JPS6151248B2 - - Google Patents
Info
- Publication number
- JPS6151248B2 JPS6151248B2 JP55003938A JP393880A JPS6151248B2 JP S6151248 B2 JPS6151248 B2 JP S6151248B2 JP 55003938 A JP55003938 A JP 55003938A JP 393880 A JP393880 A JP 393880A JP S6151248 B2 JPS6151248 B2 JP S6151248B2
- Authority
- JP
- Japan
- Prior art keywords
- photoelectric converter
- laser
- capacitor
- energy
- integrating circuit
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J1/00—Photometry, e.g. photographic exposure meter
- G01J1/42—Photometry, e.g. photographic exposure meter using electric radiation detectors
- G01J1/4257—Photometry, e.g. photographic exposure meter using electric radiation detectors applied to monitoring the characteristics of a beam, e.g. laser beam, headlamp beam
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- General Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Photometry And Measurement Of Optical Pulse Characteristics (AREA)
- Lasers (AREA)
Description
【発明の詳細な説明】
本発明はパルスレーザのパワーモニター装置に
係わる。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a pulsed laser power monitoring device.
パルスレーザ、特にパルス幅が1〜50nsec程
度のパルス幅の狭いレーザパルスは大気汚染観測
(レーザレーダ)やプラズマ計測など種々の計測
に用いられているが、測定に使用されるパルスそ
のもののエネルギーをモニターする方法には、従
来理想的なものがなかつた、特にビーム径が大き
く、ビーム断面のエネルギー分布が不均一な場合
には種々の困難が伴なつていた。一つの方法とし
ては計測に用いるパルスの前後のパルスのエネル
ギーをカロリーメータで測定し、計測に供される
レーザパルスのパワーを推定することができる。
しかし本方法では、レーザの繰返し安定度が悪い
場合には、計測に用いるパルスそのもののエネル
ギーを知ることは困難になる。その他非線形光学
現象を利用するものなど、いくつかの方法がある
がいずれにしても装置が大がかりで高価なもので
あつたり、精度が悪いものであつたりし、理想的
な方法はなかつた。 Pulsed lasers, especially narrow laser pulses with a pulse width of about 1 to 50 ns, are used for various measurements such as air pollution observation (laser radar) and plasma measurement, but the energy of the pulse itself used for measurement is Conventionally, there has been no ideal monitoring method, especially when the beam diameter is large and the energy distribution in the beam cross section is non-uniform, resulting in various difficulties. One method is to measure the energy of the pulses before and after the pulse used for measurement with a calorimeter to estimate the power of the laser pulse used for measurement.
However, with this method, if the repetition stability of the laser is poor, it becomes difficult to know the energy of the pulse itself used for measurement. There are several other methods, including those that make use of nonlinear optical phenomena, but in either case, the equipment is large and expensive, or the accuracy is poor, so there is no ideal method.
本発明は上記欠点を除き、比較的簡単な装置で
狭いパルス幅で、ビーム径が大きく、かつビーム
パターンが不均一なレーザパルスのエネルギー値
を測定し、かつ、レーザパルス中のエネルギーの
大部分は計測等他の用途に利用できる新規な方法
を提供するものである。 The present invention eliminates the above drawbacks, measures the energy value of a laser pulse with a narrow pulse width, a large beam diameter, and an uneven beam pattern using a relatively simple device, and measures most of the energy in the laser pulse. This provides a new method that can be used for other purposes such as measurement.
本発明によるパワーモニター装置はレーザパル
スエネルギーのわずかな部分を分離するビームス
プリツタと、分離されたレーザパルス光を空間的
に散乱させる拡散板と、散乱された光の一部分を
受光する高速応答の光電変換器と、光電変換器の
出力電流を積分する抵抗とコンデンサとからなる
積分回路と該積分回路と上記光電変換器の間を高
速に接断するスイツチ回路と、上記コンデンサに
充電された電圧を検出する高入力インピーダンス
の電圧検出回路とからなる。 The power monitoring device according to the present invention includes a beam splitter that separates a small portion of laser pulse energy, a diffuser plate that spatially scatters the separated laser pulse light, and a high-speed response sensor that receives a portion of the scattered light. A photoelectric converter, an integrating circuit consisting of a resistor and a capacitor that integrates the output current of the photoelectric converter, a switch circuit that quickly connects and disconnects between the integrating circuit and the photoelectric converter, and a voltage charged in the capacitor. It consists of a high input impedance voltage detection circuit that detects the
本発明によれば、パルスレーザ光のわずかな部
分を平均化して光電変換器に入射することがで
き、光電変換器の出力はコンデンサに充電されそ
の充電電圧に測定するため、もとのパルスレーザ
エネルギーのある一定の割合のエネルギーを正確
に測定することができる。 According to the present invention, a small portion of the pulsed laser light can be averaged and made incident on the photoelectric converter, and the output of the photoelectric converter is charged to the capacitor and measured at its charging voltage, so that the original pulsed laser beam is It is possible to accurately measure the energy of a certain percentage of energy.
図面を用いて本発明の一実施例を詳細に説明す
る。 An embodiment of the present invention will be described in detail using the drawings.
図において、Qスイツチルビーレーザなどのレ
ーザパルスビーム1は、ビームスプリツタ2によ
つて一部分が分離される。ビームスプリツタ2の
例として、単に無反射コーテイングされたガラス
板を使用することができる。もちろんこのビーム
スプリツタ2はガラスを透過する波長のレーザの
パワモニターにしか使用できないが、例えばルビ
ーレーザの場合には通常の光学ガラスに2層の無
反射コーテイングを施したものによつて0.5%程
度の反射率で、吸収が無視できるビームスプリツ
タとなる。さてビームスプリツタ2で取り出され
た光は、すりガラス、オパールガラスなどからな
る拡散板3によつて空間的に散乱され、散乱され
た光4の一部分はPINダイオードなどの光電変換
器5に入射する。光電変換器5としてPINダイオ
ードを用いる場合にはバイアス電源6が用いられ
る。光電変換器5の出力は抵抗7、コンデンサ8
からなる積分回路に入るが、該積分回路は当業者
にはよく知られているFETまたはダイオードブ
リツジを用いたアナログスイツチなどの高速スイ
ツチ9によつて、光電変換器5の出力がある時間
だけ電気的に接続されている。コンデンサ8に充
電された電圧は当業者にはよく知られているよう
にFETなどを用いた高入力インピーダンスの電
圧検出回路10によつて検出される。 In the figure, a laser pulse beam 1, such as a Q-switched chilby laser, is partially separated by a beam splitter 2. As shown in FIG. As an example of beam splitter 2, it is possible to simply use a glass plate with an anti-reflection coating. Of course, this beam splitter 2 can only be used to monitor the power of a laser with a wavelength that passes through glass, but for example, in the case of a ruby laser, it is made of ordinary optical glass with two layers of anti-reflection coating. It becomes a beam splitter with a moderate reflectance and negligible absorption. Now, the light extracted by the beam splitter 2 is spatially scattered by a diffuser plate 3 made of frosted glass, opal glass, etc., and a portion of the scattered light 4 enters a photoelectric converter 5 such as a PIN diode. . When using a PIN diode as the photoelectric converter 5, a bias power supply 6 is used. The output of the photoelectric converter 5 is a resistor 7 and a capacitor 8
The output of the photoelectric converter 5 is controlled by a high-speed switch 9, such as an analog switch using a FET or a diode bridge, which is well known to those skilled in the art. electrically connected. The voltage charged in the capacitor 8 is detected by a high input impedance voltage detection circuit 10 using an FET or the like, as is well known to those skilled in the art.
ビームスプリツタによつて取り出した光によつ
てレーザパルスエネルギーをモニタするため、残
りのレーザパルスエネルギーは計測等、他の用途
に用いることができ、また、計測等に使用される
レーザパルスそのもののエネルギーをモニターす
ることができる。また拡散板3の使用によりビー
ム1の直径が光電変換器5の受光面の径より大き
くても、またビーム1の空間的エネルギー分布が
不均一であつても、正確に一定の割合の光を光電
変換器5に入射することができ、レーザビーム1
のエネルギーを正確にモニターすることができ
る。また抵抗7とコンデンサ8の積分回路によ
り、レーザパルス幅にほとんど影響を受けずにエ
ネルギーを測定することができる。さらに高速ス
イツチ9と高入力インピーダンスの電圧検出回路
10により、コンデンサ8の充電電圧を正確に測
定することができる。 Since the laser pulse energy is monitored by the light extracted by the beam splitter, the remaining laser pulse energy can be used for other purposes such as measurement. Energy can be monitored. Furthermore, by using the diffuser plate 3, even if the diameter of the beam 1 is larger than the diameter of the light-receiving surface of the photoelectric converter 5, or even if the spatial energy distribution of the beam 1 is uneven, a certain proportion of light can be accurately transmitted. The laser beam 1 can be incident on the photoelectric converter 5.
energy can be accurately monitored. Furthermore, the integrating circuit including the resistor 7 and the capacitor 8 allows the energy to be measured almost unaffected by the laser pulse width. Furthermore, the charging voltage of the capacitor 8 can be accurately measured by the high-speed switch 9 and the high input impedance voltage detection circuit 10.
本発明は上記実施例に限定されるものではな
く、対象のレーザはパワモニター、拡散板、光電
変換器が有効に機能する波長域にあれば、どんな
パルスレーザであつてもかまわない。またビーム
スプリツタ、拡散板の材質は上記に限定されるも
のではない。光電変換器は光電管、光電子増倍管
などであつてもよく、また高速スイツチ、高入力
インピーダンスの電圧検出回路は上記以外の他の
方法によるものであつてもかまわない。 The present invention is not limited to the above embodiments, and the target laser may be any pulsed laser as long as it is within a wavelength range in which the power monitor, diffuser plate, and photoelectric converter function effectively. Furthermore, the materials of the beam splitter and the diffuser plate are not limited to those mentioned above. The photoelectric converter may be a phototube, a photomultiplier tube, etc., and the high speed switch and high input impedance voltage detection circuit may be of other methods than those described above.
図は本発明の一実施例を示す回路図である。
1……パルスレーザビーム、2……ビームスプ
リツタ、3……拡散板、5……光電変換器、7…
…抵抗、8……コンデンサ、9……高速スイツ
チ、10……高入力インピーダンスの電圧検出回
路。
The figure is a circuit diagram showing one embodiment of the present invention. 1... Pulse laser beam, 2... Beam splitter, 3... Diffusion plate, 5... Photoelectric converter, 7...
...Resistor, 8...Capacitor, 9...High speed switch, 10...High input impedance voltage detection circuit.
Claims (1)
ームスプリツタと、上記分離された光を散乱させ
る拡散板と、上記散乱された光の一部分を受光す
る光電変換器と、上記光電変換器の出力電流を積
分する抵抗とコンデンサとからなる積分回路と、
上記積分回路と上記光電変換器の間を高速に接断
する高速スイツチと、上記積分回路のコンデンサ
に充電された電圧を検出する高入力インピーダン
スの電圧検出回路とを有することを特徴とするエ
ネルギーモニター装置。1. A beam splitter that separates a portion of the pulsed laser beam, a diffuser plate that scatters the separated light, a photoelectric converter that receives a portion of the scattered light, and an output of the photoelectric converter. an integrating circuit consisting of a resistor and a capacitor that integrates current;
An energy monitor comprising: a high-speed switch that connects and disconnects the integrating circuit and the photoelectric converter at high speed; and a high-input impedance voltage detection circuit that detects the voltage charged in the capacitor of the integrating circuit. Device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP393880A JPS56101524A (en) | 1980-01-17 | 1980-01-17 | Monitoring device for laser energy |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP393880A JPS56101524A (en) | 1980-01-17 | 1980-01-17 | Monitoring device for laser energy |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56101524A JPS56101524A (en) | 1981-08-14 |
| JPS6151248B2 true JPS6151248B2 (en) | 1986-11-07 |
Family
ID=11571064
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP393880A Granted JPS56101524A (en) | 1980-01-17 | 1980-01-17 | Monitoring device for laser energy |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS56101524A (en) |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60183834U (en) * | 1984-05-16 | 1985-12-06 | 長田電機工業株式会社 | laser output detector |
| JPS6269577A (en) * | 1985-09-21 | 1987-03-30 | Ushio Inc | Output control device of pulse discharge type laser |
| JPH02107931A (en) * | 1988-10-17 | 1990-04-19 | Fuji Electric Co Ltd | Optical pulse measuring apparatus |
| JPH04131961U (en) * | 1991-05-28 | 1992-12-04 | 日本電気株式会社 | Monitor structure in solid-state laser equipment |
| JP4987123B2 (en) | 2008-05-26 | 2012-07-25 | 三菱電機株式会社 | Ventilation equipment |
| GB2628146A (en) * | 2023-03-16 | 2024-09-18 | Bae Systems Plc | Method and apparatus for characterizing an incoming electromagnetic energy beam |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5497082A (en) * | 1978-01-17 | 1979-07-31 | Mitsubishi Electric Corp | Intensity detector of laser beam |
-
1980
- 1980-01-17 JP JP393880A patent/JPS56101524A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56101524A (en) | 1981-08-14 |
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