JPS60202343A - Complementary type semiconductor humidity sensor - Google Patents
Complementary type semiconductor humidity sensorInfo
- Publication number
- JPS60202343A JPS60202343A JP5880184A JP5880184A JPS60202343A JP S60202343 A JPS60202343 A JP S60202343A JP 5880184 A JP5880184 A JP 5880184A JP 5880184 A JP5880184 A JP 5880184A JP S60202343 A JPS60202343 A JP S60202343A
- Authority
- JP
- Japan
- Prior art keywords
- humidity sensor
- gate
- field effect
- source
- gate electrode
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N27/00—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means
- G01N27/26—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating electrochemical variables; by using electrolysis or electrophoresis
- G01N27/403—Cells and electrode assemblies
- G01N27/414—Ion-sensitive or chemical field-effect transistors, i.e. ISFETS or CHEMFETS
Abstract
Description
【発明の詳細な説明】
イ、産業上の利用分野
本発明は、絶縁ゲート型電界効果トランジスタと同様の
構造を有し、周囲湿度に応じ変化するドレイン電流から
周囲湿度を検知する湿度センサに関する。DETAILED DESCRIPTION OF THE INVENTION A. Field of Industrial Application The present invention relates to a humidity sensor that has a structure similar to an insulated gate field effect transistor and detects ambient humidity from a drain current that changes depending on the ambient humidity.
口、従来技術
絶縁性薄膜表面の一部に電極を形成し、vGなる電圧を
与えると、電極の末端から距@xの部分の時刻tの尚膜
表面の電位Vは
に従う。ここで、Cは絶縁膜の防電率などにより定まり
、几は膜質、膜の表面状態、周囲の湿度による。湿度に
対し、Rは単調に減少することか知られているので、距
離X及びtを定めれば、■は湿度により一意的に足まる
。従って、公知の絶縁ゲート型電界効果トランジスタに
おいて、ソースまたはドレインの一方と平面的に重なり
をもたないようにゲート電極を形成し、ゲート絶縁物末
端より距離X離れたところにソース又はドレインを形成
する不純物拡散層ケ設け°C1上記の部分を被11t!
I定雰囲気に露出させることにより、ドレイン・ソース
間電流IDSの時間変化を測定し、湿度をめることかで
きる。Prior art When an electrode is formed on a part of the surface of an insulating thin film and a voltage of vG is applied, the potential V of the film surface at time t at a distance @x from the end of the electrode follows. Here, C is determined by the dielectric constant of the insulating film, and C is determined by the quality of the film, the surface condition of the film, and the ambient humidity. It is known that R monotonically decreases with respect to humidity, so if distances X and t are determined, ■ is uniquely determined by humidity. Therefore, in a known insulated gate field effect transistor, the gate electrode is formed so as not to overlap with either the source or the drain in plane, and the source or drain is formed at a distance X from the end of the gate insulator. Provide an impurity diffusion layer to cover the above part!
By exposing it to a constant atmosphere, it is possible to measure the change in the drain-source current IDS over time and determine the humidity.
すなわち、第1図(a)は従来のnチャンネルMO8F
E T型の湿度センサの断面図、同図(b)は平面図
である。第1図(a) 、 (b)において、P型基板
lにノース及びドレイン領域を形成するn型拡散層2及
び5、ゲート電極4、ゲート絶縁膜3を形成し、ゲート
電極4の端部とドレイン領域5の端部の距lL’lfを
Xとする。この素子を第2図の回路図に示すjうに結+
IJI L、時刻t = 0 テVc ≧VDD >
VT(但し、VTはこの素子のしきい値電圧)なる電圧
VGを与えると、ゲート電極4の端部からの距PilC
xの時刻tの絶縁膜3上の電位分布V(x、 t )は
式(1)に従うので、第3図のグラフのように変化する
。すると距離Xの位置で、V=Vtとなる1=1(、に
、このAd(JSF’ETにはIDSが流れ工。5(t
)はおよそ第4図のグラフに示すように変化する・22
″″C・8は方程式vT−vG ・・f°2V廓乃国の
解としてまり、一方、几が湿度依存性をもつことより、
湿度Mがtcから一意的に決められる。That is, FIG. 1(a) shows the conventional n-channel MO8F.
A cross-sectional view of an ET-type humidity sensor, and FIG. 3(b) is a plan view. In FIGS. 1(a) and 1(b), n-type diffusion layers 2 and 5 forming north and drain regions, a gate electrode 4, and a gate insulating film 3 are formed on a P-type substrate l, and an end portion of the gate electrode 4 is formed. Let X be the distance lL'lf between the end of the drain region 5 and the end of the drain region 5. This element is connected to the circuit diagram shown in Figure 2.
IJI L, time t = 0 teVc ≧VDD >
When a voltage VG of VT (where VT is the threshold voltage of this element) is applied, the distance PilC from the end of the gate electrode 4 is
Since the potential distribution V(x, t) on the insulating film 3 at time t of x follows equation (1), it changes as shown in the graph of FIG. Then, at the position of distance
) changes approximately as shown in the graph of Figure 4・22
``''C・8 is a solution of the equation vT-vG ・・f°2V Kuronokuni, and on the other hand, since 几 has humidity dependence,
Humidity M is uniquely determined from tc.
しかしながら、上記の距離又はこのようなトランジスタ
の製造工程における寸法精度、特にゲート電極と不純物
拡散層を形成する際の重ね合わせ精度により変動し、そ
の結果、センサとし°Cの素子特性が大きく変動すると
いう欠点がある。その為、測定ね変向上のためには、距
離Xの値を、マスク重ね合せ精度をはじめとする製造上
の変動値に比べ°C十分に大きくする心数があり、集積
度及びコストの点で難点がある。However, the above distance or the dimensional accuracy in the manufacturing process of such a transistor, especially the overlay accuracy when forming the gate electrode and the impurity diffusion layer, will vary, and as a result, the device characteristics of the sensor and temperature will vary greatly. There is a drawback. Therefore, in order to improve the measurement variation, it is necessary to make the value of the distance There is a problem with this.
ハ9発明の目的
本発明の目的は、検出感度および信頼性的に優れ、また
、製造上の特性のばらつきの少ない湿度検出センサを提
供するにある。C.9 Object of the Invention An object of the present invention is to provide a humidity detection sensor that is excellent in detection sensitivity and reliability and has less variation in manufacturing characteristics.
二1発明の構成
本発明によれば、上に述べた構造の湿度センサとなる絶
縁ゲート型電界効果トランジスタ素子を同一チップに二
組たがいに隣り合せに形成し、それぞれのゲート電極は
、隣り合せの間で互いに対称な位置で相補関係になるよ
うに形成し、2つのトランジスタ素子からの信号を用い
て製造上のばらつきによる特性変動が相殺される相補型
半導体湿度センサが得られる。21. Structure of the Invention According to the present invention, two sets of insulated gate field effect transistor elements serving as humidity sensors having the above-described structure are formed adjacent to each other on the same chip, and the gate electrodes of each A complementary semiconductor humidity sensor is obtained in which characteristics fluctuations due to manufacturing variations are canceled out using signals from the two transistor elements.
ホ、実施例 つぎに本発明を実施例により説明する。E, Example Next, the present invention will be explained by examples.
第5図は本発明の一実施例の断面図である。第5図にお
いて、P型の半畳体基板lの一生面側には、第1図に示
したと同様の、湿度センサを形成する絶縁ゲート型電界
効果トランジスタ素子11゜12が二組互いに隣り合せ
に形成されている。しかして、素子11.12のそれぞ
れのゲート電極4a 、4bは隣り合せの間マ゛互いに
対称な位置に配置形成されている。FIG. 5 is a sectional view of one embodiment of the present invention. In FIG. 5, two sets of insulated gate field effect transistor elements 11 and 12 forming a humidity sensor, similar to those shown in FIG. It is formed. Thus, the respective gate electrodes 4a, 4b of the elements 11, 12 are arranged and formed in symmetrical positions while adjacent to each other.
へ0発明の効果
第6図(a) l (b)は本発明の作用効果を説明す
るための平面図である。第6図(a)に示す当初の設計
値であるゲート電極4aとドレイン領域5との間の距離
XQに対し、製造工程のマスク重ね合せ誤差により、設
計値x6に対し、第6図(b)に示すように△Xの寸法
誤差が生じた場合、左方のトランジスタ素子11のx=
x6+△x1右方のトランジスタ素子12のX : X
Q−△Xとなる。したがって、これら二つの素子から
のソース・ドレイン間電流ID8の流れ初めるまでの時
間Tcを測定することにより△Xに依存する項は消去さ
れ、製造上のほらつきによる特性変動は回避される。Effects of the Invention FIGS. 6(a) and 6(b) are plan views for explaining the effects of the present invention. With respect to the distance XQ between the gate electrode 4a and the drain region 5, which is the original design value shown in FIG. 6(a), due to the mask overlay error in the manufacturing process, the distance ), if a dimensional error of △X occurs, x of the left transistor element 11 =
x6+△x1 X of right transistor element 12: X
It becomes Q-△X. Therefore, by measuring the time Tc until the source-drain current ID8 starts flowing from these two elements, the term dependent on ΔX is eliminated, and characteristic fluctuations due to manufacturing irregularities are avoided.
第1図(a)は従来の半導体湿度センサの断面図、同図
(b)は平面図、第2図は第1図の結線図、第3図は時
間ヲハラメータとしてゲート・ドレイン間距離に対する
電位分布を示すグラフ、第4図は経過時間に対するソー
ス・ドレイン電流の変化を示すグラフ、第5図は本発明
の一実施例の断面図、第6図(a) I (b)は本発
明の詳細な説明するための第5図に対応する平面図であ
る。
1・・・・・・P型基板、2・・・・・・ソース領域、
3・・・・・・ゲート絶縁膜、4・・・パ・ゲート電極
、5・・・・・・ドレイン領域、11・・・・・・左側
の素子、12・・・・・・右側の素子。
z 7 図
篤 3 図 z 4 図Figure 1 (a) is a cross-sectional view of a conventional semiconductor humidity sensor, Figure 2 (b) is a plan view, Figure 2 is the connection diagram of Figure 1, and Figure 3 is a time harameter showing the potential versus gate-drain distance. FIG. 4 is a graph showing the change in source-drain current with respect to elapsed time. FIG. 5 is a cross-sectional view of an embodiment of the present invention. FIGS. FIG. 5 is a plan view corresponding to FIG. 5 for detailed explanation; 1...P-type substrate, 2...source region,
3...Gate insulating film, 4...Par gate electrode, 5...Drain region, 11...Left side element, 12...Right side element. z 7 Atsushi 3 Figure z 4 Figure
Claims (1)
によりソースおよびドレイン領域が形成され、前記ソー
ス・ドレイン間のチャンネル上に絶縁膜を介してゲート
電極が形成された絶縁ゲート型電界効果トランジスタと
類似の構造を有し、しかし゛C1前記ゲート絶縁膜の一
部が外部雰囲気に鈷出され、さらに、前記ゲート電極の
一部は、前記ソース・ドレイン領域の一方にのみ重なり
、他方に対しては所定距離を隔てて形成された半導体湿
度センサにおいて、前記絶縁ゲート型電界効果トランジ
スタ素子の組が一つの基板上に隣り合せに二組形成され
、かつそれぞれの組のゲート電極は前記隣り合せの間で
互いに対称な位置に配置形成されていることを特徴とす
る相補型半導体湿度センサ。Insulated gate field effect in which source and drain regions are formed on the whole surface side of a substrate of one conductivity type by selectively diffusing impurities of the opposite conductivity type, and a gate electrode is formed on the channel between the source and drain via an insulating film. It has a structure similar to that of a transistor, but a part of the gate insulating film is exposed to the external atmosphere, and a part of the gate electrode overlaps only one of the source/drain regions and overlaps the other. On the other hand, in a semiconductor humidity sensor formed at a predetermined distance, two sets of the insulated gate field effect transistor elements are formed adjacently on one substrate, and the gate electrode of each set is A complementary semiconductor humidity sensor characterized in that the sensors are arranged and formed at mutually symmetrical positions between the mating parts.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5880184A JPS60202343A (en) | 1984-03-27 | 1984-03-27 | Complementary type semiconductor humidity sensor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5880184A JPS60202343A (en) | 1984-03-27 | 1984-03-27 | Complementary type semiconductor humidity sensor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS60202343A true JPS60202343A (en) | 1985-10-12 |
Family
ID=13094691
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5880184A Pending JPS60202343A (en) | 1984-03-27 | 1984-03-27 | Complementary type semiconductor humidity sensor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60202343A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH03190278A (en) * | 1989-12-20 | 1991-08-20 | Oki Electric Ind Co Ltd | Offset type mis transistor device |
US7493582B2 (en) | 2005-10-31 | 2009-02-17 | Fujitsu Limited | Pattern layout and layout data generation method |
-
1984
- 1984-03-27 JP JP5880184A patent/JPS60202343A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH03190278A (en) * | 1989-12-20 | 1991-08-20 | Oki Electric Ind Co Ltd | Offset type mis transistor device |
US7493582B2 (en) | 2005-10-31 | 2009-02-17 | Fujitsu Limited | Pattern layout and layout data generation method |
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