JPH0368539B2 - - Google Patents
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- Publication number
- JPH0368539B2 JPH0368539B2 JP56043003A JP4300381A JPH0368539B2 JP H0368539 B2 JPH0368539 B2 JP H0368539B2 JP 56043003 A JP56043003 A JP 56043003A JP 4300381 A JP4300381 A JP 4300381A JP H0368539 B2 JPH0368539 B2 JP H0368539B2
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- semiconductor region
- region
- semiconductor
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- impurity density
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/80—FETs having rectifying junction gate electrodes
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- Bipolar Transistors (AREA)
- Bipolar Integrated Circuits (AREA)
- Junction Field-Effect Transistors (AREA)
- Logic Circuits (AREA)
Description
【発明の詳細な説明】
本発明は、ベース領域が殆んどピンチオフして
おり実効的なベース幅が十分薄くなるべく構成さ
れたベース順バイアスで不飽和電流電圧特性を示
すバイポーラトランジスタを用いた集積回路の新
規な構造に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention provides an integrated circuit using a bipolar transistor exhibiting unsaturated current-voltage characteristics with a base forward bias configured such that the base region is almost pinch-off and the effective base width is sufficiently thin. Concerning novel structures of circuits.
従来の集積回路においては、高速動作を要求さ
れる論理ゲート部に、バイポーラトランジスタ
(以下BPTと称す)が使用されている。BPTは
高速度の動作は行うが、MOS電解効果トランジ
スタ(以下MOSFETと称す)等に比し、消費電
力が大きく、入力インピーダンスが小さいため、
次段との直結が行なえないなどのため、集積度を
高くできず、高集積度を要求される半導体集積回
路に用いるには不利であるという致命的な欠点を
有している。更に、BPTは各電極間の領域が大
きいこと、ベース内に注入された少数キヤリアの
蓄積効果が顕著なことなどにより動作速度が制限
されている。こうしたBPTの欠点を除いて、高
入力インピーダンスで次段との直結が行なえ、各
電極間容量が小さくして、しかも変換コンダクタ
ンスがBPTにかなり近くて大きく、駆動能力が
大きく、高速度動作が行なえ、フアン・アウト数
を多く取れるトランジスタとして、本発明者によ
り静電誘導トランジスタが提案、開発され、
BPTのI2L(Integrated Injection Logic)等相当
する集積回路に応用され成果を収めている(特許
第1181984号(特公昭58−11102号)「半導体集積
回路」、特許第1208034号(特公昭58−38938号)
「半導体集積回路」、昭和51年9月1日乃至3日固
体素子国際会議予稿集pp.53〜54)。 In conventional integrated circuits, bipolar transistors (hereinafter referred to as BPTs) are used in logic gate sections that require high-speed operation. Although BPT operates at high speed, it consumes more power and has lower input impedance than MOS field effect transistors (hereinafter referred to as MOSFETs).
It has a fatal drawback in that it cannot be directly connected to the next stage, so it cannot achieve a high degree of integration, making it disadvantageous for use in semiconductor integrated circuits that require a high degree of integration. Furthermore, the operating speed of BPT is limited by the large area between each electrode and the significant accumulation effect of minority carriers injected into the base. Aside from these drawbacks of BPT, it has high input impedance and can be directly connected to the next stage, the capacitance between each electrode is small, the conversion conductance is quite close to that of BPT, and it has a large drive capacity and high-speed operation. , the inventor proposed and developed a static induction transistor as a transistor that can achieve a large number of fan-outs.
It has been successfully applied to integrated circuits such as BPT's I 2 L (Integrated Injection Logic) (Patent No. 1181984 (Special Publication No. 11102)) ``Semiconductor integrated circuit'', Patent No. 1208034 (Special Publication No. 1983-11102). −38938)
"Semiconductor Integrated Circuits", Proceedings of the International Conference on Solid State Devices, September 1-3, 1975, pp. 53-54).
ゲート領域近傍がほとんどピンチオフした状態
にあるトランジスタがゲートに逆バイアスを印加
した時空間電荷制限電流が流れ不飽和型電流電圧
特性を示すことは個別デバイスとしてはR.
Zuleeg(ツーレーグ)などにより知られていた
(米国特許第3409812号)が、ゲートに順バイアス
を印加した時は飽和型電流電圧特性を示すもので
あつた。 The fact that a transistor in which the vicinity of the gate region is almost pinched off with a reverse bias applied to the gate causes a spatio-temporal charge limited current to flow and exhibits unsaturated current-voltage characteristics means that as an individual device, R.
This was known by Zuleeg et al. (US Pat. No. 3,409,812), but it exhibited saturated current-voltage characteristics when a forward bias was applied to the gate.
本発明は順バイアスで不飽和型電流電圧特性を
示すBPTをEFL(Emitter Follwer Logic)集積
回路を用いることにより、少数キヤリア蓄積効果
が小さく周波数特性が良好で高速度動作の行なえ
る集積回路の新規な構造を提供することを目的と
している。 The present invention uses an EFL (Emitter Follwer Logic) integrated circuit for BPT, which exhibits unsaturated current-voltage characteristics in forward bias, to create a new integrated circuit that has a small minority carrier accumulation effect, good frequency characteristics, and high-speed operation. The purpose is to provide a structure.
以下図面を参照して本発明を詳細に説明する。 The present invention will be described in detail below with reference to the drawings.
第1図は3入力2出力のANDゲートの断面構
造例である。第1図はp領域の横方向不純物拡散
が起つた場合の例であり第1図でn+領域1,
1′、n-領域2は出力npn−BPTのコレクタ、p
領域4,51,52、n+領域13,23はそれ
ぞれ出力npn−BPTのベース、エミツタであり、
p領域6は入力pnp−BPTのエミツタで、n領域
7,17,27,37,8はベース、p領域9,
9′はコレクタである。10は絶縁層、31,3
2は出力電極、71,72,73は入力電極、
6′はnpn−BPTのベースとpnp−BPTのエミツ
タとを接続する第1の配線層、18はnpn−BPT
のコレクタに接続する電源供給用の第2の配線層
である。図示していないが6′と18は抵抗
(Rc)を介して接続されている。9′は基板の裏
面の電極によつて接地されている。領域13,2
3,6の不純物密度は1018〜1021cm-3程度、1、
1′,9′は1017〜1020cm-3程度、4,7,17,
27,37は1016〜1021cm-3程度、51,52,
8は1012〜1016cm-3程度、2,9は1012〜1017cm-3
程度である。11は絶縁用ポリシリコンもしくは
絶縁性樹脂で分離領域を形成している。動作をす
るためには、npn−BPTのエミツタ、コレクタ間
に存在するベース領域51,52が、n+pもしく
はn-p接触の拡散電位だけにより殆んど空乏層と
なつていなければならない。エミツタ、コレクタ
間に存在するベース51,52はp領域4からの
拡散によつて生じているから当然その不純物密度
はもともとの領域4よりは低くなつている。同様
にpnp−BPTのベース領域8はn+領域7,17,
27,37よりも低不純物密度になつており、エ
ミツタ領域6とのp+n接合およびコレクタ領域は
9とのnp接合の拡散電位だけで殆んど空乏層と
なつている。したがつて、第1図に召される構造
でベース領域51,52および8は厚さもかなり
薄くその不純物密度が低く、反対導電型領域との
接触部に生じる拡散電位だけで殆んど空乏層とな
り殆んどピンチオフした状態になつている。ベー
ス領域がピンチオフ状態になるとベース領域の電
位はその両側に存在する反対導電型領域の電位に
接近するが、ここではベースが完全にピンチオフ
せず極く薄い中性領域が残り、その電位が両側に
ある反対導電型領域の電位にまで接近しておら
ず、まだ電位障壁が存在して、しかもその厚さが
十分に薄く、エミツタからベースに向うキヤリア
の注入量制御を行なうようになつている状態をベ
ースが殆んど、ピンチオフした状態と定義する。
こうした状態になるようにベース領域の厚さ及び
不純物密度を選定すれば、エミツタからコレクタ
に流れるキヤリアは、静電誘導トランジスタの場
合と同様に、電位障壁を越えてコレクタ側に注入
され、ドリフト走行するというように、殆んど多
数キヤリア注入と同じ振舞いになり、従来の
BPTにおける少数キヤリア注入による、ベース
領域の少数キヤリア蓄積効果は現われない。前述
したベース領域51,52および8の存在によ
り、エミツタ、コレクタ間のチヤンネル長を短く
してもノーマリオフ型にしやすくなり、エミツ
タ、コレクタ間のキヤリア走行時間が短く、導通
時の電流が大きく、変換コンダクタンスが大き
く、高速化が容易で、しかも駆動能力が大きくな
る。同時に、またベース・エミツタ間、ベース・
コレクタ間容量が減少して動作速度は速くなる。
この集積回路に使用されるBPTはその寸法が非
常に小であるが、従来のBPTの動作速度を制限
するベース抵抗は、第1図の領域4および7,1
7,27,37の不純物密度を高くするなどして
おけば殆んど問題にならない。すなわち、ベース
の電位障壁は基本的には、ベース取り出し領域
4,7,17,27,37により容量結合的に制
御される。容量結合的な制御とは、通常のBPT
のようにベースにベースの少数キヤリアを注入し
て電位障壁の高さを制御するのではなく、ベース
取り出し電極に印加する電圧で制御することをい
う。つまり通常のBPTではベースの厚みを本発
明のように薄くした場合はベースの厚み方向に垂
直な方向の抵抗が増大して、この抵抗の効果で高
速な動作が不可能であるが、本発明では容量結合
であるので、ベース抵抗には関係なく高速に制御
できる。本発明に対し、通常のBPTのベース電
流による電位障壁の高さの制御は抵抗結合的な制
御である。本発明の容量結合的な制御はMOSト
ランジスタにおける電位障壁の高さ制御と似てお
り、原理的にはベースの構造をMOS型とするこ
とも可能である。第1図に示したpn接合ベース
構造で容量結合的に電位障壁を制御するために
は、pn接合に順方向に電圧を印加する時はpn接
合の接触電位以下の電圧を印加すれば、ベースに
少数キヤリアの注入はほとんど生じない。極くわ
ずかな少数キヤリアの注入が生じても、主なる電
位障壁制御が容量結合であればかまわないのはも
ちろんである。 FIG. 1 shows an example of the cross-sectional structure of an AND gate with three inputs and two outputs. Figure 1 shows an example where lateral impurity diffusion occurs in the p region.
1', n - region 2 is the collector of the output npn-BPT, p
Regions 4, 51, 52 and n + regions 13, 23 are the base and emitter of the output npn-BPT, respectively,
P region 6 is the emitter of input pnp-BPT, n regions 7, 17, 27, 37, 8 are the base, p region 9,
9' is a collector. 10 is an insulating layer, 31, 3
2 is an output electrode, 71, 72, 73 are input electrodes,
6' is the first wiring layer connecting the base of the npn-BPT and the emitter of the pnp-BPT, and 18 is the npn-BPT.
This is the second wiring layer for power supply connected to the collector of. Although not shown, 6' and 18 are connected via a resistor (Rc). 9' is grounded by an electrode on the back side of the substrate. Area 13,2
The impurity density of 3,6 is about 10 18 ~ 10 21 cm -3 , 1,
1', 9' are about 10 17 to 10 20 cm -3 , 4, 7, 17,
27, 37 is about 10 16 ~ 10 21 cm -3 , 51, 52,
8 is about 10 12 to 10 16 cm -3 , 2 and 9 are about 10 12 to 10 17 cm -3
That's about it. Reference numeral 11 forms an isolation region using insulating polysilicon or insulating resin. In order to operate, the base regions 51 and 52 existing between the emitter and collector of the npn-BPT must almost become a depletion layer due only to the diffusion potential of the n + p or n - p contact. Since the bases 51 and 52 existing between the emitter and the collector are formed by diffusion from the p region 4, their impurity density is naturally lower than that of the original region 4. Similarly, the base region 8 of pnp-BPT is n + region 7, 17,
The impurity density is lower than that of 27 and 37, and the p + n junction with the emitter region 6 and the collector region are almost depleted layers due to only the diffusion potential of the np junction with the emitter region 6. Therefore, in the structure shown in FIG. 1, the base regions 51, 52, and 8 are quite thin and have a low impurity density, and the base regions 51, 52, and 8 almost become depletion layers only due to the diffusion potential generated at the contact portion with the opposite conductivity type region. It's almost in a pinch-off state. When the base region is in a pinch-off state, the potential of the base region approaches the potential of the opposite conductivity type regions on both sides of the base region. The potential has not approached the potential of the region of the opposite conductivity type, and a potential barrier still exists, and its thickness is sufficiently thin to control the amount of carrier injection from the emitter to the base. The state is defined as a state in which the base is almost pinched off.
If the thickness and impurity density of the base region are selected to achieve this state, the carriers flowing from the emitter to the collector will be injected into the collector side over the potential barrier, just like in the case of a static induction transistor, and will drift. The behavior is almost the same as multiple carrier injection, and the conventional
The effect of minority carrier accumulation in the base region due to minority carrier injection in BPT does not appear. Due to the presence of the base regions 51, 52 and 8 described above, it is easy to create a normally-off type even if the channel length between the emitter and the collector is shortened, the carrier travel time between the emitter and the collector is short, the current when conducting is large, and the conversion is easy. The conductance is large, the speed can be easily increased, and the driving capacity is large. At the same time, between the base and emitter, the base
The inter-collector capacitance is reduced and the operating speed is increased.
Although the BPT used in this integrated circuit is very small in size, the base resistance, which limits the operating speed of conventional BPTs, is
If the impurity density of 7, 27, and 37 is increased, there will be almost no problem. That is, the potential barrier of the base is basically controlled by the base extraction regions 4, 7, 17, 27, and 37 in a capacitive coupling manner. Capacitively coupled control is normal BPT
The height of the potential barrier is not controlled by injecting base minority carriers into the base as in the example shown in Figure 2, but rather by controlling the height of the potential barrier by the voltage applied to the base extraction electrode. In other words, in a normal BPT, when the thickness of the base is made thin as in the present invention, the resistance in the direction perpendicular to the thickness direction of the base increases, and high-speed operation is impossible due to the effect of this resistance. Because it uses capacitive coupling, it can be controlled at high speed regardless of the base resistance. In contrast to the present invention, the control of the potential barrier height by the base current of a normal BPT is resistance-coupled control. The capacitive coupling control of the present invention is similar to the height control of a potential barrier in a MOS transistor, and in principle it is also possible to use a MOS type base structure. In order to control the potential barrier capacitively in the pn junction base structure shown in Figure 1, when applying a voltage in the forward direction to the pn junction, apply a voltage below the contact potential of the pn junction. injection of minority carriers rarely occurs. Of course, even if a very small amount of minority carriers are injected, it does not matter as long as the main potential barrier control is capacitive coupling.
第1図のように、ベース領域が殆んどピンチオ
フして薄い電位障壁がエミツタ、コレクタ間に残
るように形成されたBPTの電流電圧特性は、従
来のBPTおよび前述したR.Zuleegなどによるト
ランジスタ(米国特許第3409812号)が、あるコ
レクタ電圧以上ではコレクタ電流が殆んど一定に
なる飽和特性になるのに対し、コレクタ電圧が増
加するにつれて次第にコレクタ電流が増加する不
飽和型特性を示す。電位障壁層の厚さは、導通状
態にあるときに負荷に流す電流値などによつて決
まり、負荷に十分大きな電流を流す場合、例えば
TTL(Transistor Transistor Logic)ゲートを
駆動するような場合には十分薄して、しかもエミ
ツタ領域に近く設定しなければならない。第1図
ではコレクタ側にn-高抵抗領域が存在する場合
を示したが、n+領域が直接ベースに接触してい
ても、もちろんよいわけである。 As shown in Figure 1, the current-voltage characteristics of a BPT, which is formed so that the base region is almost pinched off and a thin potential barrier remains between the emitter and collector, are different from the conventional BPT and the transistor by R. Zuleeg mentioned above. (US Pat. No. 3,409,812) exhibits a saturated characteristic in which the collector current is almost constant above a certain collector voltage, whereas it exhibits an unsaturated characteristic in which the collector current gradually increases as the collector voltage increases. The thickness of the potential barrier layer is determined by the value of the current flowing through the load when it is in a conductive state, and when a sufficiently large current is flowing through the load, for example
When driving a TTL (Transistor Transistor Logic) gate, it must be sufficiently thin and set close to the emitter region. Although FIG. 1 shows the case where the n - high resistance region exists on the collector side, it is of course possible for the n + region to be in direct contact with the base.
又、第1図ではn+領域7,17,27,37、
n領域8が直接p領域9に接触しているが、n-
領域2を7,17,27,37と9および8と9
の間に入れても良い。 Also, in Fig. 1, n + areas 7, 17, 27, 37,
Although n region 8 is in direct contact with p region 9, n -
Area 2 to 7, 17, 27, 37 and 9 and 8 and 9
You can put it in between.
第1図は3入力2出力のANDゲートであるが
必要に応じて入力数、出力数を増減しても良いこ
とは当然である。 Although FIG. 1 shows an AND gate with three inputs and two outputs, it goes without saying that the number of inputs and the number of outputs may be increased or decreased as necessary.
これまで説明した本発明に用いたBPTは、も
ちろんこれらの構造に限るものではない。ベース
領域が主動作領域において殆んど、もしくは完全
にピンチオフして薄い電位障壁層が残るべく構成
されればよいのである。これまでのもので導電型
を全く反転したものでもよいことは勿論である。 Of course, the BPT used in the present invention described so far is not limited to these structures. It is sufficient if the base region is configured so that it is almost or completely pinched off in the main active region, leaving a thin potential barrier layer. It goes without saying that the conductivity type of the conventional one may be completely reversed.
本発明はEFLに関するものであるが、本発明
の構成要素であるBPTを他の論理ゲートたとえ
ばECL(Emitter Coupled Logic)NTL(Non
Threshold Logic)、DTL(Diode Tranistor
Logic)、RTL(Resistor Transistor Logic)、
TTL(Transistor Tranistor Logic)等に用いる
と、少数キヤリア蓄積効果が少なく、電極間容量
の小さいことなどにより高速度の動作が行なえる
半導体集積回路を得ることができる。 Although the present invention relates to EFL, BPT, which is a component of the present invention, can be used with other logic gates such as ECL (Emitter Coupled Logic) and NTL (Non
Threshold Logic), DTL (Diode Tranistor
Logic), RTL (Resistor Transistor Logic),
When used in TTL (Transistor Tranistor Logic), etc., it is possible to obtain a semiconductor integrated circuit that can operate at high speed due to the small minority carrier accumulation effect and small capacitance between electrodes.
第2図は第1図の回路表示でEFL相当の回路
に前述のBPTを使用した基本論理構成例であり、
3入力のANDゲートが構成されている。第1図
の電極71,72,73が、第2図のpnp−BPT
のベース電極A、B、Cにそれぞれ対応する。
npn−BPTが無くてもANDゲートの動作は可能
である。 Figure 2 is an example of a basic logic configuration using the above-mentioned BPT in a circuit equivalent to EFL in the circuit display of Figure 1.
A 3-input AND gate is configured. The electrodes 71, 72, 73 in Fig. 1 are the pnp-BPT in Fig. 2.
correspond to base electrodes A, B, and C, respectively.
AND gate operation is possible even without npn-BPT.
第1図乃至第2図の回路は、電極間容量が小さ
く、少数キヤリア蓄積効果が少なく、飽和型から
はずれた電流電圧特性を示して、入力インピーダ
ンスが従来のBPTより高く、動作速度が速い。
これらの回路を設計条件により適宜組合せれば、
所望の全ての動作を行なわせることができる。更
に前記BPTは優れた高周波特性を有しているも
ので集積化されたアナログ型演算増幅器をはじめ
としてアナログ型各種信号処理装置にも応用でき
ることは云うまでもない。 The circuits shown in FIGS. 1 and 2 have a small interelectrode capacitance, a small minority carrier accumulation effect, a current-voltage characteristic that deviates from the saturation type, an input impedance higher than that of the conventional BPT, and a faster operating speed.
If these circuits are combined appropriately depending on the design conditions,
All desired operations can be performed. Furthermore, since the BPT has excellent high frequency characteristics, it goes without saying that it can be applied to various analog signal processing devices including integrated analog operational amplifiers.
本発明の提供した構造を用いた半導体集積回路
は、従来良く知られていれ結晶成長技術、拡散技
術、イオン打ち込み技術、微細加工技術等により
製造することができる。とくにベース領域等を制
度よく制御するときなどはイオン打ち込み技術は
有効である。 A semiconductor integrated circuit using the structure provided by the present invention can be manufactured by conventionally well-known crystal growth techniques, diffusion techniques, ion implantation techniques, microfabrication techniques, and the like. Ion implantation technology is particularly effective when controlling the base region with good precision.
ベース領域が手動作領域において殆んどピンチ
オフした状態になるべく構成された前記BPTを
用いたEFLは、従来のベースからの少数キヤリ
アの注入を用いた抵抗結合的電位障壁制御の
EFLと異なり、ベースに印加される電圧により
容量結合的な電位障壁制御を行うことにより動作
するので、少数キヤリア蓄積効果が少なく、各電
極間容量も小さく、ベース領域をキヤリアが拡散
する状態を含まず、またエミツタ、コレクタ間の
チヤンネル長を短くすることが容易で、キヤリア
の走行時間も短く、周波数特性が良好で、高速度
の動作が行え、しかも駆動能力が大きく、フア
ン・アウト数が多く取れ、その工業的価値は極め
て高い。 The EFL using the BPT, in which the base region is configured to be almost pinched off in the manual operation region, is based on conventional resistance-coupled potential barrier control using minority carrier injection from the base.
Unlike EFL, it operates by performing capacitive coupling potential barrier control using the voltage applied to the base, so there is little minority carrier accumulation effect, the capacitance between each electrode is small, and it does not include the state in which carriers diffuse through the base region. In addition, it is easy to shorten the channel length between the emitter and collector, the carrier travel time is short, the frequency characteristics are good, high speed operation is possible, and the drive capacity is large and the number of fan outs is large. Its industrial value is extremely high.
第1図は、ベース領域が殆んどピンチオフ状態
にあるBPTを用いたEFLANDゲートの構造例を
示す図、第2図は第1図の回路表示を示す図であ
る。
FIG. 1 is a diagram showing a structural example of an EFLAND gate using BPT whose base region is almost in a pinch-off state, and FIG. 2 is a diagram showing a circuit representation of FIG. 1.
Claims (1)
前記第1の半導体領域の上部に形成された第2導
電型低不純物密度の第2の半導体領域2と、前記
第2の半導体領域の上部に形成された第1導電型
高不純物密度の第3の半導体領域6と、前記第3
の半導体領域に隣接し、前記第2の半導体領域の
表面からの深さが前記第3の半導体領域よりも深
く形成された第2導電型高不純物密度の少なく共
2つ以上の第4の半導体領域7,17,27,3
7と、前記第3の半導体領域の底部に、前記第4
の半導体領域と隣接して形成された第2導電型の
不純物密度1012〜1016cm-3の第5の半導体領域8
と、前記第4の半導体領域の上部に形成された少
なく共2つ以上の独立した入力信号用電極71,
72,73と、前記第1の半導体領域の上部の一
部に形成された第2導電型高不純物密度の第6の
半導体領域1と、前記第6の半導体領域の上部に
形成された第2導電型高不純物密度の第7の半導
体領域13,23と、前記第7の半導体領域に隣
接し、前記第7の半導体領域よりも深く形成され
た第1導電型高不純物密度の第8の半導体領域4
と、前記第7の半導体領域の底部に前記第8の半
導体領域と隣接して形成された第1導電型の不純
物密度1012〜1016cm-3の第9の半導体領域51,
52と、前記第7の半導体領域の上部に形成され
た出力信号用電極31,32と、前記第3の半導
体領域と前記第8の半導体領域を接続し、共に抵
抗Rcを介して電源に接続する第1の配線層6′
と、前記第6の半導体領域の上部に前記第6の半
導体領域と隣接して形成された第2導電型高不純
物密度の第10の半導体領域1′と、前記第10の半
導体領域の上部に形成され、前記電源に接続され
た第2の配線層18と、前記第4の半導体領域と
前記第8の半導体領域の間に形成された分離領域
11とから少なく共構成され、前記第5および第
9の半導体領域がその上下の半導体領域との接触
部に生じる拡散電位で薄い中性領域を残してほと
んど空乏層となるように前記第5および第9の半
導体領域の厚みと不純物密度とが選定され、前記
薄い中性領域に形成された電位障壁の高さが、前
記第4および第8の半導体領域に印加される電圧
により容量結合的に制御されることを特徴とする
半導体集積回路。1 first conductivity type first semiconductor regions 9, 9';
A second semiconductor region 2 of a second conductivity type with a low impurity density formed above the first semiconductor region, and a third semiconductor region 2 of a first conductivity type with a high impurity density formed above the second semiconductor region. the third semiconductor region 6;
at least two or more fourth semiconductors of a second conductivity type with high impurity density, which are adjacent to the semiconductor region of the second semiconductor region and are formed deeper from the surface of the second semiconductor region than the third semiconductor region; Area 7, 17, 27, 3
7 and the fourth semiconductor region at the bottom of the third semiconductor region.
A fifth semiconductor region 8 having a second conductivity type impurity density of 10 12 to 10 16 cm -3 formed adjacent to the semiconductor region 8
and at least two or more independent input signal electrodes 71 formed on the fourth semiconductor region,
72, 73, a second conductivity type high impurity density sixth semiconductor region 1 formed in a part of the upper part of the first semiconductor region, and a second semiconductor region 1 formed in the upper part of the sixth semiconductor region. seventh semiconductor regions 13 and 23 of high impurity density of conductivity type; and an eighth semiconductor of high impurity density of first conductivity type formed adjacent to the seventh semiconductor region and deeper than the seventh semiconductor region; Area 4
and a ninth semiconductor region 51 having a first conductivity type impurity density of 10 12 to 10 16 cm -3 formed at the bottom of the seventh semiconductor region adjacent to the eighth semiconductor region,
52, the output signal electrodes 31 and 32 formed on the upper part of the seventh semiconductor region, and the third semiconductor region and the eighth semiconductor region are connected, and both are connected to a power supply via a resistor Rc. The first wiring layer 6'
a tenth semiconductor region 1' of a second conductivity type with high impurity density formed above the sixth semiconductor region and adjacent to the sixth semiconductor region; A second wiring layer 18 formed and connected to the power supply, and an isolation region 11 formed between the fourth semiconductor region and the eighth semiconductor region, and The thickness and impurity density of the fifth and ninth semiconductor regions are set such that the ninth semiconductor region becomes almost a depletion layer, leaving a thin neutral region due to the diffusion potential generated at the contact portions with the semiconductor regions above and below it. A semiconductor integrated circuit characterized in that the height of the potential barrier selected and formed in the thin neutral region is controlled in a capacitive coupling manner by voltages applied to the fourth and eighth semiconductor regions.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4300381A JPS56153774A (en) | 1981-03-23 | 1981-03-23 | Semiconductor integrated circuit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4300381A JPS56153774A (en) | 1981-03-23 | 1981-03-23 | Semiconductor integrated circuit |
Related Parent Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP52015880A Division JPS5853517B2 (en) | 1977-02-02 | 1977-02-15 | semiconductor integrated circuit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56153774A JPS56153774A (en) | 1981-11-27 |
| JPH0368539B2 true JPH0368539B2 (en) | 1991-10-28 |
Family
ID=12651815
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4300381A Granted JPS56153774A (en) | 1981-03-23 | 1981-03-23 | Semiconductor integrated circuit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS56153774A (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3409812A (en) * | 1965-11-12 | 1968-11-05 | Hughes Aircraft Co | Space-charge-limited current triode device |
-
1981
- 1981-03-23 JP JP4300381A patent/JPS56153774A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56153774A (en) | 1981-11-27 |
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