JPS5910070B2 - semiconductor equipment - Google Patents
semiconductor equipmentInfo
- Publication number
- JPS5910070B2 JPS5910070B2 JP51103822A JP10382276A JPS5910070B2 JP S5910070 B2 JPS5910070 B2 JP S5910070B2 JP 51103822 A JP51103822 A JP 51103822A JP 10382276 A JP10382276 A JP 10382276A JP S5910070 B2 JPS5910070 B2 JP S5910070B2
- Authority
- JP
- Japan
- Prior art keywords
- region
- switching element
- lateral transistor
- transistor
- collector
- 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 11
- 238000009792 diffusion process Methods 0.000 claims description 7
- 239000012535 impurity Substances 0.000 claims description 6
- 239000000758 substrate Substances 0.000 claims description 5
- 230000005684 electric field Effects 0.000 claims 2
- 239000013078 crystal Substances 0.000 description 4
- 230000003321 amplification Effects 0.000 description 3
- 238000005468 ion implantation Methods 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 238000003199 nucleic acid amplification method Methods 0.000 description 3
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 2
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 229910052698 phosphorus Inorganic materials 0.000 description 2
- 239000011574 phosphorus Substances 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- RQNWIZPPADIBDY-UHFFFAOYSA-N arsenic atom Chemical group [As] RQNWIZPPADIBDY-UHFFFAOYSA-N 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 229910052681 coesite Inorganic materials 0.000 description 1
- 229910052906 cristobalite Inorganic materials 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 230000005669 field effect Effects 0.000 description 1
- 238000002347 injection Methods 0.000 description 1
- 239000007924 injection Substances 0.000 description 1
- 239000000377 silicon dioxide Substances 0.000 description 1
- 235000012239 silicon dioxide Nutrition 0.000 description 1
- 229910052682 stishovite Inorganic materials 0.000 description 1
- 229910052905 tridymite Inorganic materials 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D89/00—Aspects of integrated devices not covered by groups H10D84/00 - H10D88/00
- H10D89/211—Design considerations for internal polarisation
- H10D89/213—Design considerations for internal polarisation in field-effect devices
- H10D89/217—Design considerations for internal polarisation in field-effect devices comprising arrangements for charge injection in static induction transistor logic [SITL] devices
Landscapes
- Bipolar Transistors (AREA)
Description
【発明の詳細な説明】
本発明は論理回路用の半導体装置に関し、低消費電力化
に適した構造を提供するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a semiconductor device for a logic circuit, and provides a structure suitable for reducing power consumption.
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領域や抵抗器を必
要とせず素子面積を節約した集積度の高いI2L(In
tegratedInjectionLogic)構造
の論理回路素子が、例えば特公昭49−35030号公
報に示されているように周知である。このI2Lは従来
のバイポーラ素子に比べて、低消費電力、高密度という
特長を有している。本出願人はI2Lの欠点を改良し、
I2Lの性能を上回る新規構造の素子を特願昭51−4
5095号にて提案した。Several semiconductor devices for logic circuits have been known in the past, one of which is the highly integrated I2L (In
A logic circuit element having a tegrated injection logic structure is well known, as shown in Japanese Patent Publication No. 49-35030, for example. This I2L has the features of lower power consumption and higher density than conventional bipolar elements. The applicant has improved the shortcomings of I2L,
Patent application for an element with a new structure that exceeds the performance of I2L
It was proposed in No. 5095.
これは、新規なる構造のスイッチング素子を備えた構造
を有し、任意の数だけファンアウトが自由に取り出せ、
かつ速度電力積及び素子面積の小さな論理回路素子を供
給することを目的としたものである。まずこの新規構造
の素子を詳細に述べる。第1図Aは同素子の部分的概略
平面図であり、第1図Bは第1図Aで示したX−X’で
切断した時の部分的概略断面図、第1図Cは第1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
。This has a structure equipped with a switching element of a new structure, and any number of fanouts can be freely taken out.
The object of the present invention is to provide a logic circuit element having a small speed-power product and a small element area. First, the device with this new structure will be described in detail. FIG. 1A is a partial schematic plan view of the same element, FIG. 1B is a partial schematic sectional view taken along the line XX' shown in FIG. 1A, and FIG. It is a partial schematic sectional view when cut|disconnected by YY' shown in FIG. A.
第1図において、1は低抵抗率例えば0.001Ωm程
度のn+形基板であり接地電位に保たれている。In FIG. 1, reference numeral 1 denotes an n+ type substrate having a low resistivity, for example, about 0.001 Ωm, and is kept at ground potential.
2は前記1上に形成した高抵抗率例えば50JΩm程度
のn−形層である。2 is an n-type layer formed on the above 1 and having a high resistivity, for example, about 50 JΩm.
3、4は前記2の表面より形成した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
の領域は部分的にとり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 from the surface of 2,
Said 3 and 4 are arranged close to each other, and said 3 is said 2
The area is formed, for example, 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T1
において4、2、3は各々エミッタ、ベース、コレク
タとなつている。また前記3で囲まれたれた2の領域の
一部2’は前記3の電位が゛O″Vでは前記3とγとで
構成されるPn接合の拡散電位により空乏層で満たされ
る様に形成される。PnP transistor and star T1 composed of the above 4, 2, and 3
4, 2, and 3 are an emitter, a base, and a collector, respectively. Further, a part 2' of the region 2 surrounded by the above 3 is formed so that it is filled with a depletion layer due to the diffusion potential of the Pn junction composed of the above 3 and γ when the potential of the above 3 is ゛O''V. be done.
5は前記2の表面に形成したn+形領域であり、1,3
,2′ ,5からなるスイツチング素子S,において各
々3はゲート、1,2′ ,5は導電路として作用する
。5 is an n+ type region formed on the surface of 2, and 1, 3
, 2', and 5, 3 serves as a gate, and 1, 2', and 5 serve as conductive paths.
前記4の端子をバイアス端子b、前記3の端子を入力端
子1、前記5の端子を出力端子0とする次にその動作を
説明すると、端子bからは電流IBが常に注入されてい
る。Terminal 4 is used as bias terminal b, terminal 3 is used as input terminal 1, and terminal 5 is used as output terminal 0.The operation will be explained next.A current IB is always injected from terminal b.
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りトランジスタT1のコ
レクタすなわちトランジスタT2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り、1−
2′−5の導電性通路が形成され、端子0の出力は″O
″Vとなる。次に端子1が接地電位、すなわち10゛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を通り放電し、ゲート3は0V
となる。この為スイツチングS1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S1とは反転回路を
形成する。以上述べた素子構造は従来のIILよりもす
ぐれた性能を有するが、次の問題を有する。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 transistor T2 increases to approximately +0.6V due to holes injected from the emitter 4 of the transistor T1. For this reason, switching element S1
There is almost no depletion layer in the conductive path region 2' of 1-
A conductive path 2'-5 is formed, and the output of terminal 0 is ``O
``V. Next, terminal 1 is at ground potential, that is, 10゛V.
When this happens, the holes accumulated in the gate 3 of the switching element S1 are discharged through the terminal 1, and the gate 3 becomes 0V.
becomes. Therefore, the conductive path region 2' of the switching S1 is
As described above, due to the diffusion potential generated at the Pn junction between gate 3 and region 2', it is filled with a depletion layer, and terminals 2 and 5 are electrically separated and terminal 0 is in a floating state. In this way, transistor T1 and switching element S1 form an inverting circuit. Although the device structure described above has better performance than the conventional IIL, it has the following problems.
(1)上記素子の動作原理及び構造から考えてラテラル
PNPトランジスタT,のベース領域は、 こn一形層
2よりなる低濃度のn領域が含まれるためにPNPトラ
ンジスタのエミツタとコレクタでパンチスルーが起こら
ないようにベース幅を大きく取る必要がある。(1) Considering the operating principle and structure of the above element, the base region of the lateral PNP transistor T includes a low concentration n region made of the n-type layer 2, so there is a punch-through between the emitter and collector of the PNP transistor. It is necessary to increase the base width to prevent this from occurring.
その為高密度が損われる。例えばベース濃度1014a
t0ms1cr1でごあれば、拡散電位で空乏層が満た
されないためにはベース幅が5.3μ以上必要である。
(2)ベース幅が広くなると、PNPトランジスタの電
流増幅率が低くなり、消費電力の点から考て不利である
。Therefore, high density is lost. For example, base concentration 1014a
If t0ms1cr1, the base width needs to be 5.3μ or more so that the depletion layer is not filled with the diffusion potential.
(2) As the base width increases, the current amplification factor of the PNP transistor decreases, which is disadvantageous in terms of power consumption.
また、上記述べた欠点を良くするために、低濃度のエピ
タキシヤル層上に、それよりも濃度の高いエピタキシャ
ル層を形成する二重エピタキシャル法があるが、これは
工程の複雑性、及びPNPトランジスタT1の電流増幅
率を上げるという点から考えて、十分効果を上げること
はできない。In addition, in order to overcome the above-mentioned drawbacks, there is a double epitaxial method in which a higher concentration epitaxial layer is formed on a lower concentration epitaxial layer, but this method is complicated due to process complexity and PNP transistor From the point of view of increasing the current amplification factor of T1, it is not possible to achieve a sufficient effect.
本発明は、先に出願した新規なる構造のスイツチング素
子において、さらに低消費電力、高密度化を満足する半
導体装置を得るものである。本発明の一実施例を第2図
及び第3図に基づいて詳細に述べる。〔ん高濃度のn形
層である単結晶Sl基板11に例えば、比抵抗約500
(−mのn形単結晶層12を堆積させる。The present invention provides a semiconductor device which satisfies lower power consumption and higher density than the previously applied switching element having a new structure. An embodiment of the present invention will be described in detail with reference to FIGS. 2 and 3. [For example, a resistivity of about 500 is applied to the single-crystal Sl substrate 11, which is a highly concentrated n-type layer.
(Deposit an n-type single crystal layer 12 of -m.
〔B〕n型単結晶層12にSiO2等の絶縁膜13をマ
スクとして、リン等のn形不純物を拡散させる。[B] An n-type impurity such as phosphorus is diffused into the n-type single crystal layer 12 using the insulating film 13 such as SiO2 as a mask.
この時形成されるn形層14は、窓15からの拡散で形
成されラテラルPNPトランジスタのベース領域の一部
を形成することになり、n形エピタキシャル層12より
も高い不純物濃度を有している。なおこのn形層14を
形成する際に、イオン注入を用いてもよい。〔C〕工程
〔B〕において、n形層14を形成したマスク窓15を
そのまま残して、さらに絶縁膜13に、マスク窓16を
開孔する。The n-type layer 14 formed at this time is formed by diffusion from the window 15, forms part of the base region of the lateral PNP transistor, and has a higher impurity concentration than the n-type epitaxial layer 12. . Note that ion implantation may be used when forming this n-type layer 14. [C] In step [B], mask windows 16 are further opened in the insulating film 13, leaving the mask windows 15 in which the n-type layer 14 is formed as they are.
これらの絶縁膜開孔部15,16より、ボロンの熱拡散
やイオン注入を用いて、P形層17,18を形成する。
このP形層7及び8はそれぞれラテラルPNPトランジ
スタのエミツタ及びコレクタとなる。1〕リンあるいは
砒素の熱拡散やイオン注入を用いて高濃度のn形層19
を形成する。P-type layers 17 and 18 are formed through these insulating film openings 15 and 16 using boron thermal diffusion and ion implantation.
The P-type layers 7 and 8 become the emitter and collector of the lateral PNP transistor, respectively. 1] Highly concentrated n-type layer 19 using thermal diffusion or ion implantation of phosphorus or arsenic
form.
(6)電極用としてAlを用い、引出電極20を形成す
る。(6) Form the extraction electrode 20 using Al as an electrode.
第3図は第2図Dにおいて、絶縁膜13を取り去つた所
の要部平面図である。FIG. 3 is a plan view of the main part of FIG. 2D with the insulating film 13 removed.
本発明によるスイツチング素子は、第2図(F))にお
いて17はPNPトランジスタT1のエミツタつまりイ
ンジエクタとして働き、18はPNPトランジスタのコ
レクタ及びスイツチ素子のゲートとなり、14はPNP
トランジスタのベース領域の一部、19はスイツチ素子
S,の出力部として働く。In the switching element according to the present invention, in FIG. 2(F)), 17 serves as the emitter or injector of the PNP transistor T1, 18 serves as the collector of the PNP transistor and the gate of the switching element, and 14 serves as the PNP transistor T1.
A portion of the base region of the transistor, 19, serves as the output of the switch element S,.
本発明の半導体装置及びその素子は次の効果を生むこと
ができる。The semiconductor device and its element of the present invention can produce the following effects.
(a) PNPトランジスタT1の活性ベース領域にn
形エピタキシヤル層12よりも高濃度のn形層14を形
成しているために、ベース幅を狭くしてもPNPトラン
ジスタのエミツタ、コレク夕間のパンチスルーを防ぐこ
とが出き、かつベース幅を狭くすることができるために
高密度化を満足することが出来る。(a) n in the active base region of PNP transistor T1
Since the n-type layer 14 is formed with a higher concentration than the type epitaxial layer 12, punch-through between the emitter and collector of the PNP transistor can be prevented even if the base width is narrowed. Since the area can be narrowed, high density can be achieved.
(b)ベース幅が狭くなること及びベース領域にエミツ
タからコレクタにかけて濃度傾斜を持つているために起
こるドリフト電界効果によりPNPトランジスタT1の
電流増幅率を上げることができる。(b) The current amplification factor of the PNP transistor T1 can be increased due to the drift field effect caused by the narrowing of the base width and the concentration gradient in the base region from the emitter to the collector.
そのため、スイツチング素子としての低消費電力化に効
果がある。(c)同じマスク孔15から、インジエク及
びベースの不純物を拡散しているためにセルフアライン
化がはかられ、かつこれに要する工程も簡単である。Therefore, it is effective in reducing power consumption as a switching element. (c) Self-alignment can be achieved because the impurities of indie and base are diffused through the same mask hole 15, and the steps required for this are simple.
(d)他のバイポーラ素子との両立性も簡単に満足する
ことができる。(d) Compatibility with other bipolar elements can also be easily satisfied.
以上のように、本発明によれば高密度化、低消費電力化
のとくにすぐれた論理回路用半導体装置を得ることがで
きる。As described above, according to the present invention, it is possible to obtain a semiconductor device for logic circuits which has particularly excellent high density and low power consumption.
第1図Aは従来の構造の論理回路用素子の平面図、第1
図B,CはA(7)X−X′ ,Y−Y′線断面図、第
2図A−Eは本発明の一実施例にかかる論理回路用半導
体装置の製造方法による工程図、第3図は第2図Dの要
部平面図である。
1−2′−5・・・・・・導電路、12・・・・・・n
形単結晶、13・・・・・・絶縁膜、14・・・・・・
高濃度n形層、15,16・・・・・・窓、17,18
・・・・・・P形層(エミツタ、コレクタ)、19・・
・・・・高濃度n形層、T1・・・・・・PNPラテラ
ルトランジスタ、S,・・・・・・スイッチング素子。Figure 1A is a plan view of a logic circuit element with a conventional structure;
Figures B and C are cross-sectional views taken along lines A(7) FIG. 3 is a plan view of the main part of FIG. 2D. 1-2'-5... Conductive path, 12...n
Single crystal, 13... Insulating film, 14...
High concentration n-type layer, 15, 16... Window, 17, 18
...P-type layer (emitter, collector), 19...
... High concentration n-type layer, T1 ... PNP lateral transistor, S, ... Switching element.
Claims (1)
導電形を有する半導体基体中に、互に間隔を隔てて、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表面より前記半導体基体に到達しか
つその周囲が前記横方向トランジスタのコレクタ領域で
とり囲まれた一方の導電形よりなる導電路を有し前記横
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
イッチング素子を備え、前記スイッチング素子の導電路
が前記ゲート領域の拡散電位により空乏層で満たされ、
前記横方向トランジスタのエミッタ領域からコレクタ領
域に向かつて内部電界が生じるごとき不純物分布を有し
、かつ前記内部電界を生じせしめる不純物濃度が前記半
導体基体中に設けられた前記スイッチング素子の導電路
の不純物濃度よりも高いことを特徴とする半導体装置。1 forming, in a semiconductor substrate having one conductivity type serving as a base region of a lateral transistor, regions of the other conductivity type serving as an emitter region and a collector region of the lateral transistor, spaced apart from each other; a conductive path of one conductivity type that reaches the semiconductor substrate from the surface of at least one of the lateral transistors and is surrounded by the collector region of the lateral transistor, in the collector region of the lateral transistor; a switching element having a collector region of the lateral transistor as a gate region, a conductive path of the switching element being filled with a depletion layer due to a diffusion potential of the gate region,
Impurities in the conductive path of the switching element, which has an impurity distribution such that an internal electric field is generated from the emitter region to the collector region of the lateral transistor, and has an impurity concentration that generates the internal electric field in the semiconductor substrate. A semiconductor device characterized by a concentration higher than that of a semiconductor device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51103822A JPS5910070B2 (en) | 1976-08-30 | 1976-08-30 | semiconductor equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51103822A JPS5910070B2 (en) | 1976-08-30 | 1976-08-30 | semiconductor equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5329083A JPS5329083A (en) | 1978-03-17 |
| JPS5910070B2 true JPS5910070B2 (en) | 1984-03-06 |
Family
ID=14364093
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP51103822A Expired JPS5910070B2 (en) | 1976-08-30 | 1976-08-30 | semiconductor equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5910070B2 (en) |
-
1976
- 1976-08-30 JP JP51103822A patent/JPS5910070B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5329083A (en) | 1978-03-17 |
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