JPH049391B2 - - Google Patents
Info
- Publication number
- JPH049391B2 JPH049391B2 JP17575882A JP17575882A JPH049391B2 JP H049391 B2 JPH049391 B2 JP H049391B2 JP 17575882 A JP17575882 A JP 17575882A JP 17575882 A JP17575882 A JP 17575882A JP H049391 B2 JPH049391 B2 JP H049391B2
- Authority
- JP
- Japan
- Prior art keywords
- voltage
- discharge
- oscillator
- power supply
- tube
- 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
- 230000007423 decrease Effects 0.000 claims description 5
- 230000010355 oscillation Effects 0.000 claims description 3
- 238000010586 diagram Methods 0.000 description 5
- 230000003247 decreasing effect Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000002184 metal Substances 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)
Description
【発明の詳細な説明】
産業上の利用分野
この発明はガスレーザ発振器に関するものであ
る。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application This invention relates to a gas laser oscillator.
従来例の構成とその問題点
ガスレーザ放電は一般にグロー放電領域を利用
しており、第1図曲線Aで示すように放電特性は
負性抵抗を示す。このためこの放電と直列に抵抗
素子を結ぶことが行われており、一般の抵抗器や
真空管などによりこの抵抗成分が与えられる。放
電開始電圧は放電長やガス圧力に依存するが、一
般には20KV/mとなる。また、放電電圧は
50mAで10KV/mであり、抵抗素子には10KVに
およぶ電圧が印加されることとなり、耐高電圧の
素子が必要とされる。このため高電圧電源を2つ
用いて第1図破線Bに示すような電源特性を持た
せることなどが行われているが、放電区間が多数
の場合には全放電を安定して起動することは難か
しいなどの問題がある。Conventional Structure and Problems Gas laser discharge generally utilizes a glow discharge region, and its discharge characteristics exhibit negative resistance as shown by curve A in FIG. For this reason, a resistance element is connected in series with this discharge, and this resistance component is provided by a general resistor, vacuum tube, etc. The discharge starting voltage depends on the discharge length and gas pressure, but is generally 20 KV/m. Also, the discharge voltage is
The voltage is 10 KV/m at 50 mA, and a voltage of up to 10 KV is applied to the resistive element, so a high voltage withstand element is required. For this reason, two high-voltage power supplies are used to provide power supply characteristics as shown in the broken line B in Figure 1, but when there are many discharge sections, it is difficult to stably start all discharges. There are problems such as difficulty.
発明の目的
この発明の目的は、放電電流を調整する抵抗素
子に加わる電圧を低電圧に維持できるとともに、
放電区間が多数におよぶ場合でも全放電を安定し
て起動できるガスレーザ発振器を提供することで
ある。Purpose of the Invention The purpose of the present invention is to maintain a low voltage applied to a resistive element that adjusts discharge current, and to
An object of the present invention is to provide a gas laser oscillator that can stably start all discharges even when there are many discharge sections.
発明の構成
この発明のガスレーザ発振器は、放電管の外周
に電極を配し、この電極に高周波発振器により高
周波電圧を印加可能とし、放電管の両管端の電圧
を制御回路により検出して放電管の両管端の電圧
が電源電圧に近い一定高電圧となるように上記高
周波発振器の発振出力を制御するようにしたもの
で、放電管の両管端の電圧を電源電圧に近い一定
高電圧に制御することで、放電管に直列接続した
可変抵抗の印加電圧を一定低電圧に維持する。Structure of the Invention The gas laser oscillator of the present invention has an electrode arranged around the outer periphery of the discharge tube, a high frequency voltage can be applied to this electrode by a high frequency oscillator, and the voltage at both ends of the discharge tube is detected by a control circuit. The oscillation output of the high frequency oscillator is controlled so that the voltage at both tube ends of the discharge tube is a constant high voltage close to the power supply voltage. Through control, the voltage applied to the variable resistor connected in series with the discharge tube is maintained at a constant low voltage.
実施例の説明
この発明の一実施例を第2図ないし第4図を用
いて説明する。第2図において、1は放電管であ
る。これには高電圧直流電源2と抵抗成分となる
抵抗素子3が直列に接続されている。ここでは抵
抗素子3として三極真空管が用いられている。抵
抗素子5は放電電流を検出するためのもので、可
変基準電圧と比較され、電流比較制御回路4によ
り三極真空管3のグリツドバイアスを変化して定
電流となるよう三極真空管3のインピーダンスが
制御される。6は電圧を変化自在な電源で、この
電源6と真空管3と抵抗素子5と電流比較制御回
路4とで可変抵抗を構成する。この状態では、放
電管1は第1図曲線Aの放電特性を示すため、三
極真空管3のプレートには10KV以上の電圧が印
加される場合が発生し、高耐圧の特殊な真空管を
使用する必要がある。しかも、三極真空管3での
発熱も大きくなり電力消費も大きくなる。DESCRIPTION OF EMBODIMENTS An embodiment of the present invention will be described with reference to FIGS. 2 to 4. In FIG. 2, 1 is a discharge tube. A high voltage DC power supply 2 and a resistance element 3 serving as a resistance component are connected in series to this. Here, a triode vacuum tube is used as the resistance element 3. The resistive element 5 is for detecting the discharge current, which is compared with a variable reference voltage, and the current comparison control circuit 4 changes the grid bias of the triode vacuum tube 3 to adjust the impedance of the triode vacuum tube 3 so as to maintain a constant current. is controlled. Reference numeral 6 denotes a power source whose voltage can be freely changed, and this power source 6, vacuum tube 3, resistance element 5, and current comparison control circuit 4 constitute a variable resistor. In this state, discharge tube 1 exhibits the discharge characteristics of curve A in Figure 1, so a voltage of 10 KV or more may be applied to the plate of triode vacuum tube 3, so a special vacuum tube with high withstand voltage is used. There is a need. Furthermore, the amount of heat generated in the triode vacuum tube 3 increases, resulting in increased power consumption.
さて、7は放電管1の外周にまかれた金属線で
構成した電極であり、出力電圧可変型の高周波発
振器8に接続されている。抵抗素子9,10は三
極真空管3のプレート電圧を分圧して検出するも
ので、制御回路11にプレート電圧を送り込むも
のである。制御回路11は、このプレート電圧を
低下させるよう高周波発振器8の発振出力を制御
するものである。 Now, reference numeral 7 denotes an electrode made of a metal wire that is placed around the outer periphery of the discharge tube 1, and is connected to a high frequency oscillator 8 of a variable output voltage type. The resistive elements 9 and 10 are used to divide and detect the plate voltage of the triode vacuum tube 3, and send the plate voltage to the control circuit 11. The control circuit 11 controls the oscillation output of the high frequency oscillator 8 so as to reduce this plate voltage.
第3図は、高周波発振器8の出力電圧を5KV,
7KV,10KVにそれぞれ設定した場合の放電管1
の放電特性を示し、周波数はそれぞれ25KHzであ
る。同図から分るように、低電流領域では高電圧
を印加し、放電電流が上昇するにつれて電圧を低
下させていくことにより、放電特性をほぼ一定に
できる。この電圧調整は制御回路11により行な
う。第4図の曲線Cは、上記原理により、放電管
1の両管端の電圧がほぼ一定に制御された放電特
性の一例であり、曲線Dは直流電源2の電源特性
である。このように、放電管1の両管端の電圧
(放電特性曲線C)が、直流電源2の電圧(電源
特性曲線D)に近いほぼ一定の高電圧に維持され
るため、可変抵抗(三極真空管3および抵抗素子
5等)にはほぼ一定の低電圧(約1〜2KV)が
印加されることになり、抵抗素子として耐電圧の
小さな素子を使用できる。そのため、抵抗成分が
消費する無効電力が低下し、従来50%以下であつ
たものが80%以上の電力を放電エネルギとして利
用できることになる。また、電極7に供給する高
周波電流は極めて小さいものでよいため(0.1mA
以下)、高周波発振器8は低容量のものを使用で
きて各放電管ごとに付設することが容易となり、
多数の放電領域を有するガスレーザ発振器におい
ても、個々の放電を制御することができて放電開
始を安定化できる。 Figure 3 shows the output voltage of the high frequency oscillator 8 at 5KV,
Discharge tube 1 when set to 7KV and 10KV respectively
The discharge characteristics are 25KHz, respectively. As can be seen from the figure, by applying a high voltage in the low current region and lowering the voltage as the discharge current increases, the discharge characteristics can be kept almost constant. This voltage adjustment is performed by the control circuit 11. Curve C in FIG. 4 is an example of a discharge characteristic in which the voltage at both ends of discharge tube 1 is controlled to be substantially constant according to the above principle, and curve D is a power supply characteristic of DC power supply 2. In this way, the voltage at both ends of the discharge tube 1 (discharge characteristic curve C) is maintained at an almost constant high voltage close to the voltage of the DC power supply 2 (power supply characteristic curve D), so the variable resistor (three-pole A substantially constant low voltage (approximately 1 to 2 KV) is applied to the vacuum tube 3, resistance element 5, etc., and an element with a small withstand voltage can be used as the resistance element. Therefore, the reactive power consumed by the resistance component is reduced, and more than 80% of the power, which was less than 50% in the past, can now be used as discharge energy. In addition, since the high frequency current supplied to the electrode 7 only needs to be extremely small (0.1mA
(below), the high-frequency oscillator 8 can be of low capacity and can be easily attached to each discharge tube.
Even in a gas laser oscillator having a large number of discharge regions, each discharge can be controlled and the start of discharge can be stabilized.
なお、上記実施例においては、高周波発振器8
として出力電圧可変型発振器を用い、放電電流の
増加・減少に応じて出力電圧を減少・増加させた
が、高周波発振器8として周波数可変型発振器を
用い放電電流の増加・減少に応じて発振器8の出
力周波数を減少・増加させてもよく、あるいは両
者を兼用してもよい。 Note that in the above embodiment, the high frequency oscillator 8
A variable output voltage type oscillator was used as the high frequency oscillator 8, and the output voltage was decreased/increased according to the increase/decrease in the discharge current. The output frequency may be decreased or increased, or both may be used.
発明の効果
この発明のガスレーザ発振器によれば、放電電
流を調整する抵抗素子に加わる電圧を低電圧に維
持できるとともに、放電区間が多数におよぶ場合
でも全放電を安定して起動できるという効果が得
られる。Effects of the Invention According to the gas laser oscillator of the present invention, the voltage applied to the resistance element that adjusts the discharge current can be maintained at a low voltage, and even when there are many discharge sections, the entire discharge can be started stably. It will be done.
第1図は従来例の放電特性と電源特性を示す
図、第2図はこの発明の一実施例の構成図、第3
図はこの実施例の効果を説明するための放電特性
を示す図、第4図はこの実施例による放電特性と
電源特性を示す図である。
1…放電管、2…電源、3…三極真空管(可変
抵抗)、4…電流比較制御回路(可変抵抗)、5…
抵抗素子(可変抵抗)、6…電源(可変抵抗)、7
…電極、8…高周波発振器、11…制御回路。
Figure 1 is a diagram showing the discharge characteristics and power supply characteristics of a conventional example, Figure 2 is a configuration diagram of an embodiment of the present invention, and Figure 3 is a diagram showing the discharge characteristics and power supply characteristics of a conventional example.
FIG. 4 is a diagram showing discharge characteristics for explaining the effects of this embodiment, and FIG. 4 is a diagram showing discharge characteristics and power supply characteristics according to this embodiment. 1...discharge tube, 2...power supply, 3...triode vacuum tube (variable resistance), 4...current comparison control circuit (variable resistance), 5...
Resistance element (variable resistance), 6... Power supply (variable resistance), 7
...electrode, 8...high frequency oscillator, 11...control circuit.
Claims (1)
放電管と、前記電源と前記放電管に直列介挿して
放電電流を調整する抵抗成分と、前記放電管の外
周に配した電極と、この電極に高周波電圧を印加
する高周波発振器と、前記放電管の両管端の電圧
を検出して両管端の電圧が前記電源電圧に近い一
定高電圧となるように前記高周波発振器の発振出
力を制御する制御回路とを備えたガスレーザ発振
器。 2 前記高周波発振器は出力電圧可変型発振器で
あり、前記制御回路は放電電流の増加・減少に応
じて前記発振器の出力電圧を減少・増加する特許
請求の範囲第1項記載のガスレーザ発振器。 3 前記高周波発振器は周波数可変型発振器であ
り、前記制御回路は放電電流の増加・減少に応じ
て前記発振器の出力周波数を減少・増加する特許
請求の範囲第1項記載のガスレーザ発振器。[Scope of Claims] 1. A power supply, a discharge tube that discharges by supplying power from the power supply, a resistance component that is inserted in series with the power supply and the discharge tube to adjust the discharge current, and a resistance component arranged around the outer periphery of the discharge tube. an electrode, a high-frequency oscillator that applies a high-frequency voltage to the electrode, and a high-frequency oscillator that detects the voltage at both tube ends of the discharge tube so that the voltage at both tube ends becomes a constant high voltage close to the power supply voltage. A gas laser oscillator equipped with a control circuit that controls oscillation output. 2. The gas laser oscillator according to claim 1, wherein the high-frequency oscillator is a variable output voltage oscillator, and the control circuit decreases or increases the output voltage of the oscillator in accordance with an increase or decrease in discharge current. 3. The gas laser oscillator according to claim 1, wherein the high-frequency oscillator is a variable frequency oscillator, and the control circuit decreases or increases the output frequency of the oscillator in accordance with an increase or decrease in discharge current.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP17575882A JPS5965493A (en) | 1982-10-05 | 1982-10-05 | Gas laser oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP17575882A JPS5965493A (en) | 1982-10-05 | 1982-10-05 | Gas laser oscillator |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5965493A JPS5965493A (en) | 1984-04-13 |
JPH049391B2 true JPH049391B2 (en) | 1992-02-20 |
Family
ID=16001733
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP17575882A Granted JPS5965493A (en) | 1982-10-05 | 1982-10-05 | Gas laser oscillator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5965493A (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6355992A (en) * | 1986-08-26 | 1988-03-10 | Mitsubishi Electric Corp | Laser beam machining apparatus |
-
1982
- 1982-10-05 JP JP17575882A patent/JPS5965493A/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPS5965493A (en) | 1984-04-13 |
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