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JP3724151B2 - Capacitance type sensor for pressure and temperature measurement, sensor device and manufacturing method thereof - Google Patents
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JP3724151B2 - Capacitance type sensor for pressure and temperature measurement, sensor device and manufacturing method thereof - Google Patents

Capacitance type sensor for pressure and temperature measurement, sensor device and manufacturing method thereof Download PDF

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JP3724151B2
JP3724151B2 JP27678197A JP27678197A JP3724151B2 JP 3724151 B2 JP3724151 B2 JP 3724151B2 JP 27678197 A JP27678197 A JP 27678197A JP 27678197 A JP27678197 A JP 27678197A JP 3724151 B2 JP3724151 B2 JP 3724151B2
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pressure
temperature
silicon
silicon member
electrode
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JPH11118644A (en
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克己 谷口
友彰 後藤
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Fuji Electric Co Ltd
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Fuji Electric Holdings Ltd
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Description

【0001】
【発明の属する技術分野】
この発明は、単結晶シリコンシリコン部材およびその両面に固着された絶縁性セラミックからなる圧力および温度計測用静電容量型センサおよびセンサ装置、およびそれらの製造方法に関する。
【0002】
【従来の技術】
図7は従来の圧力計測用静電容量型センサの断面図である。
従来の圧力計測用静電容量型センサSaの主要構成部材は単結晶シリコンのシリコン部材1とその両面に固着されたセラミック部材2である。シリコン部材1の中央にはシリコン部材より薄い電極板1eとこれを支持するさらに薄いリングダイヤフラム1dが作り込まれている。電極板1eの両面には例えばSiO2 からなる絶縁膜1iが形成されている。シリコン部材1aとほぼ同じ周形の2つのセラミック部材2aの中央にはスルーホールH1が貫通している。セラミック部材2のシリコン部材1aに対向する面には低融点ガラス薄膜2gが形成されている。低融点ガラス薄膜2gの電極板1eに対向する面、スルーホールH1の表面およびセラミック部材2aの他の表面は金属からなる薄膜電極2mにより被覆されている。シリコン部材1aとセラミック部材2aは低融点ガラス薄膜2gを介して、陽極接合されて互いに密着固定されている。
【0003】
このようにして、セラミック部材2aおよび電極板1eとリングダイヤフラム1dにより囲まれた2つの室が形成され、各室はスルーホールH1により外部空間に連なっている。電極板1eの表面と対向するセラミック部材の薄膜電極2mはその間の空間すなわちギャップG1、G2をそれぞれ挟み第1および第2の静電容量を形成している。リングダイヤフラム1dは極めて薄いので、各スルーホールH1を通じて両室に圧力差を生じさせれば、これに対応して電極板1eは動き、電極板1eの両側の第1および第2の静電容量に差が生ずる、すなわち静電容量型の圧力センサとなる。圧力差がないとき2つの静電容量は等しい。そして、図示してない回路により静電容量の差を検出し、圧力差信号を出力している。従って、一方のギャップを既知の圧力に固定すれば、他方のギャップの絶対圧力を計測することができる。
【0004】
通常は静電容量型センサ(以下センサと略記することもある)に直接外力が加わらないように、センサをパッケージに収容しセンサ装置を構成している。図8は従来の静電容量型センサ装置の断面図である。外部への開口部が形成されている第1のパッケージ部材P1は一方のセラミック部材2aに薄膜電極2mを介して接続され、スルーホールH1と開口部が連結されている。外部への開口部が形成されている第2のパッケージ部材P2は第1のパッケージ部材P1の周縁部に接続され他のセラミック部材2aのスルーホールH1は第2のパッケージ部材P2内に開口している。パッケージ部材は金属またはセラミックからなっている。
【0005】
【発明が解決しようとする課題】
上記のような陽極接合された単結晶シリコンおよびセラミックからなる静電容量型センサには以下のような問題点がある。
単結晶シリコンと絶縁性セラミックの線膨張係数はともに2 ×10-6〜4 ×10-6/℃程度であるが、その値を厳密に等しくすることは難しく、例え常温付近でその値が等しく製造できたとしても、センサの温度が変わると、見かけ上の圧力差が生じてしまう。
【0006】
この原因は、従来の製造方法、特に陽極接合方法にある。図9は従来の陽極接合工程における静電容量型センサの断面図であり、(a)は第1の陽極接合時、(b)は第2の陽極接合時である。陽極接合は、シリコン部材とセラミック部材を重ね、所定温度の金属表面(陽極接合部に電圧印加するためヒータTの表面は金属膜Tsで被覆されている)のヒータに置き、接合部に電圧印加して行う。第1の陽極接合時では、温度200 〜700 ℃で両材質が熱膨張した状態で、第1のシリコン部材1aとセラミック部材2aを接合しておき、次いで、他のセラミック部材2aに先の2層を重ね、同様に陽極接合を行っていた。いずれの場合も、ヒータ側を高温として温度勾配が生じており、セラミック部材より機械的強度の小さいシリコン部材に引張りあるいは圧縮応力が残留していた。その防止のため、第1および第2の陽極接合時の温度を同じとしても、やはり、シリコン部材の両面には数十℃の温度差が生じ、シリコン部材の両面間には残留応力の差が生じていた。従って、両室の圧力差が無い場合にも、見かけ上の圧力差が生じ、高精度な圧力計測には適さないことがあった。
【0007】
また、上記の構造のセンサでは圧力(あるいは圧力差)のみしか計測できなかった。
上記の問題点に鑑み、本発明の目的は、シリコン部材の歪みが小さくみかけの圧力差のないセンサの製造方法を提供し、さらに圧力だけでなく温度も計測できる高精度な多層の静電容量センサとその製造方法を提供することにある。
【0008】
【課題を解決するための手段】
上記の目的を達成するために、シリコン部材の厚さより薄い電極部とこれを支持するリングダイヤフラムを有する単結晶シリコンからなる第1のシリコン部材の両面に、少なくとも前記電極部に対向する薄膜電極を有する2枚のセラミック部材が低融点ガラス膜を介して陽極接合されてなり、電極部と薄膜電極が2つの静電容量を形成している圧力および温度計測用静電容量型センサにおいて、シリコン単結晶からなり平坦な凹部である電極部が形成された第2のシリコン部材が、前記セラミック部材に低融点ガラス膜を介して陽極接合されてなる4層構造の静電容量型センサであり、さらに第2のシリコン部材の電極部とこれに対向する部分に形成されたセラミック部材の第2の電極薄膜とがギャップを挟んで第3の静電容量を形成していることとする。
【0010】
前記セラミック部材には、前記第2のシリコン部材の電極部に対向する部分に開口するスルーホールが開けられており、かつ前記第2の電極薄膜はこのスルーホールの内面および前記第1のシリコン部材のスルーホールの開口部面にも拡張して形成されており、前記第1のシリコン部材が3つの静電容量の共通電極とされていると良い。
【0011】
前記第2のシリコン部材には前記ギャップに通じるスルーホールが開けられていると良い。
上記の4層構造の圧力および温度計測用静電容量型センサの製造方法であって、前記第1のシリコン部材の両面に前記2枚のセラミック部材を低融点ガラス膜を介して陽極接合するとともに、前記陽極接合は前記第1のシリコン部材と前記2枚のセラミック部材が3層に積層された状態で行われ、かつ全体が均一な温度に加熱されて行われるようにして、前記第1のシリコン部材と前記2枚のセラミック部材と3層構造に形成た後、前記セラミック部材の所定面に前記第2のシリコン部材を低融点ガラスを介して陽極接合することする。
【0012】
前記低融点ガラスは予め前記絶縁性セラミック部材上に形成された膜であると良い。
前記陽極接合は、前記3層構造および第2のシリコン部材を挟むそれぞれに独立に温度制御される2つのヒータによりなされ、陽極接合温度を任意に変化させると良い。
【0013】
上記の4層構造の圧力および温度計測用静電容量型センサに、第2のシリコン部材のスルーホールおよび第2のシリコン部材の配された方のセラミック部材のスルーホールの開口部および外部に向けて開けられた開口部を同一空間に有する第1の圧力室をなす第1のパッケージ、および他のセラミック部材のスルーホールの開口部および外部に向けて開けられた開口部を同一空間に有する第2の圧力室をなす第2のパッケージが付加されてなり、第1の圧力室には誘電率の温度係数の大きい流体を充填してあって、第1の圧力室と第2の圧力室の圧力差を計測し、また第3の静電容量の温度変化から温度計測ができることとする。
【0014】
本発明の製造方法によれば、シリコン部材とその両面に接合するセラミック部材の3層構造を3層同時に均一温度で陽極接合するので、熱応力歪みは従来の製造方法の接合時のシリコン部材の両面の状況が異なる場合よりは小さく、また、シリコン部材内部で面方向に対称である。従って、センサの温度変化によって電極部は移動せずギャップは変化しない、すなわち各静電容量は変化せず、従って、センサが温度変化してもみかけの圧力差は常に生じないことが期待できる。
【0015】
た、本発明に係る4層構造では、新たに付加されたギャップが閉空間の場合は、センサ固有の一定静電容量であり、これを基準圧力とみなすことができるので、これとの比較により絶対圧力を計測することができる。また、2つの計測用静電容量に僅かに生じた差の補正のために使用することもでき、高精度の圧力計測が可能となる。
【0016】
また開空間の場合は、新たに付加されたギャップと従来のギャップとに同じ流体を入れておくことと、静電容量は圧力変動を受けないので、ギャップ内の流体の誘電率の温度変化による静電容量の変化のみが生じ、温度測定ができる。
【0017】
【発明の実施の形態】
以下、図面に基づき本発明の実施例ついて説明する。
実施例1
図1は本発明に係る固定ギャップを有する静電容量型センサの断面図である。従来の3層構造センサのセラミック部材に新たに第2のシリコン部材を付加してある。従来のセンサ(図7)と異なっている部分のみを説明する。一方のセラミック部材2bの両面には低融点ガラス薄膜2gが形成され、さらにスルーホールH2が開けられている。スルーホールH2の表面、底(第1のシリコン部材)および低融点ガラス薄膜2gの表面には金属薄膜2mおよび2nが形成されている。
【0018】
セラミック部材2bに陽極接合されている第2のシリコン部材1bには凹部が形成されており、その底部(電極部である)は平面であり、絶縁膜1iが形成されている。この電極部と対向するセラミック部材2bの金属薄膜2nはこれらの間の空間すなわち固定ギャップG3を挟んで第3の静電容量を形成している。この第3の静電容量は圧力に依存しないので、絶対圧力とみなしたり、あるいは2つの静電容量の微差の補正に用いることができる。
【0019】
次に、上記センサの製造方法を説明する。
図2は本発明に係る第3の静電容量を有する静電容量型センサの各セラミック部材の製造工程における断面図であり、(a1)および(a2)は低融点ガラス膜形成後、(b1)および(b2)はスルーホール形成後、(c1)および(c2)は薄膜電極形成後である。
【0020】
先ず、厚さ数mmの板状のセラミック部材2aおよび2bの片面に、パイレックスガラスなどのホウ珪酸ガラスからなる厚さ数μm の低融点ガラス膜2gをスパッタリングにより形成し(図2(a1)、(a2))、超音波加工などによりスルーホールH1およびH2(セラミック部材2bのみ)を形成した(図2(b1)、(b2))。次に、両側から、スパッタなどにより、金およびクロムからなる薄膜電極2mをスルーホールH1の内面とそれに連なる両面の所定領域に蒸着した(図2(c1)、(c2))。
【0021】
図3は本発明に係る3層同時陽極接合時の状態を示す断面図である。
シリコン部材1aには、プラズマエッチングにより両面から静電容量形成のためのギャップ相当分の凹部を加工した後、リング状の溝加工を施しリングダイヤフラム1dおよびリングダイヤフラム1dに周縁部を支持された電極部1eを形成してある。電極部1eの両面には静電容量を増加させるためSiO2 等の誘電体膜1iを形成してある。
【0022】
このシリコン部材1aの両面に、上記のセラミック部材2aおよび2bの低融点融点ガラス膜2gを密着させ全3層とし、この3層を2つのヒータTで挟み加圧、加熱し、またシリコン部材1aとセラミック部材2a、2bには電圧(電源E)を印加して陽極接合を行った。
陽極接合時、加圧圧力は約100N/cm2以下とし、温度を200 〜700 ℃の範囲で保持した。印加電圧は300 〜700Vとした。特に、シリコン部材1aとセラミック部材2a、2b内部に温度差が生じないように2つのヒータの温度をそれぞれ制御した、そのため、室温に下げられたとき、シリコン部材1aとセラミック部材2a、2bの熱膨張係数の微細な差によって生ずる熱歪みはリングダイヤフラム面に対して対称であり、リングダイヤフラムがいずれかの方向にずれることはなく、この3層構造体(スルーホールH2がなければ従来のセンサと同じである)の2つの静電容量には差はなくまたその温度変化も生じなかった。
【0023】
そして、セラミック部材2bの所定領域、スルーホールH2の内面および底面(第1のシリコン部材1a)に薄膜電極2nをスパッタにより形成した。
次に、プラズマエッチングによりギャップ相当分の凹部を形成した第2のシリコン部材1bを上記の3層構造体のセラミック部材2bに取り付けた。図4は本発明に係る4層構造のセンサの第2のシリコン部材と3層構造体との陽極接合時を示す断面図である。この場合2つのヒータの温度は3層構造の陽極接合時より低くし、熱歪みが増加しないようにした。
【0024】
なお、上記の3層構造迄の製造方法は従来の3層構造の圧力計測用のセンサの製造にも適用できることは明らかである。
実施例2
図5は本発明に係る温度計測可能な静電容量型センサの断面図である。この静電容量型センサScでは、実施例1における第2のシリコン部材1bに換えて、電極部1eにギャップG3とセンサ外部とを連通するスルーホールH3が開けられている第3のシリコン部材1cが取り付けられている。この4層構造のセンサの他の部分およびその製造方法は実施例1と同じであるので説明を省略する。
【0025】
図6は本発明に係る温度計測可能な静電容量型センサ装置の断面図である。従来センサ装置と同様に、パッケージ部材P1にセラミック部材2aが取り付けられ、さらにパッケージ部材P2がスルーホールH1およびH3の開口部を内部に収めてパッケージ部材P1に接合されている。
誘電率の温度変化の大きい流体、例えばシリコンオイルをパッケージにいれ、圧力源と連結する。こうして、シリコン部材1aの静電容量変化から圧力差を計測し、シリコン部材1側の固定ギャップでの静電容量は圧力変化により変化しないので、静電容量変化から温度を計測することができる。
【0026】
【発明の効果】
本発明によれば、電極部とこれを支持するリングダイヤフラムを有する単結晶シリコンからなる第1のシリコン部材の両面に、少なくとも前記電極部に対向する薄膜電極を有する2枚のセラミック部材が低融点ガラス膜を介して陽極接合されてなり、電極部と薄膜電極がギャップを挟んで2つの静電容量を形成している少なくとも3層構造を有する圧力および温度計測用静電容量型センサの製造方法において、前記陽極接合を前記第1のシリコン部材と前記2枚のセラミック部材が3層に積層された状態で行ない、かつ全体が均一な温度に加熱したため、熱応力歪みは従来の製造方法よりは小さく、また、シリコン部材内部で面方向に対称である。従って、センサの温度変化によって電極部は移動せずギャップは変化しないすなわち各静電容量は変化せず、センサが温度変化してもみかけの圧力差は常に生じない。
【0027】
また、上記の製造方法による3層構造センサの前記セラミック部材に低融点ガラス膜を介して、シリコン単結晶からなり平坦な凹部である電極部が形成された第2のシリコン部材を陽極接合して第3の静電容量を付加したため、第3の静電容量を利用して絶対圧力や温度の計測ができるようになった。そのため他の温度計を必要としなくなり、計装が簡易化できるようになった。
【図面の簡単な説明】
【図1】本発明に係る固定静電容量を有する静電容量型センサの断面図
【図2】本発明に係る固定静電容量を有する静電容量型センサの各セラミック部材の製造工程における断面図であり、(a1)および(a2)は低融点ガラス膜形成後、(b1)および(b2)はスルーホール形成後、(c1)および(c2)は薄膜電極形成後を示す
【図3】本発明に係る3層同時陽極接合時の状態を示す断面図
【図4】本発明に係る4層構造のセンサの第2のシリコン部材と3層構造体との陽極接合時を示す断面図
【図5】本発明に係る温度計測可能な静電容量型センサの断面図
【図6】本発明に係る温度計測可能な静電容量型センサ装置の断面図
【図7】従来の静電容量型センサの断面図
【図8】従来の静電容量型センサ装置の断面図
【図9】従来の陽極接合工程における静電容量型センサの断面図であり、(a)は第1の陽極接合時、(b)は第2の陽極接合時を示す
【符号の説明】
1a 第1のシリコン部材
1b 第2のシリコン部材
1d リングダイヤフラム
1e 電極部
1i 絶縁膜
2a セラミック部材
2b セラミック部材
2g 低融点ガラス膜
2m 薄膜電極
2n 薄膜電極
H1 スルーホール
H2 スルーホール
H3 スルーホール
G1 ギャップ
G2 ギャップ
G3 固定ギャップ
Sa 従来の静電容量型センサ
Sb 本発明に係る静電容量型センサ
Sc 本発明に係る静電容量型センサ
T ヒータ
Ts ヒータの金属表面部
P1 パッケージ部材
P2 パッケージ部材
E 電源
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a pressure- and temperature-measuring capacitive sensor and sensor device comprising a single-crystal silicon silicon member and an insulating ceramic fixed to both surfaces thereof, and a method of manufacturing the same.
[0002]
[Prior art]
FIG. 7 is a cross-sectional view of a conventional capacitive sensor for pressure measurement.
The main constituent members of a conventional capacitance measuring sensor Sa for pressure measurement are a silicon member 1 made of single crystal silicon and a ceramic member 2 fixed to both surfaces thereof. In the center of the silicon member 1, an electrode plate 1e thinner than the silicon member and a thinner ring diaphragm 1d for supporting the electrode plate 1e are formed. Insulating films 1i made of, for example, SiO 2 are formed on both surfaces of the electrode plate 1e. A through hole H1 passes through the center of two ceramic members 2a having substantially the same circumferential shape as the silicon member 1a. A low melting point glass thin film 2g is formed on the surface of the ceramic member 2 facing the silicon member 1a. The surface of the low-melting glass thin film 2g facing the electrode plate 1e, the surface of the through hole H1, and the other surface of the ceramic member 2a are covered with a thin film electrode 2m made of metal. The silicon member 1a and the ceramic member 2a are anodically bonded to each other through a low melting point glass thin film 2g and are firmly fixed to each other.
[0003]
In this way, two chambers surrounded by the ceramic member 2a, the electrode plate 1e, and the ring diaphragm 1d are formed, and each chamber is connected to the external space by the through hole H1. The thin film electrode 2m of the ceramic member facing the surface of the electrode plate 1e forms first and second capacitances with a space between them, that is, gaps G1 and G2, respectively. Since the ring diaphragm 1d is extremely thin, if a pressure difference is generated between the two chambers through the through holes H1, the electrode plate 1e moves correspondingly, and the first and second electrostatic capacitances on both sides of the electrode plate 1e. Therefore, a capacitance type pressure sensor is obtained. When there is no pressure difference, the two capacitances are equal. Then, a difference in capacitance is detected by a circuit (not shown), and a pressure difference signal is output. Therefore, if one gap is fixed to a known pressure, the absolute pressure of the other gap can be measured.
[0004]
Normally, a sensor device is configured by housing the sensor in a package so that an external force is not directly applied to the capacitance type sensor (hereinafter sometimes abbreviated as “sensor”). FIG. 8 is a cross-sectional view of a conventional capacitive sensor device. The first package member P1 in which an opening to the outside is formed is connected to one ceramic member 2a via a thin film electrode 2m, and the through hole H1 and the opening are connected. The second package member P2 in which the opening to the outside is formed is connected to the peripheral edge of the first package member P1, and the through hole H1 of the other ceramic member 2a is opened in the second package member P2. Yes. The package member is made of metal or ceramic.
[0005]
[Problems to be solved by the invention]
The capacitance type sensor composed of single crystal silicon and ceramic that are anodically bonded as described above has the following problems.
The linear expansion coefficients of single crystal silicon and insulating ceramic are both about 2 × 10 -6 to 4 × 10 -6 / ° C, but it is difficult to make the values exactly the same, for example, the values are the same at around room temperature. Even if it can be manufactured, if the temperature of the sensor changes, an apparent pressure difference will occur.
[0006]
This is due to the conventional manufacturing method, particularly the anodic bonding method. 9A and 9B are cross-sectional views of the capacitance type sensor in the conventional anodic bonding process, where FIG. 9A shows the first anodic bonding and FIG. 9B shows the second anodic bonding. In anodic bonding, a silicon member and a ceramic member are stacked, placed on a heater on a metal surface at a predetermined temperature (the surface of the heater T is coated with a metal film Ts to apply a voltage to the anodic bonding portion), and voltage is applied to the bonding portion. And do it. At the time of the first anodic bonding, the first silicon member 1a and the ceramic member 2a are bonded in a state where both materials are thermally expanded at a temperature of 200 to 700 ° C., and then the other ceramic member 2a is bonded to the previous two. The layers were stacked and anodic bonded in the same way. In either case, a temperature gradient was generated with the heater side at a high temperature, and tensile or compressive stress remained on the silicon member having a mechanical strength lower than that of the ceramic member. In order to prevent this, even if the temperature at the time of the first and second anodic bonding is the same, a temperature difference of several tens of degrees Celsius still occurs on both surfaces of the silicon member, and there is a difference in residual stress between both surfaces of the silicon member. It was happening. Therefore, even when there is no pressure difference between the two chambers, an apparent pressure difference occurs, which may not be suitable for highly accurate pressure measurement.
[0007]
Moreover, only the pressure (or pressure difference) could be measured with the sensor having the above structure.
In view of the above problems, an object of the present invention is to provide a sensor manufacturing method in which the distortion of a silicon member is small and there is no apparent pressure difference, and furthermore, a highly accurate multilayer capacitance capable of measuring not only pressure but also temperature. It is to provide a sensor and a manufacturing method thereof.
[0008]
[Means for Solving the Problems]
In order to achieve the above object , at least thin film electrodes opposed to the electrode portions are provided on both surfaces of a first silicon member made of single crystal silicon having an electrode portion thinner than the thickness of the silicon member and a ring diaphragm supporting the electrode portion. In a capacitive sensor for pressure and temperature measurement in which two ceramic members are anodically bonded via a low melting point glass film, and the electrode part and the thin film electrode form two capacitances, The second silicon member made of a crystal and formed with a flat concave electrode portion is a four-layer capacitive sensor in which the ceramic member is anodically bonded to the ceramic member through a low-melting glass film, The electrode portion of the second silicon member and the second electrode thin film of the ceramic member formed on the portion facing the second silicon member form a third capacitance with a gap in between. It is assumed that.
[0010]
The ceramic member has a through hole opened at a portion facing the electrode portion of the second silicon member, and the second electrode thin film has an inner surface of the through hole and the first silicon member. It is preferable that the first silicon member is a common electrode having three capacitances.
[0011]
It is preferable that a through hole leading to the gap is opened in the second silicon member.
A method of manufacturing a capacitive sensor for measuring pressure and temperature of the above four-layer structure , wherein the two ceramic members are anodically bonded to both surfaces of the first silicon member via a low-melting glass film. The anodic bonding is performed in a state where the first silicon member and the two ceramic members are laminated in three layers, and the whole is heated to a uniform temperature, so that the first bonding is performed . after forming the said two ceramic members with silicon member in a three-layer structure, to be anodically bonded via a low-melting glass said second silicon member to a predetermined surface of the ceramic member.
[0012]
The low melting point glass may be a film formed in advance on the insulating ceramic member.
The anodic bonding is performed by two heaters that are independently temperature controlled with the three-layer structure and the second silicon member interposed therebetween, and the anodic bonding temperature may be arbitrarily changed.
[0013]
The capacitance sensor for pressure and temperature measurement of the four-layer structure described above is directed to the opening of the through hole of the second silicon member and the through hole of the ceramic member on which the second silicon member is disposed and to the outside. The first package forming the first pressure chamber having the opening opened in the same space, and the opening of the through hole of the other ceramic member and the opening opened to the outside in the same space. A second package forming two pressure chambers is added, and the first pressure chamber is filled with a fluid having a large dielectric constant temperature coefficient, and the first pressure chamber and the second pressure chamber are filled with each other. The pressure difference is measured, and the temperature can be measured from the temperature change of the third capacitance.
[0014]
According to the manufacturing method of the present invention, the three-layer structure of the silicon member and the ceramic member bonded to both surfaces thereof is anodically bonded at a uniform temperature at the same time. It is smaller than the situation where both sides are different, and is symmetrical in the plane direction inside the silicon member. Therefore, the electrode portion does not move and the gap does not change due to the temperature change of the sensor, that is, each capacitance does not change. Therefore, it can be expected that an apparent pressure difference does not always occur even if the sensor temperature changes.
[0015]
Also, in 4-layer structure according to the present invention, in the case of the closed space newly added gap, a sensor-specific constant capacitance, it can be regarded as this reference pressure, compared with this Thus, absolute pressure can be measured. Further, it can be used for correcting a slight difference between the two capacitances for measurement, and pressure measurement with high accuracy is possible.
[0016]
In the case of an open space, the same fluid is put in the newly added gap and the conventional gap, and the capacitance is not subject to pressure fluctuations. Only a change in capacitance occurs and temperature can be measured.
[0017]
DETAILED DESCRIPTION OF THE INVENTION
Embodiments of the present invention will be described below with reference to the drawings.
Example 1
FIG. 1 is a cross-sectional view of a capacitive sensor having a fixed gap according to the present invention. A second silicon member is newly added to the ceramic member of the conventional three-layer structure sensor. Only the parts different from the conventional sensor (FIG. 7) will be described. A low melting point glass thin film 2g is formed on both surfaces of one ceramic member 2b, and a through hole H2 is further opened. Metal thin films 2m and 2n are formed on the surface of the through hole H2, the bottom (first silicon member) and the surface of the low melting point glass thin film 2g.
[0018]
A recess is formed in the second silicon member 1b that is anodically bonded to the ceramic member 2b, and its bottom portion (which is an electrode portion) is a flat surface, and an insulating film 1i is formed. The metal thin film 2n of the ceramic member 2b facing the electrode portion forms a third capacitance with a space between them, that is, a fixed gap G3 interposed therebetween. Since the third capacitance does not depend on the pressure, it can be regarded as an absolute pressure or can be used to correct a slight difference between the two capacitances.
[0019]
Next, a method for manufacturing the sensor will be described.
FIG. 2 is a cross-sectional view in the manufacturing process of each ceramic member of the capacitance type sensor having the third capacitance according to the present invention, wherein (a1) and (a2) are (b1 ) And (b2) are after through-hole formation, and (c1) and (c2) are after thin-film electrode formation.
[0020]
First, a low melting glass film 2g having a thickness of several μm made of borosilicate glass such as Pyrex glass is formed on one surface of plate-like ceramic members 2a and 2b having a thickness of several mm by sputtering (FIG. 2 (a1)). (A2)), through holes H1 and H2 (only the ceramic member 2b) were formed by ultrasonic machining or the like (FIGS. 2 (b1) and (b2)). Next, a thin film electrode 2m made of gold and chrome was deposited from both sides by sputtering or the like on the inner surface of the through hole H1 and a predetermined region on both sides connected to the inner surface (FIG. 2 (c1), (c2)).
[0021]
FIG. 3 is a sectional view showing a state at the time of three-layer simultaneous anodic bonding according to the present invention.
In the silicon member 1a, a recess corresponding to a gap for forming a capacitance is processed from both surfaces by plasma etching, and then a ring-shaped groove is processed to provide a ring diaphragm 1d and an electrode whose peripheral portion is supported by the ring diaphragm 1d. Part 1e is formed. Dielectric films 1i such as SiO 2 are formed on both surfaces of the electrode portion 1e in order to increase the capacitance.
[0022]
The low melting point glass films 2g of the ceramic members 2a and 2b are adhered to both surfaces of the silicon member 1a to form a total of three layers, and these three layers are sandwiched between two heaters T and pressurized and heated, and the silicon member 1a The ceramic members 2a and 2b were subjected to anodic bonding by applying a voltage (power source E).
At the time of anodic bonding, the pressing pressure was about 100 N / cm 2 or less, and the temperature was maintained in the range of 200 to 700 ° C. The applied voltage was 300 to 700V. In particular, the temperatures of the two heaters were controlled so that there was no temperature difference between the silicon member 1a and the ceramic members 2a and 2b. Therefore, when the temperature was lowered to room temperature, the heat of the silicon member 1a and the ceramic members 2a and 2b The thermal strain caused by a small difference in expansion coefficient is symmetric with respect to the ring diaphragm surface, and the ring diaphragm does not shift in either direction, and this three-layer structure (if there is no through hole H2) No difference was found between the two capacitances and the temperature did not change.
[0023]
Then, a thin film electrode 2n was formed by sputtering on a predetermined region of the ceramic member 2b, the inner surface and the bottom surface (first silicon member 1a) of the through hole H2.
Next, the second silicon member 1b in which the recess corresponding to the gap was formed by plasma etching was attached to the ceramic member 2b having the above three-layer structure. FIG. 4 is a cross-sectional view illustrating the anodic bonding of the second silicon member and the three-layer structure of the sensor having the four-layer structure according to the present invention. In this case, the temperature of the two heaters was set lower than that in the anodic bonding of the three-layer structure so that the thermal strain did not increase.
[0024]
It is obvious that the manufacturing method up to the above three-layer structure can also be applied to the manufacture of a conventional sensor for pressure measurement having a three-layer structure.
Example 2
FIG. 5 is a cross-sectional view of a capacitive sensor capable of measuring temperature according to the present invention. In this capacitive sensor Sc, instead of the second silicon member 1b in the first embodiment, a third silicon member 1c in which a through hole H3 that communicates the gap G3 and the outside of the sensor is opened in the electrode portion 1e. Is attached. Since other parts of the sensor having the four-layer structure and the manufacturing method thereof are the same as those in the first embodiment, the description thereof is omitted.
[0025]
FIG. 6 is a sectional view of a capacitive sensor device capable of measuring temperature according to the present invention. Similarly to the conventional sensor device, the ceramic member 2a is attached to the package member P1, and the package member P2 is joined to the package member P1 with the openings of the through holes H1 and H3 inside.
A fluid having a large dielectric constant temperature change, such as silicon oil, is put in a package and connected to a pressure source. Thus, by measuring the pressure difference from the change in capacitance of the silicon member 1a, the capacitance of a fixed gap of silicon member 1 c side does not change the pressure change, it is possible to measure the temperature from the capacitance change .
[0026]
【The invention's effect】
According to the present invention, two ceramic members having at least a thin film electrode opposed to the electrode portion on both surfaces of a first silicon member made of single crystal silicon having an electrode portion and a ring diaphragm supporting the electrode portion have a low melting point. Method for manufacturing a capacitive sensor for pressure and temperature measurement, having an at least three-layer structure in which an electrode portion and a thin film electrode form two capacitances with a gap interposed therebetween, which are anodically bonded through a glass film In the above, the anodic bonding is performed in a state where the first silicon member and the two ceramic members are laminated in three layers, and the whole is heated to a uniform temperature. It is small and symmetrical in the plane direction inside the silicon member. Therefore, the electrode portion does not move and the gap does not change due to the temperature change of the sensor, that is, each capacitance does not change, and an apparent pressure difference does not always occur even if the sensor temperature changes.
[0027]
In addition, a second silicon member made of a silicon single crystal and having an electrode portion which is a flat concave portion is anodically bonded to the ceramic member of the three-layer structure sensor according to the above manufacturing method via a low melting point glass film. Since the third capacitance is added, absolute pressure and temperature can be measured using the third capacitance. As a result, no other thermometer is required and the instrumentation can be simplified.
[Brief description of the drawings]
FIG. 1 is a cross-sectional view of a capacitive sensor having a fixed capacitance according to the present invention. FIG. 2 is a cross-sectional view in the manufacturing process of each ceramic member of the capacitive sensor having a fixed capacitance according to the present invention. (A1) and (a2) are after low-melting glass film formation, (b1) and (b2) are after through-hole formation, and (c1) and (c2) are after thin-film electrode formation. FIG. 4 is a cross-sectional view showing a state at the time of three-layer simultaneous anodic bonding according to the present invention. FIG. 4 is a cross-sectional view showing at the time of anodic bonding between a second silicon member and a three-layer structure of a four-layer sensor according to the present invention. FIG. 5 is a cross-sectional view of a capacitive sensor capable of measuring temperature according to the present invention. FIG. 6 is a cross-sectional view of a capacitive sensor device capable of measuring temperature according to the present invention. Sectional view of sensor [FIG. 8] Sectional view of conventional capacitive sensor device [FIG. 9] Conventional It is a cross-sectional view of the capacitive sensor in anodic bonding step, (a) shows the time of the first anodic bonding, (b) shows a time second anodic bonding [description of symbols]
DESCRIPTION OF SYMBOLS 1a 1st silicon member 1b 2nd silicon member 1d Ring diaphragm 1e Electrode part 1i Insulating film 2a Ceramic member 2b Ceramic member 2g Low melting glass film 2m Thin film electrode 2n Thin film electrode H1 Through hole H2 Through hole H3 Through hole G1 Gap G2 Gap G3 Fixed gap Sa Conventional capacitance type sensor Sb Capacitance type sensor Sc according to the present invention Capacitance type sensor T according to the present invention T Heater Ts Metal surface portion P1 of the heater P1 Package member P2 Package member E Power source

Claims (7)

シリコン部材の厚さより薄い電極部とこれを支持するリングダイヤフラムを有する単結晶シリコンからなる第1のシリコン部材の両面に、少なくとも前記電極部に対向する薄膜電極を有する2枚のセラミック部材が低融点ガラス膜を介して陽極接合されてなり、電極部と薄膜電極が2つの静電容量を形成している圧力および温度計測用静電容量型センサにおいて、シリコン単結晶からなり平坦な凹部である電極部が形成された第2のシリコン部材が、前記セラミック部材に低融点ガラス膜を介して陽極接合されてなる4層構造の静電容量型センサであり、さらに第2のシリコン部材の電極部とこれに対向する部分に形成されたセラミック部材の第2の電極薄膜とがギャップを挟んで第3の静電容量を形成していることを特徴とする圧力および温度計測用静電容量型センサ。Two ceramic members having at least a thin film electrode facing the electrode portion on both surfaces of a first silicon member made of single crystal silicon having an electrode portion thinner than the thickness of the silicon member and a ring diaphragm supporting the electrode portion have a low melting point. An electrode that is a flat recess made of a single crystal of silicon in a capacitive sensor for pressure and temperature measurement, which is anodically bonded through a glass film, and in which the electrode part and the thin film electrode form two capacitances A second silicon member having a portion formed thereon is a four-layer capacitive sensor formed by anodically bonding the ceramic member through a low melting point glass film; and an electrode portion of the second silicon member; A pressure which is characterized in that a third electrostatic capacity is formed with a gap between the second electrode thin film of the ceramic member formed in a portion facing this and a gap; Capacitive sensor for degree measurement. 前記セラミック部材には、前記第2のシリコン部材の電極部に対向する部分に開口するスルーホールが開けられており、かつ前記第2の電極薄膜はこのスルーホールの内面および前記第1のシリコン部材のスルーホールの開口部面にも拡張して形成されており、前記第1のシリコン部材が3つの静電容量の共通電極とされていることを特徴とする請求項1に記載の圧力および温度計測用静電容量型センサ。The ceramic member has a through hole opened at a portion facing the electrode portion of the second silicon member, and the second electrode thin film has an inner surface of the through hole and the first silicon member. 2. The pressure and temperature according to claim 1, wherein the first silicon member is formed as a common electrode having three capacitances. Capacitive sensor for measurement. 前記第2のシリコン部材には前記ギャップに通じるスルーホールが開けられていることを特徴とする請求項1または2に記載の圧力および温度計測用静電容量型センサ。3. The capacitive sensor for pressure and temperature measurement according to claim 1, wherein the second silicon member is provided with a through hole leading to the gap. 請求項1ないし3に記載の圧力および温度計測用静電容量型センサの製造方法であって、前記第1のシリコン部材の両面に前記2枚のセラミック部材を低融点ガラス膜を介して陽極接合するとともに、前記陽極接合は前記第1のシリコン部材と前記2枚のセラミック部材が3層に積層された状態で行われ、かつ全体が均一な温度に加熱されて行われるようにして、前記第1のシリコン部材と前記2枚のセラミック部材とを3層構造に形成した後、前記セラミック部材の所定面に前記第2のシリコン部材を低融点ガラス を介して陽極接合することを特徴とする圧力および温度計測用静電容量型センサの製造方法。4. A method of manufacturing a capacitive sensor for pressure and temperature measurement according to claim 1, wherein the two ceramic members are anodic bonded to both surfaces of the first silicon member via a low melting point glass film. In addition, the anodic bonding is performed in a state where the first silicon member and the two ceramic members are laminated in three layers, and the whole is heated to a uniform temperature, so that the first bonding is performed. After forming one silicon member and the two ceramic members into a three-layer structure, the second silicon member is anodically bonded to a predetermined surface of the ceramic member through a low-melting glass. And a method for manufacturing a temperature sensor. 前記低融点ガラスは予め前記絶縁性セラミック部材上に形成された膜であることを特徴とする請求項4に記載の圧力および温度計測用静電容量型センサの製造方法。5. The method of manufacturing a capacitive sensor for pressure and temperature measurement according to claim 4, wherein the low-melting glass is a film formed on the insulating ceramic member in advance. 前記陽極接合は、前記3層構造および第2のシリコン部材を挟むそれぞれに独立に温度制御される2つのヒータによりなされ、陽極接合温度を任意に変化させることを特徴とする請求項4または5に記載の圧力および温度計測用静電容量型センサの製造方法。6. The anodic bonding according to claim 4 or 5, wherein the anodic bonding is performed by two heaters that are independently temperature controlled with the three-layer structure and the second silicon member interposed therebetween, and the anodic bonding temperature is arbitrarily changed. The manufacturing method of the capacitive sensor for pressure and temperature measurement of description. 請求項2に記載の4層構造の圧力および温度計測用静電容量型センサに、第2のシリコン部材のスルーホールおよび第2のシリコン部材の配された方のセラミック部材のスルーホールの開口部および外部に向けて開けられた開口部を同一空間に有する第1の圧力室をなす第1のパッケージ、および他のセラミック部材のスルーホールの開口部および外部に向けて開けられた開口部を同一空間に有する第2の圧力室をなす第2のパッケージが付加されてなり、第1の圧力室には誘電率の温度係数の大きい流体を充填してあって、第1の圧力室と第2の圧力室の圧力差を計測し、また第3の静電容量の温度変化から温度計測ができることを特徴とする圧力および温度計測用静電容量型センサ装置。3. The through-hole of the second silicon member and the through-hole of the ceramic member on which the second silicon member is disposed in the pressure and temperature measuring capacitive sensor of the four-layer structure according to claim 2 The first package forming the first pressure chamber having the opening opened to the outside in the same space, and the opening of the through hole of the other ceramic member and the opening opened to the outside are the same A second package forming a second pressure chamber in the space is added, and the first pressure chamber is filled with a fluid having a large dielectric constant temperature coefficient, and the first pressure chamber and the second pressure chamber are filled. A capacitance type sensor device for pressure and temperature measurement, characterized in that the pressure difference between the pressure chambers of the first and second pressure chambers can be measured, and the temperature can be measured from the temperature change of the third capacitance.
JP27678197A 1997-10-09 1997-10-09 Capacitance type sensor for pressure and temperature measurement, sensor device and manufacturing method thereof Expired - Fee Related JP3724151B2 (en)

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