JPH11160057A - Piezoelectric crystal oscillation type film thickness gauge - Google Patents

Piezoelectric crystal oscillation type film thickness gauge

Info

Publication number
JPH11160057A
JPH11160057A JP34405597A JP34405597A JPH11160057A JP H11160057 A JPH11160057 A JP H11160057A JP 34405597 A JP34405597 A JP 34405597A JP 34405597 A JP34405597 A JP 34405597A JP H11160057 A JPH11160057 A JP H11160057A
Authority
JP
Japan
Prior art keywords
piezoelectric crystal
film
film thickness
oscillation type
crystal
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.)
Granted
Application number
JP34405597A
Other languages
Japanese (ja)
Other versions
JP3483749B2 (en
Inventor
Atsushi Ito
敦 伊藤
Toru Okuno
亨 奥野
Takaaki Miyajima
孝明 宮嶋
Toshiharu Kurauchi
倉内  利春
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.)
Ulvac Inc
Original Assignee
Ulvac Inc
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 Ulvac Inc filed Critical Ulvac Inc
Priority to JP34405597A priority Critical patent/JP3483749B2/en
Publication of JPH11160057A publication Critical patent/JPH11160057A/en
Application granted granted Critical
Publication of JP3483749B2 publication Critical patent/JP3483749B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To provide a piezoelectric crystal oscillation type film thickness gauge capable of reducing the exchange frequency of a piezoelectric crystal and prolonging the service life than before. SOLUTION: The natural frequency of the piezoelectric crystal 3 is made lower than 5 MHz, influence by the stress of a film deposited on a surface 3a is reduced and the fundamental vibration of the piezoelectric crystal is maintained. Also, electrode films 10a and 10b formed on the front and back surfaces 3a and 3b of the piezoelectric crystal 3 are respectively formed in an island shape, the formation areas of the electrode films 10a and 10b are prevented from being overlapped on the front surface 3a and the back surface 3b at the peripheral edge part of the piezoelectric crystal 3, parasitic vibration appearing at the peripheral edge part of the piezoelectric crystal 3 is suppressed and the fundamental vibration of the piezoelectric crystal 3 is maintained. Thus, the service life of the piezoelectric crystal 3 is prolonged substantially longer than before.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、真空チャンバ内に
設置された圧電結晶上への膜の堆積を測定することによ
り、成膜対象物(基板)上に堆積される膜厚を測定する
圧電結晶発振式膜厚計に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a piezoelectric device for measuring the thickness of a film deposited on a film-forming object (substrate) by measuring the film deposition on a piezoelectric crystal installed in a vacuum chamber. It relates to a crystal oscillation type film thickness meter.

【0002】[0002]

【従来の技術】従来、真空蒸着またはスパッタリングに
おいて、成膜される膜の膜厚および成膜速度を測定する
ために、水晶振動子法という技術が用いられている。こ
の方法の原理は、圧電結晶である水晶振動子の固有振動
が、その質量の変化によって変化することを利用したも
である。すなわち、水晶振動子に薄膜が蒸着されると、
水晶振動子の質量に比べ、その薄膜の質量が十分に小さ
ければ、単に水晶振動子の質量あるいは厚さが増加した
のと同じ効果が生じ、質量変化に比例した固有振動数の
変化を生ずることを利用したものである。このときの水
晶振動子の固有振動数の変化を測定することにより膜厚
および成膜速度を測定することができる。
2. Description of the Related Art Conventionally, in vacuum deposition or sputtering, a technique called a quartz oscillator method has been used to measure the film thickness and film formation rate of a film to be formed. The principle of this method is based on the fact that the natural vibration of a crystal resonator, which is a piezoelectric crystal, changes due to a change in its mass. In other words, when a thin film is deposited on the crystal unit,
If the mass of the thin film is sufficiently small compared to the mass of the crystal unit, the same effect as simply increasing the mass or thickness of the crystal unit will occur, and the natural frequency will change in proportion to the mass change. It is a thing using. By measuring the change in the natural frequency of the crystal unit at this time, the film thickness and the film formation rate can be measured.

【0003】この種の従来の圧電結晶発振式膜厚計で
は、使いやすさの点などから固有振動数が5MHz(メ
ガヘルツ)や6MHzの水晶振動子を検出素子としたも
のが用いられており、また、水晶振動子法の校正には、
マイクロバランスという技術が用いられている(日本学
術振興会薄膜第131委員会編 薄膜ハンドブック I
編2章p.146(1983))。
In this type of conventional piezoelectric crystal oscillation type film thickness meter, a device using a quartz oscillator having a natural frequency of 5 MHz (megahertz) or 6 MHz as a detecting element is used from the viewpoint of ease of use. Also, for the calibration of the crystal oscillator method,
Microbalance technology is used (JSPS Thin Film 131st Committee, Thin Film Handbook I)
Chapter 2, p. 146 (1983)).

【0004】[0004]

【発明が解決しようとする課題】しかしながら、この技
術は取り扱いが容易で精度がよい反面、膜を厚く堆積さ
せる場合や、堆積させる物質によっては薄い膜でも圧電
結晶が寿命となり、頻繁に圧電結晶を交換する必要があ
るという問題がある。また、光学膜のように膜応力が大
きいものでは、膜が薄くても基本振動での振動ができな
くなり、他の振動モード(スプリアス(spurious)での振
動モード)に移って、測定ができなくなる。つまり、振
動子の使用限界に達して寿命となる。これは、「有限広
さの振動子では、振幅は中央部付近で最大で、縁に向か
って減少し(中略)、厚みすべり振動の高次振動や輪郭
振動の高次振動の姿態、あるいはそれらの結合した姿態
に移行する可能性を持っている」(日本学術振興会薄膜
第131委員会編 薄膜ハンドブック I編2章p.1
39(1983))もので、このような現象は固有振動
数が高い振動子、すなわち厚さが小さい振動子ほど顕著
となる。
However, this technique is easy to handle and high in accuracy, but the piezoelectric crystal has a long life when a thick film is deposited or even a thin film depending on the substance to be deposited. There is a problem that needs to be replaced. In addition, when the film stress is large, such as an optical film, even if the film is thin, it is not possible to vibrate in the basic vibration, and the measurement shifts to another vibration mode (spurious vibration mode), and measurement becomes impossible. . In other words, the use limit of the vibrator is reached and the life is reached. This is because, for a transducer of finite size, the amplitude is maximum near the center and decreases toward the edge (omitted), and the appearance of higher-order vibration of thickness shear vibration and higher-order vibration of contour vibration, or It has the potential to shift to a combined form of the thin film "(JSPS Thin Film 131st Committee, Thin Film Handbook, I, Chapter 2, p.1)
39 (1983)), such a phenomenon becomes more remarkable for a vibrator having a higher natural frequency, that is, a vibrator having a smaller thickness.

【0005】本発明は上述の問題に鑑みてなされ、圧電
結晶の交換頻度を減らして寿命を長くすることができる
圧電結晶発振式膜厚計を提供することを課題とする。
The present invention has been made in view of the above problems, and has as its object to provide a piezoelectric crystal oscillation type film thickness meter that can reduce the frequency of replacement of piezoelectric crystals and extend the life.

【0006】[0006]

【課題を解決するための手段】以上の課題は、真空チャ
ンバ内に設置された圧電結晶上へ成膜材料を堆積させ、
前記成膜材料の堆積による前記圧電結晶の固有振動数の
変化に基づいて、被処理基板上に堆積される前記成膜材
料の膜厚を測定するようにした圧電結晶発振式膜厚計に
おいて、前記圧電結晶の固有振動数を5メガヘルツより
も低くすることにより、成膜中における前記圧電結晶の
基本振動を維持させるようにしたことを特徴とする圧電
結晶発振式膜厚計、によって解決される。
The above object is achieved by depositing a film forming material on a piezoelectric crystal installed in a vacuum chamber,
Based on a change in the natural frequency of the piezoelectric crystal due to the deposition of the film forming material, in a piezoelectric crystal oscillation type film thickness meter that measures the film thickness of the film forming material deposited on the substrate to be processed, The piezoelectric crystal oscillation type film thickness meter is characterized in that the fundamental frequency of the piezoelectric crystal is maintained during film formation by lowering the natural frequency of the piezoelectric crystal to less than 5 MHz. .

【0007】従来の圧電結晶を検出素子とした膜厚計
は、固有振動数が6MHzや5MHzの水晶振動子が用
いられていた。一般に、水晶の固有振動数fとその厚さ
dとの間には、f=N/dとの関係が成り立ち、Nは水
晶の周波数定数でATカットの水晶では1670kHz
・mmである。そこで、5MHzで0.33mm、6M
Hzで0.28mmである。このように、圧電結晶の固
有振動数と厚さとは反比例する関係にあり、応答周波数
を高くするために圧電結晶の固有振動数を高くすると、
逆に薄くなって割れ易くなるということもあって、従来
より5MHzや6MHzの圧電結晶がよく用いられてい
た。そこで、本発明は、圧電結晶の固有振動数を従来用
いられる6MHz(メガヘルツ)や5MHzより下げ、
膜厚に対する圧電結晶の感度を落とすことにより膜の応
力または膜による振動の吸収に対して強くし、基本振動
を維持させることによって、圧電結晶の寿命を伸ばすよ
うにしている。
In a conventional thickness gauge using a piezoelectric crystal as a detecting element, a quartz oscillator having a natural frequency of 6 MHz or 5 MHz has been used. Generally, a relationship of f = N / d is established between the natural frequency f of the crystal and its thickness d, where N is a frequency constant of the crystal and 1670 kHz for an AT-cut crystal.
Mm. So, at 5MHz, 0.33mm, 6M
It is 0.28 mm in Hz. As described above, the natural frequency and the thickness of the piezoelectric crystal are inversely proportional, and when the natural frequency of the piezoelectric crystal is increased in order to increase the response frequency,
Conversely, a piezoelectric crystal of 5 MHz or 6 MHz has been more often used than before, because it is thinner and easily cracked. Therefore, the present invention reduces the natural frequency of the piezoelectric crystal from 6 MHz (megahertz) or 5 MHz conventionally used,
By reducing the sensitivity of the piezoelectric crystal to the film thickness, the film is made more resistant to the stress of the film or the absorption of vibration by the film, and the fundamental vibration is maintained to extend the life of the piezoelectric crystal.

【0008】[0008]

【発明の実施の形態】以下、本発明の実施の形態につい
て図面を参照して説明する。
Embodiments of the present invention will be described below with reference to the drawings.

【0009】図1から図3は、本発明の実施の形態によ
る圧電結晶発振式膜厚計に用いられる圧電結晶を示して
いる。圧電結晶3は、温度特性の良好な(熱膨張係数の
最も小さい)ATカットとよばれる方向に切断された単
結晶水晶振動子で成り、その固有振動数は3.25MH
z(厚さ0.51mm)である。なお、図2に示すよう
に、水晶振動子3の蒸着面となる表面3aは平らである
が、裏面3bはわずかに凸なる曲面となっている。これ
は、厚みすべり振動の高次振動や輪郭振動の高次振動の
姿態、あるいはそれらの結合した姿態に移行するといっ
た不安定性を抑制するための、従来から行われている技
術である。
FIGS. 1 to 3 show a piezoelectric crystal used in a piezoelectric crystal oscillation type film thickness meter according to an embodiment of the present invention. The piezoelectric crystal 3 is made of a single crystal quartz resonator cut in a direction called AT cut having a good temperature characteristic (smallest thermal expansion coefficient), and has a natural frequency of 3.25 MHz.
z (thickness 0.51 mm). In addition, as shown in FIG. 2, the front surface 3a serving as the vapor deposition surface of the crystal unit 3 is flat, while the back surface 3b is a slightly convex curved surface. This is a conventional technique for suppressing instability such as shifting to a form of higher-order vibration of thickness-shear vibration or higher-order vibration of contour vibration, or a combination thereof.

【0010】水晶振動子3の表面3aと裏面3bには金
(Au)または銀(Ag)を蒸着させた電極膜10aお
よび10bが形成されており、本実施の形態では、これ
ら電極膜10a、10bの形状を図においてハッチング
で示すようにそれぞれ島状に形成すると共に、水晶振動
子3の周縁部における表面3aと裏面3bでの電極膜1
0a、10bの形成領域が重ならないようにしている。
これにより、水晶振動子3の周縁部における寄生振動を
抑制し、水晶振動子3の寿命の向上を図っている。
Electrode films 10a and 10b on which gold (Au) or silver (Ag) is deposited are formed on the front surface 3a and the back surface 3b of the crystal unit 3, and in the present embodiment, these electrode films 10a, 10b is formed in an island shape as shown by hatching in the figure, and the electrode film 1 on the front surface 3a and the back surface 3b in the peripheral portion of the crystal unit 3 is formed.
The formation areas of 0a and 10b do not overlap.
Thereby, the parasitic vibration at the peripheral portion of the crystal unit 3 is suppressed, and the life of the crystal unit 3 is improved.

【0011】図4は、圧電結晶発振式膜厚計の構成を模
式的に示したもので、1は真空チャンバ、2は電子ビー
ム蒸発源、4は水晶振動子3を備えたセンサ、6は加熱
用電源、7は膜厚監視装置7である。センサ4は水晶振
動子3の固有振動数を膜厚監視装置7に供給する。な
お、被処理基板は図示せずともセンサ4の奥または手前
に位置し、蒸発源2から見てセンサ4と等距離に配置さ
れている。膜厚監視装置7において水晶振動子3の固有
振動数の変化が測定され、また、これに基づいて加熱用
電源6の出力を調整して成膜速度を制御するようにして
いる。
FIG. 4 schematically shows the structure of a piezoelectric crystal oscillation type film thickness meter, wherein 1 is a vacuum chamber, 2 is an electron beam evaporation source, 4 is a sensor having a quartz oscillator 3, and 6 is a sensor. A heating power supply 7 is a film thickness monitoring device 7. The sensor 4 supplies the natural frequency of the crystal resonator 3 to the film thickness monitoring device 7. The substrate to be processed is located at the back or front of the sensor 4 even though not shown, and is disposed at the same distance from the sensor 4 as viewed from the evaporation source 2. A change in the natural frequency of the quartz oscillator 3 is measured by the film thickness monitoring device 7, and the output of the heating power supply 6 is adjusted based on the change to control the film forming speed.

【0012】図5Bは、本実施の形態における3.25
MHzの水晶振動子3にMgO(酸化マグネシウム)を
成膜速度40Å/sで成膜したときの寿命および、膜厚
の増加に伴うモニタ上での成膜速度の変動を示してい
る。また、比較のため、従来用いられていた5MHzの
水晶振動子の場合について図5Aに示す。ここで、モニ
タ上での成膜速度の変動とは、平均の成膜速度に対して
の変動をいい、40Å/sで成膜する今回の実験では、
100%の変動はつまり、0〜80Å/sの間で変化し
ていることを意味する(実際の成膜速度の変化でなくモ
ニタの表示上であって、水晶振動子の固有振動数の変化
に基づいて算出される成膜速度の変動を意味する)。
FIG. 5B shows 3.25 according to the present embodiment.
The graph shows the life when MgO (magnesium oxide) is deposited on the quartz crystal resonator 3 at a deposition rate of 40 ° / s and the fluctuation of the deposition rate on a monitor with an increase in the thickness. For comparison, FIG. 5A shows a case of a conventionally used 5 MHz quartz oscillator. Here, the fluctuation of the film forming speed on the monitor means a fluctuation with respect to the average film forming speed, and in this experiment of forming a film at 40 ° / s,
A change of 100% means that the change is in the range of 0 to 80 ° / s (not a change in the actual deposition rate but on the monitor display, and a change in the natural frequency of the crystal unit). Means the fluctuation of the film forming speed calculated based on the above.)

【0013】図5Aに示す従来の5MHzの水晶振動子
にあっては、膜厚5μm付近から成膜速度の変動が起こ
り始めている。これは、膜の応力が原因で水晶振動子の
基本振動が壊され始めていることを示している。また、
成膜速度の変動も大きく、膜厚20μmに達する前に水
晶振動子が機能しなくなっている。すなわち、振動子が
寿命に達している。
In the conventional 5 MHz quartz oscillator shown in FIG. 5A, the film forming speed starts to change at a film thickness of about 5 μm. This indicates that the fundamental vibration of the crystal resonator has begun to be destroyed due to the stress of the film. Also,
The film forming speed fluctuates greatly, and the quartz oscillator stops functioning before the film thickness reaches 20 μm. That is, the vibrator has reached the end of its life.

【0014】これに対して、本実施の形態による3.2
5MHzの水晶振動子3では、膜厚20μmに達するま
では成膜速度の変動はほとんど見られず安定した基本振
動を維持していることが明瞭に示され、また、膜厚が2
0μmを越えると成膜速度の変動が現れ始めるが、従来
の5MHzの水晶振動子よりもその変動の大きさは小さ
い。これは、水晶振動子3の固有振動数を低くしたこと
による膜応力に対する抵抗力が増大したことにほかなら
ない。さらに、膜厚が40μmに達しても基本振動が維
持されていることがわかる。以上から、3.25MHz
の水晶振動子では、従来の5MHzの水晶振動子に比べ
て寿命が約3倍も延び、成膜速度の変動も小さくなっ
た。
On the other hand, 3.2 according to the present embodiment.
In the case of the 5 MHz crystal resonator 3, the film formation rate hardly changed until the film thickness reached 20 μm, and it was clearly shown that stable fundamental vibration was maintained.
When the thickness exceeds 0 μm, a change in the film forming speed starts to appear, but the change is smaller than that in the conventional 5 MHz quartz oscillator. This is nothing but an increase in the resistance to film stress due to the lowering of the natural frequency of the crystal resonator 3. Further, it can be seen that the fundamental vibration is maintained even when the film thickness reaches 40 μm. From the above, 3.25 MHz
In the crystal resonator of No. 5, the life was extended by about three times as compared with the conventional 5 MHz crystal resonator, and the fluctuation of the film forming speed was reduced.

【0015】以上のように、本実施の形態によれば、水
晶振動子の固有振動数を従来よりも低くして水晶振動子
の厚さを大きくし、水晶3の基本振動を維持させるよう
にしたので、これにより水晶3の寿命を大きくすること
ができる。また、振動子には基本振動をつかさどる主共
振以外に必ず副共振があり(周縁部の寄生振動が原
因)、この副共振の振動レベルが大きいと主共振を維持
できずに寿命となるが、本実施の形態では、電極膜10
aおよび10bの形状を上述したように島状にすると共
に、水晶振動子3の周縁部においてその表面3aと裏面
3bとで電極膜10a、10bの形成領域が重ならない
ようにすることにより、副共振のレベルを下げている。
これにより、水晶振動子3の基本振動がより安定に維持
される。
As described above, according to the present embodiment, the natural frequency of the crystal unit is made lower than before, the thickness of the crystal unit is increased, and the fundamental vibration of the crystal 3 is maintained. As a result, the life of the crystal 3 can be extended. In addition, the vibrator always has a sub-resonance other than the main resonance controlling the fundamental vibration (due to the parasitic vibration of the peripheral portion). If the vibration level of the sub-resonance is large, the main resonance cannot be maintained and the life is extended. In the present embodiment, the electrode film 10
The shapes of the electrode films 10a and 10b are not overlapped between the front surface 3a and the back surface 3b of the peripheral portion of the crystal unit 3 by making the shapes of the a and 10b islands as described above. The level of resonance has been lowered.
Thereby, the fundamental vibration of the crystal resonator 3 is more stably maintained.

【0016】また、固有振動数を低下に伴って、水晶振
動子3の分解能が低下するが、現在では膜厚モニタ(す
なわち図4における膜厚監視装置7)自体の周波数分解
能が向上しているので大きな問題にはならない。例えば
特願平6−217464に記載の回路例によれば、従来
の膜厚モニタよりも分解能は100倍上り数Å/sの低
い成膜速度にも十分対応可能である。したがって、本実
施の形態においても水晶振動子3の固有振動数の変化に
基づいて、成膜速度の制御が可能である。
Although the resolution of the quartz oscillator 3 is reduced as the natural frequency is reduced, the frequency resolution of the film thickness monitor itself (that is, the film thickness monitoring device 7 in FIG. 4) is improved at present. So it doesn't matter. For example, according to the circuit example described in Japanese Patent Application No. 6-217664, the resolution is 100 times higher than that of the conventional film thickness monitor, and it can sufficiently cope with a film formation rate of several Å / s. Therefore, also in the present embodiment, it is possible to control the film forming speed based on the change in the natural frequency of the crystal resonator 3.

【0017】以上、本発明の実施の形態について説明し
たが、勿論、本発明はこれに限定されることなく、本発
明の技術的思想に基づいて種々の変形が可能である。
Although the embodiments of the present invention have been described above, the present invention is, of course, not limited thereto, and various modifications can be made based on the technical concept of the present invention.

【0018】例えば以上の実施の形態では、水晶振動子
3の固有振動数を3.25MHzとしたが、勿論、これ
だけに限られず3MHzや2MHz、さらに1MHz以
下の圧電結晶についても本発明は適用可能である。すな
わち、固有振動数を低くすればするほど、水晶の寿命を
長くすることができる。また、圧電結晶として水晶を適
用したが、これに限らず、ロッシェル塩、あるいはチタ
ン酸バリウムやジルコン酸鉛等の圧電セラミックも可能
である。なお、成膜材料としてMgOを用いたが、勿
論、これだけに限定されることはない。
For example, in the above embodiment, the natural frequency of the quartz oscillator 3 is set to 3.25 MHz. However, the present invention is not limited to this, and the present invention is applicable to a piezoelectric crystal of 3 MHz, 2 MHz, and 1 MHz or less. It is. That is, the lower the natural frequency, the longer the life of the crystal. In addition, although quartz is used as the piezoelectric crystal, the present invention is not limited to this, and a Rochelle salt or a piezoelectric ceramic such as barium titanate or lead zirconate can be used. In addition, although MgO was used as a film forming material, of course, it is not limited to this.

【0019】また、以上の実施の形態では、水晶振動子
3の周縁部においてその表面3aと裏面3bとの間で電
極膜10a、10bの形成領域が重ならないように形成
したが、両電極膜10a、10bの形成パターンは適宜
変更可能であるのは勿論のこと、両電極膜10a、10
bの重なりが少ない場合でも上述の実施の形態と同様な
効果を得ることができる。
In the above embodiment, the electrode films 10a and 10b are formed so that the formation regions of the electrode films 10a and 10b do not overlap between the front surface 3a and the back surface 3b in the peripheral portion of the crystal resonator 3. Needless to say, the formation patterns of the electrode films 10a and 10b can be appropriately changed.
Even when the overlap of b is small, the same effect as in the above embodiment can be obtained.

【0020】[0020]

【発明の効果】以上述べたように、本発明の圧電結晶発
振式膜厚計によれば、圧電結晶の基本振動を従来よりも
低くすることにより、圧電結晶の基本振動を維持させる
ようにしたので、圧電結晶の寿命を向上させることがで
きると共に、交換頻度を低減することができる。
As described above, according to the piezoelectric crystal oscillation type film thickness meter of the present invention, the fundamental vibration of the piezoelectric crystal is maintained by lowering the fundamental vibration of the piezoelectric crystal as compared with the prior art. Therefore, the life of the piezoelectric crystal can be improved, and the frequency of replacement can be reduced.

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

【図1】本発明の実施の形態による圧電結晶発振式膜厚
計に適用される水晶振動子の平面図である。
FIG. 1 is a plan view of a crystal resonator applied to a piezoelectric crystal oscillation type film thickness meter according to an embodiment of the present invention.

【図2】同側面図である。FIG. 2 is a side view of the same.

【図3】同裏面図である。FIG. 3 is a back view of the same.

【図4】本実施の形態による圧電結晶発振式膜厚計の構
成例を示す模式図である。
FIG. 4 is a schematic diagram showing a configuration example of a piezoelectric crystal oscillation type film thickness meter according to the present embodiment.

【図5】成膜速度の変動と寿命を示す実験結果であり、
Aは従来の5MHzの圧電結晶を示し、Bは3.25M
Hzの圧電結晶を示す。
FIG. 5 is an experimental result showing a change in a film forming rate and a lifetime.
A indicates a conventional 5 MHz piezoelectric crystal, and B indicates 3.25M.
3 shows a piezoelectric crystal at Hz.

【符号の説明】[Explanation of symbols]

1 真空チャンバ 2 蒸発源 3 水晶振動子 3a 表面 3b 裏面 4 センサ 6 加熱用電源 7 膜厚監視装置 10a (表面側)電極膜 10b (裏面側)電極膜 DESCRIPTION OF SYMBOLS 1 Vacuum chamber 2 Evaporation source 3 Quartz crystal oscillator 3a Front surface 3b Back surface 4 Sensor 6 Heating power supply 7 Film thickness monitor 10a (front surface) electrode film 10b (back surface) electrode film

フロントページの続き (72)発明者 倉内 利春 茨城県つくば市東光台5−9−7 日本真 空技術株式会社筑波超材料研究所内Continued on the front page (72) Inventor Toshiharu Kurauchi 5-9-7 Tokodai, Tsukuba City, Ibaraki Pref.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 真空チャンバ内に設置された圧電結晶上
へ成膜材料を堆積させ、前記成膜材料の堆積による前記
圧電結晶の固有振動数の変化に基づいて、被処理基板上
に堆積される前記成膜材料の膜厚を測定するようにした
圧電結晶発振式膜厚計において、 前記圧電結晶の固有振動数を5メガヘルツよりも低くす
ることにより、成膜中における前記圧電結晶の基本振動
を維持させるようにしたことを特徴とする圧電結晶発振
式膜厚計。
A film forming material is deposited on a piezoelectric crystal provided in a vacuum chamber, and is deposited on a substrate to be processed based on a change in a natural frequency of the piezoelectric crystal due to the deposition of the film forming material. In the piezoelectric crystal oscillation type film thickness meter configured to measure the film thickness of the film forming material, the fundamental frequency of the piezoelectric crystal during film formation is reduced by making the natural frequency of the piezoelectric crystal lower than 5 MHz. The piezoelectric crystal oscillation type film thickness meter characterized by maintaining.
【請求項2】 前記圧電結晶の表面と裏面に形成される
電極膜をそれぞれ島状に形成すると共に、前記圧電結晶
の周縁部における前記表面と裏面での前記電極膜の形成
領域の重なりを少なく又はなくした請求項1に記載の圧
電結晶発振式膜厚計。
2. An electrode film formed on the front surface and the back surface of the piezoelectric crystal is formed in an island shape, and the overlap of the electrode film formation region on the front surface and the back surface at the peripheral portion of the piezoelectric crystal is reduced. 2. The piezoelectric crystal oscillation type film thickness meter according to claim 1, wherein the thickness is eliminated.
【請求項3】 前記圧電結晶の固有振動数の変化に基づ
いて、前記成膜材料の成膜速度を制御可能とした請求項
1または請求項2に記載の圧電結晶発振式膜厚計。
3. The piezoelectric crystal oscillation type film thickness meter according to claim 1, wherein a film forming speed of the film forming material can be controlled based on a change in a natural frequency of the piezoelectric crystal.
【請求項4】 前記圧電結晶は、水晶振動子である請求
項1から請求項3のいずれかに記載の圧電結晶発振式膜
厚計。
4. The piezoelectric crystal oscillation type thickness meter according to claim 1, wherein the piezoelectric crystal is a quartz oscillator.
JP34405597A 1997-11-28 1997-11-28 Piezoelectric crystal oscillation type film thickness gauge Expired - Fee Related JP3483749B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP34405597A JP3483749B2 (en) 1997-11-28 1997-11-28 Piezoelectric crystal oscillation type film thickness gauge

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP34405597A JP3483749B2 (en) 1997-11-28 1997-11-28 Piezoelectric crystal oscillation type film thickness gauge

Publications (2)

Publication Number Publication Date
JPH11160057A true JPH11160057A (en) 1999-06-18
JP3483749B2 JP3483749B2 (en) 2004-01-06

Family

ID=18366313

Family Applications (1)

Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JP3483749B2 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8432151B2 (en) 2008-09-22 2013-04-30 Pioneer Corporation Film-thickness measuring device using PLL circuit
CN105091804A (en) * 2014-05-15 2015-11-25 佳能特机株式会社 Quartz oscillation type film thickness gauge
WO2016017108A1 (en) * 2014-07-31 2016-02-04 株式会社アルバック Diagnostic method for film thickness sensor, and film thickness monitor
WO2022157908A1 (en) * 2021-01-22 2022-07-28 株式会社日立ハイテク Ion milling device

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8432151B2 (en) 2008-09-22 2013-04-30 Pioneer Corporation Film-thickness measuring device using PLL circuit
CN105091804A (en) * 2014-05-15 2015-11-25 佳能特机株式会社 Quartz oscillation type film thickness gauge
JP2015219053A (en) * 2014-05-15 2015-12-07 キヤノントッキ株式会社 Quartz oscillation type film thickness meter
WO2016017108A1 (en) * 2014-07-31 2016-02-04 株式会社アルバック Diagnostic method for film thickness sensor, and film thickness monitor
CN106574833A (en) * 2014-07-31 2017-04-19 株式会社爱发科 Diagnostic method for film thickness sensor, and film thickness monitor
JPWO2016017108A1 (en) * 2014-07-31 2017-04-27 株式会社アルバック Film thickness sensor diagnostic method and film thickness monitor
CN106574833B (en) * 2014-07-31 2019-12-31 株式会社爱发科 Method for diagnosing film thickness sensor and film thickness monitor
WO2022157908A1 (en) * 2021-01-22 2022-07-28 株式会社日立ハイテク Ion milling device
TWI821868B (en) * 2021-01-22 2023-11-11 日商日立全球先端科技股份有限公司 Ion milling device

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