JPH0366609B2 - - Google Patents

Info

Publication number
JPH0366609B2
JPH0366609B2 JP14106982A JP14106982A JPH0366609B2 JP H0366609 B2 JPH0366609 B2 JP H0366609B2 JP 14106982 A JP14106982 A JP 14106982A JP 14106982 A JP14106982 A JP 14106982A JP H0366609 B2 JPH0366609 B2 JP H0366609B2
Authority
JP
Japan
Prior art keywords
gauge chip
bonding layer
bonding
glass die
gauge
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
Application number
JP14106982A
Other languages
Japanese (ja)
Other versions
JPS5931431A (en
Inventor
Norio Ichikawa
Hitoshi Minorikawa
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.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP14106982A priority Critical patent/JPS5931431A/en
Publication of JPS5931431A publication Critical patent/JPS5931431A/en
Publication of JPH0366609B2 publication Critical patent/JPH0366609B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L19/00Details of, or accessories for, apparatus for measuring steady or quasi-steady pressure of a fluent medium insofar as such details or accessories are not special to particular types of pressure gauges
    • G01L19/14Housings
    • G01L19/147Details about the mounting of the sensor to support or covering means

Landscapes

  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Fluid Pressure (AREA)

Description

【発明の詳細な説明】 本発明は、半導体圧力センサに係り、特に高温
高湿の環境にて使用されるに好適な半導体圧力セ
ンサに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a semiconductor pressure sensor, and particularly to a semiconductor pressure sensor suitable for use in a high temperature and high humidity environment.

半導体圧力センサの一例として特開昭55−
62331号公報にあるように従来第1図に示された
断面構造を有するものが考案されている。
As an example of a semiconductor pressure sensor, JP-A-1988-
As disclosed in Japanese Patent No. 62331, a device having the cross-sectional structure shown in FIG. 1 has been devised.

第1図において、ダイアフラムとしてのゲージ
チツプ1はシリコン半導体から形成されており、
図において下面中央部は薄肉に、周縁部は厚肉に
形成されている。このゲージチツプ1は、パイレ
ツクガラスにより形成されたガラスダイ2上に固
着されている。ゲージチツプ1の厚肉部とガラス
ダイ2との固着は、高温の雰囲気中にて、第1図
に示された如く、ゲージチツプ1を正極、ガラス
ダイ2を負極とする直流高電圧を印加し、それら
の境界層に接合層を形成する方法、いわゆる陽極
接合法によつてなされていた。
In FIG. 1, a gauge chip 1 as a diaphragm is made of a silicon semiconductor,
In the figure, the center portion of the lower surface is thin and the peripheral portion is thick. This gauge chip 1 is fixed on a glass die 2 made of pirate glass. The thick part of the gauge chip 1 and the glass die 2 are fixed by applying a high DC voltage with the gauge chip 1 as the positive electrode and the glass die 2 as the negative electrode in a high-temperature atmosphere, as shown in FIG. This was accomplished by a method of forming a bonding layer in the boundary layer, the so-called anodic bonding method.

しかしながら、上述した陽極接合法によつて形
成された半導体圧力センサを、高温高湿の環境条
件にて使用すると、ゲージ零点出力が正方向にず
れてしまうという(いわゆるアツプシフト)欠点
があり、測定値の信頼性において極めて大きな問
題となつていた。
However, when a semiconductor pressure sensor formed by the above-mentioned anodic bonding method is used in a high temperature and high humidity environment, it has the disadvantage that the gauge zero output shifts in the positive direction (so-called upshift). There was a huge problem with the reliability of the system.

本発明の目的は、高温高湿の環境におけるアツ
プシフトを低減させて信頼性を向上させることが
できる半導体圧力センサを提供することにある。
An object of the present invention is to provide a semiconductor pressure sensor that can reduce upshift and improve reliability in a high-temperature, high-humidity environment.

本発明は、高温高湿下におけるアツプシフトの
原因を究明するため種々の実験を実施し、その原
因は主として陽極接合法によつて形成された接合
層の吸湿性に起因するものであるという結果に鑑
みなされたものであり、接合電流を制御すること
によつて形成される接合層の厚みを3〜6μmと
することにより、高温高湿下におけるアツプシフ
トを低減させようとするものである。
The present invention conducted various experiments to investigate the cause of upshift under high temperature and high humidity conditions, and the results showed that the cause was mainly due to the hygroscopicity of the bonding layer formed by the anodic bonding method. This was done in consideration of the above, and by controlling the bonding current to form a bonding layer with a thickness of 3 to 6 μm, the upshift under high temperature and high humidity is reduced.

以下、本発明によつて上記目的が達成される理
由について説明する。
Hereinafter, the reason why the above object is achieved by the present invention will be explained.

まず、本発明に適用される陽極接合法の原理に
ついて説明する。第1図に示された形状のゲージ
チツプ1とガラスダイ2とを重ね、それらを治具
で固定してチヤンバー3に収納する。このチヤン
バー3を電気炉内に設置して300〜350℃程度に加
熱し、ゲージチツプ1を正、ガラスダイ2を負と
して800〜1500V程度の直流高電圧を印加する。
この際に、ガラスダイ2のアルカリ成分である
NaOが分極され、ガラスダイ2の接合境界面か
ら次式(1)に示されたように酸素イオンが放出さ
れ、陽極側であるゲージチツプ1側へ移動され
る。
First, the principle of the anodic bonding method applied to the present invention will be explained. A gauge chip 1 having the shape shown in FIG. 1 and a glass die 2 are stacked together, fixed with a jig, and housed in a chamber 3. This chamber 3 is placed in an electric furnace and heated to about 300 to 350°C, and a high DC voltage of about 800 to 1500 V is applied, with the gauge chip 1 being positive and the glass die 2 being negative.
At this time, the alkaline component of glass die 2
NaO is polarized, and oxygen ions are released from the bonding interface of the glass die 2 as shown in the following equation (1) and moved toward the gauge chip 1, which is the anode side.

Na2O→2Na++O2- ……(1) また、ゲージチツプのシリコン(Si)もイオン
化されてSi4+となり、陰極側であるガラスダイ2
側へ移動される。これらのイオン拡散によつて、
接触境界部に次式(2)の反応によつてSiO2の接合
層が形成され、この層によつてゲージチツプ1と
ガラスダイ2が接合されると考えられる。
Na 2 O → 2Na + +O 2- ...(1) In addition, the silicon (Si) of the gauge chip is also ionized and becomes Si 4+ , and the glass die 2 on the cathode side
moved to the side. Due to these ion diffusion,
It is thought that a bonding layer of SiO 2 is formed at the contact boundary by the reaction of the following equation (2), and the gauge chip 1 and the glass die 2 are bonded by this layer.

2O2-+Si4+→SiO2 ……(2) この反応によりゲージチツプ1とガラスダイ2
間に接合電流IPが流れる。従つて、接合層の形成
には、この接合電流IPが影響しているものと考え
られる。
2O 2- +Si 4+ →SiO 2 ...(2) Due to this reaction, gauge chip 1 and glass die 2
Junction current I P flows between them. Therefore, it is considered that this junction current I P influences the formation of the junction layer.

一方、高温高湿の環境におけるアツプシフトの
原因については、ガラスダイの吸湿によるものと
接合層の吸湿によるものとが考えられる。つま
り、それらが吸湿したことによつて、ゲージチツ
プとガラスダイ又は接合層との熱膨張係数の変化
に差が生じ、これによつてアツプシフトが起きる
のである。しかも、接合層の吸湿によるアツプシ
フトの方が、はるかに大きいということが判明し
た。
On the other hand, the cause of upshift in a high temperature and high humidity environment is thought to be due to moisture absorption by the glass die and moisture absorption by the bonding layer. In other words, their absorption of moisture causes a difference in the coefficient of thermal expansion between the gauge chip and the glass die or bonding layer, resulting in an upshift. Moreover, it was found that the upshift due to moisture absorption in the bonding layer was much larger.

そこで、前述したように接合層の形成には、接
合電流IPが関与していることから、接合電流IP
パラメータとして、85℃−85%RHの高温高湿耐
久テストを行い、ゲージ零点出力の変化を実験に
より測定した。この耐久テストの結果が第2図a
〜cに示されている。
Therefore, as mentioned above, since the bonding current I P is involved in the formation of the bonding layer, we conducted a high temperature and high humidity durability test at 85°C - 85% RH using the bonding current I P as a parameter, and measured the gauge zero point. Changes in output were measured experimentally. The results of this durability test are shown in Figure 2a.
~c.

第2図a〜cは横軸に時間h、縦軸に零点出力
変化mVが示され、接合電流IPは図中曲線に付し
て示されている。これらの図から明らかなよう
に、零点出力変化は接合電流IPによつて大きく影
響を受けていることが判る。ところが、従来の陽
極接合は印加電圧を一定に制御する方式であつた
ことから、接合温度のゆらぎや、ガラスダイ寸法
のばらつき、ガラスダイ中のNaO含有量のロツ
ト間ばらつき等によつて、流される接合電流IP
一定したものでなかつた。従つて、形成される接
合層も一定したものとはなつていなかつたことが
判る。
In FIGS. 2a to 2c, time h is plotted on the horizontal axis, zero point output change mV is plotted on the vertical axis, and junction current I P is plotted along the curve in the figures. As is clear from these figures, it can be seen that the zero point output change is greatly influenced by the junction current IP . However, since conventional anodic bonding is a method that controls the applied voltage at a constant level, the bond may be washed away due to fluctuations in the bonding temperature, variations in the dimensions of the glass die, variations in the NaO content in the glass die between lots, etc. The current I P was not constant. Therefore, it can be seen that the bonding layer formed was also not constant.

次に、零点出力がアツプシフトするのは、前述
したように吸湿による影響であり、これによつて
ダイアフラム部が、第1図において下方に凹とな
ることであるということを具体的に確認した。こ
の結果の一例が第3図a〜dに示されている。
Next, it was specifically confirmed that the upshift in the zero point output is due to the effect of moisture absorption, as described above, and that this causes the diaphragm to become concave downward in FIG. An example of this result is shown in Figures 3a-d.

第3図a〜dは、半導体圧力センサの製造工程
ごとに、表面粗さ計、レーザ干渉計により、ゲー
ジチツプ表面の凹凸を測定したものである。同図
aはダイアフラム形成前のゲージチツプを示して
おり、図示したようにΔh=0.15〜0.20μmの凸に
なつていた。このゲージチツプを用いて、下面中
央部にエツチングして薄肉部を形成すると、同図
bに示したように、更に上方に凸となりΔh=
0.32μ〜0.6μmとなつた。これをガラスダイ上に
陽極接合すると、同図cに示したように逆方向に
変形され、Δh≒−0.1μmの凹となつた。このよ
うに形成された半導体圧力センサを用いて、湿度
試験(100時間)を行つたところ、同図dに示し
たように、同試験完了後前記凹量が更に増大され
てΔh=−0.15〜−0.2μmとなつた。即ち、吸湿し
たことによつて、ダイアフラム部が凹状に変形さ
れ、これによつてアツプシフトされることが確認
された。
Figures 3a to 3d show measurements of the unevenness of the gauge chip surface using a surface roughness meter and a laser interferometer during each manufacturing process of the semiconductor pressure sensor. Figure a shows the gauge chip before the diaphragm is formed, and as shown, it has a convex shape of Δh=0.15 to 0.20 μm. When this gauge chip is used to form a thin part by etching at the center of the lower surface, it becomes more convex upward, as shown in Figure b, and Δh=
It became 0.32μ to 0.6μm. When this was anodically bonded onto a glass die, it was deformed in the opposite direction as shown in FIG. When a humidity test (100 hours) was conducted using the semiconductor pressure sensor formed in this way, as shown in Figure d, after the test was completed, the concavity was further increased and Δh = -0.15 ~ -0.2 μm. That is, it was confirmed that the diaphragm part was deformed into a concave shape due to moisture absorption, and was thereby upshifted.

つまり、ゲージチツプ1の熱膨張係数αSが、ガ
ラスダイ2の熱膨張係数αGよりも大であることか
ら、第4図aの接合前の状態に対して、接合時の
加熱によつて熱膨張に差が生じ、接合後は同図b
に示したように、ダイアフラム部に図示矢印のモ
ーメントが発生し、下方に凹となるである。更
に、このように形成されたものを高温高湿の環境
に設置すると、接合層4が吸湿して膨張され、室
温に取り出すと、第4図cに示したように、接合
層4に圧縮力が、ゲージチツプ1に引張力が加わ
り、これによつてダイアフラム部は一層下に凹と
なるのである。なお、接合部を斜め研磨後XMA
(X線マイクロアナライザー)によるSiO2の分析
をしたところ、接合層4はゲージチツプ側に形成
されたSiO2薄層であることが判つた。
In other words, since the thermal expansion coefficient α S of the gauge chip 1 is larger than the thermal expansion coefficient α G of the glass die 2, the thermal expansion coefficient α S of the gauge chip 1 is larger than the thermal expansion coefficient α G of the glass die 2. There is a difference in the
As shown in , a moment indicated by the arrow in the figure is generated in the diaphragm, causing it to concave downward. Furthermore, when the product formed in this way is placed in a high temperature and high humidity environment, the bonding layer 4 absorbs moisture and expands, and when it is taken out to room temperature, a compressive force is applied to the bonding layer 4, as shown in FIG. 4c. However, a tensile force is applied to the gauge chip 1, which causes the diaphragm portion to concave further downward. In addition, after diagonally polishing the joint part, XMA
When SiO 2 was analyzed using an X-ray microanalyzer, it was found that the bonding layer 4 was a thin SiO 2 layer formed on the gauge chip side.

また、この接合層の厚みと陽極接合電流IP
は、第5図に示された相関を有しており、第2図
a〜cに示された零点出力変化と陽極接合電流と
特性とから、最適な接合層の厚さが存在すること
が判る。即ち、接合層が6μm以上になると吸湿
量が大きくなつて、零点のアツプシフトも大きく
なる。また、IPが10μAの場合には2.5μm程度の接
合層が得られるが、部分的に接合されない空隙が
残り、その水分が浸入するため見掛け上の吸水量
が増大し、これによつてアツプシフト量が大きく
なつてしまうのである。しかも、接合強度的にも
十分なものとは言えない。
In addition, the thickness of this bonding layer and the anodic junction current I P have the correlation shown in Figure 5, and the zero point output change, anodic junction current, and characteristics shown in Figures 2 a to c. It can be seen from the above that there is an optimal bonding layer thickness. That is, when the bonding layer has a thickness of 6 μm or more, the amount of moisture absorbed increases, and the upshift of the zero point also increases. In addition, when I P is 10 μA, a bonding layer of approximately 2.5 μm is obtained, but some voids remain that are not bonded, and moisture infiltrates, increasing the apparent amount of water absorption. The amount becomes large. Moreover, it cannot be said that the bonding strength is sufficient.

これらのことから、陽極接合電流IPを15〜
25μAに制御することによつて、接合層の厚みを
3〜6μmとなるように形成すれば、アツプシフ
トを大幅に低減することができるのである。
From these facts, the anodic junction current I P is set to 15~
By controlling the current to 25 μA and forming the bonding layer to have a thickness of 3 to 6 μm, upshift can be significantly reduced.

以上説明したように、本発明によれば、陽極接
合法によつて形成したものであつても、高温高湿
の環境におけるアツプシフトを大幅に低減させ、
高い信頼度を有したものとすることができる。
As explained above, according to the present invention, even when formed by an anodic bonding method, upshift in a high temperature and high humidity environment can be significantly reduced.
It can have high reliability.

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

第1図は本発明に係る陽極接合法を説明するた
めの図、第2図a〜cは本発明を説明するための
高温高湿耐久テストにより得られた零点出力変化
と接合電流の関係を示す線図、第3図a〜dは本
発明を説明するためのゲージチツプ製造工程にお
ける表面凹凸測定結果を示す図、第4図a〜cは
ゲージチツプの変形過程の説明図、第5図は実験
により得られた接合電流と接合層厚みとの関係を
示す線図である。 1……ゲージチツプ、2……ガラスダイ、4…
…接合層。
Figure 1 is a diagram for explaining the anodic bonding method according to the present invention, and Figures 2 a to c show the relationship between zero point output change and junction current obtained by a high temperature and high humidity durability test to explain the present invention. Figures 3a to 3d are diagrams showing the results of surface unevenness measurement in the gauge chip manufacturing process to explain the present invention, Figures 4a to c are explanatory diagrams of the deformation process of the gauge chip, and Figure 5 is an experimental diagram. FIG. 3 is a diagram showing the relationship between the bonding current and the bonding layer thickness obtained by the method. 1...Gauge chip, 2...Glass die, 4...
...bonding layer.

Claims (1)

【特許請求の範囲】[Claims] 1 周縁に厚肉部を有するダイアフラムから成る
ゲージチツプをガラスダイから成る支持台上に載
置し、前記ゲージチツプの厚肉部を陽極接合法に
よつて前記支持台に固着させて成る半導体圧力セ
ンサにおいて、陽極接合法によつて前記厚肉部と
支持台間に形成される接合層の厚みを、接合電流
制御によつて3乃至6μmとしたことを特徴とす
る半導体圧力センサ。
1. A semiconductor pressure sensor in which a gauge chip consisting of a diaphragm having a thick portion on the periphery is placed on a support made of a glass die, and the thick portion of the gauge chip is fixed to the support by an anodic bonding method, A semiconductor pressure sensor characterized in that the thickness of the bonding layer formed between the thick portion and the support base by an anodic bonding method is set to 3 to 6 μm by controlling the bonding current.
JP14106982A 1982-08-16 1982-08-16 semiconductor pressure sensor Granted JPS5931431A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14106982A JPS5931431A (en) 1982-08-16 1982-08-16 semiconductor pressure sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14106982A JPS5931431A (en) 1982-08-16 1982-08-16 semiconductor pressure sensor

Publications (2)

Publication Number Publication Date
JPS5931431A JPS5931431A (en) 1984-02-20
JPH0366609B2 true JPH0366609B2 (en) 1991-10-18

Family

ID=15283508

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14106982A Granted JPS5931431A (en) 1982-08-16 1982-08-16 semiconductor pressure sensor

Country Status (1)

Country Link
JP (1) JPS5931431A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20200360875A1 (en) 2019-05-14 2020-11-19 Sodastream Industries Ltd. Carbonation machine and a gas canister for a carbonation machine

Also Published As

Publication number Publication date
JPS5931431A (en) 1984-02-20

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