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JPS63104389A - Laser output measuring apparatus - Google Patents

Laser output measuring apparatus

Info

Publication number
JPS63104389A
JPS63104389A JP25014386A JP25014386A JPS63104389A JP S63104389 A JPS63104389 A JP S63104389A JP 25014386 A JP25014386 A JP 25014386A JP 25014386 A JP25014386 A JP 25014386A JP S63104389 A JPS63104389 A JP S63104389A
Authority
JP
Japan
Prior art keywords
pulse
output
conversion element
photoelectric conversion
laser
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
JP25014386A
Other languages
Japanese (ja)
Inventor
Kenji Kumamoto
健二 熊本
Akiyoshi Nawa
名和 章好
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP25014386A priority Critical patent/JPS63104389A/en
Publication of JPS63104389A publication Critical patent/JPS63104389A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/0014Monitoring arrangements not otherwise provided for

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Abstract

PURPOSE:To perform more exact control of pulse laser oscillation, by detecting pulse laser beams by a photoelectric conversion element of high responsibility and averaging the detected pulse signal to obtain a pulse average output. CONSTITUTION:Part of pulse laser beams oscillated by a laser oscillator 1 is introduced into an integral sphere 2. In this sphere 2, the pulse laser beams are reflected in multiple numbers on an inner wall surface of the integral sphere and gradually absorbed into a phetoelectric conversion element 3. A beam current corresponding to a pulse change is outputted to an image display device 4 from the element 3. A pulse wave generated in accordance with a change in beam current is displayed on a screen of the device 4 so as to provide pulse wave observation. In a sampling averaging circuit 5, high-speed sampling of the pulse signal outputted from the element 3 is performed at 10 Hz or more so that pulse average output is generated. The pulse average output is inputted as a feedback signal to a pulse oscillation power source 7. In this way, while the pulse wave form is observed, exact control of pulse laser oscillation can be performed.

Description

【発明の詳細な説明】 「産業上の利用分野」 この発明はパルスレーザ出力の平均パワー測定及びパル
ス波形観測を同時に行なうレーザ出力測定装置に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION "Field of Industrial Application" The present invention relates to a laser output measuring device that simultaneously measures the average power of pulsed laser output and observes the pulse waveform.

[従来の技術] 一般に高出力のパルスレーザ光(又は連続発振レーザ光
以降C讐・パルスレーザ光とする)を測定する場合は、
レーザセンサの耐パワー性、及びレーザ光吸収効率等の
関係より、筐体内に導入したGW・パルスレーザ光を筐
体内壁面での繰り返し反射により徐々にCl1i11パ
ルスレーザ光をレーザセンサに吸収させる多重反射形と
いう形式が用いられる。
[Prior Art] Generally, when measuring high-power pulsed laser light (or pulsed laser light after continuous wave laser light),
Due to the power resistance of the laser sensor and laser light absorption efficiency, multiple reflections are used to gradually absorb the Cl1i11 pulsed laser light into the laser sensor by repeatedly reflecting the GW/pulsed laser light introduced into the housing on the inner wall of the housing. The form called shape is used.

第3図はCW・パルスレーザ光の多重反射形を用いた従
来のレーザ出力測定装置の概略構成図である0図に基づ
いて従来のレーザ出力測定方法を説明する。!04図に
示すようなパルス波形のパルスレーザ光(1a)は全体
球面状(1分球)であり内壁面全体を鏡面とした筐体(
3)内へ開口部(3a)より導入される。するとパルス
レーザ光(la)は筐体内面において繰り返し反射を行
ない徐々に筐体(3)内面に設けられた熱電対(3b)
へ吸収される。この熱電対(3b〕に発生する熱起電力
は吸収されたレーザIB力に比例しており、予めパワー
メータ(4a)を校正しておくことでパルスレーザ出力
の平均値を容易に知ることができる。
FIG. 3 describes a conventional laser output measuring method based on FIG. 0, which is a schematic configuration diagram of a conventional laser output measuring device using a multiple reflection type of CW pulsed laser light. ! The pulsed laser beam (1a) with a pulse waveform as shown in Fig. 04 has an entirely spherical shape (one segment sphere), and the entire inner wall surface is mirror-finished in a housing (
3) Introduced into the interior through the opening (3a). Then, the pulsed laser beam (la) is repeatedly reflected on the inner surface of the casing and gradually reaches the thermocouple (3b) provided on the inner surface of the casing (3).
absorbed into. The thermoelectromotive force generated in this thermocouple (3b) is proportional to the absorbed laser IB power, and by calibrating the power meter (4a) in advance, the average value of the pulsed laser output can be easily determined. can.

[発明が解決しようとする問題点] 従来のレーザ出力δIII定装置はパルスレーザを熱電
変換素子により熟的方法で測定する為、パルスレーザの
平均出力値のみしか測定できず、また熱電変換素子の応
答性は遅い為等の問題点があった。
[Problems to be Solved by the Invention] Conventional laser output δIII determination devices measure pulsed laser using a thermoelectric conversion element in a conventional manner, and therefore can only measure the average output value of the pulsed laser. There were problems such as slow response.

この発明は上記のような問題点を解決するためになされ
たもので、パルスレーザ発振時にパルス波形を観測し得
ると共に、観測用パルス信号入力よりパルスレーザ平均
出力値を高速で出力し得るレーザ出力測定装置を提供す
ることを目的とする。
This invention was made to solve the above-mentioned problems, and it provides a laser output that allows the pulse waveform to be observed during pulsed laser oscillation and that can output the pulsed laser average output value at high speed from the observation pulse signal input. The purpose is to provide a measuring device.

L問題点を解決するための手段] この発明に係るレーザ出力測定装置はパルスレーザ出力
を検知する光電変換素子と、該光電変換素子により検知
されたパルスレーザ出力のパルス波形を画像表示する画
像表示装置と、上記検知されたパルスレーザ出力を平均
化して平均出力値を出力するパルス平均化回路を備えた
ものである。
Means for Solving Problem L] The laser output measuring device according to the present invention includes a photoelectric conversion element that detects pulsed laser output, and an image display that displays an image of the pulse waveform of the pulsed laser output detected by the photoelectric conversion element. The device includes a pulse averaging circuit that averages the detected pulsed laser output and outputs an average output value.

[作用] この発明のレーザ出力測定装置によれば、応答性が高く
、しかも赤外線吸収率の高い光電変換素子をレーザセン
サとした為、瞬時にレベルが変化するレーザパルス出力
を検知でき、この検出出力を画像表示装置に映像化する
ことでレーザパルス波形を正確に観測できると共に、上
記検出出力を平均化することでパルス波形と同時にレー
ザパルス出力平均値を測定できる。
[Function] According to the laser output measuring device of the present invention, since a photoelectric conversion element with high responsiveness and high infrared absorption rate is used as a laser sensor, it is possible to detect laser pulse output whose level changes instantaneously. By visualizing the output on an image display device, the laser pulse waveform can be observed accurately, and by averaging the detection output, the average value of the laser pulse output can be measured at the same time as the pulse waveform.

し実施例] 第1図はこの発明のレーザ出力測定装置の一実施例を示
す全体構成図である0図において(1〕はレーザ発振器
、(2)は発振パルスレーザ光の一部を出力測定用に導
入する球面形の筐体(積分球) 、 (3)は積分球(
2)内面に取り付けられた光電変換素子(赤外線センサ
: Ge(Au) 、Ge(Hg) 、Ge(Gu)、
又はCdHgTe等) 、 (4)はセンサ出力を映像
化する画像表示装置、(5)はパルス出力をサンプリン
グしサンプリング出力を積分して平均化するサンプリン
グ平均化回路、 (it) l、を平均化出力を所定レ
ベルにして出力する平均出力回路、(7)はレーザ発振
電源である。
Embodiment] FIG. 1 is an overall configuration diagram showing an embodiment of the laser output measuring device of the present invention. In FIG. (3) is a spherical casing (integrating sphere) introduced for the purpose of
2) Photoelectric conversion element attached to the inner surface (infrared sensor: Ge (Au), Ge (Hg), Ge (Gu),
or CdHgTe, etc.), (4) is an image display device that visualizes the sensor output, (5) is a sampling averaging circuit that samples the pulse output, integrates and averages the sampling output, and (it) averages the l. An average output circuit (7) is a laser oscillation power supply that outputs an output at a predetermined level.

」二記構成に基づいて本実施例の動作を説明する。レー
ザ発振器(1)より発振されるパルスレーザ光の一部は
積分球(2)へ導入される。積分球(2)において、パ
ルスレーザ光は積分球内壁面で多重反射して徐々に光電
変換素子(3)に吸収される。その結果、光電変換素子
(3)はパルス変化に応じた光電流を画像表示装置(4
)へ出力する。光電流を入力した画像表示装置(4)は
光電流の変化に基づいて生成したパルス波形を画面上に
表示しパルス波形観測に供する。一方、サンプリング平
均化回路(5)は光電変換素子(3)より出力されたパ
ルス信号(第2図参照)を10Hz以上で高速サンプリ
ングを行ない、そのサンプリング出力を積分することで
パルス平均出力を生成する。このパルス平均出力はパル
ス発振電源(7)ヘフィードバック信号としても入力さ
れる。以上のように、同一の光電変換素子(3)よりパ
ルス波形情報とパルスレーザ発振を制御するフィードバ
ック信号が得られるので、パルス波形を観測しながら適
確なパルスレーザ発振制御を行なうことができる。
The operation of this embodiment will be explained based on the configuration described in Section 2. A part of the pulsed laser light emitted from the laser oscillator (1) is introduced into the integrating sphere (2). In the integrating sphere (2), the pulsed laser beam undergoes multiple reflections on the inner wall surface of the integrating sphere and is gradually absorbed by the photoelectric conversion element (3). As a result, the photoelectric conversion element (3) converts the photocurrent according to the pulse change into the image display device (4).
). The image display device (4) into which the photocurrent is input displays the pulse waveform generated based on the change in the photocurrent on the screen, and provides the pulse waveform observation. On the other hand, the sampling averaging circuit (5) performs high-speed sampling of the pulse signal (see Figure 2) output from the photoelectric conversion element (3) at 10 Hz or higher, and generates a pulse average output by integrating the sampling output. do. This pulse average output is also input as a feedback signal to the pulse oscillation power supply (7). As described above, since pulse waveform information and a feedback signal for controlling pulsed laser oscillation are obtained from the same photoelectric conversion element (3), accurate pulsed laser oscillation control can be performed while observing the pulse waveform.

[発明の効果] 以上のようにこの発明によれば、応答性の高い光電変換
素子によりパルスレーザ光を検知するようにしたので、
パルス波形を高忠実度で画像表示装置に再現し得る共に
、検知したパルス信号を平均化することで速やかにパル
ス平均出力を得ることができるので、パルス波形とパル
ス平均出力値の双方からレーザ加工に最適なパルスレー
ザの発振制御をより適確に行える効果がある。
[Effects of the Invention] As described above, according to the present invention, since pulsed laser light is detected by a highly responsive photoelectric conversion element,
The pulse waveform can be reproduced with high fidelity on an image display device, and the pulse average output can be quickly obtained by averaging the detected pulse signal, so laser processing can be performed from both the pulse waveform and the pulse average output value. This has the effect of more accurately controlling the oscillation of a pulsed laser that is optimal for use.

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

第1図はこの発明のレーザ出力測定装置の一実施例を示
す構成図、第2図はレーザパルス波形とパルス波形モニ
タ信号を示したパルス波形図、第3図は従来のレーザ出
力測定装置の構成図、第4図は従来装置におけるレーザ
パルス波形と出力モニタ信号を示した波形図である。 図において (1a)はGW・パルスレーザ光、 (2)は筐体(積分球) 、 (3)は光電変換素子、
(4)は画像表示装置、 (5)はサンプリング平均化回路、 (6)は平均化出力回路である。 なお、各図中、同一符号は同−又は相当部分を示す。 代  理  人   大  岩  増  雄第1図 第2図 第3図 第4図
Fig. 1 is a configuration diagram showing an embodiment of the laser output measuring device of the present invention, Fig. 2 is a pulse waveform diagram showing a laser pulse waveform and a pulse waveform monitor signal, and Fig. 3 is a diagram of a conventional laser output measuring device. The configuration diagram and FIG. 4 are waveform diagrams showing laser pulse waveforms and output monitor signals in a conventional device. In the figure, (1a) is the GW/pulsed laser beam, (2) is the housing (integrating sphere), (3) is the photoelectric conversion element,
(4) is an image display device, (5) is a sampling averaging circuit, and (6) is an averaging output circuit. In each figure, the same reference numerals indicate the same or corresponding parts. Agent Masuo Oiwa Figure 1 Figure 2 Figure 3 Figure 4

Claims (2)

【特許請求の範囲】[Claims] (1)導入したパルスレーザ光を多重反射させる内壁面
を有した球面状の筐体と、該筐体内に設置したパルスレ
ーザ光吸収用の光電変換素子と、該光電変換素子より出
力される光電流に基づいてレーザパルス波形を生成し表
示する画像表示装置と、上記該光電変換素子より出力さ
れるパルスレーザ出力信号を平均化して平均化出力値を
生成するパルス平均化回路とを備えたことを特徴とする
レーザ出力測定装置。
(1) A spherical housing having an inner wall surface that multiple-reflects the introduced pulsed laser light, a photoelectric conversion element for absorbing the pulsed laser light installed inside the housing, and light output from the photoelectric conversion element. An image display device that generates and displays a laser pulse waveform based on current, and a pulse averaging circuit that averages the pulsed laser output signal output from the photoelectric conversion element to generate an averaged output value. A laser output measurement device featuring:
(2)上記光電変換素子は半導体赤外線センサであるこ
とを特徴とする特許請求の範囲第1項記載のレーザ出力
測定装置。
(2) The laser output measuring device according to claim 1, wherein the photoelectric conversion element is a semiconductor infrared sensor.
JP25014386A 1986-10-21 1986-10-21 Laser output measuring apparatus Pending JPS63104389A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25014386A JPS63104389A (en) 1986-10-21 1986-10-21 Laser output measuring apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25014386A JPS63104389A (en) 1986-10-21 1986-10-21 Laser output measuring apparatus

Publications (1)

Publication Number Publication Date
JPS63104389A true JPS63104389A (en) 1988-05-09

Family

ID=17203455

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25014386A Pending JPS63104389A (en) 1986-10-21 1986-10-21 Laser output measuring apparatus

Country Status (1)

Country Link
JP (1) JPS63104389A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPWO2003034555A1 (en) * 2001-10-16 2005-02-03 株式会社片岡製作所 Pulse oscillation type solid state laser apparatus and laser processing apparatus

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPWO2003034555A1 (en) * 2001-10-16 2005-02-03 株式会社片岡製作所 Pulse oscillation type solid state laser apparatus and laser processing apparatus

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