JPS6062184A - Nitrogen laser device - Google Patents
Nitrogen laser deviceInfo
- Publication number
- JPS6062184A JPS6062184A JP17032383A JP17032383A JPS6062184A JP S6062184 A JPS6062184 A JP S6062184A JP 17032383 A JP17032383 A JP 17032383A JP 17032383 A JP17032383 A JP 17032383A JP S6062184 A JPS6062184 A JP S6062184A
- Authority
- JP
- Japan
- Prior art keywords
- electrodes
- discharge
- main
- laser device
- outer case
- 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
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 title claims abstract description 33
- 229910052757 nitrogen Inorganic materials 0.000 title claims abstract description 13
- 229910001069 Ti alloy Inorganic materials 0.000 claims abstract description 5
- 229910052719 titanium Inorganic materials 0.000 claims abstract description 5
- 239000000956 alloy Substances 0.000 claims abstract description 3
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 claims description 3
- 239000010936 titanium Substances 0.000 claims description 3
- 239000003990 capacitor Substances 0.000 abstract description 15
- 229910001873 dinitrogen Inorganic materials 0.000 abstract description 8
- 239000000758 substrate Substances 0.000 abstract description 7
- 238000006243 chemical reaction Methods 0.000 abstract description 4
- 238000007599 discharging Methods 0.000 abstract description 4
- 239000000919 ceramic Substances 0.000 abstract description 2
- 238000000034 method Methods 0.000 abstract description 2
- 229910052751 metal Inorganic materials 0.000 description 3
- 239000002184 metal Substances 0.000 description 3
- 238000010891 electric arc Methods 0.000 description 2
- 239000004593 Epoxy Substances 0.000 description 1
- NRTOMJZYCJJWKI-UHFFFAOYSA-N Titanium nitride Chemical compound [Ti]#N NRTOMJZYCJJWKI-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000003628 erosive effect Effects 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 239000003365 glass fiber Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 150000002829 nitrogen Chemical class 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 230000035939 shock Effects 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- 239000010937 tungsten Substances 0.000 description 1
- 238000007738 vacuum evaporation Methods 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
- H01S3/02—Constructional details
- H01S3/03—Constructional details of gas laser discharge tubes
- H01S3/038—Electrodes, e.g. special shape, configuration or composition
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】
本発明は堅牢で長寿命の窒素レーザ装置に係るものであ
る。DETAILED DESCRIPTION OF THE INVENTION The present invention is a robust, long-life nitrogen laser device.
窒素レーザは、安価な大気圧窒素ガスを使い、強力なレ
ーザ光を発生できる長所を有しており、一般にいわゆる
ブルームライン回路を使用している。窒素レーザの最強
の発振線は3371A(337、lnm)であるが、放
電の立上り時間は、数ナノ秒以下にする必要があり、ブ
ルームライン回路はこれに適している。Nitrogen lasers have the advantage of being able to generate powerful laser light using inexpensive atmospheric pressure nitrogen gas, and generally use a so-called Blumlein circuit. The strongest oscillation line of the nitrogen laser is 3371A (337, lnm), but the rise time of the discharge needs to be several nanoseconds or less, and the Blumlein circuit is suitable for this.
第1図は、この回路の概略構成を示している。FIG. 1 shows a schematic configuration of this circuit.
第1図において、11と12は主放電電極で、一定の間
隔をもって並行に置かれており、それぞれ2および3の
蓄電器が接続されている。5および6は高インピーダン
ス素子で、高抵抗器か数十〜数百マイクロヘンリーの線
輪が使われ、外部の直流高電圧電源8から数万ポルトの
電圧が上記高インピーダンス素子を通して円蓋電器2お
よび3に印加されている。In FIG. 1, 11 and 12 are main discharge electrodes, which are placed in parallel with a certain interval, and are connected to two and three capacitors, respectively. 5 and 6 are high impedance elements, and a high resistor or a wire ring of tens to hundreds of microhenries is used, and a voltage of tens of thousands of ports is applied from an external DC high voltage power supply 8 to the cannula electric appliance 2 through the high impedance elements. and 3.
尚蓄電器2には並列に放電v4が接続され、外部電源を
除くレーザ装置は非金属製外箱7に納められて、適当な
圧力の窒素ガスが充填されている。A discharge v4 is connected in parallel to the capacitor 2, and the laser device excluding an external power source is housed in a non-metallic outer box 7, which is filled with nitrogen gas at an appropriate pressure.
今、両放電電極が直流高電圧で充電されているとき、放
電管4に、外部のトリガー電源9から放電開始用のトリ
ガー電圧が加えられると、蓄電器2の電圧は極短時間に
放電され電荷はゼロになる。このとき両生放電電極間に
衝撃波が発生し、開放端(直流電圧印加点の反対側)に
向って進行する。このため主放電電極間に放電が起って
窒素ガスレーザ光が発生され、主放電電極間隔に沿って
開放端から外部に紫外線レーザ光が放出される。これが
ブルームライン(Blumlein)回路による窒素レ
ーザ装置の動作原理である。Now, when both discharge electrodes are being charged with DC high voltage, when a trigger voltage for starting discharge is applied to the discharge tube 4 from the external trigger power supply 9, the voltage of the capacitor 2 is discharged in a very short time and the charge is becomes zero. At this time, a shock wave is generated between the two discharge electrodes and propagates toward the open end (the side opposite to the DC voltage application point). Therefore, a discharge occurs between the main discharge electrodes, a nitrogen gas laser beam is generated, and an ultraviolet laser beam is emitted to the outside from the open end along the main discharge electrode interval. This is the operating principle of a nitrogen laser device using a Blumlein circuit.
この窒素レーザは、前述の如く、数ナノ秒以下の鋭い立
上り時間のパルスで励起する必要があり、このためには
主放電電極、蓄電器、放電管ならびに帰線回路の直列イ
ンダクタンスおよび抵抗性を極力減少させなければなら
ない。このために、蓄電器2.3は第2図の平面図およ
び第3図の側面図に見られる如く、絶縁板10の片面に
、蓄電器2.3の電極を並べ、裏面に接地電極11を配
置して、主放電電極11と12はそれぞれ蓄電器極板に
接触させて起動用放電管4も蓄電器2の極板の中央部に
接続される。As mentioned above, this nitrogen laser needs to be excited by a pulse with a sharp rise time of several nanoseconds or less, and for this purpose, the series inductance and resistance of the main discharge electrode, capacitor, discharge tube, and return circuit must be minimized. must be reduced. For this purpose, the capacitor 2.3 is arranged such that the electrodes of the capacitor 2.3 are arranged on one side of the insulating plate 10, and the ground electrode 11 is arranged on the back side, as shown in the plan view of FIG. 2 and the side view of FIG. The main discharge electrodes 11 and 12 are brought into contact with the capacitor plates, respectively, and the starting discharge tube 4 is also connected to the center of the capacitor plate.
蓄電器の静電容量としては、充電エネルギを大にするた
めにはある程度大きい程良いが、高電圧を印加する必要
もあり、励起パルスの立上りを極力短くすることもあっ
て、数百乃至数千ピコファラドのものが使われており、
真空蒸着などの方法で、絶縁基板上に密着させる必要が
ある。The capacitance of the capacitor is preferably as large as possible in order to increase the charging energy, but it is necessary to apply high voltage and the rise of the excitation pulse should be as short as possible, so the capacitance is several hundred to several thousand. Picofarad is used,
It is necessary to adhere it closely to the insulating substrate using a method such as vacuum evaporation.
主放電電極11と12は第2図および第3図に示す如く
、蓄電器電極上に対向して固定され、その一方は調整機
構によって、放電電極間間隔を調整できるようにしてい
る。また放電の開始に当っては弱いグロー放電を起させ
るために、主放電電極の下部に金属薄板12を挿入させ
ている。放電の開始に当っては、この金属薄板間でコロ
ナ放電を生じさせ、次いで、主放電電極間のグロー放電
に移行させるために、この薄板12は、主放電電極より
も僅かに間隔を拡げている。また主放電電極の放電部は
角を丸めてアーク放電の発生を防止している。As shown in FIGS. 2 and 3, the main discharge electrodes 11 and 12 are fixed facing each other on the capacitor electrode, and one of them is provided with an adjusting mechanism to adjust the distance between the discharge electrodes. Further, at the start of discharge, a thin metal plate 12 is inserted under the main discharge electrode in order to cause a weak glow discharge. At the start of discharge, the thin metal plates 12 are spaced slightly apart from each other in order to generate a corona discharge between the metal thin plates and then transition to a glow discharge between the main discharge electrodes. There is. Furthermore, the corners of the discharge portion of the main discharge electrode are rounded to prevent the occurrence of arc discharge.
以上説明したものが、従来使用されたブルームライン回
路を使用する窒素レーザ装置であるが、最大の欠点は、
安定動作と絶縁破壊および寿命である。What has been explained above is the conventional nitrogen laser device that uses the Blumlein circuit, but the biggest drawback is:
Stable operation, dielectric breakdown, and long life.
つまり、絶縁基板としてガラス・エポキシ基板を使用し
ているため、比誘電率が3.5〜5と低く、その1酎コ
ロナ特性が悪くて焼損し易い、また、ガラス繊維を含ん
でいるので絶縁耐力にも不満が残る。In other words, since a glass/epoxy substrate is used as an insulating substrate, the dielectric constant is low at 3.5 to 5, and the corona properties are poor and easily burnt out.Also, since it contains glass fiber, it is insulating. I am also dissatisfied with the durability.
この点に関しては絶縁基板としてセラミック基板を採用
することによって一応の解決を見た。Regarding this point, a temporary solution was found by adopting a ceramic substrate as the insulating substrate.
従来のブルームライン形窒素レーザ装置の主放電電極と
しては、アルミニュームやタングステン材を使用してい
た。これらの場合、アーク放電を発生させなくとも、窒
素ガスのグロー放電によって、電極放電面が犯され、寿
命が短かった。Aluminum or tungsten materials have been used as the main discharge electrode in conventional Blumlein nitrogen laser devices. In these cases, even if arc discharge was not generated, the electrode discharge surface was damaged by the glow discharge of nitrogen gas, resulting in a short life.
そこで、本発明は主放電電極としてチタンまたはチタン
合金材を用いるもので、窒素ガスと反応して表面に窒化
チタンの薄膜が生じ、これがそれ以上の反応を防ぐため
に寿命が極端に改善され、窒化反応による寿命低下を完
全に押えることができ、長時間に安定な動作を示した。Therefore, the present invention uses titanium or a titanium alloy material as the main discharge electrode, which reacts with nitrogen gas to form a thin film of titanium nitride on the surface, which prevents further reactions and dramatically improves the lifespan. It was possible to completely suppress the decrease in life due to reactions and showed stable operation over a long period of time.
ブルームライン回路を使用しなくとも窒素ガス中で放電
を行い窒素レーザを発生させる場合には、同様の主電極
浸蝕が起るので、チタンまたはチタン合金を主放電電極
として採用することは非常に有効である。Similar main electrode erosion occurs when discharging in nitrogen gas to generate a nitrogen laser even without using a Blumlein circuit, so it is very effective to use titanium or a titanium alloy as the main discharge electrode. It is.
本発明は上記の作用、効果によって、非常に長寿命で安
定な窒素レーザ装置が得られた。The present invention provides a very long-life and stable nitrogen laser device due to the above-mentioned functions and effects.
第1図はブルームライン形窒素レーザ装置の説明図、第
2図はブルームライン回路の平面図、第3図は同側面図
である。
1□および12は主放電電極、2および3は蓄電器、4
は起動用放電管、5および6は高インピーダンス素子、
7は外箱、8は直流高電圧電源、9は起動用トリガー電
源、10は絶縁基板、11は蓄電器接地電極、12は放
電開始電極。FIG. 1 is an explanatory diagram of a Blumlein type nitrogen laser device, FIG. 2 is a plan view of a Blumlein circuit, and FIG. 3 is a side view of the same. 1□ and 12 are main discharge electrodes, 2 and 3 are capacitors, 4
is a discharge tube for starting, 5 and 6 are high impedance elements,
7 is an outer box, 8 is a DC high voltage power supply, 9 is a starting trigger power supply, 10 is an insulating substrate, 11 is a capacitor grounding electrode, and 12 is a discharge starting electrode.
Claims (1)
使用したことを特徴とする窒素レーザ装置。(1) A nitrogen laser device using a main discharge electrode, characterized in that titanium or a titanium alloy material is used as the main discharge electrode.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP17032383A JPS6062184A (en) | 1983-09-14 | 1983-09-14 | Nitrogen laser device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP17032383A JPS6062184A (en) | 1983-09-14 | 1983-09-14 | Nitrogen laser device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6062184A true JPS6062184A (en) | 1985-04-10 |
Family
ID=15902824
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP17032383A Pending JPS6062184A (en) | 1983-09-14 | 1983-09-14 | Nitrogen laser device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6062184A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63102267U (en) * | 1986-12-22 | 1988-07-02 |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3719900A (en) * | 1971-05-19 | 1973-03-06 | U Hochuli | Ultra stable symmetrical laser structures |
-
1983
- 1983-09-14 JP JP17032383A patent/JPS6062184A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3719900A (en) * | 1971-05-19 | 1973-03-06 | U Hochuli | Ultra stable symmetrical laser structures |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63102267U (en) * | 1986-12-22 | 1988-07-02 |
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