JPS6331111B2 - - Google Patents
Info
- Publication number
- JPS6331111B2 JPS6331111B2 JP54088732A JP8873279A JPS6331111B2 JP S6331111 B2 JPS6331111 B2 JP S6331111B2 JP 54088732 A JP54088732 A JP 54088732A JP 8873279 A JP8873279 A JP 8873279A JP S6331111 B2 JPS6331111 B2 JP S6331111B2
- Authority
- JP
- Japan
- Prior art keywords
- conductivity type
- gate
- polycrystalline silicon
- substrate
- type
- 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
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D64/00—Electrodes of devices having potential barriers
- H10D64/60—Electrodes characterised by their materials
- H10D64/66—Electrodes having a conductor capacitively coupled to a semiconductor by an insulator, e.g. MIS electrodes
- H10D64/671—Electrodes having a conductor capacitively coupled to a semiconductor by an insulator, e.g. MIS electrodes the conductor having lateral variation in doping or structure
Landscapes
- Electrodes Of Semiconductors (AREA)
- Semiconductor Integrated Circuits (AREA)
- Metal-Oxide And Bipolar Metal-Oxide Semiconductor Integrated Circuits (AREA)
- Non-Volatile Memory (AREA)
Description
【発明の詳細な説明】
本発明は、半導体装置に関し、特にソース・ド
レインを形成する半導体と、逆の型の半導体でゲ
ートが形成されるシリコンゲートMOSFETの構
成に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a semiconductor device, and particularly to a structure of a silicon gate MOSFET in which a gate is formed of a semiconductor of a type opposite to that of a semiconductor forming a source/drain.
本発明の目的は、ゲートの仕事関数が異なる一
対の同極性のシリコンゲートMOSFETにおい
て、両者のしきい値電圧の差電圧が設計値通りに
精度良く得られしかも該差電圧を電源電圧変動に
対して安定であるように構成することである。 An object of the present invention is to obtain a voltage difference between the threshold voltages of a pair of silicon gate MOSFETs of the same polarity with different gate work functions in accordance with a design value with high accuracy, and to maintain the voltage difference against power supply voltage fluctuations. The objective is to configure the system so that it is stable and stable.
β(β=μWCox/L、ただし、μ、W、L、
Coxはそれぞれ移動度、チヤネル幅、チヤネル
長、ゲート酸化膜の単位面積当りの容量)の値が
等しくしきい値電圧VTの値が異なる一対の同極
性のMOSFETを得る場合に、一対の同サイズの
MOSFETを、互いに極性の異なる多結晶シリコ
ンを用いてゲートを形成することにより実現する
方法がある。 β (β=μWCox/L, where μ, W, L,
When obtaining a pair of same-polarity MOSFETs with equal mobility, channel width, channel length, and capacitance per unit area of gate oxide film, and different threshold voltages V T , Cox of size
There is a method of realizing a MOSFET by forming gates using polycrystalline silicon having mutually different polarities.
上述の一対のMOSFETのうち一方はゲート極
板がP形多結晶シリコンより成り他方はN形多結
晶シリコンより成るものであつてその不純物濃度
がそれぞれNA、NDであるとする。このとき、両
MOSFETのしきい値電圧の差電圧VD両ゲート極
板の仕事関数差として与えられ、次式で表わされ
る。 It is assumed that one of the above-mentioned pair of MOSFETs has a gate plate made of P-type polycrystalline silicon and the other made of N-type polycrystalline silicon, and the impurity concentrations thereof are N A and N D , respectively. At this time, both
The difference voltage V D in the threshold voltage of the MOSFET is given as the work function difference between both gate plates, and is expressed by the following equation.
VD=KT/qlogeNA・ND/ni2 (1)
ただし、kはボルツマン定数、Tは絶対温度、
qは単位電荷、niは真性半導体の不純物濃度であ
る。式(1)で得られる電圧VDは信頼度の高い基準
電圧として広く応用が可能である。 V D = KT/qlogeN A・N D /ni 2 (1) where, k is Boltzmann's constant, T is absolute temperature,
q is the unit charge, and ni is the impurity concentration of the intrinsic semiconductor. The voltage V D obtained by equation (1) can be widely applied as a highly reliable reference voltage.
次に、第1図乃至第4図を用いて、上述の
MOSFET対の従来構成および本発明による構成
を説明する。MOSFETがPチヤネルトランジス
タである場合を例にとると第1図勿至第4図にお
いて、各記号の意味は次の通りである。 Next, using Figures 1 to 4, the above
A conventional configuration of a MOSFET pair and a configuration according to the present invention will be explained. Taking the case where the MOSFET is a P-channel transistor as an example, the meanings of each symbol in FIGS. 1 to 4 are as follows.
101,201,301,401………N型基
板
102,202,302,402………P型シ
リコン層
103,203,303,403………ゲート
酸化膜
104,304………N型多結晶シリコン
204,404,105,305……P型多結
晶シリコン
306,406……ソース・ドレイン形成以前
の工程(例:ストツパ形成時、Pウエル形成時)
において形成されたP型領域。 101,201,301,401...N-type substrate 102,202,302,402...P-type silicon layer 103,203,303,403...Gate oxide film 104,304...N-type polycrystal Silicon 204,404,105,305...P-type polycrystalline silicon 306,406...Process before source/drain formation (e.g., when forming a stopper, when forming a P well)
P-type region formed in.
一般にMOSFETを集積回路(以下、ICと略
記)の工程で作る場合、パターン設計の段階にお
いて予めマスクずれに対する配慮が必要である。 Generally, when MOSFETs are manufactured using an integrated circuit (hereinafter abbreviated as IC) process, consideration must be given to mask misalignment in advance at the pattern design stage.
この点に留意しMOSFETがセルフアラインで
形成されることを考慮すると、ソース・ドレイン
をP型半導体、ゲートをN型半導体で形成する場
合には、ゲート極板のソース側の端およびドレイ
ン側の端にP型の領域を帯状に設けなくてはなら
ない。従来は、これをP型多結晶シリコン105
がMOSFETのチヤネルの上部に重なるように第
1図の如く実現していた。また、ソース・ドレイ
ン及びゲートをP型半導体で形成する場合には、
第1図のMOSFETとチヤンネル長が等しくなる
ように第2図のごとく実現していた。この方法に
よつてMOSFET対を実現した場合、第1図でN
型多結晶シリコン104、P型多結晶シリコン1
05の両者の仕事関数が異なるため、第1図の
MOSFETと第2図のMOSFETとのしきい値の
差VDは式(1)のような簡単な式では表わされず、
設計値通りの基準電圧が得られない。本発明は、
以下に説明する手法によつてかかる欠点を除去し
たものである。 Keeping this in mind and considering that MOSFETs are formed in a self-aligned manner, if the source and drain are made of a P-type semiconductor and the gate is made of an N-type semiconductor, the edges on the source side and the drain side of the gate plate should be A P-type region must be provided in the form of a band at the end. Conventionally, this was done using P-type polycrystalline silicon 105
It was realized as shown in Figure 1 so that it overlapped the top of the MOSFET channel. In addition, when forming the source/drain and gate with a P-type semiconductor,
The MOSFET shown in Fig. 1 was realized as shown in Fig. 2 so that the channel length was equal to that of the MOSFET shown in Fig. 1. When a MOSFET pair is realized using this method, N
Type polycrystalline silicon 104, P type polycrystalline silicon 1
Since the work functions of both 05 and 05 are different, the
The difference in threshold value V D between the MOSFET and the MOSFET shown in Figure 2 cannot be expressed by a simple equation like equation (1);
The reference voltage cannot be obtained as designed. The present invention
This drawback has been eliminated by the method described below.
本発明による、ソース・ドレインがP型半導体
でゲートがN型半導体のMOSFETはP型のシリ
コン層306をソース・ドレインのチヤネル側に
設けて第3図に示すように形成される。また、こ
れと対をなす、ゲートがP型半導体のMOSFET
は第3図のMOSFETとチヤネル長が等しくなる
ように第4図に示すように形成される。第5図は
第3図のMOSFETを設計するためのパターン図
の一例であり、501がゲートの端、502がゲ
ート極板上のP型領域とN型領域との境界、50
3および504がソース・ドレイン形成以前の工
程で基板に形成するP型領域の境界である。 A MOSFET according to the present invention whose source and drain are P-type semiconductors and whose gate is an N-type semiconductor is formed as shown in FIG. 3 by providing a P-type silicon layer 306 on the channel side of the source and drain. In addition, a MOSFET with a P-type semiconductor gate is paired with this.
is formed as shown in FIG. 4 so that the channel length is equal to that of the MOSFET shown in FIG. FIG. 5 is an example of a pattern diagram for designing the MOSFET shown in FIG.
3 and 504 are boundaries of P-type regions formed on the substrate in a step before forming the source/drain.
また、505はゲートと配線とのコンタクトで
ある。パターン設計する上で注意すべき点は、拡
散工程での不純物イオンの広がりを考慮に入れ
て、第3図のチヤネルの両端320,321がそ
れぞれP型多結晶シリコンとN型多結晶シリコン
との境界310,311より内側(チヤネル側)
に形成されるようにすること及び320,321
間の距離が第4図の420,421間の距離に等
しくなるように(即ち、第3図のMOSFETと第
4図のMOSFETとでチヤネル長が等しくなるよ
うに)することである。こうすることによつて対
とするトランジスタのβを精度よく等しくでき
る。 Further, 505 is a contact between the gate and the wiring. What should be noted when designing the pattern is that both ends 320 and 321 of the channel in FIG. Inside boundaries 310 and 311 (channel side)
and 320,321
The distance between them should be equal to the distance between 420 and 421 in FIG. 4 (that is, the channel lengths of the MOSFETs in FIG. 3 and MOSFETs in FIG. 4 should be equal). By doing so, β of the paired transistors can be made equal with high precision.
ところで以上の例では、ソース・ドレインをP
型半導体で形成した場合について説明したが、ソ
ース・ドレインをN型半導体で形成した場合につ
いても全く同様のことが言える。即ち、上述の例
でP型とN型とを逆にしても本発明に該当する。 By the way, in the above example, the source and drain are connected to P.
Although the case where the source and drain are formed using an N-type semiconductor has been described, the same thing can be said about the case where the source and drain are formed using an N-type semiconductor. That is, even if the P-type and N-type are reversed in the above example, the invention falls under the present invention.
本発明の一応用例を第6図aに示す。(この回
路については特開昭53−47953に詳しい説明がな
されている。)同図において、601はゲートを
N型多結晶シリコンで形成したしきい値の高いP
チヤネルMOSFET、602乃至606は通常の
MOSFETであり、607は入力端子、608は
出力端子、609は正電源、610は負電源であ
る。607に第6図b611のような信号が入力
されると、611がローの期間608に601と
602のしきい値電圧の差電圧が出力される。こ
の本発明を用いた第6図の回路はコンパレータの
基準電源などへ適用すると効果が大きい。 An example of application of the present invention is shown in FIG. 6a. (This circuit is explained in detail in Japanese Patent Laid-Open No. 53-47953.) In the same figure, 601 is a high-threshold transistor whose gate is made of N-type polycrystalline silicon.
Channel MOSFETs, 602 to 606 are normal
607 is an input terminal, 608 is an output terminal, 609 is a positive power supply, and 610 is a negative power supply. When a signal as shown in FIG. 6B611 is input to 607, the difference voltage between the threshold voltages of 601 and 602 is output during a period 608 when 611 is low. The circuit of FIG. 6 using the present invention is highly effective when applied to a reference power source of a comparator, etc.
更に本発明の最大の効果は、基準電圧回路に応
用した場合式(1)に基づいて設計した電圧が精度良
く得られると同時に電源電圧変動除去比が極めて
高いことである。また、得られる基準電圧はツエ
ナーダイオードを用いるものなどに比較して量産
ばらつきが小さい。従つて、本発明はA/D変換
器、D/A変換器等各種のリニア回路の基準電圧
源として応用できるものである。 Furthermore, the greatest effect of the present invention is that when applied to a reference voltage circuit, the voltage designed based on equation (1) can be obtained with high accuracy, and at the same time, the power supply voltage fluctuation rejection ratio is extremely high. Further, the obtained reference voltage has smaller variations in mass production than those using Zener diodes. Therefore, the present invention can be applied as a reference voltage source for various linear circuits such as A/D converters and D/A converters.
第1図及び第2図は、従来構成による、しきい
値が相異なるシリコンゲートMOSFET対。第3
図及び第4図は、本発明の構成による。しきい値
が相異なるシリコンゲートMOSFET対。第5図
は、本発明のシリコンゲートMOSFETのパター
ン図の一例。第6図a,bは本発明の一応用例。
FIGS. 1 and 2 show a pair of silicon gate MOSFETs with different threshold values according to conventional configurations. Third
The figures and FIG. 4 are according to the configuration of the present invention. A pair of silicon gate MOSFETs with different threshold values. FIG. 5 is an example of a pattern diagram of a silicon gate MOSFET of the present invention. Figures 6a and 6b show an example of application of the present invention.
Claims (1)
成されたゲート酸化膜、前記ゲート酸化膜上の中
央部上に形成された第1導電型の多結晶シリコン
及び前記ゲート酸化膜上の端部上に形成された第
2導電型の多結晶シリコンからなるゲート、前記
ゲートの両側の前記基板中に形成された第2導電
型シリコン層及び前記第2導電型シリコン層の一
部と重なり前記第2導電型の多結晶シリコン下の
前記基板と前記第1導電型の多結晶シリコン下の
前記基板の一部にまたがつて形成された第2導電
型領域からなるソース・ドレインよりなる第1ト
ランジスタと、前記基板に形成され前記第1トラ
ンジスタと同じ極性及び同じチヤンネル長を有
し、かつ第2導電型の多結晶シリコンからなるゲ
ートよりなる第2トランジスタとを有することを
特徴とする半導体装置。1 A substrate of a first conductivity type, a gate oxide film selectively formed on the substrate, a polycrystalline silicon of the first conductivity type formed on a central portion of the gate oxide film, and a gate oxide film formed on the gate oxide film. A gate made of polycrystalline silicon of a second conductivity type formed on an end portion, a second conductivity type silicon layer formed in the substrate on both sides of the gate, and overlapping with a part of the second conductivity type silicon layer. A source/drain region comprising a second conductivity type region formed across the substrate under the second conductivity type polycrystalline silicon and a part of the substrate under the first conductivity type polycrystalline silicon. a second transistor formed on the substrate, having the same polarity and the same channel length as the first transistor, and having a gate made of polycrystalline silicon of a second conductivity type. Device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8873279A JPS5612773A (en) | 1979-07-12 | 1979-07-12 | Silicon gate mos field-effect transistor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8873279A JPS5612773A (en) | 1979-07-12 | 1979-07-12 | Silicon gate mos field-effect transistor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5612773A JPS5612773A (en) | 1981-02-07 |
| JPS6331111B2 true JPS6331111B2 (en) | 1988-06-22 |
Family
ID=13951086
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8873279A Granted JPS5612773A (en) | 1979-07-12 | 1979-07-12 | Silicon gate mos field-effect transistor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5612773A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06151828A (en) * | 1992-10-30 | 1994-05-31 | Toshiba Corp | Semiconductor device and is manufacture |
| JP2014053414A (en) * | 2012-09-06 | 2014-03-20 | Denso Corp | Manufacturing method of semiconductor device |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5286084A (en) * | 1976-01-12 | 1977-07-16 | Hitachi Ltd | Field effect transistor |
| JPS5432078A (en) * | 1977-08-16 | 1979-03-09 | Nec Corp | Semiconductor device |
-
1979
- 1979-07-12 JP JP8873279A patent/JPS5612773A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5612773A (en) | 1981-02-07 |
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