JPH06163565A - Transistor element - Google Patents

Transistor element

Info

Publication number
JPH06163565A
JPH06163565A JP4332416A JP33241692A JPH06163565A JP H06163565 A JPH06163565 A JP H06163565A JP 4332416 A JP4332416 A JP 4332416A JP 33241692 A JP33241692 A JP 33241692A JP H06163565 A JPH06163565 A JP H06163565A
Authority
JP
Japan
Prior art keywords
layer
collector
insulating layer
emitter
active region
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.)
Pending
Application number
JP4332416A
Other languages
Japanese (ja)
Inventor
Keisuke Suzui
啓介 鈴井
Mika Nagasaki
美香 長崎
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.)
Denso Corp
Original Assignee
NipponDenso 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 NipponDenso Co Ltd filed Critical NipponDenso Co Ltd
Priority to JP4332416A priority Critical patent/JPH06163565A/en
Publication of JPH06163565A publication Critical patent/JPH06163565A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】 【目的】トランジスタの耐圧を向上させる。 【構成】図1(a)は横型PNPトランジスタの平面図であ
り、図1(b)はA-A'の断面図、図1(c)はB-B'の断面図であ
る。トランジスタのエミッタ1はコレクタ拡散層3に囲
まれた構造で、エミッタ配線2がコレクタ拡散層3の上
を横切る個所に、分厚い絶縁層4が形成されている。こ
の構造で、図1(d) の逆バイアスを示す動作図におい
て、コレクタ活性層3とベース層6との関係はPN逆バ
イアスの状態になり、コレクタ活性層3の周囲に空乏層
7,8ができる。このときエミッタ配線2の電位によっ
てエピタキシャル層6の絶縁層直下の表面近傍では静電
効果によってキャリア濃度が増大するが、分厚い絶縁層
4のためにエミッタ配線2の影響をわずかしか受けない
ので空乏層8は電界集中を生じることがなく、耐電圧を
低下させない。
(57) [Summary] [Purpose] To improve the breakdown voltage of a transistor. [Structure] FIG. 1 (a) is a plan view of a lateral PNP transistor, FIG. 1 (b) is a sectional view taken along line AA ', and FIG. 1 (c) is a sectional view taken along line BB'. The emitter 1 of the transistor has a structure surrounded by a collector diffusion layer 3, and a thick insulating layer 4 is formed where the emitter wiring 2 crosses the collector diffusion layer 3. With this structure, in the operation diagram showing the reverse bias of FIG. 1 (d), the relationship between the collector active layer 3 and the base layer 6 is in the PN reverse bias state, and the depletion layers 7 and 8 are formed around the collector active layer 3. You can At this time, the potential of the emitter wiring 2 increases the carrier concentration in the vicinity of the surface of the epitaxial layer 6 immediately below the insulating layer due to the electrostatic effect, but the thick insulating layer 4 causes only a slight influence of the emitter wiring 2 and thus the depletion layer. No. 8 does not cause electric field concentration and does not lower the withstand voltage.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明はトランジスタ素子の構
造、特に配線の配置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a structure of a transistor element, and more particularly to wiring arrangement.

【0002】[0002]

【従来の技術】従来、ICなどの基板をプレーナープロ
セス技術によって形成する二次元配置の半導体装置にお
いては、回路素子をつなぐ配線は、半導体基板上に形成
された均一厚さの絶縁膜上に形成されている。この配線
は平面的に引き回されているので、ICなどで使われる
横型トランジスタの場合、その特性上エミッタの周りを
コレクタが取り囲んでいるので、P型エミッタに対する
配線はP型コレクタ活性層の上部を横切るように形成さ
れる。従来例の場合、横型PNPトランジスタでは、図
2に示すようにエミッタ配線21が薄い絶縁層23を介
してコレクタ活性層22に接近しているので静電効果の
影響が強く出て、逆バイアス動作時に活性層22の周囲
の表面近傍でできる空乏層24はかなり狭められ、それ
だけ通常の降伏電圧よりも低い降伏電圧となってしま
う。従ってそのことを考慮して降伏電圧を保証するよう
に、コレクタ拡散層の深さを大きく取ったり、エミッタ
─コレクタ間の間隔をとるなどの余裕をとって寸法の設
計がなされていた。
2. Description of the Related Art Conventionally, in a two-dimensionally arranged semiconductor device in which a substrate such as an IC is formed by a planar process technique, wiring connecting circuit elements is formed on an insulating film having a uniform thickness formed on a semiconductor substrate. Has been done. Since this wiring is laid out in a plane, in the case of a lateral transistor used in an IC or the like, the collector surrounds the emitter due to its characteristics. Therefore, the wiring for the P-type emitter is located above the P-type collector active layer. Is formed so as to cross. In the case of the conventional example, in the lateral PNP transistor, the emitter wiring 21 is close to the collector active layer 22 via the thin insulating layer 23 as shown in FIG. At times, the depletion layer 24 formed near the surface around the active layer 22 is considerably narrowed, and the breakdown voltage becomes lower than the normal breakdown voltage. Therefore, in order to guarantee the breakdown voltage in consideration of this, the dimensions have been designed with a margin such as a large depth of the collector diffusion layer or a space between the emitter and the collector.

【0003】[0003]

【発明が解決しようとする課題】しかしながら、トラン
ジスタ素子のコレクタ活性層の上部を横切る配線の電位
がそのコレクタ活性層の電位よりも差が大きい逆バイア
スである場合には、配線の静電効果の影響によりコレク
タ活性層周りのベース層の電気伝導に寄与するキャリ
ア、つまり電子または正孔の濃度が増大する。その結果
絶縁層直下の表面近傍において逆バイアスで生じたコレ
クタとベースとの空乏層が狭められて電界集中が生じ
る。そのためその部分で本来のアバランシェ降伏電圧よ
り低い電圧で降伏してしまうことになり、半導体基板の
絶縁耐圧が下がるという問題がある。横型トランジスタ
のコレクタの形状をコの字型にして、エミッタに対する
配線下のコレクタを無くした構造が実施されている。し
かし、コの字形状は上記の問題は生じないがエミッタ−
コレクタ間の注入効率を下げてしまうという問題があ
る。従って本発明はトランジスタ素子の性能を低下させ
ることなく耐圧性の向上をはかることを目的とする。
However, when the potential of the wiring that crosses the upper part of the collector active layer of the transistor element is reverse bias having a larger difference than the potential of the collector active layer, the electrostatic effect of the wiring is reduced. Due to the influence, the concentration of carriers, that is, electrons or holes, which contribute to the electric conduction of the base layer around the collector active layer, increases. As a result, the depletion layer between the collector and the base generated by the reverse bias is narrowed in the vicinity of the surface immediately below the insulating layer, and electric field concentration occurs. Therefore, at that portion, breakdown occurs at a voltage lower than the original avalanche breakdown voltage, which causes a problem that the withstand voltage of the semiconductor substrate decreases. A structure in which the collector of the lateral transistor is U-shaped and the collector under the wiring for the emitter is eliminated is implemented. However, the U-shape does not cause the above problem, but the emitter-
There is a problem that the injection efficiency between collectors is reduced. Therefore, an object of the present invention is to improve withstand voltage characteristics without deteriorating the performance of a transistor element.

【0004】[0004]

【課題を解決するための手段】上記課題を解決するため
の発明の構成は、半導体基板上に形成されたトランジス
タ素子において、前記トランジスタ素子のエミッタ活性
領域が、ベ−ス活性領域を介してコレクタ活性領域によ
って囲まれた平面配置であって、前記半導体基板上に形
成された絶縁層の上において前記エミッタ活性領域の電
極配線が前記コレクタ活性領域の上部を横切る構造を
し、前記電極配線には電圧が印加され、前記ベース活性
領域と前記コレクタ活性領域との接合領域に形成される
空乏層の幅が表面領域で狭くされた半導体装置におい
て、前記電極配線の下部の絶縁層を、前記コレクタ活性
領域を横切る部分で通常の部分の絶縁層の厚さよりも厚
くしたことを特徴とする。
SUMMARY OF THE INVENTION According to the structure of the invention for solving the above problems, in a transistor element formed on a semiconductor substrate, an emitter active region of the transistor element is a collector via a base active region. In a planar arrangement surrounded by active regions, an electrode wiring of the emitter active region crosses an upper portion of the collector active region on an insulating layer formed on the semiconductor substrate, and the electrode wiring is In a semiconductor device in which a voltage is applied and a width of a depletion layer formed in a junction region between the base active region and the collector active region is narrowed in a surface region, an insulating layer below the electrode wiring is connected to the collector active region. It is characterized in that the portion that crosses the region is thicker than the thickness of the insulating layer in the normal portion.

【0005】[0005]

【作用】コレクタ活性層の上を配線が横切る個所の絶縁
層が厚くなると、例えば絶縁層が三倍の厚さになれば、
配線によって生じる電界は距離にほぼ比例して弱くなる
ので、絶縁層下のベース活性領域とコレクタ活性領域と
の接合領域に対する影響も1/3に減少し、キャリアの
集中は緩和される。
When the insulating layer at the position where the wiring crosses the collector active layer becomes thicker, for example, when the insulating layer becomes three times thicker,
Since the electric field generated by the wiring weakens almost in proportion to the distance, the influence on the junction region between the base active region and the collector active region under the insulating layer is also reduced to 1/3, and the concentration of carriers is relaxed.

【0006】[0006]

【発明の効果】その結果、エミッタ配線下のコレクタ活
性層とベース層との接合領域に生じる空乏層の電界集中
による絶縁耐圧の低下が抑えられるので、半導体基板の
耐圧信頼度が向上する。また、横型トランジスタの構造
は、エミッタを取り囲む形のままのコレクタ形状で良い
ので注入効率は変わらず、さらに設計余裕を設けなくて
よいので耐圧を下げずに半導体装置のサイズをわずかな
がら縮小することができる。
As a result, the breakdown voltage reliability of the semiconductor substrate is improved because the reduction of the dielectric breakdown voltage due to the electric field concentration of the depletion layer generated in the junction region between the collector active layer and the base layer under the emitter wiring is suppressed. In addition, the structure of the lateral transistor may be the collector shape that is the same as the shape that surrounds the emitter, so the injection efficiency does not change, and since there is no need to provide a design margin, the semiconductor device size can be reduced slightly without lowering the breakdown voltage. You can

【0007】[0007]

【実施例】以下、本発明を具体的な実施例に基づいて説
明する。図1は、本発明の一実施例を示す模式構成図
で、図1(a) は半導体基板上に形成された横型PNPト
ランジスタの平面図であり、図1(b) は図1(a) A−
A’の断面図である。また、図1(c) は図1(a) B−
B’の断面図である。なお、いずれの図も基板の他の素
子との分離領域は図示していない。この図で示すよう
に、トランジスタのエミッタ1はコレクタ拡散層3に囲
まれた構造をしており、エミッタ1につながるエミッタ
配線2がコレクタ拡散層3の上を横切る個所に、分厚い
絶縁層4が形成されている。
EXAMPLES The present invention will be described below based on specific examples. 1 is a schematic configuration diagram showing an embodiment of the present invention, FIG. 1 (a) is a plan view of a lateral PNP transistor formed on a semiconductor substrate, and FIG. 1 (b) is FIG. 1 (a). A-
It is a sectional view of A '. Also, FIG. 1 (c) is shown in FIG. 1 (a) B-
It is a sectional view of B '. It should be noted that none of the figures shows the isolation region of the substrate from other elements. As shown in this figure, the emitter 1 of the transistor has a structure surrounded by a collector diffusion layer 3, and a thick insulating layer 4 is formed at a position where the emitter wiring 2 connected to the emitter 1 crosses the collector diffusion layer 3. Has been formed.

【0008】このような構造であるとき、図1(d) の逆
バイアスを示す動作図において、コレクタ活性層3と基
板のエピタキシャル層であるベース層6との関係はPN
逆バイアスの状態になるため、コレクタ活性層3の周囲
に空乏層7,8ができる。空乏層7,8の広がりは逆バ
イアスの程度や半導体基板エピタキシャル層6の不純物
の濃度、およびコレクタ活性層3の不純物の濃度によっ
て決まる。このときエミッタ配線2の電位によってエピ
タキシャル層6の絶縁層直下の表面近傍では静電効果に
よってキャリア濃度が増大するが、分厚い絶縁層4のた
めにエミッタ配線2の影響をわずかしか受けないので空
乏層8は電界集中を生じることがなく、耐電圧を低下さ
せない。
With such a structure, in the operation diagram showing the reverse bias of FIG. 1D, the relation between the collector active layer 3 and the base layer 6 which is the epitaxial layer of the substrate is PN.
Because of the reverse bias state, depletion layers 7 and 8 are formed around the collector active layer 3. The spread of the depletion layers 7 and 8 is determined by the degree of reverse bias, the impurity concentration of the semiconductor substrate epitaxial layer 6, and the impurity concentration of the collector active layer 3. At this time, the potential of the emitter wiring 2 increases the carrier concentration in the vicinity of the surface of the epitaxial layer 6 immediately below the insulating layer due to the electrostatic effect, but the thick insulating layer 4 causes only a slight influence of the emitter wiring 2 and thus the depletion layer. No. 8 does not cause electric field concentration and does not lower the withstand voltage.

【0009】本発明の分厚い絶縁層構造の形成は、通常
の絶縁層を形成したのち、マスクを用いて絶縁層形成プ
ロセスを繰り返し積層することで実現でき、従来の製造
プロセスに組み入れることができる。エミッタ電極から
分厚い絶縁層の上まで配線が確実になるよう階段状に積
層する。あるいは初めから分厚い絶縁層を形成したの
ち、必要部分を残すいわゆるメサエッチングをして薄く
してもよい。
The formation of the thick insulating layer structure of the present invention can be realized by forming an ordinary insulating layer and then repeatedly stacking the insulating layer forming process using a mask, which can be incorporated into a conventional manufacturing process. Laminates in a step-like manner from the emitter electrode to the thick insulating layer so that the wiring is secure. Alternatively, after forming a thick insulating layer from the beginning, so-called mesa etching that leaves a necessary portion may be performed to reduce the thickness.

【0010】本発明の別の例として、図3に示すよう
に、分厚い絶縁層の形成に対し多層配線の構造を用いて
もよい。即ち、薄い絶縁層23上の第一層配線に目的の
エミッタ配線を形成せず、平坦化層間絶縁層31を形成
し、その上の第二層配線30をエミッタ配線として形成
しても同様の効果が得られる。この方法も多層配線式の
半導体基板にそのまま製造工程の一部に組み込むことが
できる。
As another example of the present invention, as shown in FIG. 3, a multilayer wiring structure may be used for forming a thick insulating layer. That is, even if the intended emitter wiring is not formed on the first layer wiring on the thin insulating layer 23, the flattening interlayer insulating layer 31 is formed, and the second layer wiring 30 thereon is formed as the emitter wiring, the same result is obtained. The effect is obtained. This method can also be directly incorporated in a multilayer wiring type semiconductor substrate as part of the manufacturing process.

【0011】この発明は横型トランジスタに限らず、ど
のような回路素子でもここで問題にしたような逆バイア
スの静電効果による悪影響を生じる構造であれば分厚い
絶縁層構造を施して同様な効果をもたらす。また、耐圧
が上昇することから、それまで安全をとっていた設計を
省略できる効果もある。
The present invention is not limited to the lateral transistor, and if any circuit element has a structure which adversely affects by the electrostatic effect of the reverse bias as the problem here, a thick insulating layer structure is applied to obtain the same effect. Bring Further, since the breakdown voltage is increased, there is also an effect that the design which has been taking safety until then can be omitted.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の一実施例を示す模式構成図。FIG. 1 is a schematic configuration diagram showing an embodiment of the present invention.

【図2】従来の実施例を示す構成図。FIG. 2 is a configuration diagram showing a conventional embodiment.

【図3】本発明の別の実施例を示す模式断面図。FIG. 3 is a schematic sectional view showing another embodiment of the present invention.

【符号の説明】[Explanation of symbols]

1 エミッタ 2 エミッタ配線 3 コレクタ拡散層 4 分厚い絶縁層 5 エミッタ拡散層 7、8 表面近傍の空乏層領域 20 エミッタ 21 エミッタ配線 22 コレクタ拡散層 23 薄い絶縁層 24、25 表面近傍の空乏層領域 30 第二層配線のエミッタ配線 31 平坦化層間絶縁層 1 Emitter 2 Emitter Wiring 3 Collector Diffusion Layer 4 Thick Insulating Layer 5 Emitter Diffusion Layer 7, 8 Depletion Layer Region Near Surface 20 Emitter 21 Emitter Wiring 22 Collector Diffusion Layer 23 Thin Insulation Layer 24, 25 Depletion Layer Region Near Surface 30 Two-layer wiring emitter wiring 31 Flattening interlayer insulation layer

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】半導体基板上に形成されたトランジスタ素
子において、前記トランジスタ素子のエミッタ活性領域
が、ベ−ス活性領域を介してコレクタ活性領域によって
囲まれた平面配置であって、前記半導体基板上に形成さ
れた絶縁層の上において前記エミッタ活性領域の電極配
線が前記コレクタ活性領域の上部を横切る構造をし、前
記電極配線には電圧が印加され、前記ベース活性領域と
前記コレクタ活性領域との接合領域に形成される空乏層
の幅が表面領域で狭くされた半導体装置において、前記
電極配線の下部の絶縁層を、前記コレクタ活性領域を横
切る部分で通常の部分の絶縁層の厚さよりも厚くしたこ
とを特徴とするトランジスタ素子。
1. A transistor element formed on a semiconductor substrate, wherein the emitter active region of the transistor element is a planar arrangement surrounded by a collector active region via a base active region, and the transistor active region is formed on the semiconductor substrate. A structure in which the electrode wiring of the emitter active region crosses the upper portion of the collector active region on the insulating layer formed on the substrate, and a voltage is applied to the electrode wiring to connect the base active region and the collector active region. In a semiconductor device in which the width of the depletion layer formed in the junction region is narrowed in the surface region, the insulating layer below the electrode wiring is thicker than the normal insulating layer at the portion crossing the collector active region. A transistor element characterized in that
JP4332416A 1992-11-17 1992-11-17 Transistor element Pending JPH06163565A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4332416A JPH06163565A (en) 1992-11-17 1992-11-17 Transistor element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4332416A JPH06163565A (en) 1992-11-17 1992-11-17 Transistor element

Publications (1)

Publication Number Publication Date
JPH06163565A true JPH06163565A (en) 1994-06-10

Family

ID=18254730

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4332416A Pending JPH06163565A (en) 1992-11-17 1992-11-17 Transistor element

Country Status (1)

Country Link
JP (1) JPH06163565A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN119815883A (en) * 2024-12-13 2025-04-11 重庆大学 Power switch transistor
CN119815843A (en) * 2024-12-13 2025-04-11 重庆大学 A planar power diode

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN119815883A (en) * 2024-12-13 2025-04-11 重庆大学 Power switch transistor
CN119815843A (en) * 2024-12-13 2025-04-11 重庆大学 A planar power diode

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