JPH0245984A - Pulse laser oscillator - Google Patents
Pulse laser oscillatorInfo
- Publication number
- JPH0245984A JPH0245984A JP19615688A JP19615688A JPH0245984A JP H0245984 A JPH0245984 A JP H0245984A JP 19615688 A JP19615688 A JP 19615688A JP 19615688 A JP19615688 A JP 19615688A JP H0245984 A JPH0245984 A JP H0245984A
- Authority
- JP
- Japan
- Prior art keywords
- parallel
- discharge
- laser oscillator
- main electrode
- main
- 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
Links
- 239000003990 capacitor Substances 0.000 claims abstract description 26
- 230000006835 compression Effects 0.000 claims description 4
- 238000007906 compression Methods 0.000 claims description 4
- 230000010355 oscillation Effects 0.000 abstract description 4
- 238000010586 diagram Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 238000000354 decomposition reaction Methods 0.000 description 2
- 230000006866 deterioration Effects 0.000 description 2
- 230000005284 excitation Effects 0.000 description 2
- 238000012423 maintenance Methods 0.000 description 1
- 230000002123 temporal effect Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/09—Processes or apparatus for excitation, e.g. pumping
- H01S3/097—Processes or apparatus for excitation, e.g. pumping by gas discharge of a gas laser
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Lasers (AREA)
Abstract
Description
【発明の詳細な説明】 (発明の目的〕 (産業上の利用分野) 本発明はパルスレーザ発振器に関する。[Detailed description of the invention] (Purpose of the invention) (Industrial application field) The present invention relates to a pulsed laser oscillator.
(従来の技術)
従来のパルスレーザ発振器の放電部の構造(特開昭61
−90484号公報参照〉を示す第4図において、円筒
状の容器1内の大小の随円状断面を形成したダクト3内
には、下部にレーザガス5を時計方向に巡環させる送風
機4と熱交換器6が設けられ、中央上部外壁には、一端
が容器]の外側の電源16の一側に接続された主電極7
と主電極8が上下に対向して設けられ、この主電極7の
左右の外壁には、上下に一端が対向して予備電離ピン9
^、10^。(Prior art) Structure of the discharge section of a conventional pulsed laser oscillator (Unexamined Japanese Patent Publication No. 1983
In FIG. 4, which shows a duct 3 with circular cross-sections of various sizes, inside a cylindrical container 1, there is a blower 4 that circulates the laser gas 5 clockwise in the lower part, and a blower 4 that circulates the laser gas 5 in a clockwise direction. An exchanger 6 is provided, and a main electrode 7 is provided on the central upper outer wall, one end of which is connected to one side of a power source 16 outside the container.
A main electrode 8 is provided facing each other vertically, and pre-ionization pins 9 are provided on the left and right outer walls of this main electrode 7 with one end facing each other vertically.
^, 10^.
と9B、 10Bが取付られ、この予備電離ピン9A、
10^と9B、 10Bの他端は、ピーキングコンデン
サ11^、12Aと11B、 1213の一側が接続さ
れ、上側のピーキングコンデンサ11^、11Bの他側
は主電極7と電源16の一側に、下側のピーキングコン
デンサ12A、 12Bの他側は主電極8と電源16の
他側にそれぞれ接続されている。and 9B, 10B are attached, and this pre-ionization pin 9A,
The other ends of 10^, 9B, and 10B are connected to one side of peaking capacitors 11^, 12A, 11B, and 1213, and the other side of the upper peaking capacitors 11^ and 11B is connected to one side of the main electrode 7 and power source 16. The other sides of the lower peaking capacitors 12A and 12B are connected to the main electrode 8 and the other side of the power source 16, respectively.
ここで、主電極7,8間の紙面垂直方向のレーザ光は、
予備電離ピン9A、9BとIOA、 1o13間で発生
する紫外線が主電極7,8間のレーザガス2を電離して
グロー放電14させることで放出される。Here, the laser beam in the direction perpendicular to the paper between the main electrodes 7 and 8 is
The ultraviolet rays generated between the preliminary ionization pins 9A, 9B and the IOA, 1o13 are emitted by ionizing the laser gas 2 between the main electrodes 7, 8 and causing a glow discharge 14.
第5図は、第4図の構造のパルスレーザ発振器の回路図
で、図示しない元型源からの電力はまず電源16の電源
側コンデンサ17を充電しスイッチ18の投入により、
パルス変圧器19で昇圧されて二次側の磁気パルス圧縮
(以下、MPCという。)1段目のコンデンサ20を充
電する。そして、このコンデンサ20の充電電圧がある
設定値になると、負荷側に直列に接続されたMP01段
目の可飽和リアクトル21が急速に飽和して急峻な電圧
パルスをMP02段目のコンデンサ22に送り込み、同
様にして更に短い幅の電圧パルスが負荷側の主電極7゜
8に並列に接続されたピーキングコンデンサ11A。FIG. 5 is a circuit diagram of a pulsed laser oscillator having the structure shown in FIG.
It is boosted by a pulse transformer 19 and charges a capacitor 20 in the first stage of magnetic pulse compression (hereinafter referred to as MPC) on the secondary side. When the charging voltage of this capacitor 20 reaches a certain set value, the saturable reactor 21 of the first stage of MP0 connected in series on the load side rapidly saturates and sends a steep voltage pulse to the capacitor 22 of the second stage of MP0. , and a peaking capacitor 11A in which a voltage pulse with a shorter width is similarly connected in parallel to the main electrode 7.8 on the load side.
11Bと12A、 12Bを充電する。Charge 11B, 12A, and 12B.
すると、このピーキングコンデンサ11A、 11Bと
12A、 12Bの放電で、予備電離ピン9A、10^
間と98 。Then, due to the discharge of these peaking capacitors 11A, 11B and 12A, 12B, the pre-ionization pins 9A, 10^
Between and 98.
10B間で予備電離放電13A、13Bが発生して主電
極7.8間のレーザガスが電離され、主電極7,8間の
電圧が放電開始電圧になるとグロー放電14となる。Preliminary ionization discharges 13A and 13B occur between main electrodes 7 and 10B, and the laser gas between main electrodes 7 and 8 is ionized, and when the voltage between main electrodes 7 and 8 reaches a discharge starting voltage, a glow discharge 14 occurs.
第6図はこれらの放電の時間的変化を示したもので、主
電極7.8の間隙より狭い予備電極9A 。FIG. 6 shows the temporal changes in these discharges, and shows the gap between the preliminary electrodes 9A and 7.8, which is narrower than the gap between the main electrodes 7.8.
9BとIOA、 108間の予備電離放電25は、放電
部の電圧波形24のなかの低い時点で始まり、主放電開
始電圧26の後は、グロー維持電圧に下がり、レーザ光
28は主放電電流27が流れ終った時点29以後に発生
する。The pre-ionization discharge 25 between 9B and IOA, 108 starts at a low point in the voltage waveform 24 of the discharge section, and after the main discharge starting voltage 26, the voltage drops to the glow maintenance voltage, and the laser beam 28 reaches the main discharge current 27. This occurs after the time point 29 when the flow ends.
ところが、予備電離放電25が低い時点で始まると、主
放電開始時26までの時間が長くなり、紫外線が出てし
まって主放電開始時26には出なくなるだけでなく、予
備電離ピンの損傷も増え、レーザガス2の分解が進んで
レーザ装置の寿命も短かくなる。However, if the pre-ionization discharge 25 starts at a low point, the time until the main discharge starts 26 will be longer, and not only will ultraviolet rays be emitted and not emit at the main discharge start 26, but the pre-ionization pin will be damaged. This increases the decomposition of the laser gas 2 and shortens the life of the laser device.
又、予備電離放電25が低い時点で始まると、その放電
開始電圧の少しの差がそのまま放電開始時間のばらつき
となり、その結果主放電開始時26もばらつく。Furthermore, when the preliminary ionization discharge 25 starts at a low point, a slight difference in the discharge starting voltage directly causes a variation in the discharge starting time, and as a result, the main discharge starting time 26 also varies.
更に、第6図に)のように、主放電27の終了時29以
後も主放電電圧24が残るので、繰り返し運転するレー
ザ発振器ではこの電圧の高低で最初のパルス放電と次の
放電との回路条件が違い励起条件が違ってきて、上記同
様レーザ光の出力時間のばらつきとなる。これは出力時
間が重要なパルスレーザでは問題となる。Furthermore, as shown in Fig. 6), the main discharge voltage 24 remains even after the end of the main discharge 27 (29), so in a laser oscillator that is repeatedly operated, the circuit between the first pulse discharge and the next discharge is determined by the level of this voltage. The conditions are different, the excitation conditions are different, and as above, the output time of the laser beam varies. This becomes a problem in pulsed lasers where output time is important.
そこで本発明の目的は、レーザ発振の出力時間のばらつ
きがなく、寿命を延ばすことのできるパルスレーザ発振
器を1qることである。Therefore, an object of the present invention is to provide a pulsed laser oscillator that has no variation in laser oscillation output time and can extend its life.
(課題を解決するための手段と作用)
本発明は、対向して配置された主電極近傍の予備電離ピ
ンに直列にピーキングコンデンサが接続された放電部に
磁気圧縮回路を介してパルス電圧を印加して放電させる
パルスレーザ発振器において、予備電離ピン間と主電極
間に並列にインピーダンスを接続し、又は予備電離ピン
間にコンデンサを接続して、主放電の放電条件を同じに
しレーザ発振の出力時間を一定にするとともに、レーザ
ガスの劣化を防いで寿命を延ばしたパルスレーザ発振器
である。(Means and effects for solving the problem) The present invention applies a pulse voltage via a magnetic compression circuit to a discharge section in which a peaking capacitor is connected in series to a pre-ionization pin near a main electrode arranged oppositely. In a pulsed laser oscillator that discharges the main discharge, an impedance is connected in parallel between the pre-ionization pins and the main electrode, or a capacitor is connected between the pre-ionization pins to make the discharge conditions of the main discharge the same and the laser oscillation output time This is a pulsed laser oscillator that maintains a constant value and prevents the deterioration of the laser gas, extending its life.
(実施例)
以下、本発明のパルスレーザ発振器の一実施例を第1図
で説明する。但し、第5図と重複する部分は省く。(Embodiment) Hereinafter, one embodiment of the pulsed laser oscillator of the present invention will be described with reference to FIG. However, parts that overlap with Fig. 5 are omitted.
第1図において、予備電離ピン9A、10^と9B、1
0Bには、並列にインピーダンス3OA、 30Bが接
続され、主電極7,8には並列にインピーダンス31が
接続されている。In Figure 1, pre-ionization pins 9A, 10^ and 9B, 1
Impedances 3OA and 30B are connected in parallel to 0B, and impedance 31 is connected to main electrodes 7 and 8 in parallel.
このように構成したパルスレーザ発振器では、今、イン
ピーダンス30A、 308.31がインダクタンスの
きとには、主電極7,8の残留電圧は、ピーキングコン
デンサ11A、 11B、 12A、 12Bとインピ
ーダンス3OA、 30Bで決まる周波数で放電するの
で、この周波数をレーザ発振器の運転条件に合わせて決
めることで、第2図(2)のように残留電圧32を次の
パルス放電開始までに消滅させることができる。In the pulse laser oscillator configured in this way, when the impedances 30A and 308.31 are inductances, the residual voltage of the main electrodes 7 and 8 is the peaking capacitors 11A, 11B, 12A, and 12B and the impedances 3OA and 30B. By determining this frequency according to the operating conditions of the laser oscillator, it is possible to eliminate the residual voltage 32 before the next pulse discharge starts, as shown in FIG. 2 (2).
また、主電極7,8間のグロー放電14終了後に主電極
7,8間に残留する電圧は、ピーキングコンデンサ11
^、IIB、12A、12Bと並列インピーダンス30
A、 30Bで構成する回路の時定数程度の時間で放電
される。In addition, the voltage remaining between the main electrodes 7 and 8 after the glow discharge 14 between the main electrodes 7 and 8 ends is the peaking capacitor 11
^, IIB, 12A, 12B and parallel impedance 30
It is discharged in a time approximately equal to the time constant of the circuit composed of A and 30B.
なお、このとき予備電離ピン間では放電Vず、この期間
のレーザガスの劣化はない。Note that at this time, there is no discharge V between the pre-ionization pins, and there is no deterioration of the laser gas during this period.
第3図は、他の実施例を示す。FIG. 3 shows another embodiment.
第3図において、予備電極ピン9A、IOA間と9B
。In Figure 3, between the preliminary electrode pins 9A and IOA and 9B
.
10B間には、ピーキングコンデンサ11A、 IIB
、 12A。Between 10B and 11A, peaking capacitor 11A, IIB
, 12A.
12Bよりも十分に容量の大きいコンデンサ30へ。To capacitor 30 whose capacity is sufficiently larger than 12B.
30Bが並列に接続されている。そしてこのコンデンサ
30A、 30Bの容量は、ピーキングコンデンサとの
比を主電極の間隙と予備電離ピンの間隙の逆数の比の少
なくとも1/2以上とする。30B are connected in parallel. The capacitance of the capacitors 30A and 30B is such that the ratio with respect to the peaking capacitor is at least 1/2 or more of the ratio of the reciprocal of the gap between the main electrodes and the gap between the pre-ionization pins.
このような構成のパルスレーザ発振器によれば、予備電
離ピン9A、10^と913,108間に印加される電
圧は、ピーキングコンデンサ11A、 IIB、 12
^、12Bとコンデンサ30A1.30A2との分圧で
決まるので、コンデンサ3OA1.30A2が十分大き
いと放電部電圧が十分な電圧に上っても予備電離ピン間
の電圧を小さくでき、主放電までの時間を短くでき主放
電開始時間のばらつきとレーザガスの分解を防ぐことが
できる。According to the pulse laser oscillator having such a configuration, the voltage applied between the pre-ionization pins 9A, 10^ and 913, 108 is the peaking capacitor 11A, IIB, 12
^, Since it is determined by the partial voltage between 12B and the capacitor 30A1.30A2, if the capacitor 3OA1.30A2 is sufficiently large, even if the discharge section voltage reaches a sufficient voltage, the voltage between the pre-ionization pins can be reduced, and the voltage between the pre-ionization pins can be reduced until the main discharge. The time can be shortened, and variations in the main discharge start time and decomposition of the laser gas can be prevented.
以上、本発明のパルスレーザ発振器によれば、予備電離
ピンに並列にインピーダンスを接続し、主電極にも並列
にインピーダンスを設けて、主電極間の放電終了後の残
留電圧を消滅し、又は予備電離電極にコンデンサを並列
に接続して主放電までの時間を短縮して最初のパルスと
次のパルス間の放電条件を同一にし、励起条件を同一に
したので、レーザ発振時間のばらつきを防ぎ発振器の寿
命を延ばすことのできるパルスレーザ発振器を得ること
ができる。As described above, according to the pulsed laser oscillator of the present invention, an impedance is connected in parallel to the pre-ionization pin, and an impedance is also provided in parallel to the main electrode to eliminate the residual voltage after the discharge between the main electrodes ends, or A capacitor is connected in parallel to the ionization electrode to shorten the time until the main discharge, making the discharge conditions the same between the first pulse and the next pulse, and making the excitation conditions the same, preventing variations in laser oscillation time and reducing the oscillator. It is possible to obtain a pulsed laser oscillator that can extend the life of the laser.
第1図は本発明のパルスレーザ発1辰器の一実施例を示
す回路図、第2図は第1図の作用を示す説明図、第3図
は本発明のパルスレーザ発振器の他ザ発振器の作用を示
す説明図である。
7.8・・・主電極
9A、 913. IOA、 IOB・・・予備電離ピ
ン11A、 IIB、 12A、 12B・・・ピーキ
ングコンデンサ16・・・電源
@ X 図
(8733) 代理人 弁理士 猪 股 祥 晃(ほ
か1名)
第3図
レリ′土力
牛
(C)
第
図
第
図Fig. 1 is a circuit diagram showing an embodiment of the pulsed laser oscillator of the present invention, Fig. 2 is an explanatory diagram showing the operation of Fig. 1, and Fig. 3 is a circuit diagram showing an embodiment of the pulsed laser oscillator of the present invention. It is an explanatory view showing the effect of. 7.8... Main electrode 9A, 913. IOA, IOB... Preliminary ionization pins 11A, IIB, 12A, 12B... Peaking capacitor 16... Power supply @ Earthly cow (C) Figure Figure
Claims (2)
対向して設けられた予備電離ピンの両極に一側が接続さ
れ他側が前記主電極と並列に接続されたピーキングコン
デンサとよりなる放電部に磁気圧縮回路を介してパルス
電圧を印加してレーザガスを励起するパルスレーザ発振
器において、前記主電極と前記予備電離ピンそれぞれに
並列に前記主電極間の残留電圧を放電するインピーダン
スを設けたことを特徴とするパルスレーザ発振器。(1) Consisting of a main electrode provided oppositely to each other, and a peaking capacitor having one side connected to both poles of a pre-ionization pin provided oppositely near the main electrode, and the other side connected in parallel to the main electrode. In a pulsed laser oscillator that excites laser gas by applying a pulse voltage to a discharge part via a magnetic compression circuit, an impedance is provided in parallel to each of the main electrode and the pre-ionization pin to discharge the residual voltage between the main electrodes. A pulsed laser oscillator characterized by:
対向して設けられた予備電離ピンの両極に一側が接続さ
れ他側が前記主電極と並列に接続されたピーキングコン
デンサとよりなる放電部に磁気圧縮回路を介してパルス
電圧を印加してレーザガスを励起するパルスレーザ発振
器において、前記予備電離ピンに並列に前記ピーキング
コンデンサとの容量比が前記主電極の間隙と逆数と前記
予備電離ピンの間隙の逆数の比の少なくとも1/2以上
の容量のコンデンサを設けたことを特徴とするパルスレ
ーザ発振器。(2) Consists of a main electrode provided oppositely to each other, and a peaking capacitor having one side connected to both poles of a pre-ionization pin provided oppositely near the main electrode, and the other side connected in parallel to the main electrode. In a pulsed laser oscillator that excites laser gas by applying a pulse voltage to a discharge section via a magnetic compression circuit, the capacitance ratio of the peaking capacitor connected in parallel to the pre-ionization pin is equal to the gap between the main electrodes and the reciprocal of the pre-ionization. A pulsed laser oscillator comprising a capacitor having a capacitance of at least 1/2 or more of the ratio of the reciprocal of the gap between the pins.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19615688A JPH0245984A (en) | 1988-08-08 | 1988-08-08 | Pulse laser oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19615688A JPH0245984A (en) | 1988-08-08 | 1988-08-08 | Pulse laser oscillator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0245984A true JPH0245984A (en) | 1990-02-15 |
Family
ID=16353137
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP19615688A Pending JPH0245984A (en) | 1988-08-08 | 1988-08-08 | Pulse laser oscillator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0245984A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH07111349A (en) * | 1993-10-14 | 1995-04-25 | Hamamatsu Photonics Kk | Gas laser device |
-
1988
- 1988-08-08 JP JP19615688A patent/JPH0245984A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH07111349A (en) * | 1993-10-14 | 1995-04-25 | Hamamatsu Photonics Kk | Gas laser device |
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