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JPH03197832A - Vacuum measuring instrument - Google Patents

Vacuum measuring instrument

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Publication number
JPH03197832A
JPH03197832A JP33728989A JP33728989A JPH03197832A JP H03197832 A JPH03197832 A JP H03197832A JP 33728989 A JP33728989 A JP 33728989A JP 33728989 A JP33728989 A JP 33728989A JP H03197832 A JPH03197832 A JP H03197832A
Authority
JP
Japan
Prior art keywords
vacuum
degree
detection
range
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.)
Pending
Application number
JP33728989A
Other languages
Japanese (ja)
Inventor
Yutaka Ashida
裕 芦田
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP33728989A priority Critical patent/JPH03197832A/en
Publication of JPH03197832A publication Critical patent/JPH03197832A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To measure the degree of vacuum in a range from atmospheric pressure to a high vacuum efficiently by providing and putting >=2 detection parts in partial charge of the measurement range of the degree of vacuum and outputting their vacuum degree data selectively. CONSTITUTION:A composite detecting means 11 is constituted by putting >=2 detection parts 11A, 11B... which detect the degree of vacuum in partial dis charge in the same storage container 11C. For the purpose, an opening part for fitting the means 11 is only provided to a vacuum processor 16 at only one place. Further, the detection part 11A is put in partial charge of a vacuum degree measurement range of 760 - 10<-4>Torr and the detection part 11B is put in partial charge of vacuum degree measurement range of 10<-4>-10<-11>Torr and the vacuum degree data D1 and D2 are outputted selectively through 1st and 2nd signal processing means 12 and 13 and a signal output means 14 to measure the degree of vacuum within the range from the atmospheric pressure to a high vacuum.

Description

【発明の詳細な説明】 〔目次〕 概要 産業上の利用分野 従来の技術(第2図) 発明が解決しようとする課題 課題を解決するための手段(第1図) 作用 実施例(第3図) 発明の効果 〔概 要〕 真空測定装置、特に大気圧から高真空に雰囲気が移行さ
れる真空処理装置の真空度を測定する装置に関し、 該処理装置の真空度の気密保持に影響を及ぼす検知器の
設置数を削減し、大気圧から高真空に至る範囲の真空度
を測定することを目的とし、真空度の範囲を分担して検
出する二以上の検出部が同一の格納容器に格納された複
合検出手段と、前記検出部からの信号を個別に処理する
二以上の信号処理手段と、前記信号処理手段からの二以
上の真空度データを選択出力する信号出力手段と、前記
信号処理手段及び信号出力手段の入出力を制御する制御
手段とを具備することを含み構成する。
[Detailed description of the invention] [Table of contents] Overview Industrial field of application Prior art (Figure 2) Means for solving the problems to be solved by the invention (Figure 1) Working examples (Figure 3) ) Effect of the invention [Summary] Regarding a vacuum measurement device, particularly a device for measuring the degree of vacuum of a vacuum processing device in which the atmosphere is transferred from atmospheric pressure to high vacuum, the present invention provides a method for detecting effects on the airtight maintenance of the degree of vacuum in the processing device. The purpose of this system is to reduce the number of instruments installed and measure the degree of vacuum in the range from atmospheric pressure to high vacuum, and two or more detection units that share and detect the range of vacuum degrees are housed in the same containment vessel. a combined detection means, two or more signal processing means for individually processing signals from the detection section, a signal output means for selectively outputting two or more degree of vacuum data from the signal processing means, and the signal processing means. and control means for controlling input/output of the signal output means.

[産業上の利用分野] 本発明は、真空測定装置に関するものであり、更に詳℃
く言えば、大気圧から高真空の雰囲気に移行される真空
処理装置の真空度を測定する装置に関するものである。
[Industrial Application Field] The present invention relates to a vacuum measuring device, and more specifically relates to a vacuum measuring device.
Specifically, the present invention relates to a device for measuring the degree of vacuum in a vacuum processing apparatus that is transferred from atmospheric pressure to a high vacuum atmosphere.

近年、半導体簗積回路の微細加工の要求に伴いその装置
の製造工程において、スパッタ装置やCV D (Ch
emical Vapor  Deposition 
)装置等の真空処理製造装置が使用されている。
In recent years, with the demand for microfabrication of semiconductor circuits, sputtering equipment and CVD (Ch
chemical vapor deposition
Vacuum processing manufacturing equipment such as ) equipment is used.

該5!l造装置によれば、真空処理容器内の真空度を把
握するため真空計が設けられている。しかし、大気圧か
ら高真空に至る広帯域の測定範囲を満足する真空計がな
く、測定範囲を異にする複数の真空計を真空処理容器に
設けている。
Part 5! According to the manufacturing equipment, a vacuum gauge is provided to ascertain the degree of vacuum inside the vacuum processing container. However, there is no vacuum gauge that satisfies a wide measurement range from atmospheric pressure to high vacuum, and a plurality of vacuum gauges with different measurement ranges are provided in a vacuum processing container.

そこで、該装置の真空度の気密保持に影響を及ぼす複数
の真空計を設けることなく、大気圧から高真空に至る範
囲の真空度を測定することができる測定装置が望まれて
いる。
Therefore, there is a need for a measuring device that can measure the degree of vacuum in a range from atmospheric pressure to high vacuum without providing a plurality of vacuum gauges that affect airtight maintenance of the degree of vacuum in the device.

〔従来の技術] 第3図は、従来例に係る真空処理装置の真空測定システ
ムの説明図である。
[Prior Art] FIG. 3 is an explanatory diagram of a vacuum measurement system for a vacuum processing apparatus according to a conventional example.

図において、スパッタ装置やCVD装置等の真空処理装
置3は、真空処理容器3aに加工機器3b、ガス導入口
3c、排気口3d、試料人出ドア3eが設けられ、咳排
気口3dには排気装置4が設けられて構成される。
In the figure, a vacuum processing device 3 such as a sputtering device or a CVD device includes a vacuum processing container 3a provided with processing equipment 3b, a gas inlet 3c, an exhaust port 3d, and a sample exit door 3e, and a cough exhaust port 3d for exhaust gas. A device 4 is provided and configured.

当該装置3は、大気中で被加工物5が試料人出ドア3e
を開閉して出し入れされる。その後、該処理容器3aが
10”@Torr程度の高真空にされ、その加工処理が
される。
The device 3 is configured such that the workpiece 5 is exposed to the sample exit door 3e in the atmosphere.
It is put in and taken out by opening and closing. Thereafter, the processing container 3a is brought to a high vacuum of about 10''@Torr, and the processing is performed.

このような処理装置3の真空度は、真空処理容器3aに
設置された熱伝導真空計1と電離真空計2とにより把握
される。熱伝導真空計1は、該処理容器3aに設けられ
た低真空用センサIAと、その検出信号の処理をする信
号処理/表示回路IBから構成されている。
The degree of vacuum of the processing apparatus 3 is determined by a heat conduction vacuum gauge 1 and an ionization vacuum gauge 2 installed in the vacuum processing container 3a. The thermal conduction vacuum gauge 1 is composed of a low vacuum sensor IA provided in the processing container 3a and a signal processing/display circuit IB that processes the detection signal.

また、電離真空計2は同様にその容器3aに設けられた
高真空用センサ2Aと、その検出信号の処理をする信号
処理/表示回!82Bから構成されている。例えば、該
センサIA、IBは、真空処理容器3aに直径70mm
φの開口部がそれぞれ設けられ、コンフラツトフランジ
等の継ぎ手部材により係合されている。
The ionization vacuum gauge 2 also has a high vacuum sensor 2A installed in its container 3a, and a signal processing/display circuit for processing the detection signal! It is composed of 82B. For example, the sensors IA and IB are installed in a vacuum processing container 3a with a diameter of 70 mm.
Each opening has a diameter of φ and is engaged by a joint member such as a conflat flange.

[発明が解決しようとする課題] ところで、従来例によればスパッタ装置やCVD装置等
の処理装置3が、その容器3a内を大気圧から10−”
Torr程度の高真空にした後に、被加工物の加工処理
がされる。このことから、該容器3aの真空度を把握す
るため、測定可能範囲が10−4〜760 T orr
の熱伝導真空計1と、測定可能範囲が10” 〜10−
’Torrの電離真空計2とを併用することにより対処
している。
[Problems to be Solved by the Invention] According to the conventional example, the processing apparatus 3 such as a sputtering apparatus or a CVD apparatus has a temperature of 10-" within the container 3a from atmospheric pressure.
After creating a high vacuum of about Torr, the workpiece is processed. From this, in order to grasp the degree of vacuum of the container 3a, the measurable range is 10-4 to 760 Torr.
Thermal conductivity vacuum gauge 1 has a measurable range of 10" to 10-
This is handled by using Torr's ionization vacuum gauge 2 together.

このため、それぞれのセンサIA、IBが個別に真空処
理容器3aに設置される。一般に真空処理容器3a等の
高真空状態を維持するためには、気密保持劣化の原因と
なる継ぎ手部材や試料人出ドア3e等の開口部の設置数
を極力削減する必要がある。
For this reason, the respective sensors IA and IB are individually installed in the vacuum processing container 3a. Generally, in order to maintain a high vacuum state in the vacuum processing container 3a, etc., it is necessary to reduce as much as possible the number of joint members and openings such as the sample access door 3e, which cause deterioration of airtightness.

しかし、各真空計1.2の測定範囲の制限により真空処
理容器3aに最低2か所の開口部が必要となる。
However, due to limitations in the measurement range of each vacuum gauge 1.2, at least two openings are required in the vacuum processing container 3a.

これにより、気密保持劣化の原因となる開口部の削減を
図ることができず、排気装置4の効率の低下の原因にな
るという問題がある。
As a result, there is a problem in that it is impossible to reduce the number of openings that cause deterioration of airtightness, and this causes a decrease in the efficiency of the exhaust device 4.

本発明は、かかる従来例の問題点に鑑み創作されたもの
であり、真空処理装置の真空度の気密保持に影響を及ぼ
す検知器の設置数を削減し、大気圧から高真空に至る範
囲の真空度を測定することを可能とする真空計測装置の
堤供を目的とする。
The present invention was created in view of the problems of the conventional method, and reduces the number of installed detectors that affect the airtightness of vacuum processing equipment, and is capable of reducing The purpose is to provide a vacuum measuring device that can measure the degree of vacuum.

〔課題を解決するための手段] 第1図は、本発明に係る真空測定装置の原理図を示して
いる。
[Means for Solving the Problems] FIG. 1 shows a principle diagram of a vacuum measuring device according to the present invention.

真空度を分担して検出する二以上の検出部11A11B
・・・が同一の格納容器lICに格納された複合検出手
段11と、前記検出部11A、11B・・・からの信号
Sl、S2・・・を個別に処理する二以上の信号処理手
段12.13・・・と、前記信号処理手段1213・・
・からの二以上の真空度データD1、D2を選択出力す
る信号出力手段14と、前記信号処理手段12.13・
・・及び信号出力手段14の人出力を制御する制御手段
15とを具備することを特徴とし、上記目的を達成する
Two or more detection units 11A11B that share and detect the degree of vacuum
... are stored in the same containment vessel IC, and two or more signal processing means 12. which individually process the signals Sl, S2, ... from the detection units 11A, 11B, ... 13... and the signal processing means 1213...
・Signal output means 14 for selectively outputting two or more degree of vacuum data D1, D2 from , and the signal processing means 12.13.
... and a control means 15 for controlling the human output of the signal output means 14, thereby achieving the above object.

(作 用] 本発明によれば、真空度を分担して検出する二以上の検
出部11A、11B・・・が同一の格納容器11Cに格
納された複合検出手段11が設けられている。
(Function) According to the present invention, a composite detection means 11 is provided in which two or more detection units 11A, 11B, .

このため、検出手段11を取り付けるための開口部を真
空処理装置16に1か所のみ設けることで足りる。また
、例えば、第1の検出部11Aに760 ”10−’T
orrの真空度の測定範囲を分!Rさせ、第2の検出部
11Bに10−’〜10−” Torrの真空度の範囲
を分担させ、それぞれの真空度データDID2を選択出
力することにより、大気圧から商真空に至る範囲の真空
度を測定することが可能となる。
Therefore, it is sufficient to provide only one opening in the vacuum processing apparatus 16 for attaching the detection means 11. Further, for example, 760"10-'T is applied to the first detection unit 11A.
The measurement range of the degree of vacuum of orr is minute! R, the second detection unit 11B is assigned to the range of vacuum degrees from 10-' to 10-'' Torr, and by selectively outputting the respective vacuum degree data DID2, the vacuum range from atmospheric pressure to commercial vacuum can be detected. It becomes possible to measure the degree of

これにより、気密保持劣化の原因となる開口部の設置数
が削減され、排気装置の効率の向上を図ることが可能と
なる。
This reduces the number of openings that cause airtightness deterioration, making it possible to improve the efficiency of the exhaust system.

〔実施例] 次に図を参照しながら本発明の実施例について説明をす
る。
[Example] Next, an example of the present invention will be described with reference to the drawings.

第2図は、本発明の実施例に係る真空測定装置の構成図
である。
FIG. 2 is a configuration diagram of a vacuum measuring device according to an embodiment of the present invention.

回において、21は複合検出手段11の一実施例となる
複合検知器であり、格納容器21Cに設けられたピラニ
ゲージ部21A、ベアード/アルバートゲージ部(以下
B/Aゲージ部という)21B及びこれらを絶縁する絶
縁スペーサ21D、21Eから成るものである。
21, a composite detector 21 is an embodiment of the composite detection means 11, and includes a Pirani gauge section 21A, a Baird/Albert gauge section (hereinafter referred to as B/A gauge section) 21B, and a Pirani gauge section 21A provided in a containment vessel 21C. It consists of insulating spacers 21D and 21E for insulation.

ピラニゲージ部21Aは、第1の検出部11Aの一実施
例となる検知器であり、大気圧760〜中間流領域10
−’Torrの真空度の検知を分担するものである。該
ゲージ部21Aは、棒状フィラメントから成る。
The Pirani gauge section 21A is a detector that is an example of the first detection section 11A, and is a detector that is an embodiment of the first detection section 11A, and has a range from atmospheric pressure 760 to intermediate flow region 10.
-'Torr is responsible for detecting the degree of vacuum. The gauge portion 21A is made of a rod-shaped filament.

その検知原理は、フィラメントに温度の低い気体分子が
1gi突すると、衝突時の熱の授受によって該フィラメ
ントが冷却される。このフィラメントから失われる電力
が圧力に比例する。この電力の変化から被測定対象の真
空度を検知するものである。
The detection principle is that when 1 gi of low-temperature gas molecules collide with a filament, the filament is cooled by the exchange of heat during the collision. The power lost from this filament is proportional to the pressure. The degree of vacuum of the object to be measured is detected from this change in power.

B/Aゲージ部21Bは、第2の検出部11Bの一実施
例となる検知器であり、中間流fiI¥域101〜高真
空領域10−” Torrの真空度の検知を分担するも
のである。該ゲージ部21Aは、フィラメント20a、
グリッド電極20b及びコレクタ電極20cから成る。
The B/A gauge section 21B is a detector that is an example of the second detection section 11B, and is responsible for detecting the degree of vacuum from the intermediate flow fiI region 101 to the high vacuum region 10'' Torr. The gauge part 21A includes a filament 20a,
It consists of a grid electrode 20b and a collector electrode 20c.

その検知原理は、フィラメント20aから出射した電子
が150e V程度のエネルギーにより加速される。電
子は、気体分子密度に応じた割合で気体分子に衝突し、
それを電離する。この際に、コレクタ電流ICとグリッ
ド電流の比で表される電子電流を一定とすれば、電離に
よって生したイオン電流が圧力に比例する。このイオン
電流の変化から被測定対象の真空度を検知するものであ
る。
The detection principle is that electrons emitted from the filament 20a are accelerated by an energy of about 150 eV. Electrons collide with gas molecules at a rate that depends on the gas molecule density,
ionize it. At this time, if the electron current represented by the ratio of the collector current IC to the grid current is constant, the ion current generated by ionization is proportional to the pressure. The degree of vacuum of the object to be measured is detected from changes in this ion current.

ピラニゲージ部21A及びB/Aゲージ部21Bは、相
互干渉を避けるため取り付は位置が工夫されている0例
えば、熱依存性の高いピラニゲージ部21人は、B/A
ゲージ部21Bの取り付は位置よりも後退させて格納容
器21cに絶縁スペーサ21Eを介して形成される。絶
縁スペーサ21D、21Eは耐熱・耐酸化性の材料等が
用いられ、格納容器21cにそれが充填される。
The mounting positions of the Pirani gauge section 21A and the B/A gauge section 21B are designed to avoid mutual interference. For example, the Pirani gauge section 21, which is highly heat-dependent,
The gauge portion 21B is attached to the containment vessel 21c at a position recessed from the position via an insulating spacer 21E. The insulating spacers 21D and 21E are made of a heat-resistant and oxidation-resistant material, and are filled into the containment vessel 21c.

また、複合検知器21は、真空処理装置27に直径70
nnφ程度に開口された開口部28に取り付けられる。
Moreover, the composite detector 21 is installed in the vacuum processing device 27 with a diameter of 70 mm.
It is attached to an opening 28 having a diameter of about nnφ.

該検知H21は、コンフラツトフランジ(耐圧継ぎ手)
構造により超高真空状態に対処している。その構造は、
処理装置27の開口部28、複合検知器21の相互に設
けられたフランジの間に無酸化銅のガスケットを介して
、両フランジをボルト・ナツト30により係合したもの
である。
The detection H21 is a conflat flange (pressure joint)
Its structure allows it to handle ultra-high vacuum conditions. Its structure is
An oxidized copper gasket is interposed between the opening 28 of the processing device 27 and the flanges of the composite detector 21, and the flanges are engaged with bolts and nuts 30.

22は第1の信号処理手段12の一実施例となる第1の
検出処理回路であり、フィラメント電流IFの変化から
低真空度データD1を出力するものである。該回路22
は、ピラニゲージ部21Aを一定温度にする定温回路2
2a及びフィラメント電流IFの変化、すなわち、該ゲ
ージ部21Aから失われる電力に基づいて低真空度デー
タDIを出力する電力検出回路22bから成る。
A first detection processing circuit 22 is an embodiment of the first signal processing means 12, and outputs low vacuum degree data D1 based on changes in the filament current IF. The circuit 22
is a constant temperature circuit 2 that keeps the Pirani gauge part 21A at a constant temperature.
2a and a power detection circuit 22b that outputs low vacuum degree data DI based on the change in the filament current IF, that is, the power lost from the gauge section 21A.

23は第2の信号処理手段13の一実施例となる第2の
検出処理回路であり、コレクタ電流ICの変化から高真
空度データD2を出力するものである。該回路23は、
フィラメント20a、グリッド電極20b及びコレクタ
電極20cに電源を供給する直流電源回路23a及び電
子電流の変化によるイオン電流に基づいて高真空度デー
タD2を出力する電流検出回路23bから成る。
A second detection processing circuit 23 is an embodiment of the second signal processing means 13, and outputs high vacuum degree data D2 based on changes in the collector current IC. The circuit 23 is
It consists of a DC power supply circuit 23a that supplies power to the filament 20a, grid electrode 20b, and collector electrode 20c, and a current detection circuit 23b that outputs high vacuum degree data D2 based on ion current caused by changes in electron current.

24は信号出力手段14の一実施例となるデータ比較/
出力回路であり、低真空度データDI及び高真空度デー
タD2を入力して、いずれか一方のデータを出力するも
のである。この際の選択基準は、予め、両ゲージ部21
A、21Bの測定範囲の境界1例えば、中間?t SR
域10−’Torrを境界データD3とする。そのデー
タは制御手段15より入力する。
24 is a data comparison/
This is an output circuit that inputs low vacuum degree data DI and high vacuum degree data D2 and outputs either one of the data. The selection criteria at this time is that both gauge parts 21
Boundary 1 of measurement range of A, 21B For example, middle? tSR
Let the area 10-'Torr be the boundary data D3. The data is inputted from the control means 15.

25は制御手段15の一実施例となるマイクロプロセッ
サユニット(以下MPUという)であり、定温回路22
a、電力検出回路22b、直流電源回路23a、iti
流検比検出回路23bチ゛−タ比較/出力回路24の入
出力を制御するものである。
25 is a microprocessor unit (hereinafter referred to as MPU) which is an embodiment of the control means 15, and the constant temperature circuit 22
a, power detection circuit 22b, DC power supply circuit 23a, iti
The current ratio detection circuit 23b controls the input and output of the chip comparison/output circuit 24.

26は表示回路であり、データD1又はD2を入力して
真空処理装置27の真空度を表示するものである。
26 is a display circuit which inputs data D1 or D2 and displays the degree of vacuum of the vacuum processing apparatus 27.

こようにして、本発明の実施例によれば真空処理装置2
7の真空度を検出するピラニゲージ部21八及びB/A
ゲージ部21Bを直径70mmの同一の格納容器21C
に格納した複合検出器21が設けられている。
Thus, according to an embodiment of the present invention, the vacuum processing apparatus 2
Pirani gauge part 218 and B/A for detecting the degree of vacuum of 7
The gauge part 21B is connected to the same containment vessel 21C with a diameter of 70 mm.
A composite detector 21 is provided.

このため、該検出器21を取り付けるための開口部28
を真空処理装置27に1か所のみ設けることで足りる。
For this reason, an opening 28 for attaching the detector 21 is provided.
It is sufficient to provide only one location in the vacuum processing apparatus 27.

また、ピラニゲージ部21Aが大気圧760〜中間流領
域10−’Torrの真空度の測定範囲を分担し、B/
Aゲージ部21Bが中間流領域10−4〜高真空領域1
0−” Torrの真空度の範囲を分担し、それぞれの
真空度データI’)1.D2を境界データD3に基づい
て選択出力することにより、大気圧から高真空に至る範
囲の真空度を測定することが可能となる。
In addition, the Pirani gauge section 21A shares the measurement range of the degree of vacuum from atmospheric pressure 760 to intermediate flow region 10-'Torr, and B/
A gauge part 21B is intermediate flow region 10-4 to high vacuum region 1
By sharing the vacuum degree range of 0-” Torr and selectively outputting the respective vacuum degree data I')1.D2 based on the boundary data D3, it is possible to measure the degree of vacuum in the range from atmospheric pressure to high vacuum. It becomes possible to do so.

これにより、気密保持劣化の原因となる開口部28の設
置数が従来例に比べて1つ削減され、排気装24の効率
の向上を図ることが可能となる。
As a result, the number of openings 28 that cause airtightness deterioration is reduced by one compared to the conventional example, and the efficiency of the exhaust system 24 can be improved.

〔発明の効果] 以上説明したように、本発明によれば、真空度の範囲を
分担して検出する二つの検出部を同一の格納容器に格納
した複合検出器が設けられている。
[Effects of the Invention] As described above, according to the present invention, a composite detector is provided in which two detection units that detect different degrees of vacuum are housed in the same container.

このため、該検出器を取り付けるための開口部が真空処
理2iWに1か所のみ設けることで足りる。
Therefore, it is sufficient to provide only one opening in the vacuum processing 2iW for attaching the detector.

また、一方の検出部が大気圧〜中間流領域の測定範囲を
分担し、他方の検出部が中間流領域〜高真空の範囲を分
担し、それぞれの真空度データを選択出力することによ
り、大気圧から高真空に至る範囲の真空度を効率良く測
定することが可能となる。
In addition, one detection section shares the measurement range from atmospheric pressure to the intermediate flow region, and the other detection section shares the measurement range from the intermediate flow region to high vacuum, and by selectively outputting the respective degree of vacuum data, large It becomes possible to efficiently measure the degree of vacuum in the range from atmospheric pressure to high vacuum.

これにより、スパッタ装置やCVD装置等の真空処理製
造装置の性能の向上及び真空測定システムの測定効率の
向上に寄与するところが大きい。
This greatly contributes to improving the performance of vacuum processing manufacturing equipment such as sputtering equipment and CVD equipment, and to improving the measurement efficiency of vacuum measurement systems.

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

第1図は、本発明に係る真空測定装置の原理回、第2図
は、本発明の実施例に係る真空測定装置の構成図、 第3図は、従来例に係る真空処理装置の真空測定システ
ムの説明図である。 (符号の説明) 11・・・複合検知手段、 11A・・・第1の検出部、 11B・・・第2の検出部、 12・・・第1の信号処理手段、 13・・・第2の信号処理手段、 14・・・信号出力手段、 15・・・制御手段。
Fig. 1 shows the principle of a vacuum measuring device according to the present invention, Fig. 2 is a configuration diagram of a vacuum measuring device according to an embodiment of the present invention, and Fig. 3 shows vacuum measurement of a vacuum processing device according to a conventional example. FIG. 2 is an explanatory diagram of the system. (Explanation of symbols) 11... Composite detection means, 11A... First detection section, 11B... Second detection section, 12... First signal processing means, 13... Second 14... Signal output means; 15... Control means.

Claims (1)

【特許請求の範囲】[Claims] 真空度の範囲を分担して検出する二以上の検出部(11
A、11B・・・)が同一の格納容器(11C)に格納
された複合検出手段(11)と、前記検出部(11A、
11B・・・)からの信号(S1、S2・・・)を個別
に処理する二以上の信号処理手段(12、13・・・)
と、前記信号処理手段(12、13・・・)からの二以
上の真空度データ(D1、D2)を選択出力する信号出
力手段(14)と、前記信号処理手段(12、13・・
・)及び信号出力手段(14)の入出力を制御する制御
手段(15)とを具備することを特徴とする真空測定装
置。
Two or more detection units (11
A, 11B...) are housed in the same containment vessel (11C).
Two or more signal processing means (12, 13...) that individually process the signals (S1, S2...) from 11B...)
, a signal output means (14) for selectively outputting two or more degree of vacuum data (D1, D2) from the signal processing means (12, 13...), and the signal processing means (12, 13...).
.) and control means (15) for controlling input and output of the signal output means (14).
JP33728989A 1989-12-26 1989-12-26 Vacuum measuring instrument Pending JPH03197832A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP33728989A JPH03197832A (en) 1989-12-26 1989-12-26 Vacuum measuring instrument

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP33728989A JPH03197832A (en) 1989-12-26 1989-12-26 Vacuum measuring instrument

Publications (1)

Publication Number Publication Date
JPH03197832A true JPH03197832A (en) 1991-08-29

Family

ID=18307218

Family Applications (1)

Application Number Title Priority Date Filing Date
JP33728989A Pending JPH03197832A (en) 1989-12-26 1989-12-26 Vacuum measuring instrument

Country Status (1)

Country Link
JP (1) JPH03197832A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001215163A (en) * 2000-02-02 2001-08-10 Anelva Corp Ionization gauge
JP2002520613A (en) * 1998-07-16 2002-07-09 ユナキス・バルツェルス・アクチェンゲゼルシャフト Pressure sensor, pressure measuring device and method for monitoring pressure in a chamber
JP2008523410A (en) * 2004-12-14 2008-07-03 ブルックス オートメーション インコーポレイテッド Method and apparatus for storing measurement data about vacuum gauge calibration parameters and vacuum gauge structure
JP2010054518A (en) * 2009-12-08 2010-03-11 Canon Anelva Corp Hybrid vacuum gauge
JP2011191284A (en) * 2010-03-12 2011-09-29 Toyo Denshi Kenkyusho:Kk Hot-cathode type ionization vacuum gauge with cold-cathode type ionization vacuum gauge

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002520613A (en) * 1998-07-16 2002-07-09 ユナキス・バルツェルス・アクチェンゲゼルシャフト Pressure sensor, pressure measuring device and method for monitoring pressure in a chamber
JP2001215163A (en) * 2000-02-02 2001-08-10 Anelva Corp Ionization gauge
JP2008523410A (en) * 2004-12-14 2008-07-03 ブルックス オートメーション インコーポレイテッド Method and apparatus for storing measurement data about vacuum gauge calibration parameters and vacuum gauge structure
JP2010054518A (en) * 2009-12-08 2010-03-11 Canon Anelva Corp Hybrid vacuum gauge
JP2011191284A (en) * 2010-03-12 2011-09-29 Toyo Denshi Kenkyusho:Kk Hot-cathode type ionization vacuum gauge with cold-cathode type ionization vacuum gauge

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