JPS5910069B2 - semiconductor equipment - Google Patents
semiconductor equipmentInfo
- Publication number
- JPS5910069B2 JPS5910069B2 JP51098517A JP9851776A JPS5910069B2 JP S5910069 B2 JPS5910069 B2 JP S5910069B2 JP 51098517 A JP51098517 A JP 51098517A JP 9851776 A JP9851776 A JP 9851776A JP S5910069 B2 JPS5910069 B2 JP S5910069B2
- Authority
- JP
- Japan
- Prior art keywords
- region
- transistor
- collector
- switching element
- lateral transistor
- 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
Links
- 239000004065 semiconductor Substances 0.000 title claims description 10
- 238000009792 diffusion process Methods 0.000 claims description 12
- 239000000758 substrate Substances 0.000 claims description 7
- 239000012212 insulator Substances 0.000 claims description 3
- 238000000034 method Methods 0.000 description 9
- 239000012535 impurity Substances 0.000 description 6
- 229910052581 Si3N4 Inorganic materials 0.000 description 5
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 4
- 238000002347 injection Methods 0.000 description 4
- 239000007924 injection Substances 0.000 description 4
- 238000004519 manufacturing process Methods 0.000 description 4
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 3
- 229910052710 silicon Inorganic materials 0.000 description 3
- 239000010703 silicon Substances 0.000 description 3
- NBIIXXVUZAFLBC-UHFFFAOYSA-N Phosphoric acid Chemical compound OP(O)(O)=O NBIIXXVUZAFLBC-UHFFFAOYSA-N 0.000 description 2
- 238000009825 accumulation Methods 0.000 description 2
- 229910052681 coesite Inorganic materials 0.000 description 2
- 229910052906 cristobalite Inorganic materials 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000005468 ion implantation Methods 0.000 description 2
- 238000001259 photo etching Methods 0.000 description 2
- 239000000377 silicon dioxide Substances 0.000 description 2
- 235000012239 silicon dioxide Nutrition 0.000 description 2
- 229910052682 stishovite Inorganic materials 0.000 description 2
- 229910052905 tridymite Inorganic materials 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 1
- BLRPTPMANUNPDV-UHFFFAOYSA-N Silane Chemical compound [SiH4] BLRPTPMANUNPDV-UHFFFAOYSA-N 0.000 description 1
- 229910000147 aluminium phosphate Inorganic materials 0.000 description 1
- 230000003321 amplification Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 239000000969 carrier Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 230000005685 electric field effect Effects 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 238000002955 isolation Methods 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 0.000 description 1
- 229910052698 phosphorus Inorganic materials 0.000 description 1
- 239000011574 phosphorus Substances 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
Landscapes
- Bipolar Integrated Circuits (AREA)
- Bipolar Transistors (AREA)
Description
【発明の詳細な説明】
本発明はチップ面積及び速度電力積が小さくかつファン
アウトが任意の個数取り出せる論理回路用の半導体装置
に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a semiconductor device for logic circuits that has a small chip area and speed-power product and can provide an arbitrary number of fan-outs.
従来、いくつかの論理回路用半導体装置が知られている
が、その一つとして、アイソレーシヨン拡散領域もしく
は拡散抵抗器を必要とせず素子面積を節約した集積度の
高い12L(Integrated工njection
Logic構造の論理回路素子が例えば特公昭49−3
5030に示されている様に周知である。Several semiconductor devices for logic circuits have been known in the past, one of which is the 12L (Integrated Injection) which has a high degree of integration and saves device area without requiring an isolation diffusion region or a diffusion resistor.
For example, a logic circuit element with a Logic structure is
It is well known as shown in 5030.
この構造でNOR回路を構成した時の1例を第1図に示
し、その基本的な動作原理を簡単に説明する。2つのP
形拡散領域P1、P2及びP3がn形半導体基体(Ni
)中に互に分離されて配列されている。An example of a NOR circuit configured with this structure is shown in FIG. 1, and its basic operating principle will be briefly explained. two Ps
type diffusion regions P1, P2, and P3 are formed in an n-type semiconductor substrate (Ni
) are arranged separated from each other.
このP、をエミッタ、N2をベース、P2をコレクタと
して横方向トランジスタTlを、P1をエミッタ、Ni
をベース、P3をコレクタとする横方向トランジスタT
3を形成する。半導体基体N2及びP2、P3領域内の
N2N3領域をn形拡散で形成する。これによつてNi
をエミッタ、P2をベース、N3をコレクタとする垂直
方向トランジスタT2が得られる。今、トランジスタT
iとT2について動作を説明する。電流工がトランジス
タTlのエミッタPiに印加されると、注入された正孔
は部分的にトランジスタTlのコレクタP2に捕集され
る。これによV)P2とN2とのP−n接合は順方向に
バイアスされ、トランジスタT2のエミッタとして働く
Niから電子がP2に注入される。従つてAが電流源に
接続され人力E1が浮遊状態に残される時、コレクタ電
流kがトランジスタT2を流れる。しかし、もし接地電
位がE1に印加されると、10がトランジスタT2のN
2コレクタ領域を横切つて流れるのを阻止される。この
ようにPNPトランジスタT1は電流を逆方向に動作す
るNPNトランジスタT2のベースへ供給する。この時
、E1が浮遊状態にあるとPNPトランジスタT1に加
えられた電流はNPNトランジスタT2のベースP2に
流れ、かくしてトランジスタT2は飽和導電状態となる
。しかしながらElが接地電位に接続される時はT1に
印加された電流1はEtを通して流れ、T2のベースに
は流れ得ない。この場合T2は阻止される。T,のコレ
クタに生ずる電位を考えると、T1及びT2は反転回路
を形成する。他のトランジスタT3とトランジスタT4
との関係も上述のトランジスタT1とトランジスタT3
との動作と同様である。このT1〜T4のトランジスタ
によl)NOR回路が形成される。以上示した従来構造
の素子に卦いては、N1領域はトランジスタT2のエミ
ツタであると同時にトランジスタT1のベースでもある
ので、トランジスタT,のエミツタ注入効率を下げない
為に高不純物濃度にする事は許されず高々1616at
0m?/CTn3程度である。This P is the emitter, N2 is the base, P2 is the collector, and the lateral transistor Tl is formed, P1 is the emitter, and Ni
A lateral transistor T with P3 as the base and P3 as the collector
form 3. N2N3 regions within the semiconductor substrate N2, P2, and P3 regions are formed by n-type diffusion. By this Ni
A vertical transistor T2 is obtained, with P2 as the emitter, P2 as the base, and N3 as the collector. Now, transistor T
The operation will be explained regarding i and T2. When a current is applied to the emitter Pi of the transistor Tl, the injected holes are partially collected at the collector P2 of the transistor Tl. This causes the Pn junction between P2 and N2 to be biased in the forward direction, and electrons are injected into P2 from the Ni acting as the emitter of transistor T2. Therefore, when A is connected to a current source and power E1 is left floating, a collector current k flows through transistor T2. However, if a ground potential is applied to E1, then 10 is applied to N of transistor T2.
2 is prevented from flowing across the collector region. PNP transistor T1 thus supplies current to the base of NPN transistor T2, which operates in the opposite direction. At this time, when E1 is in a floating state, the current applied to the PNP transistor T1 flows to the base P2 of the NPN transistor T2, and thus the transistor T2 enters a saturated conductive state. However, when El is connected to ground potential, the current 1 applied to T1 flows through Et and cannot flow to the base of T2. In this case T2 is blocked. Considering the potential developed at the collector of T, T1 and T2 form an inverting circuit. Other transistors T3 and T4
The relationship between transistor T1 and transistor T3 described above is also
The operation is similar to that of . 1) A NOR circuit is formed by these transistors T1 to T4. Regarding the element with the conventional structure shown above, the N1 region is the emitter of the transistor T2 and at the same time the base of the transistor T1, so in order not to reduce the emitter injection efficiency of the transistor T, it is not necessary to make it a high impurity concentration. Not allowed and at most 1616at
0m? /CTn3.
このためトランジスタT2は逆トランジスタとして動作
しN2からP2へのエミツタ注人効率は悪くエミツタ接
地電流増幅率HFEは通常2〜3と非常に小さい。その
為、コレクタN2からのフアンアウトを多数個とる事は
困 5難である。また更にHFEを低下させぬためにト
ランジスタT2のベースP2は比較的低不純物濃度に押
えられるためベース抵抗が大きくな)演算速度が遅くな
る。またトランジスタT2のベース領域には逆ドリフト
電界が生じているためキヤリ 3アの拡散時間が長く、
更に少数担体蓄積時間なども必要とし演算速度が遅くな
る。そこで本発明者らは上記欠点を改善すべく特願昭5
1−49095号にて新規なる構造のスイツチング素子
を備えた構造を提案した。Therefore, the transistor T2 operates as a reverse transistor, and the emitter injection efficiency from N2 to P2 is poor, and the emitter ground current amplification factor HFE is usually very small, 2 to 3. Therefore, it is difficult to obtain a large number of fan-outs from collector N2. Furthermore, in order to prevent further reduction in HFE, the base P2 of the transistor T2 is kept at a relatively low impurity concentration, resulting in a large base resistance and a slow calculation speed. Furthermore, since a reverse drift electric field is generated in the base region of transistor T2, the diffusion time of carrier 3A is long.
Furthermore, minority carrier accumulation time is required, which slows down the calculation speed. Therefore, in order to improve the above-mentioned drawbacks, the present inventors filed a patent application in 1973.
No. 1-49095 proposed a structure equipped with a switching element of a new structure.
この装置は 4任意の数だけフアンアウトカ相由に取う
出せ、かつ速度電力積及び素子面積の小さな論理回路素
子である。本発明は先の特願昭51−45095号の発
明に訃いて、さらにゲート容敞をへらし高速ノ化をはか
るものである。This device is a logic circuit element that can be taken out in parallel with any number of four fans and has a small speed-power product and element area. The present invention is based on the invention of the previous Japanese Patent Application No. 51-45095, and further aims to reduce the gate resistance and increase the speed.
以下、本発明の一実施例を第2図に基づいて詳細に述べ
る。Hereinafter, one embodiment of the present invention will be described in detail based on FIG.
第2図はaは本発明の一実施例にかかる装置の部分的概
略平面図であ勺、第2図bは第2図aで示したX−Xで
切断した時の部分的概略断面図、第2図cは第2図aで
示したY−Y′で切断した時の部分的概略断面図である
。In FIG. 2, a is a partial schematic plan view of a device according to an embodiment of the present invention, and FIG. 2 b is a partial schematic sectional view taken along the line XX shown in FIG. 2 a. , FIG. 2c is a partial schematic sectional view taken along YY' shown in FIG. 2a.
第2図に卦いて、1は低抵抗率例えば0.001+Ω.
C!!L程度のn形基板であシ接地電位に保たれている
。In Figure 2, 1 indicates low resistivity, for example 0.001+Ω.
C! ! It is an n-type substrate with a size of about L and is kept at a ground potential.
2は前記1上にエピタキシャル形成した高抵抗率例えば
50Ω・?程度のn形層である。2 is a high resistivity film epitaxially formed on the above 1, for example, 50Ω. It is an n-type layer.
+3,4は前記2の表面よう形成したP形領域であり、
前記3と4とは近接して配置され、かつ前記3は前記2
の領域を部分的にとシ囲むように例えば網目状に形成さ
れる。+3 and 4 are P-type regions formed like the surface of 2 above,
Said 3 and 4 are arranged close to each other, and said 3 is said 2
For example, it is formed in a mesh shape so as to partially surround the area.
前記4,2,3で構成されるPnPトランジスタT,に
卦いて4,2,3は各々エミツタ・ベース、コレクタと
なつている。このトランジスタT1に卦いては、ベース
濃度が低く、エミツタ、コレクタ濃度力俳常に高いので
、エミツタから注入された正孔のコレクタへの到達率は
従来構造に比べ非常に高くなる。また前記3でと力囲ま
れた2の領域の一部7は前記3の電位が“0nvでは前
記3と7とで構成されるPn接合の拡散電位によシ空乏
層で満たされる様+に形成される。In the PnP transistor T, which is composed of 4, 2, and 3, 4, 2, and 3 serve as an emitter, a base, and a collector, respectively. In this transistor T1, the base concentration is low and the emitter and collector concentrations are high in efficiency, so that the rate of holes injected from the emitter reaching the collector is much higher than in the conventional structure. In addition, a part 7 of the region 2 surrounded by the above 3 is filled with a depletion layer due to the diffusion potential of the Pn junction composed of the above 3 and 7 when the potential of the above 3 is 0 nV. It is formed.
5は前記2の表面に形成したn形領域であり、1,2,
3,7,5からなるスイッチング素子S,が構成される
。5 is an n-type region formed on the surface of 2, and 1, 2,
A switching element S consisting of 3, 7, and 5 is configured.
この素子S,VC卦いて各々3はゲート、1,2,5は
導電路として作用する。6は前記3の電極取う出し部及
びトランジスタT,のベース対向部分を除き、その表面
よジ所定の深さで形成した絶縁物領域であわ、ゲート3
の接合容量を減じ、応答速度を速め、更に導電路2の形
成及びその電極形成を容易にするものである。In the elements S and VC, 3 serves as a gate, and 1, 2, and 5 serve as conductive paths. Reference numeral 6 denotes an insulating region formed at a predetermined depth beyond the surface of the gate 3, excluding the electrode lead-out portion of 3 and the portion facing the base of the transistor T.
This reduces the junction capacitance, increases the response speed, and facilitates the formation of the conductive path 2 and its electrodes.
前記4の端子をバイアス端子B,前記3の端子を人力端
子1,前記5の端子を出力端子0とする。次に本素子の
動作を説明する。The 4th terminal is the bias terminal B, the 3rd terminal is the manual terminal 1, and the 5th terminal is the output terminal 0. Next, the operation of this device will be explained.
端子Bからは従来構造と同様、電流1Bが常に注入され
ている。A current 1B is always injected from the terminal B as in the conventional structure.
今端子1が浮遊状態にあると、トランジスタT1のエミ
ツタ4から注入された正孔によジトランジスタT1のコ
レクタすなわちスイツチング素子S1のゲート3の電位
は上昇し約+0.6Vとなる。この為スイツチング素子
S1の導電路領域2中に空乏層はほとんどなくなジ、1
一2′−5の導電性通路が形成され、端子0の出力は6
0″Vとなる。次に端子1が接地電位、すなわち60″
Vとなつた時には、スイツチング素子S1のゲート3に
たまつていた正孔は端子1を通ジ放電し、ゲート3は0
Vとなる。この為スイツチング素子S,の導電路領域2
は、前述のごとく、ゲート3と領域2′とのPn接合に
発生する拡散電位のため空乏層で満たされ2と5とは電
気的に分離され端子0は浮遊状態になる。このようにし
てトランジスタT1とスイツチング素子S,とは反転回
路を形成する。本構造の素子に卦いては、従来構造の素
子の様に逆トランジスタ構造を用いていず、ただ単にゲ
ートの開閉によつてのみ端子0に信号の伝達を行なつて
いるのでフアンアウトは、任意の個数だけ自由に選んで
動作させることができるという利点を有している。If the terminal 1 is now in a floating state, the potential of the collector of the transistor T1, that is, the gate 3 of the switching element S1 increases to approximately +0.6V due to holes injected from the emitter 4 of the transistor T1. Therefore, there is almost no depletion layer in the conductive path region 2 of the switching element S1.
A conductive path of 12'-5 is formed, and the output of terminal 0 is 6
0″V. Next, terminal 1 is at ground potential, i.e. 60″V.
When the voltage becomes V, the holes accumulated in the gate 3 of the switching element S1 are discharged through the terminal 1, and the gate 3 becomes 0.
It becomes V. For this reason, the conductive path region 2 of the switching element S,
As described above, is filled with a depletion layer due to the diffusion potential generated at the Pn junction between gate 3 and region 2', and terminals 2 and 5 are electrically separated and terminal 0 is in a floating state. In this way, the transistor T1 and the switching element S form an inverting circuit. Elements with this structure do not use an inverted transistor structure like elements with conventional structures, and the signal is transmitted to terminal 0 only by opening and closing the gate, so fan-out is arbitrary. It has the advantage of being able to freely select and operate as many as .
また、トランジスタT1及びスイツチング素子S1の各
々ベース、導電路となる領域2をできるだけ低濃度、例
えば1014at0m・?−3程度に選ぶことが可能で
あジこれによりトランジスタT1の注入効果を大幅に改
善できる。この時、チヤンネル領域2′の最大寸法dは
、拡散電位例えば0.6でチヤンネル領域が完全に空乏
層で満たされるという条件よジ、d=2×V?J.>l
−[ャ[ロ,4キ5.3μmである。Further, the base of each of the transistor T1 and the switching element S1 and the region 2 which becomes a conductive path are made as low in concentration as possible, for example, 1014at0m. It is possible to select approximately -3, and thereby the injection effect of the transistor T1 can be greatly improved. At this time, the maximum dimension d of the channel region 2' is based on the condition that the channel region is completely filled with a depletion layer at a diffusion potential of 0.6, for example, d=2×V? J. >l
-[Black, 4 x 5.3 μm.
更に従来構造では不可能であつたスイツチング素子S1
のゲート3の不純物濃度を任意に高く選べる為、ゲート
抵抗を低下させる事ができ、更に実効的なゲート領域3
以外は絶縁物領域6になつているのでゲート接合容量を
も減少できるので演算速度を速くすることができるとい
う長所をも有している。また、本構造素子のスイツチン
グ素子は多数担体で動作し、従来構造での様な担体の蓄
積効果、逆ドリフト電界作用などは無く、チヤンネル2
′中も容易に速く動作することができる。更に従来構造
ではトランジスタT2のHFEが小さいため大きなトラ
ンジスタT1のコレクタ電流を必要としたが、本構造で
はスイツチング素子S1のゲート3と導電路2及び7間
のストレイ容量を充電するだけのコレクタ電流で良いた
めトランジスタT3の電力を非常に小さくでき、また、
スイツチング素子S1の動作が本質的に従来のトランジ
スタT2の動作と異なり効率が良く小面積で大きなスイ
ツチング電流がとD扱えるのでスイツチング素子の面積
を小さくできるという利点も有している。次に第3図を
参照して本構造素子の製造方法の一実施例について述べ
る。Furthermore, the switching element S1, which was impossible with the conventional structure,
Since the impurity concentration of the gate 3 can be arbitrarily selected to be high, the gate resistance can be lowered and the effective gate area 3 can be reduced.
Since the other regions are insulator regions 6, the gate junction capacitance can also be reduced, which has the advantage of increasing the calculation speed. In addition, the switching element of this structure operates with a large number of carriers, and there is no carrier accumulation effect or reverse drift electric field effect as in conventional structures, and channel 2
'It can be operated easily and quickly during the process. Furthermore, in the conventional structure, the HFE of the transistor T2 is small, so a large collector current of the transistor T1 is required, but in this structure, the collector current is sufficient to charge the stray capacitance between the gate 3 of the switching element S1 and the conductive paths 2 and 7. Because of this, the power of transistor T3 can be made very small, and
The operation of the switching element S1 is essentially different from the operation of the conventional transistor T2, and it is efficient and can handle a large switching current with a small area, so it also has the advantage that the area of the switching element can be reduced. Next, an embodiment of the method for manufacturing this structural element will be described with reference to FIG.
低抵抗率例えば0.001Ω・確のn+形シリコン1上
に高抵抗率例えば50Ω・?のn+形シリコン2をエピ
タキシャル形成したものを基板とする(第3図a)。Low resistivity, for example, 0.001Ω, on n+ type silicon 1, and high resistivity, for example, 50Ω? A substrate is formed by epitaxially forming n+ type silicon 2 (FIG. 3a).
次に前記2の表面より所定の形状でP形を与える不純物
例えばボロンを含む領域3及び4を周知の熱拡散法もし
くはイオン注入法によV)2μm程度の深さに形成する
。Next, regions 3 and 4 containing a P-type impurity, for example, boron, are formed from the surface of the second layer in a predetermined shape to a depth of about 2 μm by a well-known thermal diffusion method or ion implantation method.
ここで3はトランジスタT1のコレクタ及びスイツチン
グ素子S1のゲートとなる。領域4は各々が前記領域2
の一部領域7を所定の表面形状例えば網目状でとジ囲む
ように形成され、かつ前記7の領域が領域4と領域2′
との間のPn接合の拡散電位のみによシほぼ完全に空乏
層で満たされるように形成する。今、2′の不純物濃度
が1X1014at0m/?3(50Ω−Cm)だとす
ると、前記2′の最大寸法は約5.3μmとなる。(第
3図b)。次に、前記層2上にSi3N4膜10を例え
ばSiH4とNH3とを約750℃の温度で数分間反応
させることによジ約1000Aの厚さに形成する。Here, 3 is the collector of the transistor T1 and the gate of the switching element S1. Each region 4 corresponds to the region 2.
A predetermined surface shape, for example, a mesh shape, is formed so as to surround a partial region 7 of
It is formed so that it is almost completely filled with a depletion layer only by the diffusion potential of the Pn junction between the two. Now, the impurity concentration of 2' is 1X1014at0m/? 3 (50 Ω-Cm), the maximum dimension of 2' is approximately 5.3 μm. (Figure 3b). Next, a Si3N4 film 10 is formed on the layer 2 to a thickness of about 1000 Å by, for example, reacting SiH4 and NH3 at a temperature of about 750° C. for several minutes.
しかる後、周知のフオトエツチング法により、ゲート電
極取ジ出し部及びトランジスタT1+のベース対向部分
を除きP形領域4上のSi3N4膜を除去し開口部11
を設ける。Thereafter, the Si3N4 film on the P-type region 4 is removed by a well-known photoetching method except for the gate electrode extraction part and the part facing the base of the transistor T1+, and the opening 11 is removed.
will be established.
次に前記Si3N4膜1.0をマスクとしてシリコンエ
ツチングを行ない前記基板の開口部11VC0.6μm
程度の深さを有する凹領域を形成した後、水蒸気雰囲気
中1100℃で2時間の処理を行ない1μm程度の,S
iO2膜を形成し前記凹領域をSiO2膜6で埋め、前
記層2の表面をほぼ平坦にする。(第3図c)。次に前
記6の領域で囲まれた領域上の前記Si3N4膜10を
約160℃の熱リン酸で数分間つ 処理レC完全に除去
した後、前記2の表面よりn形を与える不純物例えばリ
ンを含む領域5を周知の熱拡散法もしくはイオン注人法
により前記6の領域で囲まれた領域内に0.5μm程度
の深さに形成する。Next, silicon etching is performed using the Si3N4 film 1.0 as a mask to form an opening 11VC of 0.6 μm in the substrate.
After forming a concave region with a depth of approximately 1 μm, S
An iO2 film is formed and the recessed area is filled with a SiO2 film 6, so that the surface of the layer 2 is made substantially flat. (Figure 3c). Next, the Si3N4 film 10 on the region surrounded by the region 6 is completely removed by treatment with hot phosphoric acid at about 160° C. for several minutes, and then impurities such as phosphorus that give n-type are removed from the surface of the region 2. A region 5 including the above-described region 6 is formed to a depth of about 0.5 μm within the region surrounded by the region 6 by a well-known thermal diffusion method or ion implantation method.
ここで5は前記スイツチング素子S1の出力部となる。
次に前記Si3N4膜10を前述の方法で全面除去した
後、前記2の表面に数千Aの厚さのSiO2膜(図示せ
ず)を形成する。Here, 5 is an output section of the switching element S1.
Next, after the Si3N4 film 10 is completely removed by the method described above, an SiO2 film (not shown) with a thickness of several thousand amps is formed on the surface of the film 2.
しかる後周知のフオトエツチング法により必要部分のS
iO2膜を除去した後、金属配線を行ない、領域3,4
,5に対して各々トランジスタT1のエミツタ端子13
,T1のベース及びスイツチング素子S1のゲート端子
14,S1の出力端子15を形成する。(第3図e)。
1以上の製造方法は製
造工程の制御性が良くかつ容易に本発明の構造が実現で
き、しかも他のバイボーラトランジスタと同一の工程で
製造可能であるという秀れた特徴を有するものである。
以上のように、本発明はチツプ面積、速度電力E積が小
さく、ゲート容量の小さい高速化をはかることができる
論理回路用半導体装置を得ることができる。After that, the necessary portions are etched using a well-known photoetching method.
After removing the iO2 film, metal wiring is performed to form regions 3 and 4.
, 5 respectively for the emitter terminal 13 of the transistor T1.
, T1, the gate terminal 14 of the switching element S1, and the output terminal 15 of S1. (Figure 3e).
One or more of the manufacturing methods have excellent characteristics in that the manufacturing process can be easily controlled, the structure of the present invention can be easily realized, and moreover, it can be manufactured in the same process as other bibolar transistors.
As described above, the present invention can provide a semiconductor device for logic circuits that has a small chip area, a small speed-power E product, a small gate capacitance, and is capable of achieving high speed.
第1図は従来のIIL構造の論理回路素子の構造図、第
2図は本発明の論理回路素子の要部を示し、aは要部平
面概略図、B,cはそれぞれB−B′,C−C線断面図
、第3図a−eは本発明にかかる素子の製造工程の一例
を示す工程断面図である。
1・・・・・・n+基板、2・・・・・・n一形M(ベ
ース)、7・・・・・・導電路、3・・・・・・ゲート
領域、4・・・・・・エミッタ領域、5・・・・・・n
+形領域、6・・・・・・絶縁物領域、1・・・・・・
入力端子、0t,02,0,・・・・・・出力端子、B
・・・・・・バイアス端子。FIG. 1 is a structural diagram of a conventional IIL-structured logic circuit element, and FIG. 2 shows the main parts of the logic circuit element of the present invention, where a is a schematic plan view of the main parts, B and c are B-B', respectively. A sectional view taken along the line C--C and FIGS. 3 a-e are process sectional views showing an example of the manufacturing process of an element according to the present invention. 1...n+ substrate, 2...n type M (base), 7...conducting path, 3...gate region, 4... ...Emitter area, 5......n
+ type area, 6...Insulator area, 1...
Input terminal, 0t, 02, 0, ... Output terminal, B
...Bias terminal.
Claims (1)
一方の導電形を有する半導体基体中に、互いに間隔を隔
てた前記横方向トランジスタのエミッタ領域及びコレク
タ領域として働く他方の導電形を有する少なくとも2つ
の領域を形成し、前記横方向トランジスタのコレクタ領
域中に、少なくとも1個の前記横方向トランジスタのコ
レクタ領域の表面より前記半導体基体中に到達しかつそ
の周囲が前記横方向トランジスタのコレクタ領域の表面
に近い領域では絶縁物からなる第1の領域で、それより
下部では前記横方向トランジスタのコレクタ領域でとり
囲まれた一方の導電形よりなる導電路を有し、この導電
路および前記横方向トランジスタのコレクタ領域をゲー
ト領域とするスイッチング素子を構成し、前記スイッチ
ング素子の導電路の少なくとも1部が前記ゲート領域の
拡散電位により空乏層で満たされていることを特徴とす
る半導体装置。 2 横方向トランジスタ構造のエミッタ領域に接続され
た電流源と、上記トランジスタ構造のコレクタ領域に接
続された入力信号源と、前記スイッチング素子の導電路
の上記トランジスタ構造のベース領域と異なる一端に接
続された出力端子とを備えたことを特徴とする特許請求
の範囲第1項に記載の半導体装置。Claims: 1. In a semiconductor body having one conductivity type serving as a base region of a lateral transistor, the other conductivity type serving as an emitter region and a collector region of said lateral transistor spaced apart from each other. forming at least two regions in the collector region of the lateral transistor, which reach into the semiconductor substrate from the surface of the collector region of at least one of the lateral transistors and whose periphery is the collector region of the lateral transistor; A first region made of an insulator in a region close to the surface of the region, and a conductive path of one conductivity type surrounded by a collector region of the lateral transistor below the first region; A semiconductor device comprising a switching element whose gate region is a collector region of a lateral transistor, wherein at least a portion of a conductive path of the switching element is filled with a depletion layer due to a diffusion potential of the gate region. 2. A current source connected to the emitter region of the lateral transistor structure, an input signal source connected to the collector region of the transistor structure, and a current source connected to one end of the conductive path of the switching element different from the base region of the transistor structure. 2. The semiconductor device according to claim 1, further comprising an output terminal.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51098517A JPS5910069B2 (en) | 1976-08-17 | 1976-08-17 | semiconductor equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51098517A JPS5910069B2 (en) | 1976-08-17 | 1976-08-17 | semiconductor equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5323583A JPS5323583A (en) | 1978-03-04 |
| JPS5910069B2 true JPS5910069B2 (en) | 1984-03-06 |
Family
ID=14221833
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP51098517A Expired JPS5910069B2 (en) | 1976-08-17 | 1976-08-17 | semiconductor equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5910069B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5482181A (en) * | 1977-12-14 | 1979-06-30 | Semiconductor Res Found | Electrostatic inductive integrated circuit device |
| JPS5482180A (en) * | 1977-12-14 | 1979-06-30 | Semiconductor Res Found | Electrostatic inductive integrated circuit device |
| JPS5518049A (en) * | 1978-07-25 | 1980-02-07 | Mitsubishi Electric Corp | Semiconductor device |
-
1976
- 1976-08-17 JP JP51098517A patent/JPS5910069B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5323583A (en) | 1978-03-04 |
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