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JPS6317236B2 - - Google Patents

Info

Publication number
JPS6317236B2
JPS6317236B2 JP55151251A JP15125180A JPS6317236B2 JP S6317236 B2 JPS6317236 B2 JP S6317236B2 JP 55151251 A JP55151251 A JP 55151251A JP 15125180 A JP15125180 A JP 15125180A JP S6317236 B2 JPS6317236 B2 JP S6317236B2
Authority
JP
Japan
Prior art keywords
switch
pulse
acousto
optic
frequency signal
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
Application number
JP55151251A
Other languages
Japanese (ja)
Other versions
JPS5775482A (en
Inventor
Noriaki Sekiguchi
Reiji Machida
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.)
NEC Corp
Original Assignee
Nippon Electric Co 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP15125180A priority Critical patent/JPS5775482A/en
Publication of JPS5775482A publication Critical patent/JPS5775482A/en
Publication of JPS6317236B2 publication Critical patent/JPS6317236B2/ja
Granted 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
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/11Mode locking; Q-switching; Other giant-pulse techniques, e.g. cavity dumping
    • H01S3/1123Q-switching
    • H01S3/117Q-switching using intracavity acousto-optic devices
    • 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
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/106Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity
    • H01S3/1068Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity using an acousto-optical device
    • 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
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/13Stabilisation of laser output parameters, e.g. frequency or amplitude
    • H01S3/1306Stabilisation of the amplitude

Landscapes

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

Description

【発明の詳細な説明】 この発明はQスイツチレーザ装置に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a Q-switch laser device.

Qスイツチは固体レーザの発振を幅の狭い尖頭
出力値の極めて高いパルスに変換する技術として
知られており、レーザ光の精密加工、レーザレー
ダ、非線形光学などへの応用に不可欠な技術とな
つている。Qスイツチの方法として、機械的方
法、電気光学的方法、音響光学的方法、光化学的
方法どがあり、実現される繰返し周波数、スイツ
チ速度、動損失の大きさ、構成の容易さなどにそ
れぞれ特徴を有しているため、用途によつて最も
適切な使いわけがなされている。
Q-switches are known as a technology that converts the oscillation of solid-state lasers into narrow pulses with extremely high peak output values, and are an essential technology for applications such as precision processing of laser light, laser radar, and nonlinear optics. ing. Q-switching methods include mechanical, electro-optical, acousto-optic, and photochemical methods, each with its own characteristics in terms of repetition frequency, switching speed, magnitude of dynamic loss, ease of construction, etc. Because of this, it can be used most appropriately depending on the purpose.

近年、応用例の飛躍的に増大している精密加工
への応用を考える場合、加工速度をあげ、処理時
間を短縮し、生産コストの低減が求められ、上述
の方法のうち音響光学的方法が最も実用的で広く
使用されている。
When considering the application of precision machining, which has been increasing dramatically in recent years, there is a need to increase machining speed, shorten processing time, and reduce production costs. The most practical and widely used.

音響光学的方法は超音波Qスイツチとも呼ば
れ、アール・ビー・チエスラー(R.B.Chesler)
らによつて提出され雑誌「プロシーデイングス・
オゴ・アイ・イー・イー・イー(Proceedings
of the IEEE)」58巻.12号(1970年12月)の
1899頁に詳細に記述されているとうり溶融石英板
中の進行縦波超音波による位相回折格子を光変調
器として利用しているものである。通常、位相回
折格子は溶融石英板に接着されたXカツト水晶板
などのトランスデユーサ(電気−音響変換子)に
40MHz程度の高周波電界を印加することにより形
成され、Qスイツチはこの高周波電界をパルス的
に変調することにより実現されている。このQス
イツチ法では、Qスイツチパルスの繰返し周波数
とオン・オフの制御は高周波電界を変調する変調
回路により純電気的に行われるため、繰返し周波
数が高く、幅の狭いQスイツチパルスが得られ
る。
The acousto-optic method is also called an ultrasonic Q-switch and is developed by RBChesler.
Submitted by et al. and published in the journal ``Proceedings
Proceedings
of the IEEE)” Volume 58. No. 12 (December 1970)
As described in detail on page 1899, a phase diffraction grating created by traveling longitudinal ultrasonic waves in a fused silica plate is used as an optical modulator. Typically, a phase grating is attached to a transducer (electro-acoustic transducer) such as an X-cut quartz plate glued to a fused silica plate.
It is formed by applying a high frequency electric field of about 40 MHz, and the Q switch is realized by modulating this high frequency electric field in a pulse manner. In this Q-switch method, the repetition frequency and on/off control of the Q-switch pulse is performed purely electrically by a modulation circuit that modulates a high-frequency electric field, so that a Q-switch pulse with a high repetition frequency and a narrow width can be obtained.

例えば、連続励起の固体レーザであるNd:
YAGレーザに応用すると、繰返し周波数は10数
KHz、パルス幅約100nsecが得られる。
For example, Nd, a continuously pumped solid-state laser:
When applied to a YAG laser, a repetition frequency of 10 KHz and a pulse width of about 100 ns can be obtained.

しかしながら、この超音波Qスイツチによつて
高い繰返しのQスイツチパルスを得る場合、最大
の欠点は繰返し周波数と共に尖頭出力値が減少す
ることにあり、Nd:YAGレーザの場合、Nd:
YAG結晶の螢光寿命が約230μsecであるために
2KHz位までの繰返し周波数では尖頭値が一定に
維持され、その後は繰返し周波数に比例して尖頭
値は減少する。
However, when obtaining high-repetition Q-switch pulses using this ultrasonic Q-switch, the biggest drawback is that the peak output value decreases with the repetition frequency.
Because the fluorescence lifetime of YAG crystal is approximately 230μsec,
The peak value remains constant at a repetition frequency up to about 2KHz, and thereafter decreases in proportion to the repetition frequency.

精密加工への応用、例えば薄膜抵抗トリミング
などへ応用しようとする場合、繰返し周波数が
2KHz以上になるとレーザ光をオフ状態からオン
状態にした第1発目のQスイツチパルスの尖頭値
が大きく、この個所だけ深く大きな加工軌跡を残
し基板の破損などをひき起こす危険性がある。
When applying to precision machining, such as thin film resistor trimming, the repetition frequency is
When the frequency exceeds 2KHz, the peak value of the first Q-switch pulse that turns the laser beam from the OFF state to the ON state is large, leaving a deep and large machining trajectory in this area, which may cause damage to the board.

この発明の目的は音響光学的Qスイツチ法にお
いて、印加する高周波電界の変調パルス幅をQス
イツチ発生時に徐徐に広げ、尖頭パルス幅を一定
に維持しうるQスイツチレーザ装置を提供するこ
とである。
An object of the present invention is to provide a Q-switch laser device that can gradually widen the modulation pulse width of an applied high-frequency electric field when a Q-switch occurs and maintain a constant peak pulse width in an acousto-optic Q-switch method. .

次にこの発明について図面を参照して説明す
る。
Next, the present invention will be explained with reference to the drawings.

第1図はこの発明の一実施例の概略構成を、ま
た第2図は信号波形およびQスイツチパルス波形
を模型的に表わしたものである。
FIG. 1 shows a schematic configuration of an embodiment of the present invention, and FIG. 2 schematically shows signal waveforms and Q switch pulse waveforms.

固体レーザ物質11は励起光源12と集光器1
3により励起され、反射鏡14,15から構成さ
れるレーザ共振器中に置かれている。一方このレ
ーザ共振器中に置かれレーザ発振をパルス化する
ための音響光学的光変調器16は溶融石英板で作
られた超音波セル17に超音波位相回折格子18
を形成する電気音響変換子19から構成されてい
る。この電気音響変換子19には高周波ドライバ
20からの高周波信号が印加されている。高周波
ドライバ20はVHF例えば40MHzで発振する発
振器21とパルス変調回路22、変調信号発生回
路23、高周波増幅回路24から構成され、変調
信号発生回路23はQスイツチ制御外部信号25
により制御されている。
A solid-state laser material 11 includes an excitation light source 12 and a condenser 1
3 and placed in a laser resonator composed of reflecting mirrors 14 and 15. On the other hand, an acousto-optic light modulator 16 placed in this laser resonator for pulsating laser oscillation has an ultrasonic phase diffraction grating 18 in an ultrasonic cell 17 made of a fused silica plate.
It is composed of an electroacoustic transducer 19 that forms a. A high frequency signal from a high frequency driver 20 is applied to this electroacoustic transducer 19 . The high frequency driver 20 is composed of an oscillator 21 that oscillates at VHF, for example, 40 MHz, a pulse modulation circuit 22, a modulation signal generation circuit 23, and a high frequency amplification circuit 24.
controlled by.

次にQスイツチ制御外部信号25、変調信号発
生回路23、およびQスイツチパルス波形の関係
を図により説明する。第2図の横軸は時間を、縦
軸は信号強度を相対的に表わすものである。
Next, the relationship among the Q-switch control external signal 25, the modulation signal generation circuit 23, and the Q-switch pulse waveform will be explained using the diagram. In FIG. 2, the horizontal axis represents time, and the vertical axis represents relative signal strength.

Qスイツチ制御外部信号25の波形101はQ
スイツチ発生時間だけローレベルに維持される。
これにより変調信号発生回路23はあらかじめ定
められた周期とパルス幅で波形104の様に変化
する。波形102は従来技術による変調信号波形
であり、パルス幅Tが6μs、周期数ms以下で使
用されるのが普通である。もし周期が0.5ms以
下であると得られるQスイツチパルス波形103
は最初の1パルス目だけ尖頭値の高いパルス発振
となつてしまう、なぜならば変調信号波形102
がハイレベルにある間はレーザ発振は抑止されエ
ネルギーが蓄積されるが、最初のパルスに対して
のみハイレベルの時間が長く、完全に飽和される
まで蓄積されるからである。Qスイツチパルス波
形103の第1パルスの尖頭値は第2パルス以降
に比較し容易に10倍以上となり、精密加工などの
応用に対して重大な影響を与えてしまう。この発
明による変調信号波形104は従来波形102と
異なり立上り時のパルス幅T′が一定でなく、Q
スイツチ制御外部信号波形101がローレベルに
なつた時から徐々に広がり数パルス後に一定値約
6μsに制御されている。このためにQスイツチパ
ルス波形105は最初の数パルスだけ、尖頭値が
除々に立上ることになる。この理由は変調信号波
形104のパルス幅が狭いと立上つたQスイツチ
発振に対して損失を与えて、あたかも光シヤツタ
ーが完全に開き切れない状態を等価的に形成する
からである。これによつて従来の第1Qスイツチ
パルスの尖頭値が異常に高くなることは抑止さ
れ、ほぼ尖頭値の等しいQスイツチパルス列が得
られることになる。
The waveform 101 of the Q switch control external signal 25 is Q
It is maintained at a low level for the time the switch occurs.
As a result, the modulation signal generation circuit 23 changes like a waveform 104 with a predetermined period and pulse width. The waveform 102 is a modulation signal waveform according to the prior art, and is normally used with a pulse width T of 6 μs and a cycle number of ms or less. Q switch pulse waveform 103 obtained if the period is less than 0.5ms
becomes a pulse oscillation with a high peak value only for the first pulse, because the modulation signal waveform 102
While laser oscillation is at a high level, laser oscillation is suppressed and energy is accumulated, but only the first pulse is at a high level for a long time, and the energy is accumulated until it is completely saturated. The peak value of the first pulse of the Q-switch pulse waveform 103 is easily 10 times or more compared to the second and subsequent pulses, which has a serious impact on applications such as precision machining. The modulated signal waveform 104 according to the present invention differs from the conventional waveform 102 in that the pulse width T' at the rising edge is not constant, and the Q
From the time the switch control external signal waveform 101 becomes low level, it gradually spreads to a constant value of approximately
Controlled to 6μs. For this reason, the peak value of the Q switch pulse waveform 105 gradually rises for the first few pulses. The reason for this is that if the pulse width of the modulation signal waveform 104 is narrow, a loss is caused to the Q-switch oscillation that has started, equivalently creating a state in which the optical shutter cannot be opened completely. As a result, the peak value of the conventional first Q switch pulse is prevented from becoming abnormally high, and a Q switch pulse train having approximately the same peak value can be obtained.

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

第1図はこの発明の実施例の概略構成を示すブ
ロツク図、第2図は信号波形およびQスイツチパ
ルス波形を模型的に表わす。11は固体レーザ物
質、12は励起光源、13は集光器、14,15
はレーザ共振器を構成する反射鏡、16は音響光
学的光変調器、17は超音波セル、18は超音波
位相回折格子、19は電気音響変換子、20は高
周波ドライバ、21はVHF発振器、22はパル
ス変調回路、23は変調信号発生回路、24は高
周波増幅回路、25はQスイツチ制御外部信号、
101はQスイツチ制御外部信号波形、102は
従来技術による変調信号波形、103は従来技術
によるQスイツチパルス波形、104はこの発明
による変調信号波形、105はこの発明によつて
得られるQスイツチパルス波形である。
FIG. 1 is a block diagram showing a schematic configuration of an embodiment of the present invention, and FIG. 2 schematically shows signal waveforms and Q-switch pulse waveforms. 11 is a solid-state laser material, 12 is an excitation light source, 13 is a condenser, 14, 15
16 is an acousto-optic light modulator, 17 is an ultrasonic cell, 18 is an ultrasonic phase diffraction grating, 19 is an electroacoustic transducer, 20 is a high frequency driver, 21 is a VHF oscillator, 22 is a pulse modulation circuit, 23 is a modulation signal generation circuit, 24 is a high frequency amplification circuit, 25 is a Q switch control external signal,
101 is a Q switch control external signal waveform, 102 is a modulation signal waveform according to the prior art, 103 is a Q switch pulse waveform according to the prior art, 104 is a modulation signal waveform according to the present invention, and 105 is a Q switch pulse waveform obtained by the present invention. It is.

Claims (1)

【特許請求の範囲】[Claims] 1 連続励起固体レーザを音響光学的Qスイツチ
法によりQスイツチパルス発振させるQスイツチ
レーザ装置において、音響光学的Qスイツチ素子
と、前記音響光学的Qスイツチ素子に位相回析格
子を形成するに十分な周波数の高周波信号を発生
する高周波信号源と、所定周期を有しパルス幅が
次第に増大して一定幅に達するパルス信号で前記
高周波信号を変調し前記パルス幅に応じて前記高
周波信号が遮断される駆動信号を発生する変調回
路と、前記駆動信号を前記音響光学的Qスイツチ
素子に供給する手段とを有し、Qスイツチパルス
の第1パルスの尖頭値を抑制し、尖頭値のほぼ一
定なQスイツチパルス列を得ることを特徴とする
Qスイツチレーザ装置。
1. In a Q-switch laser device in which a continuously pumped solid-state laser is oscillated with Q-switch pulses by an acousto-optic Q-switch method, an acousto-optic Q-switch element and an acousto-optic Q-switch element with a sufficient amount to form a phase diffraction grating are provided. a high-frequency signal source that generates a high-frequency signal at a certain frequency; the high-frequency signal is modulated with a pulse signal having a predetermined period and a pulse width that gradually increases until it reaches a certain width; and the high-frequency signal is cut off according to the pulse width. The modulation circuit includes a modulation circuit that generates a drive signal, and means for supplying the drive signal to the acousto-optic Q-switch element, suppresses the peak value of the first pulse of the Q-switch pulse, and maintains the peak value substantially constant. A Q-switch laser device characterized in that it obtains a Q-switch pulse train.
JP15125180A 1980-10-28 1980-10-28 Q switch laser device Granted JPS5775482A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15125180A JPS5775482A (en) 1980-10-28 1980-10-28 Q switch laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15125180A JPS5775482A (en) 1980-10-28 1980-10-28 Q switch laser device

Publications (2)

Publication Number Publication Date
JPS5775482A JPS5775482A (en) 1982-05-12
JPS6317236B2 true JPS6317236B2 (en) 1988-04-13

Family

ID=15514568

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15125180A Granted JPS5775482A (en) 1980-10-28 1980-10-28 Q switch laser device

Country Status (1)

Country Link
JP (1) JPS5775482A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02277859A (en) * 1989-04-12 1990-11-14 Atago:Kk Lining sheet of framework for concrete

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4845719A (en) * 1986-03-28 1989-07-04 Hamamatsu Photonics K.K. Ultrasonic laser modulator
JP2673303B2 (en) * 1988-04-22 1997-11-05 三菱電機株式会社 Negative branch unstable laser cavity

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5287391A (en) * 1976-01-16 1977-07-21 Nec Corp Q switch laser equipment

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02277859A (en) * 1989-04-12 1990-11-14 Atago:Kk Lining sheet of framework for concrete

Also Published As

Publication number Publication date
JPS5775482A (en) 1982-05-12

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