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JPS6223459B2 - - Google Patents
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JPS6223459B2 - - Google Patents

Info

Publication number
JPS6223459B2
JPS6223459B2 JP54048232A JP4823279A JPS6223459B2 JP S6223459 B2 JPS6223459 B2 JP S6223459B2 JP 54048232 A JP54048232 A JP 54048232A JP 4823279 A JP4823279 A JP 4823279A JP S6223459 B2 JPS6223459 B2 JP S6223459B2
Authority
JP
Japan
Prior art keywords
region
semiconductor
connection body
insulating film
electric field
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP54048232A
Other languages
Japanese (ja)
Other versions
JPS55140246A (en
Inventor
Teruo Kusaka
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Corp
Original Assignee
Nippon Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP4823279A priority Critical patent/JPS55140246A/en
Publication of JPS55140246A publication Critical patent/JPS55140246A/en
Publication of JPS6223459B2 publication Critical patent/JPS6223459B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D64/00Electrodes of devices having potential barriers
    • H10D64/111Field plates

Landscapes

  • Internal Circuitry In Semiconductor Integrated Circuit Devices (AREA)
  • Electrodes Of Semiconductors (AREA)

Description

【発明の詳細な説明】 本発明は半導体装置に係り、特に高耐圧半導体
集積回路の回路の回路構成素子の性能を損うこと
なく、Al配線等の回路接続体を形成し得る構造
に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a semiconductor device, and particularly to a structure in which circuit connections such as Al wiring can be formed without impairing the performance of circuit components of a high-voltage semiconductor integrated circuit.

半導体集積回路は、回路素子を互いに素子間分
離することと、所定の回路構成にAl配線等によ
り接続することよりなる。上記Al配線等の接続
体の形成は、基本的には回路素子主表面を被覆す
る絶縁膜上に金属薄膜配線を形成して行うのが通
常である。その場合、バルク結晶と該接続体の電
位関係により、しばしば、バルク結晶表面に反転
層を形成し、それが電流チヤネルとなり、寄生電
流リークを発生することが多かつた。このような
問題は、特にバルク結晶濃度が全般に低い高耐圧
半導体集積回路において顕著である。
A semiconductor integrated circuit consists of separating circuit elements from each other and connecting them to a predetermined circuit configuration using Al wiring or the like. The connection body such as the Al wiring is basically formed by forming a metal thin film wiring on an insulating film covering the main surface of the circuit element. In that case, an inversion layer is often formed on the surface of the bulk crystal due to the potential relationship between the bulk crystal and the connection body, which often becomes a current channel and causes parasitic current leakage. Such problems are particularly noticeable in high-voltage semiconductor integrated circuits in which the bulk crystal concentration is generally low.

従来、上記表面の寄生電流リークの防止法とし
て第1図に示すように反転層3を局部的な高濃度
領域で切断する方法(例えばP+あるいはN+チヤ
ネルストツパー法)が知られていた。しかしなが
ら、このような方法では、高濃度ストツパー領域
で局部的な破壊(ブレークダウン)が発生してお
り、これが高耐圧化をさまたげていることを、実
験を通じて見い出した。本発明は、該知見に基づ
いて行つたものである。
Conventionally, as a method for preventing parasitic current leakage on the surface, a method has been known in which the inversion layer 3 is cut in a localized high concentration region (for example, P + or N + channel stopper method) as shown in Fig. 1. . However, it has been found through experiments that in such a method, local breakdown occurs in the high concentration stopper region, and this hinders the ability to achieve a high breakdown voltage. The present invention has been made based on this knowledge.

本発明の特徴は例えば、電気的に絶縁分離され
た半導体単結晶に形成され該電極が主表面より引
き出され金属配線等主表面絶縁膜上に形成する接
続体により他の半導体素子と接続されて半導体集
積回路を構成せしめる集積形半導体素子におい
て、上記主表面に形成される接続体相当部分ある
いはその近傍を含んだ部分に絶縁膜中に埋め込ま
れ該接続体と絶縁分離されバルク電位に固定され
る電界電極(フイールドプレート)を形成したこ
とにある。
A feature of the present invention is, for example, that an electrode is formed on a semiconductor single crystal that is electrically insulated and separated, and that the electrode is drawn out from the main surface and connected to other semiconductor elements by a connection body formed on the main surface insulating film such as a metal wiring. In an integrated semiconductor element constituting a semiconductor integrated circuit, a portion corresponding to or near a connecting body formed on the main surface is embedded in an insulating film, insulated from the connecting body, and fixed at a bulk potential. The reason lies in the formation of an electric field electrode (field plate).

以下、順を追つて従来の高濃度チヤネルストツ
パー法が高耐圧化をさまたげる現象と、次に本発
明による一構造例の詳細とを説明する。
Hereinafter, the phenomenon in which the conventional high-concentration channel stopper method hinders the increase in breakdown voltage, and the details of one structural example according to the present invention will be explained in order.

第2図は、第1図のチヤネル・ストツパー領域
の近辺を拡大したものであり、図中に示したφN
、φP、φ1NV、φN は、それぞれN-バルク
1、P形拡散層2、表面反転層3、および高濃度
N形チヤネルストツパー4の電位である。また、
PN接合および表面反転層3近傍の破線で示した
領域は、空乏層5である。
Figure 2 is an enlarged view of the vicinity of the channel stopper area in Figure 1, and the φ N
, φ P , φ 1NV , and φ N + are the potentials of the N bulk 1, P type diffusion layer 2, surface inversion layer 3, and high concentration N type channel stopper 4, respectively. Also,
The region shown by the broken line near the PN junction and the surface inversion layer 3 is the depletion layer 5.

さて、PN接合は阻止状態であることより、金
属等接続体8a,8b、P形拡散層2、およびN
形バルク1等、自由キヤリアの存在する各領域の
電位は均一と見なしてよい。さらに、表面反転層
3にも、誘起された自由キヤリアが存在してお
り、表面反転層3の電位も阻止状態においては位
置に依存せず、均一と見なしてよい。
Now, since the PN junction is in a blocking state, the metal connectors 8a, 8b, the P-type diffusion layer 2, and the N
The potential of each region where free carriers exist, such as the bulk 1, may be considered to be uniform. Furthermore, induced free carriers exist in the surface inversion layer 3 as well, and the potential of the surface inversion layer 3 in the blocked state is independent of position and may be considered to be uniform.

今、表面反転層を形成するのに必要な、バイア
ス電圧をVTとし、φN を基準電位、VRをPN
合の逆バイアスとすると、それぞれの領域の電位
は次式で与えられる。
Now, assuming that the bias voltage required to form the surface inversion layer is V T , φ N - is the reference potential, and V R is the reverse bias of the P N junction, the potential of each region is given by the following equation. .

φN =φN =O φ1NV=φP−VT ………(1) φP=VR 従つて、N+ストツパー4と表面反転層間の電
位差Δφは(1)式より次のように与えられる。
φ N + = φ N = O φ 1NV = φ P −V T ………(1) φ P = V R Therefore, the potential difference Δφ between the N + stopper 4 and the surface inversion layer is as follows from equation (1). It is given as follows.

Δφ=φN −φ1NV=−VR+VT ………(2) (2)式より、PN接合に加えられた逆バイアス
は、表面反転層と高濃度ストツパー領域の間に実
効的に形成される接合にVT分を除いて、ダイレ
クトに加えられることが分かる。そのため、局部
的なブレークダウンが発生し、高耐圧化をさまた
げている。実験結果に基づき、具体的な数値を示
すと、単体素子としての耐圧が350V以上あつた
ものが半導体集積回路化するために、従来の高濃
度ストツパーを使用して接続したとき、250V程
度に下落した。そのときのVTは25V前後であ
り、(2)式より明らかな如く、外部逆バイアスの多
くの部分が反転層3と高濃度ストツパー4間とに
形成される実効的な接合に加えられていることが
実験的にも分かる。
Δφ=φ N −φ 1NV = −V R +V T ………(2) From equation (2), the reverse bias applied to the PN junction is effectively applied between the surface inversion layer and the high concentration stopper region. It can be seen that the voltage is applied directly to the formed junction, except for V T . As a result, local breakdown occurs, which hinders the ability to achieve high voltage resistance. Based on experimental results, specific figures show that when a device with a withstand voltage of 350V or more as a single element is connected using a conventional high-concentration stopper for semiconductor integrated circuits, the voltage drops to around 250V. did. At that time, V T is around 25V, and as is clear from equation (2), most of the external reverse bias is added to the effective junction formed between the inversion layer 3 and the high concentration stopper 4. It is known experimentally that

第3図a、第3図bは、以上の知見に基づき行
つた本発明の実施例の構造を示す平面図とA−
A′線の断面図である。これらの図の構造は次の
ようになつている。すなわち、第1図と同様、支
持基体6の中に誘電体、もしくはPN接合よりな
る絶縁領域7で絶縁分離されたNアイランド1が
あり、その中に回路の素子の領域1,2等が形成
される。この回路を構成するための接続体8aお
よび8bが素子の各領域(N+層)から引き出さ
れている。第1図と異つているのは、高濃度チヤ
ネルストツパー4の代りにバルク結晶と第3図a
中、破線で示した(絶縁膜10の)穴11を通じ
てオーミツク接続した電界電極(フイールド・プ
レート)9が表面反転層3を切断する形状にバル
ク結晶表面を被覆する絶縁膜10中に埋め込まれ
て形成されていることである。本発明により設け
る電界電極9について、さらに詳細について説明
するならば、それは次のような条件を満足してい
る必要がある。第3図b中、lで示した距離が外
部逆バイアスによる空乏層5の伸びに基づく十分
な大きさを備えている必要がある。この点は、従
来の高濃度ストツパー法と全く異つた概念であ
り、また後述するように本発明による構造が高耐
圧化をさまたげない、云い換えれば耐圧の下落を
発生しない理由である。該電界電極9が、満足す
べき、今1つの条件は、該電界電極9は被覆の絶
縁膜10により、回路接続体8aと絶縁分離され
ているが、その絶縁耐圧が少くとも、加えられる
予想される最高逆バイアス以上であることであ
る。それは、該電界電極9が、バルク1とオーミ
ツク接続されており、阻止状態を得るために必要
である。
FIGS. 3a and 3b are a plan view showing the structure of an embodiment of the present invention based on the above knowledge, and FIG.
FIG. The structure of these figures is as follows. That is, as in FIG. 1, there is an N island 1 insulated and isolated by an insulating region 7 made of a dielectric or a PN junction in a support base 6, and circuit element regions 1, 2, etc. are formed therein. be done. Connectors 8a and 8b for configuring this circuit are drawn out from each region (N + layer) of the element. What is different from Fig. 1 is that the high concentration channel stopper 4 is replaced by a bulk crystal and Fig. 3 a
In the middle, an electric field electrode (field plate) 9 which is ohmic-connected through a hole 11 (in the insulating film 10) indicated by a broken line is embedded in the insulating film 10 covering the bulk crystal surface in a shape that cuts the surface inversion layer 3. It is being formed. To explain in more detail the electric field electrode 9 provided according to the present invention, it must satisfy the following conditions. In FIG. 3b, the distance indicated by l must have a sufficient size based on the extension of the depletion layer 5 due to the external reverse bias. This point is a completely different concept from the conventional high-concentration stopper method, and is also the reason why the structure according to the present invention does not hinder the increase in breakdown voltage, or in other words, does not cause a drop in breakdown voltage, as will be described later. Another condition that the electric field electrode 9 should satisfy is that the electric field electrode 9 is insulated from the circuit connection body 8a by the covering insulating film 10, and the dielectric strength of the electric field electrode 9 is at least as high as expected. must be greater than or equal to the maximum reverse bias applied. This is necessary for the electric field electrode 9 to be in ohmic connection with the bulk 1 in order to obtain a blocking state.

本発明による構造であれば、高濃度チヤネルス
トツパー法で発生した局部的なブレークダウンに
よる耐圧の下落を起こさない。なぜならば、本発
明による構造で設けた電界電極9の阻止PN接合
側近傍で、切断された表面反転層3の端には、第
1図の場合と同様、外部逆バイアスの多くの部分
が加えられるが第1図の場合と異なり、その領域
は不純物濃度が低く、空乏層3が伸長し、空乏層
内最高電界強度を押え、局部的なブレークダウン
を発生し難くするからである。
With the structure according to the present invention, a drop in breakdown voltage due to local breakdown that occurs in the high concentration channel stopper method does not occur. This is because, as in the case of FIG. 1, a large portion of the external reverse bias is applied to the cut end of the surface inversion layer 3 near the blocking PN junction side of the electric field electrode 9 provided in the structure according to the present invention. However, unlike the case shown in FIG. 1, the impurity concentration in that region is low, and the depletion layer 3 extends, suppressing the maximum electric field strength within the depletion layer and making local breakdown difficult to occur.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、従来の高濃度ストツパー法を使用し
た構造を説明する半導体装置の断面図、第2図は
従来構造が引き起こす耐圧下落現象を説明するた
めの第1図のストツパー近傍を拡大した断面図で
ある。第3図aおよび第3図bは、本発明による
一実施例の構造を説明するための平面図および断
面図である。 尚、図において、1……アイランド、2……P
型拡散層、3……表面反転層、4……チヤネル・
ストツパー、5……空乏層、6……支持基体、7
……分絶島、8a,8b……接続体、9……電界
電極(フイールド・プレート)、10……絶縁
膜、11……穴11。
Figure 1 is a cross-sectional view of a semiconductor device illustrating a structure using the conventional high-concentration stopper method, and Figure 2 is an enlarged cross-section of the vicinity of the stopper in Figure 1, illustrating the breakdown voltage drop phenomenon caused by the conventional structure. It is a diagram. FIGS. 3a and 3b are a plan view and a sectional view for explaining the structure of an embodiment according to the present invention. In addition, in the figure, 1...Island, 2...P
Type diffusion layer, 3... Surface inversion layer, 4... Channel.
Stopper, 5... Depletion layer, 6... Support base, 7
... Separated island, 8a, 8b ... Connection body, 9 ... Electric field electrode (field plate), 10 ... Insulating film, 11 ... Hole 11.

Claims (1)

【特許請求の範囲】[Claims] 1 支持基体中に絶縁領域で囲まれた一導電型の
複数半導体島領域を有し、各半導体島領域内にそ
れぞれ形成された回路素子が接続体によつて接続
された半導体装置において、前記半導体島領域は
他の導電型領域を備え、該他の導電型領域と前記
絶縁領域との間の前記島領域上に前記接続体が絶
縁膜を介して設けられており、前記接続体下の前
記絶縁膜中に前記半導体島領域の電位に固定され
た導電層による電界電極が設けられていることを
特徴とする半導体装置。
1. A semiconductor device having a plurality of semiconductor island regions of one conductivity type surrounded by an insulating region in a supporting base, and in which circuit elements formed in each semiconductor island region are connected by a connecting body, wherein the semiconductor The island region includes a region of another conductivity type, and the connection body is provided on the island region between the other conductivity type region and the insulating region with an insulating film interposed therebetween, and the connection body is provided under the connection body. A semiconductor device characterized in that an electric field electrode formed of a conductive layer fixed to the potential of the semiconductor island region is provided in an insulating film.
JP4823279A 1979-04-19 1979-04-19 Semiconductor device Granted JPS55140246A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4823279A JPS55140246A (en) 1979-04-19 1979-04-19 Semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4823279A JPS55140246A (en) 1979-04-19 1979-04-19 Semiconductor device

Publications (2)

Publication Number Publication Date
JPS55140246A JPS55140246A (en) 1980-11-01
JPS6223459B2 true JPS6223459B2 (en) 1987-05-22

Family

ID=12797687

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4823279A Granted JPS55140246A (en) 1979-04-19 1979-04-19 Semiconductor device

Country Status (1)

Country Link
JP (1) JPS55140246A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58124953U (en) * 1981-09-18 1983-08-25 三洋電機株式会社 Semiconductor integrated circuit device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5322384A (en) * 1976-08-13 1978-03-01 Hitachi Ltd Semiconductor device

Also Published As

Publication number Publication date
JPS55140246A (en) 1980-11-01

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