JPS596573A - Lateral bi-polar transistor - Google Patents

Lateral bi-polar transistor

Info

Publication number
JPS596573A
JPS596573A JP57115729A JP11572982A JPS596573A JP S596573 A JPS596573 A JP S596573A JP 57115729 A JP57115729 A JP 57115729A JP 11572982 A JP11572982 A JP 11572982A JP S596573 A JPS596573 A JP S596573A
Authority
JP
Japan
Prior art keywords
region
emitter
current
collector
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.)
Pending
Application number
JP57115729A
Other languages
Japanese (ja)
Inventor
Yuichi Hirofuji
裕一 広藤
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP57115729A priority Critical patent/JPS596573A/en
Publication of JPS596573A publication Critical patent/JPS596573A/en
Pending legal-status Critical Current

Links

Classifications

    • H—ELECTRICITY
    • H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D48/00—Individual devices not covered by groups H10D1/00 - H10D44/00
    • H10D48/30—Devices controlled by electric currents or voltages
    • H10D48/32—Devices controlled by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
    • H10D48/34—Bipolar devices
    • H10D48/345—Bipolar transistors having ohmic electrodes on emitter-like, base-like, and collector-like regions

Landscapes

  • Bipolar Transistors (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 本発明はバイポーIラトランジスタに関するものであっ
て、特に高注入領域に於ける電流増幅率の減少率を低減
することのできる横型バイポーラトランジスタに関する
。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a bipolar I-type transistor, and more particularly to a lateral bipolar transistor that can reduce the rate of decrease in current amplification in a high injection region.

バイポーラ型半導体集積回路の高速化、低消費電力化、
低電圧駆動化に伴って、NPN)ランシスタと同程度の
性能、すなわち、簡単な製造工程で、高耐圧・高電流増
幅率・高周波特性を有し、かつ高密度化に適したPIP
)ランシスタに対する要求が高まってきた。
Increased speed and lower power consumption of bipolar semiconductor integrated circuits,
With the trend toward lower voltage driving, PIPs have been developed that have performance comparable to NPN (NPN) Lancistors, that is, have high withstand voltage, high current amplification factor, and high frequency characteristics with a simple manufacturing process, and are suitable for high density.
) Demand for Runcissta has increased.

しかしながら、パターンの微細化に伴い電流増幅率(以
下hFlcと記す)の電流依存性が小さいPNP)ラン
シスタを形成することが困難になってきた。第」図は横
型PNP )ランシスタを示すもので、同図ムはマスク
パターン、同図Bはその人−A′断面構造図である。同
図において、11はP型エミッタ領域、12はN型ベー
ス領域、13はP型コレクタ領域、14はベースコンタ
クト領域、’ 5 LP型基板、16はN型エピタキシ
アル領域、17はN 埋込領域である。エピタキシ1ル
領域16は比抵抗1Ω−cmを有し、P型エミッタ領域
11とP型コレクタ領域13とは、NPNトランジスタ
の活性ベース領域を形成するためのホウ素拡散時に同時
形成され約0.7μmの拡散深さを持つ。
However, with the miniaturization of patterns, it has become difficult to form a PNP transistor whose current amplification factor (hereinafter referred to as hFlc) has a small dependence on current. Figure 1 shows a horizontal PNP (transistor) transistor, where Figure 1 shows a mask pattern and Figure B shows its cross-sectional structure along line A'. In the figure, 11 is a P-type emitter region, 12 is an N-type base region, 13 is a P-type collector region, 14 is a base contact region, 5 is an LP-type substrate, 16 is an N-type epitaxial region, and 17 is an N-type buried region. It is an area. The epitaxial region 16 has a specific resistance of 1 Ω-cm, and the P-type emitter region 11 and the P-type collector region 13 are formed simultaneously during boron diffusion to form the active base region of the NPN transistor, and have a resistivity of about 0.7 μm. has a diffusion depth of

今、PNP、)ランシスタとして最も重要な部分である
エミッタ領域11とコレクタ領域13との間に注目し、
第2図に要部を示す。同図に於て、エミッタ領域11の
端部からコレクタ領域13の端部までの距離WBはベー
ス幅であって、エミッタ領域11とコレクタ領域13と
を同時に拡散する場合の拡散マスクとなる酸化シリコン
膜180幅札 よりも、ホウ素の横方向拡散の影響で小
さくなる。WB′を4μmとするとwBは約3μmとな
る。このような構造ではエミッタ領域11とコレクタ領
域13との間隔はエピタキシアル層160表面で最も小
さいので、動作状態に於て電流がベース領域12の表面
に集中し、電流通路の断面積は小さい。従ってこの部分
ではキアリアであるホールの密度が高くなって、エミッ
タ効率の低下や、ベース領域中での再結合の増加によっ
て、電流増幅率hFE−の低下を招く。
Now, we will focus on the area between the emitter region 11 and the collector region 13, which is the most important part of the PNP, ) run transistor.
Figure 2 shows the main parts. In the figure, the distance WB from the end of the emitter region 11 to the end of the collector region 13 is the base width, and the distance WB from the end of the emitter region 11 to the end of the collector region 13 is the base width. It is smaller than the membrane 180 width plate due to the influence of lateral diffusion of boron. When WB' is 4 μm, wB is approximately 3 μm. In such a structure, the distance between the emitter region 11 and the collector region 13 is smallest at the surface of the epitaxial layer 160, so that in the operating state, current is concentrated on the surface of the base region 12, and the cross-sectional area of the current path is small. Therefore, the density of holes, which are chiaria, increases in this portion, resulting in a decrease in emitter efficiency and an increase in recombination in the base region, resulting in a decrease in the current amplification factor hFE-.

第3図は、hFKのエミッタ電流依存性を示すグラフで
あって、第1図に示すPNP )ランシスタに於て、マ
スクパターン上のベース幅Wdを4μmから7μmまで
変化させた各トランジスタに場合にはhFEはエミッタ
電流が60μA程度の時に最大となり、エミッタ電流の
増加につれて急峻に減少する。この現像は、ベース領域
の不純物濃度と電流密度に支配され、不純物濃度に比し
て電流密度が高くなるとhFKは減少する。tなわちエ
ミッタとコレクタの間の距離WBが小さい程、エミッタ
電流が表面付近に集中することによる。
FIG. 3 is a graph showing emitter current dependence of hFK, and shows the results for each transistor in the PNP transistor shown in FIG. 1 with the base width Wd on the mask pattern varied from 4 μm to 7 μm. hFE reaches its maximum when the emitter current is about 60 μA, and decreases sharply as the emitter current increases. This development is controlled by the impurity concentration in the base region and the current density, and as the current density becomes higher than the impurity concentration, hFK decreases. This is because the smaller the distance WB between the emitter and the collector, the more the emitter current is concentrated near the surface.

一方、ベース幅WB′が大きくなると、hFKが最大と
なるエミッタ電流は大きくなるが、hFEが小さいこと
が欠点である。
On the other hand, as the base width WB' increases, the emitter current at which hFK becomes maximum increases, but the disadvantage is that hFE is small.

そこで従来は、Wdが小さくても、高いhFEを高電流
領域まで保持する手段として電流密度を小さくするため
に電流通路の平面的な面積を拡大し、エミッタとコレク
タの対向面積を大きくすることが行なわれてきた。しか
し、この方法では極端に面積が犬きくなることが欠点で
ある。面積が犬きくなると、高密度集積回路に応用する
のは不向きであるばかシでなく、容量の助人により高速
化も制限を受ける。
Conventionally, even if Wd is small, as a means to maintain high hFE up to the high current region, it has been possible to increase the planar area of the current path and increase the facing area of the emitter and collector in order to reduce the current density. It has been done. However, this method has the disadvantage that the area becomes extremely small. As the area becomes too large, it is not only unsuitable for application to high-density integrated circuits, but also speed increases are limited by capacity.

本発明は上記欠点にかんがみなされたもので、高電流領
域でも高hFEを維持し得る高密度バイポーラトランジ
スタを提供することを目的とする。
The present invention has been made in view of the above drawbacks, and an object of the present invention is to provide a high-density bipolar transistor that can maintain high hFE even in a high current region.

第4図に、本発明の第1の実施例を示すホトマスクパタ
ーン図を示す。図中エミッタ領域11とコレクタ領域1
3とは同時に形成され、ベース幅はエミッタ領域11と
コレクタ領域13の間隙12によシ支配的に決定される
。尚、第4図で第1図と同一番号は同一部分を示す。今
、正方形であるエミッタ領域11の各辺について定義さ
れるマスクパターン上のベース幅をそれぞれa 、 b
’。
FIG. 4 shows a photomask pattern diagram showing the first embodiment of the present invention. Emitter region 11 and collector region 1 in the figure
3 are formed at the same time, and the base width is predominantly determined by the gap 12 between the emitter region 11 and the collector region 13. In FIG. 4, the same numbers as in FIG. 1 indicate the same parts. Now, the base widths on the mask pattern defined for each side of the square emitter region 11 are a and b, respectively.
'.

c、dとし、例えば a二4μm b二d二5μm c == 6μm とした場合、hFE のエミッタ電流依存性を第6図に
示す。同図で、図中曲線aは第3図中の曲線a 、!l
: 同U W B = 4μmのトランジスタの特性を
、曲線8は本発明の第1の実施例に示すトランジスタの
特性を示す。
FIG. 6 shows the emitter current dependence of hFE when c and d are set as, for example, a24μm b2d25μm c ==6μm. In the figure, the curve a in the figure is the curve a in Figure 3,! l
: Curve 8 shows the characteristics of the transistor shown in the first embodiment of the present invention.

本実施例によれば、エミッタ電流の大きい100μ人を
超える領域で、電流増幅率の改善がなされる。改善の割
合はエミッタ電流が200μAの時、hFEは約3Q%
、500μAの時には100係以上にも及ぶ。これは、
エミッタ電流の小さい場合には、マスクパターン上では
4μmの狭いベース幅が作用して高いhFICを提供し
、電流の増加に伴って、広いベース幅が作用しhFEの
急激な低下を防止することによる。
According to this embodiment, the current amplification factor is improved in a region where the emitter current is large and exceeds 100 μm. The improvement rate is approximately 3Q% for hFE when the emitter current is 200μA.
, at 500 μA, it reaches over 100 factors. this is,
When the emitter current is small, a narrow base width of 4 μm acts on the mask pattern to provide high hFIC, and as the current increases, a wide base width acts to prevent a sudden drop in hFE. .

以上、本発明による実施例によれば、簡単な工程で、面
積増加が少なくして、低電流領域では、ベース幅が狭い
部分が作用してhFEが高く、高電流領域では、ベース
幅の広い部分の効果により、hFKの低下を改善するこ
とができる。
As described above, according to the embodiments of the present invention, the area increase is small through simple steps, and hFE is high in the low current region due to the effect of the narrow base width, and in the high current region, the hFE is high. The decrease in hFK can be ameliorated by the effect of this drug.

次に本発明の応用例として、横形PNP l−ランシス
タのエミッタおよびコレクタ領域の平面的パターンをい
くつか示す。第6図は本発明の第2の実施例を示すマス
クパターンであって、エミッタ11の外周およびコレク
タ13の内周はそれぞれ円であって、その直径はそれぞ
れ10μm、20μmで両口の中氾・を一致させず1μ
m偏心させている。このためエミッタ11の外周円とコ
レクタ13の内周円との距離、すなわちベース幅は連続
的に変化する。この構造によっても第1の実施例と同様
の効果を有する。
Next, as an application example of the present invention, some planar patterns of emitter and collector regions of a lateral PNP l-transistor are shown. FIG. 6 is a mask pattern showing a second embodiment of the present invention, in which the outer periphery of the emitter 11 and the inner periphery of the collector 13 are circles, with diameters of 10 μm and 20 μm, respectively.・1μ without matching
It is eccentric by m. Therefore, the distance between the outer circumferential circle of the emitter 11 and the inner circumferential circle of the collector 13, that is, the base width, changes continuously. This structure also has the same effects as the first embodiment.

第7図(徒、本発明の第3の実施例を示すマスクパター
ンであって、エミッタ領域は11aと11bとに分割さ
れておシ、各々のエミッタ領域11a。
FIG. 7 is a mask pattern showing a third embodiment of the present invention, in which the emitter region is divided into 11a and 11b, each emitter region 11a.

11 bitこ対してそれぞれマスク上で4μmと5μ
mの相異なるベース12a、12bの幅を隔ててコレク
タ13が周囲をそれぞれ取り囲んでいる。
11 bits, respectively 4μm and 5μm on the mask
A collector 13 surrounds the bases 12a, 12b with m different widths between them.

この構造によっても第1の実施例と同様の効果を有する
。
This structure also has the same effects as the first embodiment.

以上の様に、本発明に係る横型バイポーラトランジスタ
はバイポーラ集積回路の高密度化、高速化が可能となる
ばか9でなく、電流振幅の大きな回路に使用することに
より、インピーダンス変′化による歪の減少等、集積回
路の特性向上にも寄与できる。
As described above, the lateral bipolar transistor according to the present invention not only makes it possible to increase the density and speed of bipolar integrated circuits, but also reduces distortion due to impedance changes by using it in circuits with large current amplitudes. It can also contribute to improving the characteristics of integrated circuits.

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

第1図Aは従来の横型PNP )ランシスタの平面図、
同図BはそのA −A’断面図、第2図は第1図Bの要
部断面図、第3図は従来の横型PNP トランジスタの
hFE のエミッタ電流依存性を示す特性図、第4図は
本発明の実施例に係る横型PNPトランジスタの平面図
、第5図は本発明に係るlj[PNP)ランシスタのh
FEのエミッタ電流依存性を示す特性図、第6図、第7
図は本発明の他の実施例を示す平面図である。 11・・・・・・エミッタ領域、12・・・・・・ベー
ス領域、13・・・・・・コレクタ領域0 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 第2図 第3図 第4図 第5図
Figure 1A is a plan view of a conventional horizontal PNP Runcistor.
Figure B is a sectional view taken along line A-A', Figure 2 is a cross-sectional view of the main part of Figure 1B, Figure 3 is a characteristic diagram showing the emitter current dependence of hFE of a conventional lateral PNP transistor, and Figure 4. 5 is a plan view of a lateral PNP transistor according to an embodiment of the present invention, and FIG.
Characteristic diagrams showing emitter current dependence of FE, Figures 6 and 7
The figure is a plan view showing another embodiment of the present invention. 11...Emitter area, 12...Base area, 13...Collector area 0 Name of agent Patent attorney Toshio Nakao and 1 other person 1st
Figure 2 Figure 3 Figure 4 Figure 5

Claims (2)

【特許請求の範囲】[Claims] (1)平面的に、少なくとも、中空形状のコレクタ領域
と、前記コレクタ領域の中空部分に形成されたエミッタ
領域とを備え、前記エミッタおよびコレクタ領域の対向
面間の距離が、場所により異なる部分を有することを特
徴とする横型バイポーラトランジスタ。
(1) Planarly, it includes at least a hollow collector region and an emitter region formed in the hollow portion of the collector region, and the distance between the opposing surfaces of the emitter and collector regions varies depending on the location. A lateral bipolar transistor comprising:
(2)  コレクタ領域とエミッタ領域が同時に形成さ
れていることを特徴とする特許請求の範囲第1項に記載
の横型バイポーラトランジスタ。
(2) The lateral bipolar transistor according to claim 1, wherein a collector region and an emitter region are formed at the same time.
JP57115729A 1982-07-02 1982-07-02 Lateral bi-polar transistor Pending JPS596573A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57115729A JPS596573A (en) 1982-07-02 1982-07-02 Lateral bi-polar transistor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57115729A JPS596573A (en) 1982-07-02 1982-07-02 Lateral bi-polar transistor

Publications (1)

Publication Number Publication Date
JPS596573A true JPS596573A (en) 1984-01-13

Family

ID=14669652

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57115729A Pending JPS596573A (en) 1982-07-02 1982-07-02 Lateral bi-polar transistor

Country Status (1)

Country Link
JP (1) JPS596573A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58148629A (en) * 1982-02-25 1983-09-03 株式会社東芝 Power system stabilizing system
JPS62260367A (en) * 1986-05-06 1987-11-12 Mitsubishi Electric Corp Semiconductor integrated circuit device

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5029172A (en) * 1973-07-17 1975-03-25
JPS55156361A (en) * 1979-05-25 1980-12-05 Hitachi Ltd Semiconductor device
JPS55165674A (en) * 1979-06-12 1980-12-24 Toshiba Corp Semiconductor device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5029172A (en) * 1973-07-17 1975-03-25
JPS55156361A (en) * 1979-05-25 1980-12-05 Hitachi Ltd Semiconductor device
JPS55165674A (en) * 1979-06-12 1980-12-24 Toshiba Corp Semiconductor device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58148629A (en) * 1982-02-25 1983-09-03 株式会社東芝 Power system stabilizing system
JPS62260367A (en) * 1986-05-06 1987-11-12 Mitsubishi Electric Corp Semiconductor integrated circuit device

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