JPH0747890Y2 - Excitation lamp for laser - Google Patents

Excitation lamp for laser

Info

Publication number
JPH0747890Y2
JPH0747890Y2 JP1987009199U JP919987U JPH0747890Y2 JP H0747890 Y2 JPH0747890 Y2 JP H0747890Y2 JP 1987009199 U JP1987009199 U JP 1987009199U JP 919987 U JP919987 U JP 919987U JP H0747890 Y2 JPH0747890 Y2 JP H0747890Y2
Authority
JP
Japan
Prior art keywords
electrodes
laser
lamp
electrode
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 - Lifetime
Application number
JP1987009199U
Other languages
Japanese (ja)
Other versions
JPS63118256U (en
Inventor
和義 数藤
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.)
Amada Miyachi Co Ltd
Original Assignee
Amada Miyachi 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 Amada Miyachi Co Ltd filed Critical Amada Miyachi Co Ltd
Priority to JP1987009199U priority Critical patent/JPH0747890Y2/en
Publication of JPS63118256U publication Critical patent/JPS63118256U/ja
Application granted granted Critical
Publication of JPH0747890Y2 publication Critical patent/JPH0747890Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【考案の詳細な説明】 (産業上の利用分野) 本考案は、レーザ用励起ランプの改良、特にランプ形状
の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION (Industrial field of application) The present invention relates to an improvement in an excitation lamp for a laser, and in particular to an improvement in a lamp shape.

(従来の技術) 第3図に、従来のレーザ物質を光励起するための励起ラ
ンプの典型的な構造を示す。石英ガラス製の透明管100
の中にはキセノンもしくはクリプトン等の希ガスが封入
されている。この管100の両端内部に陰極102と陽極104
が互いに向かい合うように配置され、それぞれの一端は
管100の両端から気密に突出している電極端子と電気的
に結合されている。
(Prior Art) FIG. 3 shows a typical structure of a conventional pump lamp for optically pumping a laser material. Quartz glass transparent tube 100
A rare gas such as xenon or krypton is enclosed in the box. Inside both ends of this tube 100 are a cathode 102 and an anode 104.
Are arranged so as to face each other, and one end of each of them is electrically coupled to the electrode terminals protruding from both ends of the tube 100 in an airtight manner.

(考案が解決しようとする問題点) ところで、上述したような従来の励起ランプでは、長時
間の使用により電極102,104の材料が飛散して放電能力
が低下し、またその飛散物が管壁に付着して発光輝度が
減少するという問題がある。
(Problems to be solved by the invention) By the way, in the conventional excitation lamp as described above, the material of the electrodes 102 and 104 scatters due to long-term use to lower the discharge capacity, and the scattered matter adheres to the tube wall. Then, there is a problem that the emission brightness is reduced.

一般に、電極基体はタングステン製で、陰極には電子放
出力を高めタングステンの飛散を防止するために少量の
バリュウムなどのエミッション材料が含有されている。
しかし、このエミッション材料は経時的に消耗し、さら
に電極基体のタングステンが飛散することにより、ラン
プの輝度は著しく低下してしまう。
Generally, the electrode substrate is made of tungsten, and the cathode contains a small amount of an emission material such as barium in order to enhance electron emission output and prevent tungsten from scattering.
However, this emission material is consumed with time, and the tungsten of the electrode substrate is scattered, so that the brightness of the lamp is significantly reduced.

また、ランプの輝度を高めるためには、ランプに供給す
る電流を増加すれば良いが、電極の消耗もそれに連れて
増すので電極径を大きくしなければならず、したがって
透明管の径も太くなる。このような太径の励起ランプは
細径のものに比べ、輝度が同じ場合には楕円鏡によりレ
ーザ物質に集光される光が弱く、レーザ物質への照射効
率は悪くなる。
Further, in order to increase the brightness of the lamp, it is sufficient to increase the current supplied to the lamp, but since the consumption of the electrode also increases, the electrode diameter must be increased, and therefore the diameter of the transparent tube also becomes thicker. . When such a large-diameter excitation lamp has the same luminance, the light condensed by the elliptic mirror on the laser material is weaker than that of a small-diameter excitation lamp, and the irradiation efficiency of the laser material is deteriorated.

本考案は、かかる問題点に鑑みてなされたものであり、
電極の消耗度が低く、高輝度で寿命の長いレーザ用励起
ランプを提供することを目的とする。
The present invention has been made in view of such problems,
It is an object of the present invention to provide an excitation lamp for a laser, which has low electrode consumption, high brightness, and a long life.

(問題点を解決するための手段) 上記の目的を達成するために、本考案のレーザ用励起ラ
ンプは、両端内部に放電用電極(12,14)が設けられた
透明管(10)と、前記電極(12,14)に一端を固着し他
端を前記透明管(10)から気密に突出させた電極端子
(20,22)とからなるレーザ用励起ランプにおいて、前
記透明管(10)の中間部(10b)の内径を前記電極(12,
14)の直径よりも細くし、両電極(12,14)の前面部(1
2a,14a)と前記透明管(10)の中間部(10b)との間に
前記電極(12,14)の基体の飛散物を溜めかつ電気力線
の流れをなだらかにするための空間(30,32)を設ける
構成とした。
(Means for Solving the Problems) In order to achieve the above object, the laser excitation lamp of the present invention comprises a transparent tube (10) provided with discharge electrodes (12, 14) inside both ends, An excitation lamp for a laser comprising an electrode terminal (20, 22), one end of which is fixed to the electrodes (12, 14) and the other end of which is hermetically protruded from the transparent tube (10). The inner diameter of the intermediate part (10b) is set to the electrode (12,
14) smaller than the diameter of both electrodes (12, 14) front part (1
2a, 14a) and the intermediate portion (10b) of the transparent tube (10), a space (30) for accumulating scattered substances of the substrate of the electrode (12, 14) and smoothing the flow of electric force lines. , 32).

(作用) ランプ輝度は、供給される電流が高いほど、透明管また
はランプ管内の電流密度が高いほど高輝度である。
(Function) The lamp brightness is higher as the supplied current is higher and the current density in the transparent tube or the lamp tube is higher.

本考案では、ランプ管の中間部の内径を電極の直径より
細くしてあるために、線光源に近くなりかつ中間部の電
流密度が高くなることから高輝度になる。また電極の直
径がランプ管より太くなっているため、電極の消耗にも
耐え、ランプ寿命は長くなる。
In the present invention, since the inner diameter of the middle portion of the lamp tube is made smaller than the diameter of the electrode, the lamp tube is close to the linear light source and the current density in the middle portion is high, resulting in high brightness. Further, since the diameter of the electrode is thicker than that of the lamp tube, the electrode wears out and the lamp life is extended.

(実施例) 以下、第1図および第2図を参照して本考案の実施例を
説明する。
(Embodiment) An embodiment of the present invention will be described below with reference to FIGS. 1 and 2.

第1図は、本考案の一実施例によるレーザ用励起ランプ
の全体的な構造を示す。
FIG. 1 shows the overall structure of an excitation lamp for a laser according to an embodiment of the present invention.

石英ガラス製の円筒状放電管10の中には、キセノンもし
くはクリプトン等の希ガスが管10の径に応じた所定のガ
ス圧で封入されている。この管10の両端内部に前面部12
a,14aが丸められた円柱形状の陰極12と陽極14が互いに
向かい合うようにして入れられている。陰極12は適当な
エミッション材料を含むポーラスタングステンからな
り、陽極14は純タングステンからなる。これら両電極1
2,14はそれぞれ冷却用の熱伝導体16,18を介して電極端
子20,22に電気的に結合されている。
A rare gas such as xenon or krypton is sealed in a cylindrical discharge tube 10 made of quartz glass at a predetermined gas pressure according to the diameter of the tube 10. Inside both ends of this tube 10 the front part 12
A cylindrical cathode 12 and an anode 14 in which a and 14a are rounded are inserted so as to face each other. Cathode 12 is made of porous tungsten with a suitable emission material and anode 14 is made of pure tungsten. Both these electrodes 1
2, 14 are electrically coupled to the electrode terminals 20, 22 via cooling heat conductors 16, 18, respectively.

さて、本実施例では、両電極12,14の直径が管中間部10b
の内径よりも太くなっており、そのために両電極12,14
の周りの管部分10a,10cは管中間部10bよりも太くなって
いる。そして、両電極12,14の前面部12a,14aと管中間部
10bとの間にそれぞれ空間30,32が設けられている。これ
らの空間30(32)は、電極基体の飛散物の溜めになり、
また第2図に示すように電気力線40の流れをなだらかに
するような大きさであればよい。
Now, in the present embodiment, the diameter of both electrodes 12, 14 is the tube middle portion 10b.
Is thicker than the inner diameter of the
The pipe portions 10a and 10c around the are thicker than the pipe middle portion 10b. The front portions 12a and 14a of both electrodes 12 and 14 and the tube middle portion
Spaces 30 and 32 are provided between the space 10 and 10b, respectively. These spaces 30 (32) serve as a reservoir for the scattered particles of the electrode substrate,
Further, as shown in FIG. 2, the size may be such as to make the flow of the lines of electric force 40 smooth.

以上、好適な一実施例を説明したが、本考案はそれに限
定されるものではなく、その技術的思想の範囲内で種々
の変形,変更が可能である。例えば、電極前面部の形状
を球面形状から放電効率を高めるような形状にすること
である。
Although the preferred embodiment has been described above, the present invention is not limited thereto, and various modifications and changes can be made within the scope of the technical idea thereof. For example, the shape of the front surface of the electrode is changed from a spherical shape to a shape that improves discharge efficiency.

(考案の効果) 以上のように、本考案によれば、ランプ管の中間部の内
径を電極の直径よりも細くすることにより、電流密度を
高めて発光輝度を上げ、消費電力を軽減し、また、電極
前部に空間をもたせることにより、電極基体の飛散物を
溜め、効率も良くなり、ランプ寿命を長くすることがで
きる。
(Effect of the Invention) As described above, according to the present invention, by making the inner diameter of the middle portion of the lamp tube smaller than the diameter of the electrode, the current density is increased, the emission brightness is increased, and the power consumption is reduced. Further, by providing a space in the front part of the electrode, scattered substances on the electrode base body can be collected, efficiency can be improved, and lamp life can be extended.

【図面の簡単な説明】[Brief description of drawings]

第1図は、本考案の一実施例によるレーザ用励起ランプ
の全体的な構造を示す正面図、 第2図は、上記実施例の作用を説明するための部分拡大
図、 第3図は、従来のレーザ用励起ランプの典型的な構造を
示す正面図である。 10……放電管、10b……管中間部、12……陰極、14……
陽極、16,18……熱伝導体、20,22……電極端子。
FIG. 1 is a front view showing the entire structure of a laser excitation lamp according to an embodiment of the present invention, FIG. 2 is a partially enlarged view for explaining the operation of the above embodiment, and FIG. It is a front view which shows the typical structure of the conventional excitation lamp for lasers. 10 …… Discharge tube, 10b …… Tube middle part, 12 …… Cathode, 14 ……
Anode, 16,18 ... Heat conductor, 20,22 ... Electrode terminal.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】両端内部に放電用電極(12,14)が設けら
れた透明管(10)と、前記電極(12,14)に一端を固着
し他端を前記透明管(10)から気密に突出させた電極端
子(20,22)とからなるレーザ用励起ランプにおいて、 前記透明管(10)の中間部(10b)の内径を前記電極(1
2,14)の直径よりも細くし、両電極(12,14)の前面部
(12a,14a)と前記透明管(10)の中間部(10b)との間
に前記電極(12,14)の基体の飛散物を溜めかつ電気力
線の流れをなだらかにするための空間(30,32)を設け
たことを特徴とするレーザ用励起ランプ。
1. A transparent tube (10) having discharge electrodes (12, 14) inside both ends, and one end fixed to the electrodes (12, 14) and the other end airtight from the transparent tube (10). In an excitation lamp for a laser, which comprises an electrode terminal (20, 22) which is protruded in the direction of the electrode (1
The diameter of the electrodes (12, 14) is smaller than the diameter of the electrodes (12, 14) between the front parts (12a, 14a) of both electrodes (12, 14) and the intermediate part (10b) of the transparent tube (10). An excitation lamp for a laser, characterized in that a space (30, 32) is provided for accumulating scattered substances on the substrate of (1) and for smoothing the flow of lines of electric force.
JP1987009199U 1987-01-24 1987-01-24 Excitation lamp for laser Expired - Lifetime JPH0747890Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1987009199U JPH0747890Y2 (en) 1987-01-24 1987-01-24 Excitation lamp for laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1987009199U JPH0747890Y2 (en) 1987-01-24 1987-01-24 Excitation lamp for laser

Publications (2)

Publication Number Publication Date
JPS63118256U JPS63118256U (en) 1988-07-30
JPH0747890Y2 true JPH0747890Y2 (en) 1995-11-01

Family

ID=30794288

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1987009199U Expired - Lifetime JPH0747890Y2 (en) 1987-01-24 1987-01-24 Excitation lamp for laser

Country Status (1)

Country Link
JP (1) JPH0747890Y2 (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4096450A (en) * 1977-04-22 1978-06-20 Hughes Aircraft Company Conductively cooled flashlamp

Also Published As

Publication number Publication date
JPS63118256U (en) 1988-07-30

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