JPH02304964A - Semiconductor integrated circuit - Google Patents
Semiconductor integrated circuitInfo
- Publication number
- JPH02304964A JPH02304964A JP12575789A JP12575789A JPH02304964A JP H02304964 A JPH02304964 A JP H02304964A JP 12575789 A JP12575789 A JP 12575789A JP 12575789 A JP12575789 A JP 12575789A JP H02304964 A JPH02304964 A JP H02304964A
- Authority
- JP
- Japan
- Prior art keywords
- diffusion
- diffused
- resistors
- resistance
- wells
- 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
- 239000004065 semiconductor Substances 0.000 title claims abstract description 20
- 239000000758 substrate Substances 0.000 claims abstract description 14
- 238000009792 diffusion process Methods 0.000 abstract description 17
- 239000012535 impurity Substances 0.000 abstract description 3
- 230000000717 retained effect Effects 0.000 abstract 1
- 230000000694 effects Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 1
Landscapes
- Semiconductor Integrated Circuits (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野]
本発明は拡散抵抗を用いた半導体集積回路装置に関し、
特に拡散抵抗を直列に接続して電圧を分圧する半導体集
積回路装置に関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a semiconductor integrated circuit device using a diffused resistor,
In particular, the present invention relates to a semiconductor integrated circuit device that divides voltage by connecting diffused resistors in series.
従来、同一の半導体基板に複数個の拡散抵抗を構成する
構造を第4図に示す。図において、1はN型半導体基板
、2はこのN型半導体基板1に形成したPウェルであり
、このPウェル2内にN型不純物を拡散させた2つの拡
散抵抗3,4を形成している。この構成では、基板電位
V s u bが変動しても、Pウェル2の電位が固定
なため、拡散抵抗3.4の空乏層の広がりは一定となり
、拡散抵抗3.4の抵抗値は一定に保持される。A conventional structure in which a plurality of diffused resistors are formed on the same semiconductor substrate is shown in FIG. In the figure, 1 is an N-type semiconductor substrate, 2 is a P-well formed in this N-type semiconductor substrate 1, and two diffused resistors 3 and 4 in which N-type impurities are diffused are formed in this P-well 2. There is. In this configuration, even if the substrate potential V s u b changes, the potential of the P well 2 is fixed, so the spread of the depletion layer of the diffused resistor 3.4 is constant, and the resistance value of the diffused resistor 3.4 is constant. is maintained.
[発明が解決しようとする課題]
上述した従来の拡散抵抗を利用して電圧を分圧する場合
、例えば第3図に示すように、拡散抵抗3.4を用いて
電圧■。を1/2VDDに分圧する際には、第4図に併
せて示すように、拡散抵抗3゜4を直列に接続し、その
一端に電圧■。を、他端を接地し、拡散抵抗3,4の接
続点aから分圧を取り出している。[Problems to be Solved by the Invention] When voltage is divided using the conventional diffused resistors described above, for example, as shown in FIG. When dividing the voltage to 1/2 VDD, as shown in FIG. 4, a 3.4-diffusion resistor is connected in series, and a voltage is applied to one end. The other end is grounded, and the partial voltage is taken out from the connection point a between the diffused resistors 3 and 4.
しかしながら、従来の構成では、1つのPウェル2内に
拡散抵抗3,4をそれぞれ形成しているため、上述した
配線接続では、拡散抵抗3.4にそれぞれ加えられる電
圧とPウェル2との間の電位差に差が生じ、拡散抵抗3
,4の各空乏層3d1゜4dLの広がりが相違されるこ
とになる。このため、抵抗値R,,R,が相違され、a
点の分圧を正しく1/2・■。にすることができなくな
る。However, in the conventional configuration, the diffused resistors 3 and 4 are formed in one P-well 2, so in the above-mentioned wiring connection, the voltage applied to each of the diffused resistors 3 and 4 and the P-well 2 are A difference occurs in the potential difference between the diffusion resistance 3
, 4, the spread of each depletion layer 3d1°4dL is different. Therefore, the resistance values R,,R, are different, and a
The partial pressure at the point is correctly 1/2・■. be unable to do so.
これら拡散抵抗3.4の抵抗値R,,R,を等しくする
ためには各拡散抵抗3.4の長さを調整する必要がある
。しかしながら、この調整を行ってもVDDが変動する
と、空乏層3 dL+ 4dlが変動し、抵抗値R,
,R,が相違してしまい、必ずしもを効ではない。In order to equalize the resistance values R, , R, of these diffused resistors 3.4, it is necessary to adjust the length of each diffused resistor 3.4. However, even with this adjustment, if VDD fluctuates, the depletion layer 3 dL + 4 dl will fluctuate, and the resistance value R,
, R, are different, and it is not necessarily effective.
本発明は複数個の拡散抵抗の抵抗値を等しくして、所要
の分圧を得ることを可能にした半導体装置集積回路装置
を提供することを目的とする。SUMMARY OF THE INVENTION An object of the present invention is to provide a semiconductor device integrated circuit device that makes it possible to obtain a desired partial voltage by making the resistance values of a plurality of diffused resistors equal.
〔課題を解決するための手段]
本発明の半導体集積回路装置は、半導体基板にはそれぞ
れ独立した複数個のウェルを形成し、これらウェル内に
それぞれ拡散抵抗を形成している。[Means for Solving the Problems] In the semiconductor integrated circuit device of the present invention, a plurality of independent wells are formed in a semiconductor substrate, and a diffused resistor is formed in each of these wells.
(作用〕
上述した構成では、各拡散抵抗においては、拡散層とウ
ェルとの間の電位差を等しくし、それぞれにおける空乏
層の広がりを等しくして抵抗値を等しくすることが可能
となる。(Function) In the above-described configuration, it is possible to equalize the potential difference between the diffusion layer and the well in each diffused resistor, equalize the extent of the depletion layer in each, and equalize the resistance value.
次に、本発明を図面を参照して説明する。 Next, the present invention will be explained with reference to the drawings.
第1図は本発明の第1実施例の断面図である。FIG. 1 is a sectional view of a first embodiment of the present invention.
図において、1はN型半導体基板であり、このN型半導
体基板lにはそれぞれ独立した複数個のPウェル2A、
2Bを形成している。そして、各Pウェル2A、2Bに
はそれぞれN型不純物を拡散させた拡散層からなる拡散
抵抗3,4を形成している。In the figure, 1 is an N-type semiconductor substrate, and this N-type semiconductor substrate 1 has a plurality of independent P wells 2A,
2B is formed. In each of the P wells 2A and 2B, diffused resistors 3 and 4 made of diffusion layers in which N-type impurities are diffused are formed.
そして、この拡散抵抗3,4を用いて、第3図に示した
ようにvoの分圧を行うために、拡散抵抗3,4を直列
に接続し、一端を■。。に接続し、他端を接地し、拡散
抵抗3,4の接続点aから1/2・■、。を取り出して
いる。但し、この配線に際しては、各拡散抵抗3.4の
低電位側をそれぞれPウェル2A、2Bに接続している
。Then, in order to perform voltage division of vo using the diffused resistors 3 and 4 as shown in FIG. 3, the diffused resistors 3 and 4 are connected in series, and one end is connected to . . and ground the other end, 1/2·■, from the connection point a of the diffused resistors 3 and 4. is being taken out. However, in this wiring, the low potential side of each diffused resistor 3.4 is connected to the P wells 2A and 2B, respectively.
この構成によれば、各拡散抵抗3.4においては、いず
れも拡散抵抗3.4を構成する拡散層とPウェル2A、
2Bとの電位差が等しくなり、したがってそれぞれにお
ける空乏層3.い 4dtの広がりが等しくなる。した
がって、各拡散抵抗3゜4の抵抗値Rs、Raは等しく
なり、接続点8点の電位を正しく1/2・VDDとする
ことができる。According to this configuration, in each diffused resistor 3.4, the diffused layer constituting the diffused resistor 3.4, the P well 2A,
2B, and therefore the depletion layer 3.2B in each becomes equal. The spread of 4dt becomes equal. Therefore, the resistance values Rs and Ra of each diffused resistor 3.4 are equal, and the potential at the eight connection points can be set correctly to 1/2.VDD.
なお、この構成では■、。が変化されても各拡散抵抗3
.4の空乏層3414 dlをそれぞれ等しくでき、抵
抗値R3,R4を等しく保持することができる。In this configuration, ■. Even if the value is changed, each diffused resistance 3
.. The four depletion layers 3414 dl can be made equal to each other, and the resistance values R3 and R4 can be kept equal.
第2図は本発明の第2実施例の断面図である。FIG. 2 is a sectional view of a second embodiment of the invention.
この例では、電圧■、。を3つの拡散抵抗3.4゜5で
分圧する例を示しており、各拡散抵抗3,4゜5をそれ
ぞれ独立したPウェル2A、2B、2Cに形成している
。そして、拡散抵抗3,4.5を■Dl)と接地との間
に直列に接続し、a点又はb点 。In this example, the voltage ■,. An example is shown in which the voltage is divided by three diffused resistors 3.4°5, and the diffused resistors 3 and 4°5 are formed in independent P wells 2A, 2B, and 2C, respectively. Then, connect the diffused resistors 3 and 4.5 in series between (Dl) and the ground, and connect them to point a or point b.
からそれぞれ分圧を得ている。The partial pressure is obtained from each.
この場合にも、各拡散抵抗3,4.5の低電位側をそれ
ぞれPウェル2A、2B、2Cに接続することで、各拡
散抵抗における空乏層3 at、 4 dl+5□の
広がりを等しくし、各抵抗値R3、R−。In this case as well, by connecting the low potential side of each diffused resistor 3, 4.5 to the P wells 2A, 2B, 2C, respectively, the spread of the depletion layer 3 at, 4 dl+5□ in each diffused resistor is made equal, Each resistance value R3, R-.
R6を等しくすることが可能となる。It becomes possible to make R6 equal.
なお、前記各実施例ではN型半導体基板にPウェルを形
成してN型拡散抵抗を形成した例を示したが、逆の導電
型で構成しても良いことは言うまでもない。但し、この
場合には■。の接続が逆になることは勿論である。In each of the above embodiments, an example was shown in which a P well was formed in an N type semiconductor substrate to form an N type diffused resistor, but it goes without saying that the structure may be of the opposite conductivity type. However, in this case ■. Of course, the connections are reversed.
以上説明したように本発明は、半導体基板に独立して設
けた複数個のウェルにそれぞれ拡散抵抗を形成している
ので、各拡散抵抗における拡散層とウェルとの間の電位
差を等しくしてその空乏層の広がりを等しくし、各拡散
抵抗の抵抗値を■。0の変動等に関わらず等しく保持す
ることができ、所要の分圧を得ることができる効果があ
る。As explained above, the present invention forms a diffused resistor in each of a plurality of wells independently provided in a semiconductor substrate, so that the potential difference between the diffused layer and the well in each diffused resistor is equalized. Make the spread of the depletion layer equal and set the resistance value of each diffused resistor to ■. It is possible to maintain the same voltage regardless of fluctuations in 0, etc., and has the effect of obtaining the required partial pressure.
第1図は本発明の第1実施例の断1面図、第2図は本発
明の第2実施例の断面図、第3図は分圧回路の回路図、
第4図は従来の拡散抵抗の断面図である。
1・・・N型半導体基板、2.2A、、2B、2C・・
・Pウェル、3,4.5・・・拡散抵抗。FIG. 1 is a cross-sectional view of a first embodiment of the present invention, FIG. 2 is a cross-sectional view of a second embodiment of the present invention, and FIG. 3 is a circuit diagram of a voltage dividing circuit.
FIG. 4 is a cross-sectional view of a conventional diffused resistor. 1...N-type semiconductor substrate, 2.2A, 2B, 2C...
・P well, 3, 4.5...diffused resistance.
Claims (1)
体集積回路装置において、前記半導体基板にはそれぞれ
独立した複数個のウェルを形成し、これらウェル内にそ
れぞれ拡散抵抗を形成したことを特徴とする半導体集積
回路装置。1. A semiconductor integrated circuit device in which a plurality of diffused resistors are formed on the same semiconductor substrate, characterized in that a plurality of independent wells are formed in the semiconductor substrate, and a diffused resistor is formed in each of these wells. Semiconductor integrated circuit device.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12575789A JPH02304964A (en) | 1989-05-19 | 1989-05-19 | Semiconductor integrated circuit |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12575789A JPH02304964A (en) | 1989-05-19 | 1989-05-19 | Semiconductor integrated circuit |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02304964A true JPH02304964A (en) | 1990-12-18 |
Family
ID=14918064
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP12575789A Pending JPH02304964A (en) | 1989-05-19 | 1989-05-19 | Semiconductor integrated circuit |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02304964A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5416357A (en) * | 1991-12-17 | 1995-05-16 | Rohm Co., Ltd. | Semiconductor integrated circuit device |
JPH08204209A (en) * | 1995-01-30 | 1996-08-09 | Hitachi Ltd | Semiconductor composite sensor |
JP2006284979A (en) * | 2005-04-01 | 2006-10-19 | Hitachi Displays Ltd | Display apparatus |
US8723294B2 (en) | 2010-10-20 | 2014-05-13 | Asahi Kasei Microdevices Corporation | Resistance element and inverting buffer circuit |
-
1989
- 1989-05-19 JP JP12575789A patent/JPH02304964A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5416357A (en) * | 1991-12-17 | 1995-05-16 | Rohm Co., Ltd. | Semiconductor integrated circuit device |
JPH08204209A (en) * | 1995-01-30 | 1996-08-09 | Hitachi Ltd | Semiconductor composite sensor |
JP2006284979A (en) * | 2005-04-01 | 2006-10-19 | Hitachi Displays Ltd | Display apparatus |
US8723294B2 (en) | 2010-10-20 | 2014-05-13 | Asahi Kasei Microdevices Corporation | Resistance element and inverting buffer circuit |
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