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JPH0411315B2 - - Google Patents
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JPH0411315B2 - - Google Patents

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Publication number
JPH0411315B2
JPH0411315B2 JP60058286A JP5828685A JPH0411315B2 JP H0411315 B2 JPH0411315 B2 JP H0411315B2 JP 60058286 A JP60058286 A JP 60058286A JP 5828685 A JP5828685 A JP 5828685A JP H0411315 B2 JPH0411315 B2 JP H0411315B2
Authority
JP
Japan
Prior art keywords
laser
mirror
integrating sphere
output
laser beam
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 - Lifetime
Application number
JP60058286A
Other languages
Japanese (ja)
Other versions
JPS61219489A (en
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 filed Critical
Priority to JP60058286A priority Critical patent/JPS61219489A/en
Publication of JPS61219489A publication Critical patent/JPS61219489A/en
Publication of JPH0411315B2 publication Critical patent/JPH0411315B2/ja
Granted legal-status Critical Current

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  • Testing Of Optical Devices Or Fibers (AREA)
  • Laser Beam Processing (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、レーザ加工装置におけるレーザ光
の出力制御装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a laser beam output control device in a laser processing device.

〔従来の技術〕[Conventional technology]

第3図は従来のレーザ出力制御装置を示す構成
図であり、容器1内にレーザ媒質ガス2を満し、
電源4の出力電圧により電極3A,3B間に放電
をさせてレーザ媒質ガス2を励起し、全反射鏡5
と部分透過鏡6間でレーザ発振を起して部分透過
鏡6からレーザ光7を出力させる。
FIG. 3 is a configuration diagram showing a conventional laser output control device, in which a container 1 is filled with a laser medium gas 2,
The output voltage of the power source 4 causes a discharge between the electrodes 3A and 3B to excite the laser medium gas 2, and the total reflection mirror 5
Laser oscillation is generated between the partially transmitting mirror 6 and the partially transmitting mirror 6, and a laser beam 7 is output from the partially transmitting mirror 6.

このレーザ光7はベンドミラー8A,8B,8
Cにより任意の位置に伝送され、加工ヘツド9に
取付けたレンズ10により集光し、焦点位置近傍
で被加工物11を加工する。この場合、レーザ光
7の光路に部分透過鏡12を挿入し、レーザ光7
の一部を取り出して積分球13に入射させる。こ
の積分球13は内面が反射材料でできており、ビ
ームが内部で反射をくり返すことにより均一にな
るので、レーザ光検出器14により均一に減光さ
れたレーザ光7の一部を検出してレーザ出力設定
器15の出力信号と比較し、その偏差を増幅器1
6により増幅して電源4に信号を送り、レーザ光
7の強度を一定に保つようにフイードバツク制御
を行つている。
This laser beam 7 is transmitted to bend mirrors 8A, 8B, 8
The light is transmitted to an arbitrary position by C, and is focused by a lens 10 attached to the processing head 9, and the workpiece 11 is processed near the focal position. In this case, a partially transmitting mirror 12 is inserted in the optical path of the laser beam 7, and the laser beam 7 is
A part of it is taken out and made incident on the integrating sphere 13. The inner surface of this integrating sphere 13 is made of a reflective material, and the beam becomes uniform by repeating reflections inside, so the laser light detector 14 detects a portion of the laser light 7 that has been uniformly attenuated. is compared with the output signal of the laser output setting device 15, and the deviation is determined by the amplifier 1.
6 and sends the signal to the power source 4, and feedback control is performed to keep the intensity of the laser beam 7 constant.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

従来のレーザ出力制御装置は以上のように構成
されているので、第4図に示すように部分透過鏡
12の反射光17は積分球13に入射して内部で
反射をくり返すが、光取入口18が大きいと19
のように外部へもれて行くので、レーザ検出器1
4は正確なレーザ強度を測定できない。また、モ
ニター以後のベンドミラー8A,8B,8Cが汚
れた場合にレーザ光17の減衰が生じても、部分
透過鏡12以後の光路におけるレーザ光7の減衰
は検出できない等の問題があつた。
Since the conventional laser output control device is configured as described above, the reflected light 17 from the partially transmitting mirror 12 enters the integrating sphere 13 and is repeatedly reflected inside, as shown in FIG. 19 if the entrance 18 is large
Laser detector 1
4 cannot measure accurate laser intensity. Further, even if the laser beam 17 is attenuated when the bend mirrors 8A, 8B, and 8C after the monitor become dirty, there is a problem that the attenuation of the laser beam 7 in the optical path after the partially transmitting mirror 12 cannot be detected.

この発明は上記のような問題点を解消するため
になされたもので、積分球の取入口からの光のも
れが無く、正確なレーザ出力で加工することがで
きるレーザ出力制御装置を得ることを目的とす
る。
This invention was made in order to solve the above-mentioned problems, and it is an object of the present invention to obtain a laser output control device that can perform processing with accurate laser output without light leakage from the inlet of the integrating sphere. With the goal.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係るレーザ出力制御装置は、ベンド
ミラーで光を伝送するものにおいて、ベンドミラ
ーを部分透過鏡とし、積分球の光取入口をベンド
ミラーの透過側に密着させたもので、レーザ光の
強度を検出してレーザ出力設定器の出力と比較
し、その偏差信号をフイードバツクしてレーザ出
力を制御するようにしたものである。
The laser output control device according to the present invention transmits light using a bend mirror, in which the bend mirror is a partially transmitting mirror, and the light intake port of the integrating sphere is brought into close contact with the transmitting side of the bend mirror, so that the laser beam can be transmitted. The intensity is detected and compared with the output of the laser output setting device, and the deviation signal is fed back to control the laser output.

〔作用〕[Effect]

この発明は、加工レンズに最も近いベンドミラ
ーの透過側に積分球の光取入口を密着して取り付
けたので、積分球取入口からのレーザ光のもれが
なく、加工に使用されるレーザパワーを正確に検
出、制御する。
In this invention, the light intake port of the integrating sphere is closely attached to the transmission side of the bend mirror closest to the processing lens, so there is no leakage of laser light from the integrating sphere intake port, and the laser power used for processing is reduced. accurately detect and control.

〔発明の実施例〕[Embodiments of the invention]

以下、この発明の一実施例を図について説明す
る。第1図において、1〜6は従来例を示した第
3図における同符号のものと同一または相当部分
であり、加工レンズ10に最も近いベンドミラー
を部分透過鏡20とし、レーザパワーの一部を透
過するようになつている。
An embodiment of the present invention will be described below with reference to the drawings. In FIG. 1, numerals 1 to 6 are the same or corresponding parts as those with the same symbols in FIG. It is becoming more transparent.

第2図は検出部を拡大した図であり、20は部
分反射鏡で、積分球13の光取入口が透過側に密
着して取付けられている。21は積分球13内で
の反射光、22は入射レーザ光、23は全反射コ
ーテイングである。
FIG. 2 is an enlarged view of the detection section, and 20 is a partial reflection mirror, which is attached so that the light intake port of the integrating sphere 13 is in close contact with the transmission side. 21 is reflected light within the integrating sphere 13, 22 is an incident laser beam, and 23 is a total reflection coating.

次に動作について説明する。第2図において、
入射レーザ光22は部分透過鏡20の全反射コー
テイング23ではほとんど反射されるが1〜2%
透過される。透過したレーザ光は積分球13の内
面に当り、内面は金等の反射材で構成されている
ので反射をくり返す。また、部分透過鏡20の部
分は積分球13の光取入口になるが、反射光21
のように外へもれようとする光は、部分透過鏡2
0の全反射コーテイング23で反射されるため外
へもれない。このため、積分球13の内面に当る
レーザ光の強度は平均化され、レーザ光検出器に
より均一されたレーザ光の一部を正確に検出でき
る。
Next, the operation will be explained. In Figure 2,
Most of the incident laser beam 22 is reflected by the total reflection coating 23 of the partially transmitting mirror 20, but only 1 to 2%.
Transparent. The transmitted laser beam hits the inner surface of the integrating sphere 13, and since the inner surface is made of a reflective material such as gold, it is repeatedly reflected. In addition, the part of the partially transmitting mirror 20 becomes the light inlet of the integrating sphere 13, but the reflected light 21
The light that tries to leak outside like this is partially transmitted by the partially transmitting mirror 2.
Since it is reflected by the total reflection coating 23 of 0, it does not leak to the outside. Therefore, the intensity of the laser light hitting the inner surface of the integrating sphere 13 is averaged, and a portion of the uniform laser light can be accurately detected by the laser light detector.

正確に検出されたレーザ出力信号は、レーザ出
力設定器15の信号との偏差を増幅器16により
増幅し、電源4へフイードバツクすることにより
電極3A,3B間の放電強度を変え、励起強度を
変えることによりレーザ発振強度を制御すること
ができる。もし、レーザ発振効率が下がつたり、
ベンドミラー8A,8Bが汚れても、検出部にお
けるレーザ強度が一定になるように制御されてい
るため、電源4の励起出力を高くして、検出部で
は常に正確なレーザパワーにすることができ、安
定なレーザ加工ができるようになつている。
The accurately detected laser output signal is used to amplify the deviation from the signal from the laser output setting device 15 using an amplifier 16 and feed it back to the power source 4, thereby changing the discharge intensity between the electrodes 3A and 3B and changing the excitation intensity. The laser oscillation intensity can be controlled by If the laser oscillation efficiency decreases,
Even if the bend mirrors 8A and 8B are dirty, the laser intensity at the detection section is controlled to be constant, so the excitation output of the power source 4 can be increased to always provide accurate laser power at the detection section. , it has become possible to perform stable laser processing.

なお上記実施例では、レンズに最も近いベンド
ミラーに積分球による検出機構を設けたが、他の
ベンドミラーであつてもよく、上記実施例と同様
の効果を奏する。
In the above embodiment, the detection mechanism using an integrating sphere is provided on the bend mirror closest to the lens, but other bend mirrors may be used and the same effects as in the above embodiment can be achieved.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明によればベンドミラー
に積分球を密着して取り付け、レーザパワーを検
出してレーザ出力を制御するように構成したの
で、積分球取入口からレーザ光がもれず、レーザ
発振効率の変動に影響がなく、安定したレーザ加
工を行なうことができる。
As described above, according to the present invention, since the integrating sphere is closely attached to the bend mirror and the laser power is detected to control the laser output, the laser light does not leak from the integrating sphere inlet, and the laser There is no effect on fluctuations in oscillation efficiency, and stable laser processing can be performed.

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

第1図はこの発明の一実施例による積分球型レ
ーザ出力制御装置の構成図、第2図は第1図にお
ける検出部分の拡大図、第3図は従来のレーザ出
力制御装置の構成図、第4図は第3図における検
出部分の拡大図である。 図において、2はレーザ媒質ガス、5は全反射
鏡、6は部分透過鏡、7はレーザ光、8A,8B
はベンドミラー、10はレンズ、13は積分球、
20は部分透過鏡である。 なお、図中同一符号は同一または相当部分を示
す。
FIG. 1 is a block diagram of an integrating sphere laser output control device according to an embodiment of the present invention, FIG. 2 is an enlarged view of the detection portion in FIG. 1, and FIG. 3 is a block diagram of a conventional laser output control device. FIG. 4 is an enlarged view of the detection portion in FIG. 3. In the figure, 2 is a laser medium gas, 5 is a total reflection mirror, 6 is a partial transmission mirror, 7 is a laser beam, 8A, 8B
is a bend mirror, 10 is a lens, 13 is an integrating sphere,
20 is a partially transmitting mirror. Note that the same reference numerals in the figures indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】 1 レーザ発振器より出力するレーザ光をベンド
ミラーにより任意の位置へ伝送して加工レンズに
より集光し、焦点位置近傍でレーザ加工を行うレ
ーザ加工装置において、 上記ベンドミラーを部分透過鏡とし、該ベンド
ミラーの透過側にレーザ出力設定器の出力と比較
するレーザ光を出力する積分球の光取入口を密着
して取り付けたことを特徴とするレーザ出力制御
装置。
[Scope of Claims] 1. A laser processing device that transmits a laser beam output from a laser oscillator to an arbitrary position using a bend mirror, focuses it on a processing lens, and performs laser processing near the focal position, wherein the bend mirror is partially 1. A laser output control device comprising a transmitting mirror, and a light inlet of an integrating sphere that outputs a laser beam to be compared with the output of a laser output setting device is closely attached to the transmitting side of the bend mirror.
JP60058286A 1985-03-25 1985-03-25 Method for controlling laser output Granted JPS61219489A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60058286A JPS61219489A (en) 1985-03-25 1985-03-25 Method for controlling laser output

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60058286A JPS61219489A (en) 1985-03-25 1985-03-25 Method for controlling laser output

Publications (2)

Publication Number Publication Date
JPS61219489A JPS61219489A (en) 1986-09-29
JPH0411315B2 true JPH0411315B2 (en) 1992-02-28

Family

ID=13079953

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60058286A Granted JPS61219489A (en) 1985-03-25 1985-03-25 Method for controlling laser output

Country Status (1)

Country Link
JP (1) JPS61219489A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03107806A (en) * 1989-09-22 1991-05-08 Graphtec Corp Optical distributor
JP2720744B2 (en) * 1992-12-28 1998-03-04 三菱電機株式会社 Laser processing machine
US6538229B1 (en) * 1996-05-08 2003-03-25 Infineon Technologies Ag Method for the positionally accurate adjustment and fixing of a microoptical element
DE112018006927B4 (en) 2018-02-22 2022-02-10 Mitsubishi Electric Corporation Laser oscillation device and method for controlling a laser oscillation device

Also Published As

Publication number Publication date
JPS61219489A (en) 1986-09-29

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