JPH02112143A - Cylindrical discharge luminous tube - Google Patents

Cylindrical discharge luminous tube

Info

Publication number
JPH02112143A
JPH02112143A JP26431188A JP26431188A JPH02112143A JP H02112143 A JPH02112143 A JP H02112143A JP 26431188 A JP26431188 A JP 26431188A JP 26431188 A JP26431188 A JP 26431188A JP H02112143 A JPH02112143 A JP H02112143A
Authority
JP
Japan
Prior art keywords
cathode
anode
discharge
cylindrical
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.)
Granted
Application number
JP26431188A
Other languages
Japanese (ja)
Other versions
JPH0530018B2 (en
Inventor
Kenji Fukumitsu
憲志 福満
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.)
Hamamatsu Photonics KK
Original Assignee
Hamamatsu Photonics KK
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 Hamamatsu Photonics KK filed Critical Hamamatsu Photonics KK
Priority to JP26431188A priority Critical patent/JPH02112143A/en
Publication of JPH02112143A publication Critical patent/JPH02112143A/en
Publication of JPH0530018B2 publication Critical patent/JPH0530018B2/ja
Granted legal-status Critical Current

Links

Abstract

PURPOSE:To obtain a cylindrical discharge luminous tube having increased luminous intensity and capable of generating a spectrum which requires high excitation by applying a high voltage between an anode and a cathode in a gas sealed in a slender cylindrical gas-tight container so as to generate a glow discharge. CONSTITUTION:10 torrs of helium gas is filled in a gas-tight container 15 made of cylindrical covar glass tube through an introduction tube, and also a discharge between anode groups 171 to 17n and a cathode 16 is caused from outside by using a high voltage power supply and a current limit resistor. As the result, owing to the condition of a blocking discharge, each of anode electorle groups 171 to 17n becomes cathode dark space region and the negative glow part 18 of a luminous part is concentrated along the periphery of the anode groups 171 to 17n. Also, the tube voltage reaches 1000 to 1500 volts which can not be observed in any normal glow phenomenon. Thus, a cylindrical discharge luminous tube having its luminous intensity greatly increased and capable of generating a spectrun which requires high excitation, also having a uniform intensity and distribution along its longitudinal direction can be obtained.

Description

【発明の詳細な説明】 「産業上の利用分野」 本発明は照明、分析用光源、固体レーザ励起用光源など
に用いられる放電発光管に関するもので、さらに詳しく
は輝度の増加、高励起放電によって得られる特定スペク
1ヘルを全周から発生させる円筒状の放電発光管に関す
るものである。
Detailed Description of the Invention "Field of Industrial Application" The present invention relates to a discharge arc tube used for illumination, analytical light sources, solid-state laser excitation light sources, etc. This invention relates to a cylindrical discharge luminous tube that generates the specific spectrum 1H from the entire circumference.

「従来の技術」 従来より円筒状の光源として、照明用には蛍光ランプ、
分析用には低圧水銀ランプ、固体レーザ励起用にはキセ
ノンアークランプまたはクリプトンアークランプなどが
使われている。これらはそれぞれに長所があり、各光源
共揺るぎない用途を確立している。
``Conventional technology'' Traditionally, cylindrical light sources have been used for lighting, such as fluorescent lamps,
Low-pressure mercury lamps are used for analysis, and xenon arc lamps or krypton arc lamps are used for solid-state laser excitation. Each of these light sources has its own advantages, and each light source has established its use.

通常のグロー放電は、第4図に示すように、平板状の陰
極1と陽極2を301m+程度の間隔をもって気密容器
3内に配置し、またこの気密容器3内に例えばヘリウム
ガスを封入し、前記陰極1と陽極2との間に高電圧を印
加する。すると放電が開始し、気体原子を励起すること
によって発光を生ずる。このとき陰極1と陽極2との間
には発光部と暗部が交互に存在する。代表的な発光部、
暗部として、陰極上側より陰極暗部4、負グロ一部(発
光部)5、ファラデー暗部6、陽光柱(発光部)7、陽
極暗部8となる。このとき放電を維持するために必要な
陰極1と陽極2との間の電圧(以下管電圧と呼ぶ)は、
通常150〜500ボルトである。
In a normal glow discharge, as shown in FIG. 4, a flat cathode 1 and an anode 2 are arranged in an airtight container 3 with an interval of about 301 m+, and for example, helium gas is sealed in this airtight container 3. A high voltage is applied between the cathode 1 and anode 2. Then, a discharge starts, exciting the gas atoms and producing light emission. At this time, light-emitting areas and dark areas alternately exist between the cathode 1 and the anode 2. Typical light emitting part,
The dark areas include, from the upper side of the cathode, a cathode dark area 4, a negative glow part (light emitting area) 5, a Faraday dark area 6, a positive column (light emitting area) 7, and an anode dark area 8. At this time, the voltage between cathode 1 and anode 2 (hereinafter referred to as tube voltage) required to maintain the discharge is:
Usually 150-500 volts.

ところで放電発光管の輝度を増加させたり、エネルギー
準位の高いスペクトルを発生させるためには、放電電流
密度が増加する放電を用いるなどして、気体原子を高励
起することが必要である。
By the way, in order to increase the brightness of a discharge arc tube or generate a spectrum with a high energy level, it is necessary to highly excite gas atoms by using a discharge that increases the discharge current density.

これを達成する方法として、阻止放電が提案されている
Blocking discharge has been proposed as a method to achieve this.

この阻止放電の応用例として第5図の縦断正面図と第6
図の縦断側面図に示すように円筒状の気密容器9内に、
円筒状の陰極10を配置し、この円筒状陰極10の内側
に複数本の棒状陽極1.11〜11.を配置する。
As an application example of this blocking discharge, the longitudinal sectional front view shown in Fig. 5 and the Fig. 6
As shown in the vertical side view of the figure, inside the cylindrical airtight container 9,
A cylindrical cathode 10 is arranged, and inside the cylindrical cathode 10, a plurality of rod-shaped anodes 1.11 to 11. Place.

このとき、各陽極11□、113間、11□、113間
、・・の距離d1と、陰極10と各陽極11□、11□
間のd2を前記第4図の陰極暗部4の厚さももより小さ
くする。そして、前記気密容器9内にバッファガスとし
例えばヘリウムガスを11トール、レーザ媒質としての
クリブ1−ンガスを75ミリトール封入する。陰極10
と陽極111〜11nとの間に、高電圧を印加し放電を
開始すると、電極間が狭くて放電は充分達成できず、狭
い空間に閉じ込められるので、電離が困難になり、管電
圧の上昇を強いられ、1000〜1500ボルトにも達
する。また負グロ一部12は中心軸上に集約され、気密
容器9の両端に共振器鏡13.14を配置することによ
って、気密容器9の両端から通常のグロー放電では発振
しない469.4nmのレーザ発振が得られる。
At this time, the distance d1 between each anode 11□, 113, between 11□, 113, etc., and the distance d1 between each anode 10 and each anode 11□, 11□
The distance d2 is made smaller than the thickness of the cathode dark part 4 in FIG. 4. In the airtight container 9, for example, 11 torr of helium gas as a buffer gas and 75 mtorr of crib gas as a laser medium are sealed. Cathode 10
When a high voltage is applied between the electrodes and the anodes 111 to 11n and a discharge is started, the distance between the electrodes is narrow and sufficient discharge cannot be achieved.Since the electrodes are confined in a narrow space, ionization becomes difficult and the tube voltage increases. It is forced to reach 1000 to 1500 volts. Further, the negative glow portion 12 is concentrated on the central axis, and by arranging resonator mirrors 13 and 14 at both ends of the airtight container 9, a 469.4 nm laser that does not oscillate in normal glow discharge is emitted from both ends of the airtight container 9. Oscillation is obtained.

「発明が解決しようとする課題」 従来の第4図のグロー放電では気密容器3の全外周方向
に発光するが、定在波の移動によって強度分布が不均一
なること、目的とするスペクトル・11 線を発生させることが1できないことなどの問題があっ
た。また、第5図および第6図の阻止放電では目的とす
るスペクトル線を発生させることかできるが、気密容器
9の両端より発光するため気密容器9の全外周から発光
させることができないという問題があった。
"Problems to be Solved by the Invention" In the conventional glow discharge shown in FIG. There were problems such as the inability to generate lines. Furthermore, although the blocking discharge shown in FIGS. 5 and 6 can generate the desired spectral line, there is a problem in that the light cannot be emitted from the entire outer periphery of the airtight container 9 because the light is emitted from both ends of the airtight container 9. there were.

本発明は発光強度の増加と高励起を必要とするスペクト
ルを発生するための筒状放電発光管を得ることを目的と
するものである。
The object of the present invention is to obtain a cylindrical discharge arc tube for generating a spectrum that requires increased emission intensity and high excitation.

「課題を解決するための手段」 本発明は細長筒状気密容器に封入された気体中で陽極と
陰極間に高電圧を印加してグロー放電を発生させること
によって前記気密容器の外周方向に発光を得るようにし
た放電発光管において、前記陰極は前記気密容器の長手
方向に配置された少なくとも1本の棒状電極からなり、
前記陽極はこの棒状陰極の周囲に複数本の棒状電極を配
置してなり、前記相隣る各陽極間距離と、各陽極と陰極
間距離とを、グロー放電の陰極暗部長より小さくなるよ
うに配置したものである。
"Means for Solving the Problems" The present invention applies a high voltage between an anode and a cathode in a gas sealed in an elongated cylindrical airtight container to generate glow discharge, thereby emitting light in the direction of the outer circumference of the airtight container. In the discharge arc tube, the cathode comprises at least one rod-shaped electrode arranged in the longitudinal direction of the airtight container,
The anode is formed by arranging a plurality of rod-shaped electrodes around the rod-shaped cathode, and the distance between the adjacent anodes and the distance between each anode and the cathode are set to be smaller than the dark length of the cathode of glow discharge. This is what was placed.

「作用」 気密容器内に例えばヘリウムガスを10トール封入し、
外部から高電圧電源と電流制限抵抗を用いて各陽極と陰
極間に放電を開始させる。すると、相隣る各陽極間距離
と、各陽極と陰極間距離とがグロー放電の陰極暗部長よ
り小さく配置したので、阻止放電の条件により、各陽極
は陰極暗部領域となり、発光部である負クロ一部は陽極
の周囲に集約されて筒状気密容器の全外周から放射され
る。
"Operation" For example, 10 torr of helium gas is sealed in an airtight container,
Discharge is started between each anode and cathode using an external high voltage power supply and a current limiting resistor. Then, since the distance between adjacent anodes and the distance between each anode and cathode are arranged to be smaller than the cathode dark region of glow discharge, each anode becomes a cathode dark region and the light emitting region of the negative A portion of the chromium is concentrated around the anode and emitted from the entire outer periphery of the cylindrical airtight container.

また管電圧は通常のグロー放電の現象ではみられないよ
うな値(1000〜1500ボルト)となる。
Further, the tube voltage reaches a value (1000 to 1500 volts) that is not seen in normal glow discharge phenomena.

「実施例」 以下1本発明の一実施例を第1図および第2図に基づき
説明する。
``Example'' An example of the present invention will be described below with reference to FIGS. 1 and 2.

」−5は透明な円筒状コバールガラス管からなる気密容
器で、この気密容器15の中心には長平方向にコバール
金属からなる円柱状の陰極1−6が配置され、また、こ
の陰極16の外周には、やはりコバール金属からなる細
い棒状の陽極]7.〜コアnが配置されている。ここで
、相隣る陽極171.177間、]72.1−73間・
の表面の距離d1と、陽極]7.〜17nと陰極16の
表面の距離d2は、グロー放電の前記第4図の陰極暗部
長tよりも短くなるように配置されている。
``-5 is an airtight container made of a transparent cylindrical Kovar glass tube. In the center of this airtight container 15, a cylindrical cathode 1-6 made of Kovar metal is arranged in the longitudinal direction, and the outer periphery of this cathode 16 is A thin rod-shaped anode also made of Kovar metal]7. ~Core n is arranged. Here, between adjacent anodes 171.177, ]72.1-73,
distance d1 between the surfaces of and the anode]7. The distance d2 between ~17n and the surface of the cathode 16 is arranged to be shorter than the cathode dark length t in FIG. 4 of the glow discharge.

なお、前記陽極群17.・は気密容器コ5との間に負グ
ロ一部]−8が存在できるだけの空間を持って設置され
る。また、前記陰極16の空胴19内には冷却液20を
循環させて冷却する冷却装置が設けられる。
Note that the anode group 17.・ is installed with enough space between it and the airtight container 5 to allow for the presence of negative globules 1-8. Further, a cooling device is provided in the cavity 19 of the cathode 16 for circulating a cooling liquid 20 to cool the cathode 16 .

以」二のような構成において、気密容器1−5内に導入
管から例えばヘリウムガスを10トール封入し、かつ外
部から高電圧電源と電流制限抵抗(ともに図示せず)を
用いて陽極群17□〜]−7oと陰極16の間で放電を
開始する。すると、阻止放電の条件により各陽極群17
、〜コア、1は陰極暗部領域となり、発光部である負グ
ロ一部18は陽極群171〜17nの周囲に集約される
。また、管電圧は通常のグロー現象ではみられないよう
な値(1000〜1500ポル1−)となる。
In the configuration as shown in 2 below, for example, 10 Torr of helium gas is sealed from the introduction tube into the airtight container 1-5, and the anode group 17 is connected to the anode group 17 from the outside using a high voltage power source and a current limiting resistor (both not shown). □~] -7o and the cathode 16 start discharging. Then, depending on the blocking discharge conditions, each anode group 17
, ~core, 1 is a cathode dark region, and the negative glow part 18, which is a light emitting part, is concentrated around the anode groups 171 to 17n. Further, the tube voltage takes on a value (1000 to 1500 pol 1-) that is not seen in normal glow phenomena.

なお、前記電極間距離d1、d、はグロー放電の陰極暗
部長しによって規制され、また、このしはガス圧と電流
密度によって法定される。具体的にはdl、d2は0.
5〜1.01ffll、ガス圧は1〜201〜−ル、電
流密度は1−0〜30m A / cyKである。
Note that the inter-electrode distances d1 and d are regulated by the length of the cathode dark length of the glow discharge, and this distance is also determined by the gas pressure and current density. Specifically, dl and d2 are 0.
5~1.01ffll, gas pressure is 1~201~l, current density is 1~0~30 mA/cyK.

前記実施例では陽極群17□〜】71、として多数の棒
状電極を用いたが、これに限られるものではなく第3図
に示すような網状の円筒陽極17.を用いることもでき
る。この場合、阻止放電の条件を満すには網の孔21の
寸法d3を前記グロー放電の陰極暗部長tより小さくな
るように形成する。
In the embodiment described above, a large number of rod-shaped electrodes were used as the anode groups 17□ to ]71, but the present invention is not limited to this, and a mesh-shaped cylindrical anode 17. as shown in FIG. 3 was used. You can also use In this case, in order to satisfy the conditions for blocking discharge, the size d3 of the mesh holes 21 is formed to be smaller than the cathode dark length t of the glow discharge.

前記実施例では気密容器を細長の円筒状としたが、これ
に限られるものではなく、楕円筒、多角筒、半円筒など
の筒状とすることができる。
In the above embodiments, the airtight container has an elongated cylindrical shape, but it is not limited to this, and may have a cylindrical shape such as an elliptical cylinder, a polygonal cylinder, or a semi-cylindrical cylinder.

「発明の効果」 本発明は上述のように構成したので、従来に比し大[1
」に輝度増加させることができること、高励起を必要と
するスペクトルを発生できること、長手方向に亘って均
一な強度・分布が得られることなどのすぐれた効果を有
する。
"Effects of the Invention" Since the present invention is configured as described above, the present invention has a larger [1.
It has excellent effects such as being able to increase the brightness to a maximum of 30%, being able to generate a spectrum that requires high excitation, and being able to obtain uniform intensity and distribution over the longitudinal direction.

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

第1図は本発明による筒状放電発光管の一実施例を示す
A、 −A線断面図、第2図は同上B −1’3線断面
図、第3図は本発明の他の実施例を示す部分斜視図、第
4図は従来のグロー放電管の断面図、第5図は従来の阻
止放電管の0−C線断面図、第6図は同」−D−D線断
面図である。 1 陰極、2 陽極、3・気密容器、4 陰極暗部、5
 負グロ一部、6・ファラデー暗部、7陽光柱、8 ・
陽極暗部、9・・気密容器、10・陰極、]−11〜1
1n・・陽極、12・・・負グロ一部、13、]−4・
共振器鏡、]5・気密容器、16・陰極、178〜17
n 陽極、18・・・負グロ一部、19 空胴、20 
・冷却液、21 孔。
FIG. 1 is a sectional view taken along line A, -A showing one embodiment of the cylindrical discharge luminous tube according to the present invention, FIG. 2 is a sectional view taken along line B-1'3 of the same as above, and FIG. 3 is another embodiment of the present invention. A partial perspective view showing an example, FIG. 4 is a sectional view of a conventional glow discharge tube, FIG. 5 is a sectional view taken along the line 0-C of a conventional blocking discharge tube, and FIG. It is. 1 cathode, 2 anode, 3 airtight container, 4 cathode dark area, 5
Negative gloss part, 6. Faraday dark part, 7 positive column, 8.
Anode dark part, 9...Airtight container, 10. Cathode, ]-11~1
1n... Anode, 12... Negative glow part, 13, ]-4.
Resonator mirror,] 5. Airtight container, 16. Cathode, 178-17
n Anode, 18... Negative glow part, 19 Cavity, 20
・Cooling liquid, 21 holes.

Claims (3)

【特許請求の範囲】[Claims] (1)細長筒状気密容器に封入された気体中で陽極と陰
極間に高電圧を印加してグロー放電を発生させることに
よって前記気密容器の外周方向に発光を得るようにした
放電発光管において、前記陰極は前記気密容器の長手方
向に配置された少なくとも1本の棒状電極からなり、前
記陽極はこの棒状陰極の周囲に複数本の棒状電極を配置
してなり、前記相隣る各陽極間距離と、各陽極と陰極間
距離とを、グロー放電の陰極暗部長より小さくなるよう
に配置したことを特徴とする筒状放電発光管。
(1) In a discharge luminous tube in which a high voltage is applied between an anode and a cathode in a gas sealed in an elongated cylindrical airtight container to generate glow discharge, thereby emitting light in the direction of the outer periphery of the airtight container. , the cathode consists of at least one rod-shaped electrode arranged in the longitudinal direction of the airtight container; the anode consists of a plurality of rod-shaped electrodes arranged around the rod-shaped cathode; A cylindrical discharge arc tube characterized in that the distance and the distance between each anode and cathode are arranged so as to be smaller than the cathode dark length of a glow discharge.
(2)細長筒状気密容器に封入された気体中で陽極と陰
極間に高電圧を印加してグロー放電を発生させることに
よって前記気密容器の外周方向に発光を得るようにした
放電発光管において、前記陰極は前記気密容器の長手方
向に配置された少なくとも1本の棒状電極からなり、前
記陽極はこの棒状陰極の周囲に網状電極を配置してなり
、この網状陽極の孔の径と、各陽極と陰極間距離とを、
グロー放電の陰極暗部長より小さくなるように配置した
ことを特徴とする筒状放電発光管。
(2) In a discharge luminous tube in which a glow discharge is generated by applying a high voltage between an anode and a cathode in a gas sealed in an elongated cylindrical airtight container, thereby emitting light in the direction of the outer periphery of the airtight container. , the cathode consists of at least one rod-shaped electrode arranged in the longitudinal direction of the airtight container, the anode consists of a mesh electrode arranged around the rod-shaped cathode, and the diameter of the hole of the mesh anode and each The distance between the anode and the cathode is
A cylindrical discharge luminous tube characterized in that the tube is arranged so as to be smaller than a cathode dark section of a glow discharge.
(3)陰極は中空とし、内部に冷却液を循環してなる請
求項(1)または(2)記載の筒状放電発光管。
(3) The cylindrical discharge arc tube according to claim 1 or 2, wherein the cathode is hollow and a cooling liquid is circulated inside.
JP26431188A 1988-10-20 1988-10-20 Cylindrical discharge luminous tube Granted JPH02112143A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26431188A JPH02112143A (en) 1988-10-20 1988-10-20 Cylindrical discharge luminous tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26431188A JPH02112143A (en) 1988-10-20 1988-10-20 Cylindrical discharge luminous tube

Publications (2)

Publication Number Publication Date
JPH02112143A true JPH02112143A (en) 1990-04-24
JPH0530018B2 JPH0530018B2 (en) 1993-05-07

Family

ID=17401419

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26431188A Granted JPH02112143A (en) 1988-10-20 1988-10-20 Cylindrical discharge luminous tube

Country Status (1)

Country Link
JP (1) JPH02112143A (en)

Also Published As

Publication number Publication date
JPH0530018B2 (en) 1993-05-07

Similar Documents

Publication Publication Date Title
EP0766286B1 (en) Discharge lamp and discharge lamp producing method
US5994849A (en) Method for operating a lighting system and suitable lighting system therefor
US6518692B2 (en) Discharge device having cathode with micro hollow array
US5013966A (en) Discharge lamp with external electrodes
KR900008618B1 (en) Discharge lamp
JPH0896767A (en) Dielectric barrier discharge lamp device
EP0779767B1 (en) A rare gas discharge fluorescent lamp device
JP4783074B2 (en) Dielectric barrier discharge lamp
EP0000842B1 (en) Low pressure metal vapour discharge lamp
US6222317B1 (en) Flat light emitter
US6252352B1 (en) Flat light emitter
JPH02112143A (en) Cylindrical discharge luminous tube
JPS60136156A (en) Laser-triggered xenon flash lamp
JPH0449222B2 (en)
JPH08227695A (en) Surface light source device
JPH01309250A (en) Discharge lamp
KR100330087B1 (en) Flat type lamp using the plasma cathode
RU2120152C1 (en) Gas-discharge tube
JPH06314561A (en) Electric discharge lamp
KR20030045540A (en) A platelike electrodeless fluorescent lamp having linear micro hollow cathodes
SU1739399A1 (en) Metal halide lamp
SU1552256A1 (en) Spectral intensive lamp
JPS62252056A (en) Cathode for discharge lamp
SU803047A1 (en) Spectral tube
RU2300177C1 (en) Gas-discharge device

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees