JPH0351735A - Semiconductor pressure sensor - Google Patents

Semiconductor pressure sensor

Info

Publication number
JPH0351735A
JPH0351735A JP18774889A JP18774889A JPH0351735A JP H0351735 A JPH0351735 A JP H0351735A JP 18774889 A JP18774889 A JP 18774889A JP 18774889 A JP18774889 A JP 18774889A JP H0351735 A JPH0351735 A JP H0351735A
Authority
JP
Japan
Prior art keywords
resistance
contact
diffused
resistors
resistor
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
JP18774889A
Other languages
Japanese (ja)
Inventor
Yuji Kondo
祐司 近藤
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.)
NEC Corp
Original Assignee
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP18774889A priority Critical patent/JPH0351735A/en
Publication of JPH0351735A publication Critical patent/JPH0351735A/en
Pending legal-status Critical Current

Links

Landscapes

  • Measuring Fluid Pressure (AREA)

Abstract

PURPOSE:To decrease contact resistance and to improve temperature characteristics by forming diffused resistors constituting a pressure detecting element by plural times of diffusing steps, and connecting the diffused resistors to a conductive material through diffused parts for contact. CONSTITUTION:Diffused resistors 11 - 13 are connected to a conducting material 17 comprising aluminum and the like through contact diffusing parts 14 - 16. At this time, the contact resistances are contact resistance DELTA1 between the resistors 11 - 13 and the diffused parts 14 - 16 and contact resistance DELTAR2 at the contact plane between the diffused part 14 - 16 and the material 17 at contact hole 18. Since the resistance DELTAR1 is the resistance between the diffused resistors in silicon 7, the value is very small. The resistance DELTAR2 is proportional to the sheet resistance of the contact resistor part. In general, the sheet resistance of a gage resistor is higher than the sheet resistance of the contact resistor part by about 10 times. Therefore, the resistance DELTAR2 becomes small to a large extent. Thus the contact resistance can be decreased.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、半導体圧力センサに関し、特にオフセット
やオフセットの温度特性を改善できる拡散抵抗の構造に
関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a semiconductor pressure sensor, and particularly to a structure of a diffused resistor that can improve offset and offset temperature characteristics.

〔従来の技術〕[Conventional technology]

従来、この種の半導体圧力センサは、第3図(a)に示
すように、ダイアフラム1の周辺部にゲージ抵抗2aが
ホイートストンブリッジを構成するように4個形成して
あった。ここでゲージ抵抗2aはシリコンに不純物を拡
散して形成した拡散抵抗で構成してあり、このゲージ抵
抗2aは、第3図(b)に示すように複数本の拡散抵抗
11を直列に接続して構成され、各抵抗間は導電性の金
属21で接続されていた。この拡散抵抗11の抵抗値が
被測定流体の圧力によって励起されたダイアフラム1の
上の歪みによって変化することにより、ホイートストン
ブリッジのバランスが変化し、圧力に比例した出力が得
られるものとなっていた。なお、導電性金属21と拡散
抵抗11との間にスルーホール18が設けられている。
Conventionally, in this type of semiconductor pressure sensor, four gauge resistors 2a were formed around a diaphragm 1 to form a Wheatstone bridge, as shown in FIG. 3(a). Here, the gauge resistor 2a is composed of a diffused resistor formed by diffusing impurities into silicon, and this gauge resistor 2a is formed by connecting a plurality of diffused resistors 11 in series as shown in FIG. 3(b). Each resistor was connected with a conductive metal 21. When the resistance value of the diffusion resistor 11 changes due to the strain on the diaphragm 1 excited by the pressure of the fluid to be measured, the balance of the Wheatstone bridge changes, and an output proportional to the pressure is obtained. . Note that a through hole 18 is provided between the conductive metal 21 and the diffused resistor 11.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上述した従来の半導体圧力センサの構成では、複数本の
拡散抵抗11が直列に接続されていたために、シリコン
7中の拡散抵抗部とシリコン上の接続部の間に生ずる接
触抵抗値が抵抗の本数に比例して増加していた。この接
触抵抗と実際の拡散抵抗11の値の合計がゲージ抵抗値
になるわけであるが、その接触抵抗値がばらつくため4
個のゲージ抵抗2aにより構成されているホビー1〜ス
トンブリツジのオフセット値がデバイスによってばらつ
いていた。また、この接触抵抗と拡散抵抗の各々が持つ
抵抗値の温度係数が異なるために、ホイートストンブリ
ッジのオフセットの温度特性のばらつきを招いていた。
In the configuration of the conventional semiconductor pressure sensor described above, since the plurality of diffused resistors 11 are connected in series, the contact resistance value generated between the diffused resistor part in the silicon 7 and the connection part on the silicon is equal to the number of resistors. was increasing in proportion to. The sum of this contact resistance and the value of the actual diffusion resistance 11 is the gauge resistance value, but since the contact resistance value varies,
The offset values of Hobby 1 to Stone Bridge, which are composed of gauge resistors 2a, varied depending on the device. Furthermore, since the contact resistance and the diffused resistance each have different temperature coefficients of resistance, this causes variations in the temperature characteristics of the offset of the Wheatstone bridge.

この拡散抵抗の抵抗値をR,アルミニウム等の導電性物
質と拡散抵抗の接触抵抗を△R3とすれば、この場合の
ゲージ抵抗値GR2は水式となる。
If the resistance value of this diffused resistor is R, and the contact resistance between the conductive material such as aluminum and the diffused resistor is ΔR3, then the gauge resistance value GR2 in this case is expressed by the water formula.

GR2= (R+△R3X2)X3=RX3+ΔR3×
に の場合、アルミニウム等の導電性物質21とシリコン上
の拡散抵抗1との間の接触抵抗ΔR3は、拡散抵抗のシ
ート抵抗値に比例した値となり、接触抵抗ΔR3は、拡
散抵抗11のシート抵抗に比例する。一般的に、ゲージ
抵抗2aのシート抵抗はコンタクト用抵抗部のシート抵
抗より10倍程度は高いので、接触抵抗ΔR3が太きい 本発明の目的は、複数本の拡散抵抗を複数回の拡散によ
り形成することにより、接触抵抗を少くし、ゲージ抵抗
のばらつきを少くし、オフセット値を抑え、センサ特性
を改善した半導体圧力センサを提供することにある。
GR2= (R+△R3X2)X3=RX3+ΔR3×
In the case of is proportional to. Generally, the sheet resistance of the gauge resistor 2a is about 10 times higher than the sheet resistance of the contact resistor part, so the purpose of the present invention, which has a large contact resistance ΔR3, is to form multiple diffused resistors by multiple diffusions. By doing so, it is an object of the present invention to provide a semiconductor pressure sensor in which contact resistance is reduced, variation in gauge resistance is reduced, offset value is suppressed, and sensor characteristics are improved.

〔課題を解決するための手段〕[Means to solve the problem]

本発明の構成は、薄膜ダイアフラム部と圧力検知素子か
らなる半導体圧力センサにおいて、前記圧力検知素子を
構成する拡散抵抗を複数回の拡散工程により形成し、こ
れら拡散抵抗をコンタクト用拡散部を介して導電性物質
と接続したことを特徴とする。
The structure of the present invention is that in a semiconductor pressure sensor consisting of a thin film diaphragm part and a pressure sensing element, a diffused resistor constituting the pressure sensing element is formed by a plurality of diffusion steps, and these diffused resistors are connected via a contact diffusion part. It is characterized by being connected to a conductive substance.

〔実施例〕〔Example〕

以下、この発明の実施例を図面を用いて説明する。 Embodiments of the present invention will be described below with reference to the drawings.

第1図(a)、(b)は本発明の半導体圧力センサの一
実施例の斜視図およびそのゲージ抵抗の平面図である。
FIGS. 1(a) and 1(b) are a perspective view of an embodiment of the semiconductor pressure sensor of the present invention and a plan view of its gauge resistance.

本実施例でダイアフラム1は、被測定流体の圧力を受け
てシリコン7の上に歪みを誘起する。ダイアフラム1の
周辺部にゲージ抵抗2.3,4.5を形成する。これら
ゲージ抵抗2.3,4.5は、アルミニウムのような導
電性物質6によって接続され、ホイートストンブリッジ
を構成している。
In this embodiment, the diaphragm 1 induces strain on the silicon 7 in response to the pressure of the fluid to be measured. Gauge resistors 2.3 and 4.5 are formed around the diaphragm 1. These gauge resistors 2.3, 4.5 are connected by a conductive material 6 such as aluminum to form a Wheatstone bridge.

これらゲージ抵抗の構成は、第1図(b)のように、拡
散抵抗11〜13の3本を使用している。これら拡散抵
抗11〜13はコンタクト用拡散部14〜16を介して
アルミニウム等の導電性物質17によって接続されてい
る。この場合、その接触抵抗は拡散抵抗11〜13とコ
ンタクト用拡散部14〜16間の抵抗、およびコンタク
トホール18における拡散部14〜16と導電性物質1
7の接触面の抵抗である。拡散抵抗11〜13の1本当
たりの抵抗をR1拡散抵抗11〜13とコンタクト用拡
散部14〜16間の接触抵抗をΔR1、コンタクトホー
ル18におけるコンタクト用拡散部14〜16と導電性
物質17の接触抵抗を△R2としたとき、ゲージ抵抗の
抵抗値GR1は次のようになる。
The configuration of these gauge resistors uses three diffused resistors 11 to 13, as shown in FIG. 1(b). These diffused resistors 11 to 13 are connected by a conductive material 17 such as aluminum through contact diffusion parts 14 to 16. In this case, the contact resistance is the resistance between the diffusion resistors 11 to 13 and the contact diffusion parts 14 to 16, and the resistance between the diffusion parts 14 to 16 in the contact hole 18 and the conductive material 1.
7 is the resistance of the contact surface. The resistance per diffused resistor 11 to 13 is R1, the contact resistance between the diffused resistors 11 to 13 and the contact diffusion parts 14 to 16 is ΔR1, and the contact resistance between the contact diffusion parts 14 to 16 and the conductive material 17 in the contact hole 18 is When the contact resistance is ΔR2, the resistance value GR1 of the gauge resistance is as follows.

GR,= (R+ΔR1×2+ΔR2X2)X3=R×
3+ΔR1×6+ΔR2×6 一方、従来の半導体圧力センサにおいては、第3図(b
)のように、3本の拡散抵抗11を用いてゲージ抵抗を
構成している。このゲージ抵抗GR2は、前述のように
次式となる。
GR, = (R+ΔR1×2+ΔR2X2)X3=R×
3+ΔR1×6+ΔR2×6 On the other hand, in the conventional semiconductor pressure sensor, as shown in Fig. 3 (b
), three diffused resistors 11 are used to constitute a gauge resistor. This gauge resistance GR2 is expressed by the following formula as described above.

GR2= (R,+△R3X2)X3=RX3+ΔR3
×に れら接触抵抗ΔR1、ΔR2、ΔR3の値を比較する。
GR2= (R, +△R3X2)X3=RX3+∆R3
The values of the contact resistances ΔR1, ΔR2, and ΔR3 are compared.

接触抵抗△R1は同じシリコン7の中の拡散抵抗同士な
ので、極めて小さい値になる。
Since the contact resistance ΔR1 is a pair of diffused resistors in the same silicon 7, it has an extremely small value.

また、アルミニウム等の導電性物質とシリコン上の拡散
抵抗の間の接触抵抗△R2、ΔR3は、拡散抵抗のシー
ト抵抗値に比例した値となる。従って、接触抵抗ΔR2
はコンタクト用抵抗部のシート抵抗に比例し、接触抵抗
ΔR3は、拡散抵抗のシート抵抗に比例する。一般に、
ゲージ抵抗のシート抵抗はコンタクト用抵抗部のシート
抵抗より10倍程度は高いめで、接触抵抗ΔR2の方が
ΔR3より大幅に小さく、従って、△R1くくΔR2〈
くΔR3となる。
Further, contact resistances ΔR2 and ΔR3 between a conductive substance such as aluminum and a diffused resistor on silicon have values proportional to the sheet resistance value of the diffused resistor. Therefore, contact resistance ΔR2
is proportional to the sheet resistance of the contact resistance section, and the contact resistance ΔR3 is proportional to the sheet resistance of the diffused resistance. in general,
The sheet resistance of the gauge resistor is about 10 times higher than the sheet resistance of the contact resistance part, and the contact resistance ΔR2 is much smaller than ΔR3, so ΔR1 × ΔR2
ΔR3.

第2図は本発明の第2の実施例のゲージ抵抗部分の平面
図であり、拡散抵抗11〜13の3本を並列使用してい
る。これら拡散抵抗11〜13は、コンタクト用拡散部
19を介してアルミニウム等の導電性物質17により、
ブリッジを構成している0本実施例も第1の実施例の場
合と同様に、拡散抵抗11〜13の1本当たりの抵抗を
R、ゲージ抵抗とコンタクト用拡散部19の接触抵抗を
ΔR1、コンタクト用拡散部1つと導電性物質17の接
触抵抗を△R2としたときのゲージ抵抗の抵抗値GR3
は次のようになる。
FIG. 2 is a plan view of the gauge resistor portion of the second embodiment of the present invention, in which three diffused resistors 11 to 13 are used in parallel. These diffused resistors 11 to 13 are connected to a conductive material 17 such as aluminum through a contact diffusion part 19.
In this embodiment as well as in the first embodiment, the resistance of each diffused resistor 11 to 13 is R, and the contact resistance between the gauge resistor and the contact diffusion part 19 is ΔR1. When the contact resistance between one contact diffusion part and the conductive material 17 is △R2, the resistance value GR3 of the gauge resistance
becomes as follows.

GR9=R/4+ΔR1×2+△R2×2従って、本実
施例では、第1の実施例の場合より接触抵抗の影響が軽
減される。
GR9=R/4+ΔR1×2+ΔR2×2 Therefore, in this embodiment, the influence of contact resistance is reduced compared to the case of the first embodiment.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明の半導体圧力センサにおい
ては、ゲージ抵抗を複数回の拡散工程により形成した事
により、次の様な効果を有する。
As explained above, the semiconductor pressure sensor of the present invention has the following effects by forming the gauge resistor through a plurality of diffusion steps.

(1)接触抵抗が低下するため、ゲージ抵抗値のばらつ
きが少なくなり、オフセットが減少する。
(1) Since the contact resistance is reduced, variations in gauge resistance values are reduced, and offset is reduced.

(2)接触抵抗が低下するため、接触抵抗の温度係数の
影響を軽減でき、半導体圧力センサのオフセット温度特
性が改善される。
(2) Since the contact resistance is reduced, the influence of the temperature coefficient of contact resistance can be reduced, and the offset temperature characteristics of the semiconductor pressure sensor are improved.

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

第1図(a)、(b)は本発明の半導体圧力センサの一
実施例の斜視断面図およびその半導体圧力センサのゲー
ジ抵抗部分の平面図、第2図は本発明の第2の実施例の
ゲージ抵抗の平面図、第3図(a)、(b)は従来の半
導体圧力センサの一例の斜視断面図およびそのゲージ抵
抗の一例の平面模式図である。 1・・・ダイアフラム、2,3,4.5・・・ゲージ抵
抗、6・・・導電性金属、7・・・シリコン、8・・・
パッド、11〜13・・・拡散抵抗、14〜16.19
・・・コンタクト用拡散部、17・・・導電性物質、1
8・・・帛 1 図(幻 声 2 図 声  70  ζb)
1(a) and 1(b) are perspective sectional views of one embodiment of a semiconductor pressure sensor of the present invention and a plan view of a gauge resistance portion of the semiconductor pressure sensor, and FIG. 2 is a second embodiment of the present invention. FIGS. 3(a) and 3(b) are a perspective sectional view of an example of a conventional semiconductor pressure sensor and a schematic plan view of an example of the gauge resistor. DESCRIPTION OF SYMBOLS 1... Diaphragm, 2, 3, 4.5... Gauge resistance, 6... Conductive metal, 7... Silicon, 8...
Pad, 11-13... Diffused resistance, 14-16.19
... Contact diffusion part, 17 ... Conductive material, 1
8...File 1 figure (phantom voice 2 figure voice 70 ζb)

Claims (1)

【特許請求の範囲】[Claims] 薄膜ダイアフラム部と圧力検知素子からなる半導体圧力
センサにおいて、前記圧力検知素子を構成する拡散抵抗
を複数回の拡散工程により形成し、これら拡散抵抗をコ
ンタクト用拡散部を介して導電性物質と接続したことを
特徴とする半導体圧力センサ。
In a semiconductor pressure sensor consisting of a thin film diaphragm portion and a pressure sensing element, a diffused resistor constituting the pressure sensing element is formed by multiple diffusion steps, and these diffused resistors are connected to a conductive material via a contact diffusion portion. A semiconductor pressure sensor characterized by:
JP18774889A 1989-07-19 1989-07-19 Semiconductor pressure sensor Pending JPH0351735A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18774889A JPH0351735A (en) 1989-07-19 1989-07-19 Semiconductor pressure sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18774889A JPH0351735A (en) 1989-07-19 1989-07-19 Semiconductor pressure sensor

Publications (1)

Publication Number Publication Date
JPH0351735A true JPH0351735A (en) 1991-03-06

Family

ID=16211514

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18774889A Pending JPH0351735A (en) 1989-07-19 1989-07-19 Semiconductor pressure sensor

Country Status (1)

Country Link
JP (1) JPH0351735A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2018021923A (en) * 2017-09-12 2018-02-08 株式会社東芝 Pressure sensor, microphone, and sound processing system

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2018021923A (en) * 2017-09-12 2018-02-08 株式会社東芝 Pressure sensor, microphone, and sound processing system

Similar Documents

Publication Publication Date Title
JP3203560B2 (en) Piezoresistive silicon pressure sensor design
US4333349A (en) Binary balancing apparatus for semiconductor transducer structures
US4320664A (en) Thermally compensated silicon pressure sensor
US3858150A (en) Polycrystalline silicon pressure sensor
US3270554A (en) Diffused layer transducers
GB2042257A (en) Pressure sensor
US4683755A (en) Biaxial strain gage systems
WO1997049998A1 (en) Accelerometer without proof mass
US3537319A (en) Silicon diaphragm with optimized integral strain gages
US20070289388A1 (en) High temperature pressure transducer employing a metal diaphragm
JP2000340805A (en) Electronic part and manufacture
JPH0239574A (en) Semiconductor pressure sensor
JPH0748565B2 (en) Semiconductor pressure sensor
JPS5887880A (en) Semiconductor diaphragm sensor
CN212988661U (en) MEMS pressure chip
JP3323032B2 (en) Design method of semiconductor pressure detector
US4445108A (en) Piezoresistive transducers employing the spreading resistance effect
JPH0455542B2 (en)
JP2001124645A (en) Semiconductor pressure sensor
JPS5833136A (en) Temperature sensor
JPH06102128A (en) Semiconductor multi-function sensor
JPS629243A (en) Semiconductor tactile sensor
JPH05326985A (en) Semiconductor pressure sensor
JPH04119672A (en) Semiconductor pressure sensor
JP2621984B2 (en) Semiconductor pressure sensor