JPS584825B2 - Hand tie souchi - Google Patents

Hand tie souchi

Info

Publication number
JPS584825B2
JPS584825B2 JP50096785A JP9678575A JPS584825B2 JP S584825 B2 JPS584825 B2 JP S584825B2 JP 50096785 A JP50096785 A JP 50096785A JP 9678575 A JP9678575 A JP 9678575A JP S584825 B2 JPS584825 B2 JP S584825B2
Authority
JP
Japan
Prior art keywords
region
conductivity type
base
layer
substrate
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
JP50096785A
Other languages
Japanese (ja)
Other versions
JPS5220778A (en
Inventor
中井正則
徳丸征也
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura 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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP50096785A priority Critical patent/JPS584825B2/en
Publication of JPS5220778A publication Critical patent/JPS5220778A/en
Publication of JPS584825B2 publication Critical patent/JPS584825B2/en
Expired legal-status Critical Current

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Classifications

    • H—ELECTRICITY
    • H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D84/00—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
    • H10D84/60—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers characterised by the integration of at least one component covered by groups H10D10/00 or H10D18/00, e.g. integration of BJTs
    • H10D84/65—Integrated injection logic

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  • Bipolar Integrated Circuits (AREA)
  • Logic Circuits (AREA)
  • Bipolar Transistors (AREA)

Description

【発明の詳細な説明】 この発明は互に極性の異る横方向及び縦方向の二個のト
ランジスタ、(以後Trと略記する。
DETAILED DESCRIPTION OF THE INVENTION The present invention provides two transistors (hereinafter abbreviated as Tr), one in the horizontal direction and the other in the vertical direction, which have mutually different polarities.

)を備えて論理回路を構成する半導体装置に関する。) to constitute a logic circuit.

近年、DTL,TTL,CML等の従来からある論理回
路とは異って、これらより構造が簡単で製造歩留りが高
く、集積度を向上し、かつ消費電力の少ない論理回路が
注目されている。
In recent years, unlike conventional logic circuits such as DTL, TTL, and CML, logic circuits that have a simpler structure, higher manufacturing yield, improved integration, and lower power consumption have attracted attention.

例えば半導体基体にインバータ素子として働く縦方向T
rと、このTrのベース領域に少数キャリアを注入する
横方向Trとが設けられ、この少数キャリアをインバー
タTrのベース領域へ注入しつつ、入力を制御してコレ
クタ出力を有効に制御しようとするものがある。
For example, in the vertical direction T that acts as an inverter element on a semiconductor substrate
r and a lateral Tr that injects minority carriers into the base region of this Tr, and attempts to effectively control the collector output by controlling the input while injecting the minority carriers into the base region of the inverter Tr. There is something.

この論理素子の構造を第1図断面図で説明する。The structure of this logic element will be explained with reference to the sectional view in FIG.

任意の例えばN導電型を有する半導体基板1に気相成長
法でこの半導体基板1より不純物濃度の低いN導電型の
エビタキシャル層2を積層し、ここにP導電型領域3,
4を約1017〜1019atoms/cm3の硼素を
選択拡散して形成する。
For example, an N conductivity type epitaxial layer 2 having a lower impurity concentration than this semiconductor substrate 1 is laminated on an arbitrary semiconductor substrate 1 having an N conductivity type by a vapor phase growth method, and a P conductivity type region 3,
4 is formed by selectively diffusing boron at about 1017 to 1019 atoms/cm3.

このP導電型領域3には1018〜1021atoms
/cm3の燐を拡散してN導電型領域5を形成する。
This P conductivity type region 3 has 1018 to 1021 atoms.
/cm3 of phosphorus is diffused to form an N conductivity type region 5.

尚前記エビタキシャル層2の不純物濃度ぱP導電型領域
3,4のそれより低濃度にしてある。
The impurity concentration of the epitaxial layer 2 is lower than that of the P conductivity type regions 3 and 4.

この結果、P導電型領域4をエミッタ領域、エビタキシ
ャル層2をベース領域、P導電型領域3をコレクタ領域
とした横力向PNPTrと、エビタキシャル層2をエミ
ツタ領域、P導電型領域3をベース領域、N導電型領域
5をコレクタ領域とした縦方向NPNTrとが形成され
る。
As a result, a lateral force direction PNPTr is obtained in which the P conductivity type region 4 is an emitter region, the epitaxial layer 2 is a base region, and the P conductivity type region 3 is a collector region. A base region and a vertical NPNTr with N conductivity type region 5 as a collector region are formed.

ここでP導電型領域4と、エビタキシャル層2から形成
されたPN接合に順方向電圧を印加したとすると正孔は
この領域4からエビタキシャル層2を通ってP導電型領
域3へと注入される。
Here, if a forward voltage is applied to the PN junction formed from the P conductivity type region 4 and the epitaxial layer 2, holes will be injected from this region 4 through the epitaxial layer 2 into the P conductivity type region 3. be done.

第2図はこの論理素子の等価回路を示すもので、ここで
Epぱ定電流源接続端子、Bは信号入力端子、Cは出力
端子、ENは接地端子とする。
FIG. 2 shows an equivalent circuit of this logic element, where Ep is a constant current source connection terminal, B is a signal input terminal, C is an output terminal, and EN is a ground terminal.

今端子Bの入力信号が“1”レベル(例えば0.7ボル
ト)であると、端子EPより注入された外部エミッタ電
流IHPは横力向PNPTrのベース接地電流増巾率α
PNP倍つまりIEP×αPNPとなってこのTrのコ
レクタ領域であると共に縦方向NPNTrのベース領域
であるP導電型領域3へ流れる。
Now, when the input signal of terminal B is at "1" level (for example, 0.7 volts), the external emitter current IHP injected from terminal EP has a base ground current amplification rate α of lateral force direction PNPTr.
PNP times that is, IEP×αPNP, and flows to the P conductivity type region 3, which is the collector region of this Tr and the base region of the vertical NPNTr.

従って縦方向NPNTrがオンとなり、端子Cの出力ぱ
“0“レベルとなる。
Therefore, the vertical NPNTr is turned on, and the output of the terminal C becomes the "0" level.

更にこの出力端子Cに生ずるコレクタ出力電流は前記縦
方向NPNTrのベース電流をその電流増巾率βNPN
倍した値まで許るされる。
Furthermore, the collector output current generated at this output terminal C increases the base current of the longitudinal NPNTr by its current amplification rate βNPN.
Up to the multiplied value is allowed.

逆に端子Bの入力信号が“0”レベル(例えばOボルト
)であると、端子EPから注入された外部エミツタ電流
IBPは入力端子Bへと流出して縦方向NPNTrのベ
ース電流とはならず、このために縦方向NPNTrはオ
フ状態となって端子Cの出力は“1”レヘルとなる。
Conversely, when the input signal at terminal B is at the "0" level (for example, O volts), the external emitter current IBP injected from terminal EP flows to input terminal B and does not become the base current of the vertical NPNTr. Therefore, the vertical NPNTr is turned off, and the output of the terminal C becomes "1" level.

このように入出力信号レベルが互に反転するインバータ
特性を持った論理素子はこれを組合せてNAND,NO
R,FUP・FLOP等基本的な論理回路を構成できる
し、更に複雑な機能を持った高密度集積回路も実現可能
にする。
In this way, logic elements with inverter characteristics where the input and output signal levels are mutually inverted can be combined into NAND, NO
It is possible to configure basic logic circuits such as R, FUP, FLOP, etc., and it also makes it possible to realize high-density integrated circuits with more complex functions.

このような論理素子の消費電力は横方向PNPTrの特
性、即ちベース接地された電流増巾率αPNPにより大
きく影響を受け、とのαPNPの値が理想値1に近づく
程少なくなる。
The power consumption of such a logic element is greatly influenced by the characteristics of the lateral PNPTr, that is, the base-grounded current amplification factor αPNP, and decreases as the value of αPNP approaches the ideal value 1.

またインバータ素子の最高スピード周波数特性、ファン
アウト雑音余裕度等は縦方向NPNTrの特性、とりわ
けエミツタ接地された電流増巾率βNPN及び利得帯域
巾積hによって影響を受ける。
Further, the maximum speed frequency characteristics, fan-out noise margin, etc. of the inverter element are influenced by the characteristics of the vertical NPNTr, especially the current amplification factor βNPN whose emitter is grounded and the gain bandwidth h.

従ってこの論理素子では横方向PNPTrと縦方向NP
NTrのそれぞれの電流増巾率と縦力向NPNTrの
利得帯域巾積fTを同時に高めることが重要である。
Therefore, in this logic element, the horizontal direction PNPTr and the vertical direction NP
It is important to simultaneously increase the current amplification factor of each NTr and the gain band width fT of the NPNTr in the longitudinal force direction.

一般にTrの電流増巾率はキャリアの注入効率とその輸
送効率との良否によって大きな影響をうける。
Generally, the current amplification rate of a Tr is greatly influenced by the quality of carrier injection efficiency and carrier transport efficiency.

単位入力電流に対して、どれだけの少数キャリアがエミ
ツタ領域からベース領域からベース領域へ注入されるか
という効率を示すのが、キャリアの注入効率であシ、エ
ミツタ電流Ie、そのうちのベース領域での電流成分■
epをそれぞれ仮定するとき;次式で示される。
The carrier injection efficiency indicates how many minority carriers are injected from the emitter region to the base region for a unit input current. Current component of ■
When assuming each ep; it is expressed by the following equation.

それ故キャリア注入効率を改善するためには、エミツタ
領域の不純物濃度をベース領域のそれに対して適当な比
に設定するとともに、エミツタ・ベースの接合面には適
当な不純物濃度の勾配をもたせて、ベース領域に注入さ
れるキャリアの数を増大せしめるとともに、注入された
キャリアに正方向の加速電界が働くようにすればよい。
Therefore, in order to improve the carrier injection efficiency, the impurity concentration in the emitter region is set to an appropriate ratio to that in the base region, and the emitter-base junction interface has an appropriate impurity concentration gradient. What is necessary is to increase the number of carriers injected into the base region and apply an accelerating electric field in the positive direction to the injected carriers.

一方、ベース領域内でのキャリアの輸送効率に関しては
、ベース領域内でのキャリアの拡散距離Lb、ベース領
域の巾Wをそれぞれ仮定するとき次式で示される。
On the other hand, the transport efficiency of carriers within the base region is expressed by the following equation, assuming the carrier diffusion distance Lb within the base region and the width W of the base region.

したがってこのキャリアの輸送効率を改善するためには
、エミツタ領域から注入されたベース領域中のキャリア
がコレクタ領域に到達するまでの実効的な距離すなわち
ベース巾Wをできるだけ狭くして、かつこのキャリアが
ベース領域内の再結合中心に補獲され消失しないように
することが重要である。
Therefore, in order to improve the transport efficiency of carriers, the effective distance for the carriers injected from the emitter region to reach the collector region, that is, the base width W, should be made as narrow as possible, and the carriers should be It is important to prevent the recombination center in the base region from being captured and lost.

ところで前記第1図の構造素子で横方向PNPTrのエ
ミツタ領域4とベース領域2の不純物濃度の比を適当な
値に設定し、かつベース領域内での再結合中心密度を低
くすることは比較的容易に行なうことができる。
By the way, in the structural element shown in FIG. 1, it is relatively easy to set the ratio of the impurity concentrations of the emitter region 4 and the base region 2 of the lateral PNPTr to an appropriate value and to lower the density of recombination centers in the base region. It can be done easily.

しかしキャリアの輸送効率を改善ナるためにベース巾を
狭くすることは写真蝕刻技術、とくにマスク精度に大き
く制約されていて、その技術的限界が5〜10μmの現
状においては、一定の限界がある。
However, narrowing the base width in order to improve carrier transport efficiency is greatly restricted by photoetching technology, especially mask accuracy, and at present, the technical limit is 5 to 10 μm, so there is a certain limit. .

しかも、エミツタ領域とコレクタ領域はともにN導電型
エビタキシャル層2に相対して拡散形成されたP導電型
不純物拡散領域4,3からそれぞれ成るので、双方とも
対向する拡散側面は深さ方向で末広がりに遠去かる。
Furthermore, since both the emitter region and the collector region are composed of P-conductivity type impurity diffusion regions 4 and 3 which are diffused and formed opposite to the N-conductivity type epitaxial layer 2, the opposing diffusion side surfaces of both sides widen toward the end in the depth direction. go far away.

このためN導電型エビタキシャル層2の内部において、
拡散が深くなる程、相対する二箇のP導電型領域4,3
間に形成されるベース巾は急激に増大する。
Therefore, inside the N-conductivity type epitaxial layer 2,
The deeper the diffusion, the more the two opposing P conductivity type regions 4, 3
The width of the base formed between them increases rapidly.

したがって接合面積を広くしようとすればする程ベース
巾が拡がシキャリアの輸送効率は著しく劣化する。
Therefore, the wider the bonding area is, the wider the base width is, and the transport efficiency of carriers is significantly degraded.

またエミツタ領域4とベース領域2の全接合面部におい
ては前述の様にP導電型不純物が対向する領域側面を深
さ方向で遠去けるよう拡散されているので、不純物濃度
勾配はきわめて緩やかであり、キャリアの注入効率が悪
い。
Furthermore, in the entire junction area between the emitter region 4 and the base region 2, as mentioned above, the P conductivity type impurity is diffused so as to be far away from the side surfaces of the opposing regions in the depth direction, so the impurity concentration gradient is extremely gentle. , carrier injection efficiency is poor.

したがって従来の構造において横方向PNPTrの高い
電流増巾率を得ることは非常に困難である。
Therefore, it is very difficult to obtain a high current amplification rate for the lateral PNPTr in the conventional structure.

又前記第1図の構造を有する従来の縦方向NPNTrに
おいては、N導電型エビタキシャル層2をエミツタ領域
K用い、さらにそこに形成した二重拡散層をペース領域
とコレクタ領域として用いているので、ベース巾を狭く
することは比較的容易であるが、エミツタ領域の不純物
濃度はベース領域のそれより低くならざるを得ない。
Furthermore, in the conventional vertical NPNTr having the structure shown in FIG. 1, the N-conductivity type epitaxial layer 2 is used as the emitter region K, and the double diffusion layer formed therein is used as the pace region and the collector region. Although it is relatively easy to narrow the base width, the impurity concentration in the emitter region must be lower than that in the base region.

その上、ベース領域に注入されたキャリアにはその不純
物濃度勾配に基因して減速電界がかかるため、注入効率
を低下し、N導電型エビタキシャル層2をエミツタ領域
とする、いわゆる逆方向動作の電流増巾率は極めて低い
。
Furthermore, carriers injected into the base region are subjected to a decelerating electric field due to the impurity concentration gradient, which reduces injection efficiency and prevents so-called reverse operation in which the N-conductivity type epitaxial layer 2 is used as an emitter region. Current amplification rate is extremely low.

さらにこの論理素子においては横方向PNPTrと縦方
向NPNTrの領域の一部が互に併合されているので、
一方のTrの電流増巾率をより高める方向に不純物濃度
比を設定しても、それは他方のTrの電流増巾率にとっ
てはより悪い結果となってしまう。
Furthermore, in this logic element, parts of the horizontal PNPTr and vertical NPNTr regions are merged with each other, so
Even if the impurity concentration ratio is set so as to further increase the current amplification rate of one Tr, this results in a worse result for the current amplification rate of the other Tr.

例えば横方向PNPTrのキャリア注入効率を改善しよ
うとして、ベース領域即ちN導電型エビタキシャル層2
の不純物濃度を下げると、とのN導電型エビタキシャル
層2は縦方向NPNTrのエミツタ領域そのものでもあ
るので縦方向NPNTrのキャリア注入効率が著しく悪
くなってしまう。
For example, in an attempt to improve the carrier injection efficiency of a lateral PNPTr, the base region, that is, the N-conducting type epitaxial layer 2
When the impurity concentration of is lowered, the carrier injection efficiency of the vertical NPNTr becomes significantly worse because the N-conductivity type epitaxial layer 2 is also the emitter region of the vertical NPNTr.

尚この縦方向NPNTrの利得帯域巾積fTは、今まで
の説明で明らかなように、低い電流増巾率とエミツタ領
域がN導電型エビタキシャル層2全体で構成されている
ことにより、やはり低い値しか得ることができなかった
。
As is clear from the above explanation, the gain band width fT of this vertical NPNTr is still low due to the low current amplification rate and the fact that the emitter region is composed of the entire N-conducting type epitaxial layer 2. I could only get value.

これ等種々の欠点は、この論理素子の低消費電力性、高
速性に一定の限界があることを示唆し、とくに高周波領
域での動作がほとんど不可能であることを明示していた
。
These various drawbacks suggested that there were certain limits to the low power consumption and high speed performance of this logic element, and in particular made it clear that operation in a high frequency region was almost impossible.

本発明は上記の欠点を除去し改良された半導体装置を提
供するもので、第一に電源及び負荷となるTrの電流増
巾率を改善することによシ、消費電力を少なくし、第二
にインバータ素子となるTrの順逆両方向の電流増巾率
を同時に改善し、電流ホツキング現象を防止するととも
に、素子の高速化、高周波化を図るものである。
The present invention eliminates the above-mentioned drawbacks and provides an improved semiconductor device.First, by improving the current amplification rate of the transistor serving as a power source and load, power consumption is reduced; The present invention simultaneously improves the forward and reverse current amplification factors of the Tr, which serves as an inverter element, to prevent the current hocking phenomenon, and to increase the speed and frequency of the element.

即ちこの発明は一方導電型半導体基体表面から深さ方向
に設けられる他方導電型堰層と、堰層の底領域に接続し
て基体内に基体分離域を区界する他方導電型遮断層と、
堰層の内側に形成され分離域をコレクタ領域とし堰層を
ベース領域とする横方向Trのエミツタ領域となる一方
導電型領域と、基体分離域の内側に形成され基体分離域
をベース領域とし遮断層をエミツタ領域とする縦方向T
rのコレクタ領域となる他方導電型領域と、縦方向Tr
のベース領域に設けられ電極で互に接続されるベース接
続用領域及び一方導電型キャリア吸出し領域と、縦方向
Trベース領域表面に形成される一乃至複数箇の金属半
導体間整流性接触ダイオードを備える半導体装置にある
。
That is, the present invention provides a barrier layer of the other conductivity type provided in the depth direction from the surface of the semiconductor substrate of the one conductivity type, a blocking layer of the other conductivity type connected to the bottom region of the barrier layer and demarcating a substrate separation region within the substrate;
A conductivity type region is formed inside the weir layer and serves as an emitter region of a lateral Tr, with the isolation region as the collector region and the weir layer as the base region, and a conductivity type region is formed inside the substrate separation region and serves as the base region for isolation. Vertical direction T with layer as emitter region
the other conductivity type region which becomes the collector region of r, and the longitudinal direction Tr
A base connection region and a one conductivity type carrier extraction region provided in the base region and connected to each other by electrodes, and one or more metal-semiconductor rectifying contact diodes formed on the surface of the vertical Tr base region. Found in semiconductor devices.

この発明で一方導電型半導体基体はP導電型又はN導電
型の何れか一方であって良い。
In this invention, one conductivity type semiconductor substrate may be either P conductivity type or N conductivity type.

そしてこの基体は一体であって良く、又例えば基板上に
形成された気相成長層のように積層体の一層であっても
良い。
The substrate may be integral or may be one layer of a laminate, such as a vapor growth layer formed on a substrate.

他方導電型遮断層は一方導電型基体の一側とPN接合を
形成する層であって、一方導電型基体より高濃度とし、
普通他方導電型堰層と同一濃度であるか又はより高濃度
とする。
The other conductivity type blocking layer is a layer that forms a PN junction with one side of the one conductivity type substrate, and has a higher concentration than the one conductivity type substrate,
Usually, the concentration is the same as that of the other conductive type weir layer, or the concentration is higher.

一方導電型堰層は他方導電型遮断層に到達し、一方導電
型基体より高濃度とする。
The weir layer of one conductivity type reaches the blocking layer of the other conductivity type and has a higher concentration than the substrate of one conductivity type.

基体分離域は他方導電型堰層及び他方導電型遮断層で囲
まれた基体の一部一方導電型領域を意味する。
The substrate separation region refers to a portion of one conductivity type region of the substrate surrounded by a weir layer of the other conductivity type and a barrier layer of the other conductivity type.

このようなこの発明の半導体装置では、堰層をベース領
域としこの堰層内にエミツタ領域を形成して分離域をコ
レクタ領域とする横方向Tr分離域をベース領域としこ
の分離域内にコレクタ領域を形成して遮断層をエミツタ
領域とする第二の縦方向Tr、前記縦方向Trのベース
領域に設けられ特設又はベース電極の何れかであって良
い電極の直下のベース接続用領域及びベース領域とは反
対導電型のキャリア吸出し領域、並びに縦方向Trのベ
ース領域に設けられた金属半導体間整流性接触ダイオー
ドが併設されている。
In such a semiconductor device of the present invention, the weir layer is used as a base region, the emitter region is formed within this weir layer, and the isolation region is used as a collector region.The lateral Tr isolation region is used as a base region, and a collector region is formed within this isolation region. a second longitudinal Tr formed and having a blocking layer as an emitter region; a base connection region and a base region immediately below an electrode that is provided in the base region of the longitudinal Tr and may be either a special electrode or a base electrode; A carrier extraction region of opposite conductivity type and a metal-semiconductor rectifying contact diode provided in the base region of the vertical Tr are also provided.

従って横方向Trに於いてはエミツタ領域からベース領
域へのキャリアの注入効率が著しく改善され、さらにキ
ャリアに加速電界がかかるので高い電流増巾率が実現さ
れる。
Therefore, in the lateral Tr, the injection efficiency of carriers from the emitter region to the base region is significantly improved, and furthermore, since an accelerating electric field is applied to the carriers, a high current amplification rate is realized.

一方縦方向Trに於いては、コレクタ領域とベース領域
並びにこれと対峙して設置されたエミツタ領域となる遮
断層との不純物濃度比を適当にとることが可能となり、
さらにベース領域の不純物濃度がほゞ一定であるので遮
断層をエミツタ領域として行わせる順方向動作の電流増
巾率は広い電流範囲にわたって高い値をとることが出来
る。
On the other hand, in the vertical direction Tr, it is possible to set an appropriate impurity concentration ratio between the collector region, the base region, and the blocking layer which is the emitter region and is placed facing the collector region.
Further, since the impurity concentration in the base region is approximately constant, the current amplification factor in the forward direction operation in which the blocking layer is used as the emitter region can take a high value over a wide current range.

ここで順方向動作の電流増巾率が十分に高いことはこの
論理素子の高速性、ファンアウト、雑音余裕度等が従来
のものに比較して著しく改善されることを示す。
Here, the fact that the current amplification factor in the forward direction operation is sufficiently high indicates that the high speed performance, fan-out, noise margin, etc. of this logic element are significantly improved compared to conventional ones.

また分離域内の他方導電型領域をエミツタ領域として行
わせる逆方向動作の電流増巾率を適切な値に設定できる
ことは、DCTL回路で問題であったいわゆる大ファイ
ン・ゲート数による入力電流のホツギング現象の防止を
完全なものとし、更にベース領域と短絡されたキャリア
吸い出し領域の存在と相まって過剰少数キャリアの蓄積
を少くして素子の高速化を図ることができることを意味
する。
In addition, being able to set the current amplification factor of the reverse operation in which the other conductivity type region in the isolation region is performed as an emitter region to an appropriate value is a problem in the hogging of the input current due to the so-called large number of fine gates, which was a problem in DCTL circuits. This means that the device can be completely prevented from accumulating excess minority carriers, and the speed of the device can be increased by combining this with the presence of the carrier sucking region short-circuited with the base region.

又金属一半導体整流性接触ダイオードが組み込まれてい
るために縦方向Trの論理振幅がその順方向電圧分だけ
下り作動を高速にする。
Further, since a metal-semiconductor rectifying contact diode is incorporated, the logical amplitude of the vertical Tr increases the speed of the downward operation by the forward voltage thereof.

更にもしもこのダイオードを複数個と縦方mTrのコレ
クタ領域を複数箇設けるとこの素子は多入力多出力NA
ND機能を備えるものとならて集積度を良好にする。
Furthermore, if a plurality of diodes and a plurality of vertical mTr collector regions are provided, this element becomes a multi-input multi-output NA
Since it is equipped with an ND function, the degree of integration is improved.

この場合ダイオード及びコレクタの個数は対応しても対
応しなくても良い。
In this case, the numbers of diodes and collectors may or may not correspond.

以下実施例について述べる。Examples will be described below.

この例の断面図を第3図に、等価回路図を第4図に示す
。
A cross-sectional view of this example is shown in FIG. 3, and an equivalent circuit diagram is shown in FIG.

第3図で遮断層として用いられる例えばN導電型ケイ素
基板は高濃度N十導電型基板11上に半導体基体として
用いられる低濃度P−導電型或いはπ導電型基体12を
形成する。
For example, an N conductivity type silicon substrate used as a blocking layer in FIG. 3 forms a low concentration P-conductivity type or π conductivity type substrate 12 used as a semiconductor substrate on a high concentration N0 conductivity type substrate 11.

基体12の不純物濃度は遮断層11のそれよりも著しく
低くするため例えば10l4〜1016cm−3とし、
ホウ素をP導電型不純物として添加してある。
In order to make the impurity concentration of the substrate 12 significantly lower than that of the blocking layer 11, the impurity concentration is set to, for example, 10l4 to 1016 cm-3,
Boron is added as a P conductivity type impurity.

基体12は通常のケイ素エビタキシャル成長法を用いて
遮断層上に形成し、その膜厚は例えば2〜5μmとする
。
The substrate 12 is formed on the barrier layer using a conventional silicon epitaxial growth method, and has a thickness of, for example, 2 to 5 μm.

次に基体12の表面に絶縁膜として通常の高温酸化雰囲
気中で二酸化ケイ素膜を被着形成し、横力向Trのベー
ス領域となる堰層13を形成するために光蝕刻を行って
この二酸化ケイ素膜を所定パターンで開孔する。
Next, a silicon dioxide film is deposited as an insulating film on the surface of the base 12 in a normal high-temperature oxidation atmosphere, and photoetching is performed to form a weir layer 13 that will become the base region of the transverse force direction Tr. A silicon film is perforated in a predetermined pattern.

この状態で基体表面にリンを添加した二酸化ケイ素膜を
500℃程度の低温で気相成長させ非酸化性雰囲気中で
熱拡散してN導電型堰層13を形成する。
In this state, a silicon dioxide film doped with phosphorus is grown on the surface of the substrate in a vapor phase at a low temperature of about 500° C., and thermally diffused in a non-oxidizing atmosphere to form an N-conductivity type weir layer 13.

こゝで拡散は凡そ1200℃とし基体をつきぬけて遮断
層に到達するように行う。
Here, the diffusion is carried out at approximately 1200° C. so as to penetrate through the substrate and reach the blocking layer.

又堰層の濃度は1016〜1017cm−3として基体
よりも高濃度とする。
Further, the concentration of the weir layer is set to be 1016 to 1017 cm-3, which is higher than that of the substrate.

この結果堰層と遮断層により基体分離域12′が区界さ
れる。
As a result, the substrate separation region 12' is delimited by the weir layer and the barrier layer.

再び光蝕刻を行って二酸化ケイ素膜を開孔し保層の一部
表面及び基体分離域表面の他の一部を露出して、この開
孔部からホウ素を高温酸化雰囲気中で熱拡散する。
Photoetching is performed again to open holes in the silicon dioxide film to expose a portion of the surface of the storage layer and another portion of the surface of the substrate separation region, and boron is thermally diffused through the openings in a high-temperature oxidizing atmosphere.

この拡散によって横方向TrのP電型エミソタ領域14
及びP電型ベース接続領域18が形成される。
Due to this diffusion, the P-type emitter region 14 of the lateral Tr
and a P-type base connection region 18 are formed.

ベース接続領域はこゝでは横方向Trのエミツタ領域と
同時に形成しているが、別に工程を設けて形成してもさ
し支えない。
Although the base connection region is formed at the same time as the emitter region of the lateral transistor here, it is also possible to form it in a separate process.

又これ等両領域共拡散法によらず別の例えばイオン打込
み法によって形成してもよい。
Further, instead of using the co-diffusion method, the regions may be formed using another method such as an ion implantation method.

次に縦方向Trにコレクタ領域を複数箇とキャリア吸出
し領域を一個形成するために二酸化ケイ素層を一部基体
分離域上で開孔しリンを高温酸化雰囲気中で熱拡散しN
導電型領域151,152,19を形成する。
Next, in order to form multiple collector regions and one carrier suction region in the vertical direction Tr, holes are formed in a portion of the silicon dioxide layer above the substrate separation region, and phosphorus is thermally diffused in a high temperature oxidizing atmosphere.
Conductivity type regions 151, 152, and 19 are formed.

即ち領域151,152はコレクタ領域でありそして領
域19はキャリア吸出し領域で先に設けたベース接続領
域18と短絡するように設けられる。
That is, regions 151 and 152 are collector regions, and region 19 is a carrier suction region and is provided so as to be short-circuited with the base connection region 18 provided previously.

これ等各領域表面の絶縁物層を電極を取り出すため所望
に開孔U用孔部101,102,103,104並びに
301,302,303を設ける。
Opening U holes 101, 102, 103, 104 and 301, 302, 303 are provided as desired to take out the electrodes from the insulating layer on the surface of each of these regions.

但し開孔部101けN導電型キャリア吸出し領域19と
P導電型ベース接続領域18の両領域に渡って開孔され
ることが必要である。
However, it is necessary that the opening 101 be opened across both the N-conductivity type carrier suction region 19 and the P-conductivity type base connection region 18 .

次に公知の配線技術により電極配線が形成され電極10
2′と103′は出力端子B1,B2へ、104′は電
源端子EPへそれぞれ接続され、101′によってN導
電型キャリア吸出し領域19とベース接続領域18とが
短絡される。
Next, electrode wiring is formed using a known wiring technique to form the electrode 10.
2' and 103' are connected to the output terminals B1 and B2, and 104' is connected to the power supply terminal EP, respectively, and the N conductivity type carrier extraction region 19 and the base connection region 18 are short-circuited by 101'.

又聞孔部301,302,303に設けられた各電極3
01,302,303 はそれぞれ基体分離域12′側
を陽極側とするダイオード121,122,123の陰
極を構成する。
Moreover, each electrode 3 provided in the perforation portions 301, 302, 303
01, 302, and 303 constitute cathodes of diodes 121, 122, and 123, respectively, whose anodes are on the substrate separation region 12' side.

ダイオードの設置箇数はこの例では三箇であるが一箇又
は複数箇でよい。
The number of diodes installed is three in this example, but it may be one or more.

電極金属はチタン、白金、アルミニウム等でよい。The electrode metal may be titanium, platinum, aluminum, etc.

そして各電極301′,302,303は入力端子A1
,A2,A3にそれぞれ接続される。
And each electrode 301', 302, 303 is an input terminal A1
, A2, and A3, respectively.

但しここで入力端子部に組み込まれたダイオードの順方
向電圧は縦方向NPNTrのエミツタベース接合め順方
向電圧より低いように構成しなければならない。
However, the forward voltage of the diode incorporated in the input terminal section must be configured to be lower than the forward voltage of the emitter-base junction of the vertical NPNTr.

第4図でEPは電源端子で横方向PNPTrのエミッタ
領域に接続され、A1,A2,A3は入力端子で横方向
PNPTrのコレクタ領域、即ち縦方向NPNTrのベ
ース領域に接続され、またB1,B2は出力端子で縦方
向NPNTrのコレクタ領域に、Enは接地端子で横力
向PNPTrのベース領域と縦力向NPNTrのエミツ
タ領域に各々接続される。
In FIG. 4, EP is a power supply terminal connected to the emitter region of the horizontal PNPTr, A1, A2, A3 are input terminals connected to the collector region of the horizontal PNPTr, that is, the base region of the vertical NPNTr, and B1, B2 is an output terminal connected to the collector region of the vertical NPNTr, and En is a ground terminal connected to the base region of the lateral force direction PNPTr and the emitter region of the longitudinal force direction NPNTr, respectively.

まず端子Enを零電位にして、端子EPにプラス0.7
ボルトを印加すると横方向PNPTrが動作状態となっ
てエミツタ領域14からベース領域13に注入された正
孔はこの領域を通ってコレクタ領域12′即ち縦方向N
PNTrのベース領域に到達する。
First, set the terminal En to zero potential, and add 0.7 to the terminal EP.
When a voltage is applied, the horizontal PNPTr is activated, and the holes injected from the emitter region 14 to the base region 13 pass through this region to the collector region 12', that is, the vertical direction N.
The base region of PNTr is reached.

縦方向NPNTrにおいては、このベース領域内に注入
された過剰正孔により縦方向NPNTrのエミツタ領域
11からベース領域12 に新たに電子が注入される。
In the vertical NPNTr, electrons are newly injected from the emitter region 11 of the vertical NPNTr to the base region 12 due to the excess holes injected into the base region.

つまり縦方向NPNTrのエミツタベース接合は順方向
バイアスされ、動作状態となり、その出力端子B1,B
2の電位はほゞ零電位となる。
In other words, the emitter-base junction of the vertical NPNTr is forward-biased and becomes operational, and its output terminals B1, B
The potential at point 2 is almost zero potential.

但しこの時、入力端子A1,A2,A3は開放状態にあ
るか、或はエミツタ接地縦方向NPNTrのしきい値電
圧以上の適当な正の電圧が印加された状態にある。
However, at this time, the input terminals A1, A2, and A3 are in an open state, or are in a state where an appropriate positive voltage higher than the threshold voltage of the vertical NPNTr with the emitter grounded is applied.

又この入力端子A1,A2,A3の少くとも一個を零電
位にすると縦方向NPNTrは遮断状態となり、出力端
子B1,B2は正電位となる。
Further, when at least one of the input terminals A1, A2, and A3 is set to zero potential, the vertical NPNTr is cut off, and the output terminals B1 and B2 are set to a positive potential.

即ち入力が全て“1”の時のみ出力が“0”となる多入
力多出力のNAND機能を持った論理素子が構成される
ことになる。
In other words, a multi-input multi-output NAND function logic element is constructed in which the output is "0" only when all the inputs are "1".

尚複数個の整流性ダイオード部分はAND機能を、縦方
向NPNTrの部分はインバータ機能を持つことは自明
である。
It is obvious that the plurality of rectifying diodes have an AND function, and the vertical NPNTr part has an inverter function.

ところで前記説明では半導体基体をP導電型としてP型
からスタートしているが、N導電型からスタートしても
勿論良い。
Incidentally, in the above description, the semiconductor substrate is of P conductivity type and starts from P type, but it is of course possible to start from N conductivity type.

したがってこの場合には各領域及び層の導電型及び電源
をすべて反転しておけば同様に動作する。
Therefore, in this case, if the conductivity type and power source of each region and layer are all reversed, the device will operate in the same way.

このような新論理素子では電流源及び負荷となる横方向
Trのベース巾を、従来の横方向Trのようにマスク巾
によらないで、拡散により制御できるので極めて狭くで
き、不純物プロファイルからキャリアに対して加速電界
がかかるのでキャリアの注入効率及び輸送効率が著しく
改善される。
In such a new logic element, the base width of the lateral transistor that serves as a current source and load can be controlled by diffusion, without depending on the mask width as in conventional lateral transistors, so it can be made extremely narrow, and carriers can be controlled from the impurity profile. On the other hand, since an accelerating electric field is applied, carrier injection efficiency and transport efficiency are significantly improved.

この為、広い電流範囲に渡り高い電流増巾率を得ること
かでき、論理回路としての消費電力が著しく減少する。
Therefore, a high current amplification rate can be obtained over a wide current range, and power consumption as a logic circuit is significantly reduced.

又遮断層11をエミッタとする縦方向Trをインバータ
素子として用いるので、広い電流範囲にわたって高い電
流増巾率を実現することはもちろん高い利得帯域巾積∫
Tを得ることができる。
Furthermore, since a vertical transistor with the blocking layer 11 as an emitter is used as an inverter element, it is possible to realize a high current amplification rate over a wide current range as well as a high gain band width ∫
You can get T.

更に又縦方向NPNTrのベース領域に短絡するキャリ
ア吸出し領域の存在によってベース領域及びコレクタ領
域に蓄積される過剰少数キャリアを抑制出来、出力の反
転速度を高めることを可能にしている9更に入力端子に
インバータ機能を持つ縦方向Trのエミツタベース接合
の順方向電圧より低い順方向電圧特性を持つ金属半導体
整流性接触ダイオードを、その陽極側を縦方向Trのベ
ース領域自体で形成しているため多入力多出力NAND
機能を一素子で実現出来る効果をも併せる。
Furthermore, due to the presence of a carrier extraction region short-circuited to the base region of the longitudinal NPNTr, excessive minority carriers accumulated in the base region and collector region can be suppressed, making it possible to increase the output reversal speed. A metal-semiconductor rectifying contact diode, which has a forward voltage characteristic lower than the forward voltage of the emitter-base junction of a vertical transistor having an inverter function, is formed on the anode side by the base region of the vertical transistor itself. Output NAND
It also has the effect of realizing functions with a single element.

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

第1図は従来の半導体装置断面図、第2図は第1図装置
の等価回路図、第3図はこの発明の半導体装置断面図、
第4図はその等価回路図である。 第3図で12・・・基体、13・・・堰層、12 ・・
・基体分離域、11・・・遮断層、14・・・横方向T
rのエミッタ領域、151,152・・・縦方向Trの
コレクタ領域、18・・・ベース接続用領域、19・・
・キャリア吸出し領域、121,122,123・・・
ダイオード。
FIG. 1 is a sectional view of a conventional semiconductor device, FIG. 2 is an equivalent circuit diagram of the device shown in FIG. 1, and FIG. 3 is a sectional view of a semiconductor device of the present invention.
FIG. 4 is its equivalent circuit diagram. In Fig. 3, 12...base body, 13...weir layer, 12...
-Substrate separation region, 11...blocking layer, 14...lateral direction T
r emitter region, 151, 152... collector region of vertical Tr, 18... base connection region, 19...
・Carrier suction area, 121, 122, 123...
diode.

Claims (1)

【特許請求の範囲】[Claims] 1 一方導電型半導体基体表面から深さ方向に設けられ
る他方導電型堰層と、堰層の底領域に接続して基体内に
基体分離域を区界する他方導電型遮断層と、堰層の内側
に形成され分離域をコレクタ領域とし堰層をベース領域
とする横方向トランジスタのエミッタ領域となる一方導
電型領域と、基体分離域の内側に形成され基体分離域を
ベース領域とし遮断層をエミツタ領域とする縦方向トラ
ンジスタのコレクタ領域となる他方導電型領域と、縦方
向トランジスタのベース領域に設けられ電極で互に接続
されるベース接続用領域及び一方導電型キャリア吸出し
領域と、縦方向トランジスタのベース領域表面に形成さ
れる一乃至複数箇の金属半導体間整流性接触ダイオード
を備える半導体装置。
1. A weir layer of the other conductivity type provided in the depth direction from the surface of the semiconductor substrate of the one conductivity type, a blocking layer of the other conductivity type connected to the bottom region of the weir layer and demarcating a substrate separation region within the substrate, and a barrier layer of the weir layer. A conductivity type region is formed inside the substrate isolation region and serves as the emitter region of a lateral transistor in which the isolation region is the collector region and the weir layer is the base region. A region of the other conductivity type that serves as the collector region of the vertical transistor as a region, a base connection region and a carrier extraction region of one conductivity type provided in the base region of the vertical transistor and connected to each other by electrodes, A semiconductor device comprising one or more metal-semiconductor rectifying contact diodes formed on the surface of a base region.
JP50096785A 1975-08-09 1975-08-09 Hand tie souchi Expired JPS584825B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP50096785A JPS584825B2 (en) 1975-08-09 1975-08-09 Hand tie souchi

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP50096785A JPS584825B2 (en) 1975-08-09 1975-08-09 Hand tie souchi

Publications (2)

Publication Number Publication Date
JPS5220778A JPS5220778A (en) 1977-02-16
JPS584825B2 true JPS584825B2 (en) 1983-01-27

Family

ID=14174276

Family Applications (1)

Application Number Title Priority Date Filing Date
JP50096785A Expired JPS584825B2 (en) 1975-08-09 1975-08-09 Hand tie souchi

Country Status (1)

Country Link
JP (1) JPS584825B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5440718B2 (en) * 1973-08-27 1979-12-05
JPS5459088A (en) * 1977-10-20 1979-05-12 Toshiba Corp Integrated circuit

Also Published As

Publication number Publication date
JPS5220778A (en) 1977-02-16

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