應對電路。 即,當在與電容元件CE相對向之淺η型井281内形成空 乏層時,由於空乏層之電容串聯連接於電容元件CE之閘極 電容Cc,因此難以獲得具有相對於Nmis 285η之閘極電容 137166.doc -46- 200950059A cross-sectional view of the main part of the area of 254η. The gate electrode of the pMIS 254p formed in the shallow n-type well 251 is, for example, a structure in which a polycrystalline germanium film 503 to which a p-type impurity is added and a germanide layer 505 are laminated, and a gate of nMIS 254η formed in the shallow p-type well 252. The electrode electrode is, for example, a structure in which a polycrystalline ft w film 504 to which an n-type impurity is added and a vaporized layer 505 are laminated, and a gate electrode of the pMIS 254p and a gate electrode of the nMIS 254η are formed by a vaporization layer 505. And connected. Further, the gate electrode of the pMIS 254p and the gate electrode of the nMIS 254n are electrically connected to the shallow n-type well 251 by the first to eighth wirings M1 to Μ8. Further, the shallow p-type well 252 is formed in the p-type substrate 1 and is electrically connected to the substrate 1. (Embodiment 4) A semiconductor device having a triple well structure according to Embodiment 4 will be described with reference to Fig. 16 . Here, an example of implementing the first method for negative charging will be described. Fig. 16 is a circuit diagram showing an example of a 1/0 (input/output) circuit portion and a logic circuit portion of the circuit of the fourth embodiment which constitutes the audio image processing device of Fig. 1 described above. As shown in FIG. 16, since the shallow p type well 202 formed in the deep n-type well 200 and the shallow p type well 302 formed in the deep n type well 300 have a large area, if placed in the shallow p type well 202, 302 In the case of negative charging, the amount of charge will increase, which will easily cause insulation damage of MIS. Therefore, in order to prevent the negative p-type wells 202 and 302 from being negatively charged, an inverter circuit INV5 composed of pMIS 271p and nMIS 271η 137166.doc -35- 200950059 is formed in the deep n-type well 200, and is deep η-type well An inverter circuit 11'6 composed of pMIS 371p and 11]^118 3 7111 is formed in 300. In the inverter circuit 1]^¥5, the gate electrodes of 卩?418 271? and the gate electrodes of 111^18 27111 are processed while being connected, and the gate electrodes and the shallow n-type wells are connected. 201 is connected by the eighth layer wiring 272 (Μ8) of the uppermost layer. Similarly, in the inverter circuit INV6, the gate electrode of the pMIS 371p and the gate electrode of the nMIS 371 η are processed while being connected, and the gate electrode and the shallow n-well 301 are connected by the uppermost layer. The eighth layer wiring 3 72 (Μ8) is connected. The other wiring used to form the inverter circuit is performed by the first layer wiring. Other circuit configurations and the like are the same as in the above-described third embodiment. Next, the effects obtained by the fourth embodiment will be described. In the fourth embodiment, the gate electrode of the inverter circuit INV5 including the pMIS 271ρ and the nMIS 271n is maintained in a floating state until the step of forming the eighth layer wiring of the uppermost layer is performed, and thus The step of forming the connection hole in the interlayer insulating film on the seventh layer wiring is maintained between the shallow well 202 and the deep n well 200 via the shallow n-type well 201. As a result, the negative charge flowing into the shallow well 202 is discharged toward the substrate 1 via the shallow n-well 201 and the deep n-well 200. Similarly, the gate electrode of the inverter circuit INV6 composed of the pMIS 37 lp and the nMIS 37 In is maintained in a floating state until the step of forming the eighth layer wiring of the uppermost layer is performed, and thus is formed in the seventh The shallow p-type well 302 and the deep n-type well 300 are maintained in an ON state via the shallow n-type well 301 until the step of forming a connection hole in the interlayer insulating film on the layer wiring. The crucible flows into the shallow p-type 137166.doc -36- 200950059 The negative charge of well 3 02 is discharged toward the substrate 1 via the shallow n-type well 3 01 and the deep n-type well 300. Further, similarly to the above-described third embodiment, the positive charging of the deep n-type wells 200, 300 is also prevented. Thereby, the dielectric breakdown of the gate insulating film formed on the pMIS 203p or the nMIS 203n constituting the inverter circuit and the dielectric breakdown of the gate insulating film generated on the nMIS 308 can be suppressed. (Fifth Embodiment) A semiconductor device having a triple well structure according to the fifth embodiment will be described with reference to Figs. 17 to 19 . Here, an example of implementing the second method for positive charging will be described. Fig. 17 is a circuit diagram showing an example of a 1/〇 (input/output) circuit unit and a logic circuit unit of the audio image processing device of Fig. 1 of the fifth embodiment, and Fig. 18 is a view for explaining the application of the fifth embodiment. FIG. 19 is a cross-sectional view showing a circuit element of the MIS according to the second embodiment, and FIG. 19 is a schematic cross-sectional view showing the circuit element of the MIS according to the second embodiment. As shown in Fig. 17, in the deep n-type well 200, as in the second embodiment, the inverter circuit INV1 composed of the pMIS 254p and the nMIS 254n and the inclusive pMIS 254p are not formed, which does not contribute to the circuit operation. The n-type well 251 and the shallow p-type well 252 containing nMIS 254η. Instead of preventing the formation of the inverter circuit for charging, it is possible to prevent the application of a voltage to the gate insulating film of the pMIS 203p and the nMIS 203n constituting the inverter circuit even when the deep n-well 200 is charged, by the uppermost layer. The eighth layer wiring 3 (Μ8) is used to form the gate electrodes of the pMIS 203ρ and nMIS 203n constituting the inverter circuit and the gate of the nMIS 103!1 (the n-type semiconductor region formed in the shallow p-type well 102). connection. 137166.doc •37- 200950059 In the deep η-type well 300, the inverter circuit mv2 composed of PMIS 354ρ and nMIS 354η, the shallow n-type well 351 containing PMIS 354P, and the inner package nMls are not formed in the deep η-type well 300. Shallow p-well 352 of 354n. Further, the connection between the shallow p-well 304 and the substrate 进行 is performed by the eighth layer wiring 314 (M8) of the uppermost layer. Other circuit configurations and the like are the same as those in the first embodiment. Next, the effect obtained by the second method of the fifth embodiment will be described with reference to Fig. 18. Fig. 18 is a schematic cross-sectional view showing a state in which a semiconductor device is charged by plasma discharge in a step of forming a connection hole in an interlayer insulating film formed on a wiring of a seventh layer. In the stage of the manufacturing process (the step of forming a connection hole on the interlayer insulating film formed on the wiring of the seventh layer), the gate electrode of the pMIS 203p and the gate of the nMIS 2 311 constituting the inverter circuit The electrode electrode is not connected to the drain of the nMIS 103n located in the substrate 1, and the gate insulating film does not generate a potential difference, so that dielectric breakdown does not occur. In the other circuit components that are located in the deep n-type well and must be connected to the substrate 1, the eighth layer wiring is also used for wiring to the substrate 1, so that the insulation of the gate insulating film of MI s can be suppressed. damage. Further, in the step of forming the connection hole on the interlayer insulating film formed on the interlayer wiring of the seventh layer, the deep n-type well 2 is not connected to the substrate ^, thereby suppressing the gate of the MIS. Insulation damage of the insulating film. Further, in the step of forming the connection holes formed in the insulating film formed on the eighth layer wiring, the deep n-type well 200 has a small amount of charge, so that the MIS gate insulating film does not cause dielectric breakdown. Next, the effect of 137166.doc •38·200950059 obtained by the second method of the fifth embodiment will be described with reference to Fig. 19 . Fig. 19 is a schematic cross-sectional view showing the case where the deep n-well 300 is charged in the step of forming a connection hole in the interlayer insulating film formed on the wiring of the seventh layer. At this stage (the step of forming a connection on the interlayer insulating film formed on the wiring of the seventh layer), the shallow well 3〇4 is not connected to the substrate, so the deep η type well is entirely charged, and as a result, the whole is charged. The gate insulating film of nMIS 3G8 does not generate a potential difference, so that dielectric breakdown does not occur. In other circuit components φ, the dielectric breakdown of the MIS gate insulating film can also be suppressed. Further, in the step of forming the connection hole on the interlayer insulating film formed on the seventh layer wiring, the shallow p-type well 304 is also insulated from the substrate ,, thereby suppressing dielectric breakdown of the MIS gate insulating film . Further, similarly to the deep n-type well 2, in the step of forming the connection hole formed in the insulating film formed on the eighth layer wiring, the deep n-type well 300 has a small amount of charge, and thus the MIS gate insulating film No insulation damage will occur. Further, in the fifth embodiment, the case where the second method is applied to the connection between the gate electrode of the inverter circuit including the pMIS 2 and the φ nM1S 203n and the nMIS l〇3n is exemplified, and The connection between the shallow p-type well 304 in which nMls 3〇8 is formed and the substrate 1 is applied to the second method, but is not limited thereto. (Embodiment 6) A semiconductor device having a triple well structure according to Embodiment 6 will be described with reference to Fig. 20 . Here, another example of the first method different from the above-described embodiments 1, 2 and 3 for positive charging will be described. Fig. 20 is a circuit diagram showing an example of the I/O (input/output) electric power 137166.doc-39-200950059 road portion and logic circuit portion of the sixth embodiment which constitutes the audio image processing device of Fig. 1 described above. As shown in FIG. 20, among the PMIS 254p and the nMIS 254n constituting the inverter circuit INV1 for preventing the deep n-well 2〇〇 from being charged, the nMIS 25 is formed as the shallow P-well 252 is different from the above-described embodiment i. It is electrically connected to the shallow p-well 205 by the ith layer wiring 256 (M1). The shallow p-well 2〇5 is connected to the substrate 1 by the first layer wiring 206 (M1), so the shallow well 252 is indirectly connected to the substrate 1 via the shallow p-well 205. Further, among the pMIS 354P and nMIS 354n constituting the inverter circuit inv2 for preventing the deep n-well 300 from being charged, the shallow p-well 352 of #nMIS 354n is formed and the above embodiment! Differently, it is electrically connected to the shallow P-well 304 by the ith layer wiring 356 (mi). The shallow p-type well 3 is connected to the substrate 1 by the first layer wiring 305 (M1), so the shallow p-well 352 is indirectly connected to the substrate via the shallow p-well 408. Other circuit configurations and the like are the same as in the first embodiment described above. (Embodiment 7) A semiconductor device having a triple well structure according to Embodiment 7 will be described. In the above-described Embodiments i, 3 or 6, for example, the inverter circuit INV1 is used to cause the positive electric charge flowing into the well 2, the shallow n-well "I or the shallow P-well 202" toward the substrate due to the discharge of the plasma. In the seventh embodiment, the positive electric charge that has flowed into the deep n-type well is discharged to the substrate 1 by the inverter circuit INV2, but in the seventh embodiment, the inverter circuit can be obtained without using the inverter circuit. The charging response circuit having the same effects as those of the first, third or sixth embodiments will be described. Hereinafter, the fourth to thirteenth examples of the charging response circuit will be described. 'These examples are representative circuit configurations, of course, 137166 .doc • 40· 200950059 Various modifications can be made without departing from the spirit and scope of the invention. The charging response circuit of the first example of the seventh embodiment will be described. Fig. 21 is a schematic cross-sectional view showing the charging response circuit of the first example. A shallow n-type well 281 and a shallow p-type well 282 are formed in mutually different regions in the well 200, and an n-type semiconductor region 284n and a p-type semiconductor region 284p are formed in mutually different regions in the shallow n-type well 281. And The nMIS 285n is formed in the shallow p well 282. Further, the gate electrode of the nMIS 285η and the germanium semiconductor region 284ρ formed in the shallow n-well 281 are connected by the wiring 283a, and the nMIS w 285η has a drain and a shallow n-type. The n-type semiconductor region 284n formed in the well 281 is wired by the wiring 283b, and the source of the nMIS 285n is connected to the ground potential GND via the wiring 283c via the p-type semiconductor region 286 formed in the shallow p-well 282. The first wiring is used for the wirings 283a, 283b, and 283c. The charging response circuit of the first example is formed by the n-type semiconductor region 284n and the p-type semiconductor region 284p formed in the shallow n-well 281, and the shallow p-well. The nMIS 285 η formed in 282 does not have any effect in the circuit operation of the semiconductor device. For example, in the manufacturing step, when the plasma is discharged, the deep n-well 200 and the shallow n-well 281 are accumulated. When a large amount of positive charge is applied, the potential of the p-type semiconductor region 284p is substantially equal to the potential of the shallow n-type well 281 by the pn junction capacitance, etc., thereby applying a greater than the gate electrode of the nMIS 285n. Limit voltage potential When the nMIS 285 η is turned on, the positive charges flowing into the deep n-type well 200 and the shallow n-type well 281 are discharged to the ground potential GND via the wiring 283b, the nMIS 285n channel, the wiring 283c, and the p-type semiconductor region 286. The charging response circuit of the second example of 7 is explained. Fig. 22 137166.doc • 41 · 200950059 shows the schematic diagram of the charging circuit of the second example. The charging response circuit of the second example has the same circuit configuration as the charging response circuit of the first example, but differs from the charging response circuit of the first example in that the p-type semiconductor region 284p formed in the shallow n-well 281 The p-type semiconductor region 286 formed in the shallow p-type well 282 is wired by a wiring 287 which is a step subsequent to a step which may cause dielectric breakdown of the gate insulating film due to plasma discharge. Formed in the middle. This wiring is preferably carried out by wiring of the uppermost layer. By fixing the p-type semiconductor region 284p to the ground potential GND, the nMIS 285n is always turned off during the circuit operation of the semiconductor device, and the nMIS 285n is not adversely affected by leakage of other circuits. The charging response circuit of the third example of the seventh embodiment will be described. The charging response circuit of the third example has the same circuit configuration as that of the charging and discharging circuit of the first or second example described above, and the thickness of the gate insulating film of the nMIS 285n is set to a thickness of 1 〇 nm or more. For example, the thickness of the gate insulating film of the MISFET formed on the 1/0 (input/output) circuit portion may be the same. By forming the gate insulating film of the nMIS 285n to be thick, the leakage can be reduced and the operation can be reliably performed. The charging response circuit of the fourth example of the seventh embodiment will be described. 23(a) and 23(b) are a plan view and a cross-sectional view, respectively, of the charging response circuit of the fourth example. The charging response circuit of the fourth example has the same circuit configuration as the charging response circuit of the first example, but differs from the charging response circuit of the first example in that the wiring is not used for the wirings 283a, 283b, and 283c. A wiring formed of a conductor film 137166.doc • 42- 200950059 (for example, a laminated film of a polysilicon film and a germanide layer) in the same layer as the common contact and the gate electrode. That is, the gate electrode of the nMIS 285n and the p-type semiconductor region 284p formed in the shallow n-type well 281 are wired by the plug electrode PLG embedded in the connection hole CNT formed across the both. Further, the n-type semiconductor region 284n formed in the drain of the nMIS 28 5n and the shallow n-type well 281 forms a wiring 288a composed of a conductor film having the same layer as the gate electrode, and is buried by a plug electrode PLG that is inserted into the connection hole CNT formed between the drains of the wiring 288a and the nMIS 285n, and a plug that is buried inside the connection hole CNT formed between the wiring 288a and the n-type semiconductor region 284n. The electrode PLG is used for wiring. Further, the source of the nMIS 285η and the p-type semiconductor region 286 formed in the shallow p-type well 282 form a wiring 288b composed of a conductor film of the same layer as the gate electrode, and is buried therein. a plug electrode PLG inside the connection hole CNT formed across the source of the wiring 288b and the nMIS 285n, and a plug electrode buried inside the connection hole CNT formed across the wiring 288b and the p-type semiconductor region 286 PLG to wire. As described above, for example, even when the charging of the first layer wiring is caused by the plasma discharge, the wiring 283a, 283b, and 283c composed of the first layer wiring are not used in the charging countermeasure circuit, so that charging can be prevented. The charging response circuit of the fifth example of the seventh embodiment will be described. Fig. 24 is a cross-sectional view showing the charging circuit of the fifth example. The charging response circuit of the fifth example has the same circuit configuration as the charging response circuit of the first example, but differs from the charging response circuit of the first example in that the capacitive element CE formed on the shallow n-well 281 is used. Instead of the p-type semiconductor region 137166.doc -43- 200950059 284p. Similarly to the charging response circuit of the first example described above, for example, in the manufacturing step, when a large amount of positive charges are accumulated in the deep n-type well 200 and the n-type well 281 due to plasma discharge, the gate capacitance of the capacitive element CE is utilized. The potential of the gate of the capacitive element CE is substantially equal to the potential of the n-type well 28 1 . Thereby, when a potential greater than the threshold voltage is applied to the gate electrode of the nMIS 285η, the nMIS 285η is turned on, and the positive charges flowing into the deep n-well 200 and the shallow n-well 281 pass through the wiring 283b, nMIS 285η. The channel, the wiring 283c, and the p-type semiconductor region 286 are discharged toward the ground potential GND. The capacitor element CE can be composed of a shallow n-type well 281, an insulating film of the same layer as the gate insulating film of the nMIS 285n, and a conductor film of the same layer as the gate electrode of the nMIS 285n. The charging response circuit of the sixth example of the seventh embodiment will be described. Fig. 25 is a cross-sectional view showing the charging circuit of the sixth example. The charging response circuit of the sixth example has the same circuit configuration as the charging response circuit of the fifth example, but differs from the charging response circuit of the fifth example described above in the gate of the capacitive element CE formed on the shallow n-well 281. The p-type semiconductor region 286 formed in the pole and shallow p-well 282 is wired by a wiring 287 which is followed by a step which may cause dielectric breakdown of the gate insulating film due to plasma discharge. Formed in the steps. This wiring is preferably carried out by wiring of the uppermost layer. As described above, by fixing the gate of the capacitor element CE to the ground potential GND, the nMIS 285n is always turned off during the operation of the circuit, so that the nMIS 28 5n does not cause an adverse effect such as leakage of other circuits. The charging countermeasure circuit of the seventh example of the seventh embodiment will be described. Figure 137166.doc • 44- 200950059 26(a) and 26(b) respectively show a schematic cross-sectional view and an equivalent circuit diagram of the charged response circuit of the seventh example. The charging circuit of the seventh example has the same circuit configuration as the charging circuit of the fifth example, but differs from the charging circuit of the fifth example in that the gate capacitance Cc of the capacitive element CE is relative to the nMIS 285η. The gate capacitance Cg is set sufficiently large, and the input potential of the nMIS 285η (the potential applied to the gate electrode) can be followed by the coupling with respect to the potential (V(NW)) of the shallow n-well 28 1 . When the gate capacitance Cc of the capacitive element CE is smaller than the gate capacitance Cg of nMIS 285η (Cc "Cg", the voltage of the wiring 283a of the gate of the capacitive element CE and the gate electrode of the nMIS 285η (V(node_x)) Close to the ground potential GND. On the other hand, when the gate capacitance Cc of the capacitance element CE is larger than the gate capacitance Cg of the nMIS 285η (Cc "Cg), the potential of the gate of the capacitance element CE and the potential of the n-type well 281 (V(NW)) are substantially Equally, the potential of the shallow n-type well 281 (V(NW)) is applied to the gate electrode of the nMIS 285n via the wiring 283a. Thereby, the nMIS 285 η is easily turned on, and the positive charges flowing into the deep n-type well 200 and the shallow n-type well 281 are directed to the ground potential GND via the wiring of the wiring 283b, the nMIS 285n, the wiring 283c, and the p-type semiconductor region 286. Discharge. The charging response circuit of the eighth example of the seventh embodiment will be described. 27(a) and 27(b) are respectively a cross-sectional schematic view and an equivalent circuit diagram of the charging response circuit of the eighth example. The charging response circuit of the eighth example has the same circuit configuration as the charging response circuit of the fifth example, but differs from the charging response circuit of the fifth example described above in that it is complementary to the shallow n-type opposite to the capacitive element CE. The vacant layer 289 formed in the well 281 is reduced by the 137166.doc -45-200950059 gate capacitance Cc of the capacitive element CE, and the capacitive element CE in which the reduction is taken into account is designed. That is, when the depletion layer 289 is formed in the shallow n-well 281 opposite to the capacitance element CE, since the capacitance Cx of the depletion layer 289 is connected in series to the gate capacitance Cc of the capacitance element CE, the gate of the actual capacitance element CE is The pole capacitance is smaller than the gate capacitance Cc obtained according to the design size of the capacitive element CE. Therefore, the design of the capacitive element CE in which the amount of decrease in the gate capacitance Cc of the capacitive element CE due to the formation of the depletion layer 289 is taken into consideration is performed. The charging response circuit of the ninth example of the seventh embodiment will be described. 28(a) and 28(b) are respectively a cross-sectional schematic view and an equivalent circuit diagram of the charging response circuit of the ninth example. Further, 29(a) and 29(b) are respectively a schematic cross-sectional view and an equivalent circuit diagram showing a modification of the charging circuit of the ninth example. The charging response circuit of the ninth example has the same circuit configuration as the charging response circuit of the fifth example, but differs from the charging response circuit of the fifth example in that it is prevented from being shallow n-type with respect to the capacitive element CE. The depletion layer formed in the well 28 1 causes the gate capacitance Cc of the capacitive element CE to decrease, and a channel (inversion layer) is formed at a position opposite to the capacitive element CE at the shallow n-type well 281. Fig. 28 shows a charging countermeasure circuit in which a p-type semiconductor region 290 is formed in the n-type well 281 under the one side surface of the gate of the capacitor element CE. Fig. 29 shows a charging countermeasure circuit in which a p-type semiconductor region 290 is formed in the n-type well 28 1 under the side faces on both sides of the gate of the capacitor element CE. That is, when the depletion layer is formed in the shallow n-well 281 opposite to the capacitance element CE, since the capacitance of the depletion layer is connected in series to the gate capacitance Cc of the capacitance element CE, it is difficult to obtain a gate having a threshold of Nmis 285η. Capacitor 137166.doc -46- 200950059
Cg為充分大之閘極電容Cc之電容元件CE。因此,為防止 上述空乏層之形成,預先於淺η型井281之與電容元件CE相 對向之位置上形成通道(反轉層),從而防止因空乏層之形 成而導致之電容元件CE之閘極電容Cc之減少。 對本實施形態7之第10例之帶電應對電路進行說明。圖 30(a)及圖30(b)分別表示第10例之帶電應對電路之剖面示 意圖及等效電路圖。第10例之帶電應對電路具有與上述第 1例之帶電應對電路同樣之電路構成,但與上述第1例之帶 電應對電路之不同點在於,p型半導體區域284p之接面電 容Cj相對於nMIS 285η之閘極電容Cg而設計得充分大,且 nMIS 285η之輸入電位(對閘極電極施加之電位)相對於淺η 型井281之電位(V(NW))可藉由耦合而追隨。 當p型半導體區域284p之接面電容Cj大於Nmis 285η之閘 極電容Cg時(Cj》Cg),電容元件CE之閘極之電位與η型井 281之電位(V(NW))大致相等,淺η型井281之電位(V(NW)) 經由配線283a而被施加至Nmis 285η之閘極電極。藉此, nMIS 285η容易成為導通狀態,從而使流入深η型井200及 淺η型井281中之正電荷經由配線283b、nMIS 285η之通道、 配線283 c及ρ型半導體區域286而朝接地電位GND放電。 對本實施形態7之第11例之帶電應對電路進行說明。圖 3 1表示第11例之帶電應對電路之剖面示意圖。第11例之帶 電應對電路係於深η型井200内之彼此不同之區域中形成有 淺η型井281與淺ρ型井282,並於淺ρ型井282内形成有nMIS 285η,但於淺η型井281内僅形成有η型半導體區域284η。 137166.doc •47· 200950059 又,nMIS 28511之汲極與淺η型井281内形成之η型半導體區 域284η藉由配線283b而接線,nMIS 28 5η之源極藉由配線 283c並經由淺ρ型井282内形成之ρ型半導體區域286而連接 於接地電位GND,於nMIS 285η之閘極電極上連接有浮動 狀態之配線291。 當nMIS 285η根據浮動狀態之配線291之中間電位而成為 導通狀態時,流入深η型井200及淺η型井281中之正電荷會 經由配線283b、nMIS 285η之通道、配線283c及ρ型半導體 區域286而朝接地電位GND放電。配線29 1於有可能會因電 漿放電而導致閘極絕緣膜產生絕緣破壞之步驟更後之步驟 中,施加使nMIS 285η成為斷開狀態之電位,從而不會造 成nMIS 285η向其他電路漏電等不良影響。 對本實施形態7之第12例之帶電應對電路進行說明。圖 32表示第12例之帶電應對電路之剖面示意圖。第12例之帶 電應對電路具有與上述第11例之帶電應對電路同樣之電路 構成,但與上述第11例之帶電應對電路之不同點在於, nMIS 285η之閘極電極與淺ρ型井282内形成之ρ型半導體區 域286係藉由配線292來進行接線,該配線292係於有可能 會因電漿放電而導致閘極絕緣膜產生絕緣破壞之步驟更後 之步驟中所形成。該接線較理想的是藉由最上層之配線來 進行。如此,藉由將nMIS 285η之閘極電極固定為接地電 位GND,而於半導體裝置之電路動作時使nMIS 285η始終 為斷開狀態,從而不會造成nMIS 285η向其他電路漏電等 不良影響。 137166.doc -48· 200950059 對本實施形態7之第j 3例册 例之贡電應對電路進行說明。上 述第1例〜第12例之帶電岸對雷 愿野電路係以深η型井200内產生之 f電為對象之應對電路,.死 仁以冰p型井内產生之帶電為對 象之應對電路亦可藉由將栢柯 田將極性反轉而同樣地形成。即,上Cg is a capacitive element CE of a sufficiently large gate capacitance Cc. Therefore, in order to prevent the formation of the depletion layer, a channel (inversion layer) is formed in advance with respect to the position of the shallow n-type well 281 opposite to the capacitive element CE, thereby preventing the gate of the capacitive element CE due to the formation of the depletion layer. The reduction of the pole capacitance Cc. The charging response circuit of the tenth example of the seventh embodiment will be described. 30(a) and 30(b) are cross-sectional views and equivalent circuit diagrams of the charging response circuit of the tenth example, respectively. The charging response circuit of the tenth example has the same circuit configuration as the charging response circuit of the first example, but differs from the charging response circuit of the first example in that the junction capacitance Cj of the p-type semiconductor region 284p is relative to the nMIS. The gate capacitance Cg of 285η is designed to be sufficiently large, and the input potential of nMIS 285η (the potential applied to the gate electrode) can be followed by the coupling with respect to the potential (V(NW)) of the shallow n-type well 281. When the junction capacitance Cj of the p-type semiconductor region 284p is larger than the gate capacitance Cg of Nmis 285η (Cj"Cg), the potential of the gate of the capacitive element CE is substantially equal to the potential of the n-type well 281 (V(NW)). The potential (V(NW)) of the shallow n-well 281 is applied to the gate electrode of Nmis 285n via wiring 283a. Thereby, the nMIS 285η is easily turned on, and the positive charges flowing into the deep n-type well 200 and the shallow n-type well 281 are directed to the ground potential via the wiring of the wiring 283b, the nMIS 285n, the wiring 283c, and the p-type semiconductor region 286. GND discharge. The charging response circuit of the eleventh example of the seventh embodiment will be described. Fig. 3 is a schematic cross-sectional view showing the charging response circuit of the eleventh example. The charged response circuit of the eleventh example is formed by a shallow n-type well 281 and a shallow p-type well 282 in a different region of the deep n-type well 200, and nMIS 285η is formed in the shallow p-type well 282, but Only the n-type semiconductor region 284n is formed in the shallow n-well 281. 137166.doc •47· 200950059 Further, the n-type semiconductor region 284η formed in the drain of the nMIS 28511 and the shallow n-type well 281 is connected by the wiring 283b, and the source of the nMIS 28 5n is connected via the wiring 283c via the shallow p-type The p-type semiconductor region 286 formed in the well 282 is connected to the ground potential GND, and a floating wiring 291 is connected to the gate electrode of the nMIS 285n. When the nMIS 285η is turned on according to the intermediate potential of the wiring 291 in the floating state, the positive charges flowing into the deep n-well 200 and the shallow n-well 281 pass through the wiring of the wiring 283b, the nMIS 285n, the wiring 283c, and the p-type semiconductor. The region 286 is discharged toward the ground potential GND. In the step of the wiring 29 1 which may cause dielectric breakdown of the gate insulating film due to plasma discharge, the potential for turning off the nMIS 285η is applied, so that the nMIS 285η does not leak to other circuits, etc. Bad effects. The charging response circuit of the twelfth example of the seventh embodiment will be described. Figure 32 is a cross-sectional view showing the charging response circuit of the twelfth example. The charging response circuit of the twelfth example has the same circuit configuration as the charging response circuit of the eleventh example, but differs from the charging response circuit of the eleventh example in that the gate electrode of the nMIS 285n and the shallow p-well 282 are The formed p-type semiconductor region 286 is wired by a wiring 292 which is formed in a step subsequent to the step of causing dielectric breakdown of the gate insulating film due to plasma discharge. This wiring is preferably carried out by the wiring of the uppermost layer. By fixing the gate electrode of the nMIS 285n to the ground potential GND, the nMIS 285η is always turned off during the operation of the circuit of the semiconductor device, and the nMIS 285η is not adversely affected by leakage to other circuits. 137166.doc -48· 200950059 The power supply circuit of the j3th example of the seventh embodiment will be described. The charging ground of the first to the twelfth examples is a response circuit for the electric power generated in the deep n-type well 200, and the response circuit for the dead body generated by the ice p-type well is also It can be formed in the same manner by inverting the polarity of the cypress. That is, on
述第!例〜第12例之帶電應對電路中,係於深p型井細内之 彼此不同之區域中形成淺n型井281與淺p型井-,於淺p 型井以2内形成消除井間電位差之—285n,並將淺n型 井281作為帶電應對用井’但於第Π例之帶電應對電路 中’係於深η型井内之彼此不同之區域中形成淺ρ型井與淺 η型井’於淺η型井内形成消除井間電位差之pms,並將淺 P型井作為帶電應對用井。 再者,於說明上述第!不良產生機構時,記載有「由基 板1上形成之淺η型井101内形成之pMIS(未圖示)與淺p型井 1〇2内形成之nMIS(未圖示)構成之反相器電路」,具體而言 係指如下所述之反相器電路。 圖33表示上述反相器電路之剖面示意圖。於基板1之彼 此不同之區域中形成有淺n型井1〇1與淺p型井丨〇2,進而於 淺η型井1〇1内形成有pMIS,於淺ρ型井1〇2内形成有 nMIS。由該等PMIS及nMIS形成反相器電路,pMIS之閘極 電極與nMIS之閘極電極彼此接線並處於浮動狀態。 以上’根據實施形態具體說明了由本發明者所研發之發 明,但本發明並不限定於上述實施形態,於不脫離其主旨 之範圍内當可實施各種變更。 [產業上之可利用性] 137166.doc -49- 200950059 本發明可適用於例如通用soc產品所採用之具有三重井 構造之半導體裝置中所應用之有效技術。 【圖式簡單說明】 圖1係本發明者等人用於分析之聲音圖像處理裝置之 成圖; 圖2係表示構成圖!之聲音圖像處理裝置之ι/〇(輸入輸出) 電路部及邏輯電路部之一例之電路圖; 圖3係用於說明深井中蓄積有正電荷時之第丨不良產生機 構之電路元件之剖面示意圖; 圖4(a)及圖4(b)係用於說明反相器電路中之電荷流動之 示意圖; 圖5係用於說明深井中蓄積有正電荷時之第2不良產生機 構之電路元件之剖面示意圖; 圖6係表示構成圖1之聲音圖像處理裝置之1/〇(輸入輸出) 電路部及邏輯電路部之其他例之電路圖; 圖7係用於說明形成於深井内且具有與基板相同之導電 性之淺井中蓄積有負電荷時之第3不良產生機構之電路元 件之剖面示意圖; 圖8係用於說明形成於深井内且具有與基板相同之導電 性之淺井中蓄積有負電荷時之第4不良產生機構之電路元 件之剖面示意圖; 圖9係表示實施形態1之構成聲音圖像處理裝置之1/〇(輸 入輸出)電路部及邏輯電路部之一例之電路圖; 圖10係本實施形態1之包含構成適用第1方法之反相器電 137166.doc -50- 200950059 路之pMIS及nMIS之區域之主要部分剖面圖; 圖11係用於說明本實施形態1之適用第1方法之反相器電 路之電路元件之剖面示意圖; 圖12係用於說明本實施形態1之適用第1方法之MIS之電 路元件之剖面示意圖; •圖13係表示實施形態2之構成聲音圖像處理裝置之 1/〇(輸入輸出)電路部及邏輯電路部之一例之電路圖; 圖14係表示實施形態3之構成聲音圖像處理裝置之 響 1/〇(輸入輸出)電路部及邏輯電路部之一例之電路圖; 圖15係本實施形態3之包含構成適用第1方法之反相器電 路之pMIS及nMIS之區域之主要部分剖面圖; 圖16係表示實施形態4之構成聲音圖像處理裝置之 1/◦(輸入輸出)電路部及邏輯電路部之一例之電路圖; 圖17係表示實施形態5之構成聲音圖像處理裝置之 1/〇(輸入輸出)電路部及邏輯電路部之一例之電路圖; φ 圖18係用於說明本實施形態5之適用第2方法之反相器電 路之電路元件之剖面示意圖; 圖19係用於說明本實施形態5之適用第2方法之MIS之電 • 路元件之剖面示意圖; 圖20係表示實施形態6之構成聲音圖像處理裝置之 1/0(輸入輸出)電路部及邏輯電路部之一例之電路圖; 圖21係實施形態7之第1例之帶電應對電路之剖面示意 圖; 圖22係實施形態7之第2例之帶電應對電路之剖面示意 137166.doc -51· 200950059Said the first! In the charging response circuit of the example to the twelfth example, shallow n-type wells 281 and shallow p-type wells are formed in different regions of the deep p-type wells, and the shallow p-type wells are formed in 2 to eliminate the interwells. The potential difference is -285n, and the shallow n-type well 281 is used as the charging response well', but in the charged response circuit of the third example, the shallow p-type well and the shallow n-type are formed in different regions of the deep η-type well. The well 'in the shallow n-type well forms a pms that eliminates the potential difference between wells, and the shallow P-type well is used as a charging response well. Furthermore, to explain the above! In the case of a defective generation mechanism, an inverter composed of a pMIS (not shown) formed in the shallow n-type well 101 formed on the substrate 1 and an nMIS (not shown) formed in the shallow p-type well 1〇2 is described. The circuit, in particular, refers to an inverter circuit as described below. Figure 33 is a cross-sectional view showing the inverter circuit. Shallow n-type wells 1〇1 and shallow p-type wells 2 are formed in different regions of the substrate 1, and pMIS is formed in the shallow n-type well 1〇1, and is in the shallow p-type well 1〇2 Formed with nMIS. An inverter circuit is formed by the PMIS and nMIS, and the gate electrode of the pMIS and the gate electrode of the nMIS are connected to each other and are in a floating state. The invention has been described in detail with reference to the embodiments, and the invention is not limited thereto, and various modifications can be made without departing from the spirit and scope of the invention. [Industrial Applicability] 137166.doc -49- 200950059 The present invention is applicable to, for example, an effective technique applied to a semiconductor device having a triple well structure employed in a general-purpose soc product. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a diagram of a sound image processing apparatus used by the inventors of the present invention for analysis; Fig. 2 is a diagram showing the composition! A circuit diagram of an example of a circuit portion and a logic circuit portion of the audio image processing device; FIG. 3 is a schematic cross-sectional view showing a circuit component of a third defect generating mechanism when a positive charge is accumulated in a deep well; 4(a) and 4(b) are diagrams for explaining the flow of charges in the inverter circuit; FIG. 5 is a circuit element for explaining the second defective generation mechanism when a positive charge is accumulated in the deep well. FIG. 6 is a circuit diagram showing another example of a 1/〇 (input/output) circuit unit and a logic circuit unit constituting the audio image processing apparatus of FIG. 1. FIG. 7 is a view for explaining that it is formed in a deep well and has a substrate. A schematic cross-sectional view of a circuit element of a third defect generating mechanism in which a negative charge is accumulated in a shallow well of the same conductivity; FIG. 8 is a view showing a negative charge accumulated in a shallow well formed in a deep well and having the same conductivity as the substrate FIG. 9 is a cross-sectional view showing a circuit component of the fourth defect generating means in the first embodiment; FIG. 9 is a view showing one of the 1/〇 (input/output) circuit unit and the logic circuit unit of the audio image processing device according to the first embodiment. Fig. 10 is a cross-sectional view showing a principal part of a region including the pMIS and nMIS constituting the inverter 137166.doc-50-200950059 of the first embodiment. Fig. 11 is a view for explaining the present invention. FIG. 12 is a schematic cross-sectional view showing a circuit element of the MIS to which the first method is applied according to the first embodiment; FIG. 12 is a cross-sectional view showing the circuit element of the MIS according to the first embodiment; Fig. 14 is a circuit diagram showing an example of a 1/〇 (input/output) circuit unit and a logic circuit unit of the audio image processing device of the second embodiment; Fig. 14 is a diagram showing the response of the audio image processing device of the third embodiment. FIG. 15 is a cross-sectional view showing a principal part of a region including a pMIS and an nMIS which constitute an inverter circuit to which the first method is applied, and FIG. 15 is a cross-sectional view showing a portion of a circuit portion and a logic circuit portion of the inverter circuit according to the third embodiment; A circuit diagram of an example of a 1/◦ (input/output) circuit unit and a logic circuit unit of the audio image processing device; FIG. 17 shows a 1/〇 (input) of the audio image processing device of the fifth embodiment. FIG. 18 is a schematic cross-sectional view showing a circuit element of an inverter circuit to which the second method is applied in the fifth embodiment; FIG. 19 is a view for explaining the present embodiment. FIG. 20 is a circuit diagram showing an example of a 1/0 (input/output) circuit unit and a logic circuit unit of the audio image processing device according to the sixth embodiment; Figure 21 is a cross-sectional view showing a charging response circuit according to a first example of the seventh embodiment; and Figure 22 is a cross-sectional view showing a charging response circuit of a second example of the seventh embodiment. 137166.doc -51· 200950059
電應對 面示专 面示音Electric response
圖23(a)及圖23(b)分別係實施形態7之第4例之帶 電路之平面示意圖及剖面示意圖; 圖24係實施形態7之第5例之帶電應對電路之剖 圖; 圖25係實施形態7之第6例之帶電應對電路之剖 圖; 圖26(a)及圖26(b)分別係實施形態7之第7例之帶 電路之剖面示意圖及等效電路圖;23(a) and 23(b) are a plan view and a cross-sectional view, respectively, of a circuit with a fourth example of the seventh embodiment; and FIG. 24 is a cross-sectional view of the charging circuit of the fifth example of the seventh embodiment; FIG. 26(a) and FIG. 26(b) are respectively a schematic cross-sectional view and an equivalent circuit diagram of a circuit with a seventh example of the seventh embodiment;
圖27(a)及圖27(b)分別係實施形態7之第8例之帶·番 電路之剖面示意圖及等效電路圖; 圖28(a)及圖28(b)分別係實施形態7之第9例之*赴 罨應對 電路之剖面示意圖及等效電路圖; 圖29(a)及圖29(b)分別係實施形態7之第9例之 电應對 電路之其他剖面示意圖及等效電路圖;27(a) and 27(b) are respectively a cross-sectional view and an equivalent circuit diagram of a tape circuit of an eighth example of the seventh embodiment; and Figs. 28(a) and 28(b) are respectively a seventh embodiment. FIG. 29(a) and FIG. 29(b) are respectively a schematic cross-sectional view and an equivalent circuit diagram of the electrical response circuit of the ninth example of the seventh embodiment;
圖30(a)及圖30(b)分別係實施形態7之第〗〇例之帶電應對 電路之剖面示意圖及等效電路圖; 圖31係實施形態7之第u例之帶電應對電路之 圖; 思 圖32係實施形態7之第12例之帶電應對電路之剖面示音 圖;及 心 圖33係用於說明淺n型井與淺㈣井之導 電路之剖面示意圖。 【主要元件符號說明】 137l66.doc -52· 200950059 1 基板 2 ' 3 配線 101 淺η型井 102 淺Ρ型井 103η η通道型MIS_FET 1〇3ρ ρ通道型MIS_FET 200 深n型井 201 淺η型井 w 202 淺ρ型井 203η η通道型MIS_FET 203ρ ρ通道型MIS_FET 204 淺η型井 205 淺Ρ型井 206 配線 207η η通道型MIS‘FET 〇 207Ρ ρ通道型MIS_FET 208 > 209 配線 251 淺η型井 . 252 淺ρ型井 253 配線 254η η通道型MIS_FET 254ρ ρ通道型MIS_FET 255 ' 256 配線 271η η通道型MIS_FET 137166.doc -53 -30(a) and 30(b) are respectively a schematic cross-sectional view and an equivalent circuit diagram of a charging countermeasure circuit according to a seventh embodiment of the present invention; and FIG. 31 is a diagram showing a charging response circuit of a fifth example of the seventh embodiment; Figure 32 is a cross-sectional sound map of the charging response circuit of the twelfth example of the seventh embodiment; and the heart chart 33 is a schematic cross-sectional view for explaining the guiding circuits of the shallow n-type well and the shallow (four) well. [Main component symbol description] 137l66.doc -52· 200950059 1 Substrate 2 ' 3 Wiring 101 shallow n-well 102 shallow well 103 η channel type MIS_FET 1〇3ρ ρ channel type MIS_FET 200 deep n-well 201 shallow n-type Well w 202 shallow p type well 203η n channel type MIS_FET 203ρ ρ channel type MIS_FET 204 shallow n type well 205 shallow well type 206 wiring 207η n channel type MIS'FET 〇207Ρ ρ channel type MIS_FET 208 > 209 wiring 251 shallow η Well. 252 Shallow p type well 253 Wiring 254η η channel type MIS_FET 254ρ ρ channel type MIS_FET 255 ' 256 wiring 271η n channel type MIS_FET 137166.doc -53 -
200950059 271ρ p通道型MIS FET 272 配線 281 淺n型井 282 淺p型井 283a、283b、283c 配線 284η η型半導體區域 284p ρ型半導體區域 285η η通道型MIS FET 286 ρ型半導體區域 287 配線 288a、288b 配線 289 空乏層 290 P型半導體區域 291 、 292 配線 300 深η型井 301 淺η型井 302 淺ρ型井 303 淺η型井 304 淺Ρ型井 305 配線 306n η通道型MIS_FET 306p ρ通道型MIS‘FET 307n η通道型MIS‘FET 307p ρ通道型MIS'FET 137166.doc ·54- 200950059 參 ⑩ 308 n通道型MIS_FET 309η n通道型MIS_FET 309ρ p通道型MISTET 310、 311 、 312 、 配線 313 ' 314 351 淺n型井 352 淺p型井 353 配線 354η η通道型MIS_FET 354ρ p通道型MIS_FET 355 ' 356 配線 371η n通道型MIS_FET 371ρ p通道型MIS_FET 372 配線 503、 504 多晶矽膜(閘極電極) 505 矽化物層 C 電容 Cc 閘極電容 CE 電容元件 Cg 閘極電容 Cj 接面電容 CNT 連接孔 D 汲極 G 閘極電極 137166.doc -55- 200950059200950059 271ρ p-channel type MIS FET 272 wiring 281 shallow n-well 282 shallow p-well 283a, 283b, 283c wiring 284n n-type semiconductor region 284p p-type semiconductor region 285n n-channel type MIS FET 286 p-type semiconductor region 287 wiring 288a, 288b Wiring 289 Depletion layer 290 P-type semiconductor region 291, 292 Wiring 300 Deep η-type well 301 Shallow η-type well 302 Shallow-p-type well 303 Shallow η-type well 304 Shallow-type well 305 Wiring 306n η-channel type MIS_FET 306p ρ-channel type MIS'FET 307n n-channel type MIS'FET 307p ρ channel type MIS'FET 137166.doc ·54- 200950059 1010 308 n channel type MIS_FET 309η n channel type MIS_FET 309ρ p channel type MISTET 310, 311, 312, wiring 313 ' 314 351 shallow n-well 352 shallow p-type well 353 wiring 354η n-channel type MIS_FET 354ρ p-channel type MIS_FET 355 ' 356 wiring 371η n-channel type MIS_FET 371ρ p-channel type MIS_FET 372 wiring 503, 504 polysilicon film (gate electrode) 505 Telluride layer C capacitor Cc gate capacitance CE capacitance element Cg gate capacitance Cj junction capacitor CNT connection hole D bungee G gate electrode 137166.doc -55- 200950059
GNDGND
INV1、INV2、INV3、 INV4、INV5、INV6 IO LSIINV1, INV2, INV3, INV4, INV5, INV6 IO LSI
Ml、M2、M3、M4、 M5、M6、M7、M8 n-well p-sub p-wellMl, M2, M3, M4, M5, M6, M7, M8 n-well p-sub p-well
PLGPLG
S 接地電位 反相器電路 I/O電路部 聲音圖像處理裝置 配線 η型井 基板 Ρ型井 插塞電極 源極 137166.doc -56-S Ground potential Inverter circuit I/O circuit part Sound image processing device Wiring η type well Substrate Ρ type well Plug electrode source 137166.doc -56-
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| JP2008006436 | 2008-01-16 | ||
| JP2008311085A JP2009194369A (en) | 2008-01-16 | 2008-12-05 | Semiconductor device |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| TWI513011B (en) * | 2011-07-06 | 2015-12-11 | United Microelectronics Corp | Differential varactor device |
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| JP4743917B2 (en) | 2009-08-25 | 2011-08-10 | Necシステムテクノロジー株式会社 | Optical unit |
| JP5868682B2 (en) * | 2011-12-01 | 2016-02-24 | 株式会社ソシオネクスト | Semiconductor device |
| JP6776192B2 (en) | 2017-06-28 | 2020-10-28 | ルネサスエレクトロニクス株式会社 | Semiconductor devices and their manufacturing methods |
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2008
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| Publication number | Priority date | Publication date | Assignee | Title |
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| TWI513011B (en) * | 2011-07-06 | 2015-12-11 | United Microelectronics Corp | Differential varactor device |
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