JPS6159787A - Solid laser exciting lamp - Google Patents

Solid laser exciting lamp

Info

Publication number
JPS6159787A
JPS6159787A JP18033484A JP18033484A JPS6159787A JP S6159787 A JPS6159787 A JP S6159787A JP 18033484 A JP18033484 A JP 18033484A JP 18033484 A JP18033484 A JP 18033484A JP S6159787 A JPS6159787 A JP S6159787A
Authority
JP
Japan
Prior art keywords
electrodes
active medium
laser active
vacuum container
discharge
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
JP18033484A
Other languages
Japanese (ja)
Other versions
JPH06105810B2 (en
Inventor
Satoru Amano
覚 天野
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.)
Hoya Corp
Original Assignee
Hoya Corp
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 Hoya Corp filed Critical Hoya Corp
Priority to JP18033484A priority Critical patent/JPH06105810B2/en
Publication of JPS6159787A publication Critical patent/JPS6159787A/en
Publication of JPH06105810B2 publication Critical patent/JPH06105810B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/09Processes or apparatus for excitation, e.g. pumping
    • H01S3/091Processes or apparatus for excitation, e.g. pumping using optical pumping
    • H01S3/0915Processes or apparatus for excitation, e.g. pumping using optical pumping by incoherent light
    • H01S3/092Processes or apparatus for excitation, e.g. pumping using optical pumping by incoherent light of flash lamp

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  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Abstract

PURPOSE:To uniformly excite a plate-shaped laser active medium, by providing beltlike facing electrodes within a flat vacuum container and adhering conductive films which can transmit light in the effective absorption band of the laser active medium along the discharge passage between these electrodes. CONSTITUTION:Beltlike facing electrodes 2A and 2B are disposed within a flat vacuum container 1 of quartz glass. A high voltage in the order of 2-3kV is applied between the electrodes 2A and 2B through electrode outlets 3A and 3B so as to cause electric discharge. Transparent conductive films 5A and 5B of indium oxide mixed with tin oxide are adhered on the opposed outer surfaces of the vacuum container 1. These transparent electrodes 5A and 5B are provided such that the ends thereof are superposed on the edges 4A and 4B of the electrodes 2A and 2B to ensure that the discharge passage between the facing electrodes 2A and 2B is completely covered with the transparent electrodes. Thus, an induction passage for electric discharge is provided over the whole discharge passage between the electrodes, whereby generally uniform electric discharge can be realized.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は固体レーザ励起用ランプに関し、特に板状のレ
ーザ活性媒体を備えた表面励起形固体レーザの励起用ラ
ンプに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a lamp for excitation of a solid-state laser, and more particularly to a lamp for excitation of a surface-pumped solid-state laser equipped with a plate-shaped laser active medium.

〔従来の技術〕[Conventional technology]

従来の代表的な固体レーザ装置は、ともに円柱状の、レ
ーザ活性媒体と励起用ランプとを、それぞれ楕円体形状
のり7レクタの焦点に配置し、励起用ランプの励起光を
リフレクタにより反射させてレーザ活性媒体に集光嘔せ
る構造であったが、レーザ光出力が大きくなると、レー
ザ活性媒体の中心と表面での温度差が原因で、出力が不
安定になったシ、レーザ活性媒体が破壊したりする問題
があった。
In a typical conventional solid-state laser device, a laser active medium and an excitation lamp, both of which are cylindrical, are placed at the focal point of an ellipsoidal reflector, and the excitation light from the excitation lamp is reflected by the reflector. The structure was designed to focus light on the laser active medium, but when the laser light output became large, the output became unstable due to the temperature difference between the center and the surface of the laser active medium, and the laser active medium was destroyed. There was a problem.

このため、近年、スラブ(Stab)形といわれる表面
冷却・光面励起形の固体レーザ装置が開発でれ使用され
ている。
For this reason, in recent years, a surface-cooled, light-pumped solid-state laser device called a slab type has been developed and used.

これは、板状のレーザ活性媒体を挾んで励起用ランプを
配置し、その間に冷却媒体を流したもので、レーザ光は
、レーザ活性媒体の励起用ランプに面する対向表面間で
反射をくシ返すことによpジグザグの光路を通り、その
際、冷却でれた表面の低温部分と中心の高温部分とを交
互にくり返して進行するところから、平均化された温度
分布状態の媒体中を伝搬することになる。
In this system, an excitation lamp is placed between a plate-shaped laser active medium, and a cooling medium is flowed between them.The laser light is reflected between the opposing surfaces of the laser active medium facing the excitation lamp. By turning the light, the optical path passes through a p-zigzag path, and at that time, the light travels through the medium with an averaged temperature distribution, alternating between the low-temperature part on the cooled surface and the high-temperature part in the center. It will spread.

ところが、従来のこの種の固体レーザ装置では、円柱状
の励起ランプを用いているため、板状のレーザ活性媒体
の厚み方向については上述したように温度分布が平均化
されるものの、励起用ランプの延在方向に垂直で上記厚
み方向に垂直な幅方向については、光量がランプから離
れるほど低下する分布をもつことから、温度分布も同様
に不均一となジ、それに伴って屈折率も同様の分布を有
することになる。
However, in this type of conventional solid-state laser device, a cylindrical excitation lamp is used, so although the temperature distribution in the thickness direction of the plate-shaped laser active medium is averaged as described above, the excitation lamp In the width direction, which is perpendicular to the extending direction of the lamp and perpendicular to the above-mentioned thickness direction, the light intensity has a distribution that decreases as the distance from the lamp increases, so the temperature distribution is similarly uneven, and accordingly, the refractive index is also the same. will have a distribution of

このため、レーザ光の高出力化に限界を来たしていた。For this reason, there has been a limit to increasing the output of laser light.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

本発明はこのような事情に鑑みてなされたもので、その
目的は、板状のレーザ活性媒体を均一に励起できる固体
レーザ励起用ランプを提供するこ゛とにある。
The present invention has been made in view of these circumstances, and its object is to provide a solid-state laser excitation lamp that can uniformly excite a plate-shaped laser active medium.

〔問題点を解決するための手段〕[Means for solving problems]

このような目的を達成するために1本発明は、偏平状の
真空容器内に帯状の対向電極を備えた放電管で構成し、
かつ対向電極間の放電経路に沿って真空容器の少なくと
も一方の主面外表面に、少なくともレーザ活性媒体の有
効吸収帯の光に対して透光性を有する導電性膜を被着し
たものである。
In order to achieve such an object, the present invention consists of a discharge tube equipped with a band-shaped counter electrode inside a flat vacuum vessel,
and a conductive film that is transparent to at least light in the effective absorption band of the laser active medium is coated on the outer surface of at least one main surface of the vacuum container along the discharge path between the opposing electrodes. .

〔作用〕[Effect]

偏平形状の励起用ランプを板状のレーザ活性媒体に、そ
れらの主面、つまp最も広い面が相互に平行になるよう
に隣接して配置することによりレーザ活性媒体の主面全
体を均一に励起する。また、対向IE極を帯状としたこ
とによ9局部的に放電が生ずるおそれがあるが、真空容
器の主面外表面に被着した導電性膜にトリガ電圧を印加
して放電の誘導路を作ることにより、帯状の対向電極の
全体にわたり均一な放電を行なわせることができる。
By arranging flat excitation lamps adjacent to a plate-shaped laser active medium so that their main surfaces and widest surfaces are parallel to each other, the entire main surface of the laser active medium can be uniformly distributed. excite. In addition, since there is a risk of localized discharge due to the band-shaped facing IE electrode, a trigger voltage is applied to the conductive film attached to the outer surface of the main surface of the vacuum container to create a guide path for the discharge. By creating such a structure, it is possible to cause a uniform discharge to occur over the entire band-shaped counter electrode.

〔実施例〕〔Example〕

第1図に、本発明の一実施例を示す。同図(−)は平面
図、同図(b)は正面図、同図(C)は側面図でおる。
FIG. 1 shows an embodiment of the present invention. The figure (-) is a plan view, the figure (b) is a front view, and the figure (C) is a side view.

同図において、1は幅34醪、厚き4間、長さ120鵡
の外形を有し、肉厚はぼ1rIrsの石英ガラスからな
る偏平状の:A空容器でおる。この真空容器1の内部に
は、その長手方向両端に、上記幅方向に沿って長ぢ30
園の帯状の対向電M2A、2Bが配置されている。両電
極の対向部分は、電界を有効に集中して効率良く放電を
起こさせるために、ナイフェツジ状に形成しであるが、
必ずしもこのようにする必要はなく、例えば一方はめる
程度の曲率半径を有する曲面状としてもよい。
In the figure, 1 is a flat empty vessel made of quartz glass and having an external shape of 34 mm wide, 4 mm thick, and 120 mm long, and has a wall thickness of about 1 rIrs. Inside the vacuum container 1, there are long lengths 30 along the width direction at both ends in the longitudinal direction.
A band-shaped opposing electric wire M2A, 2B is arranged. The opposing portions of both electrodes are formed into a knife shape in order to effectively concentrate the electric field and cause efficient discharge.
It does not necessarily have to be this way; for example, it may be a curved surface having a radius of curvature that allows one side to be fitted.

ココテ、l11fii’!ff12A、2B間K t 
極取出シ部aA 。
Cocote, l11fii'! K t between ff12A and 2B
Pole extraction part aA.

3Bを介して図上省略した電源により2〜3KV(エネ
ルギとして500〜900 J )程度の高電圧を印加
し、放電を起こす場合、電極2A、 2Bが帯状に延在
することがら、その延在方向(真空容器の幅方向)にお
いて、エツジ部4A、 4Bの表面状態により凸部が存
在すると、その凸部のみに電界が集中して局部的な放電
をおこし、上記真空容器の幅方向全体にわたって均一な
放電を得ることができない場合がおる。
When a high voltage of about 2 to 3 KV (500 to 900 J in terms of energy) is applied by a power supply not shown in the figure through the electrode 3B to cause a discharge, the electrodes 2A and 2B extend in a band shape, so the extension If a convex portion is present due to the surface condition of the edge portions 4A and 4B in the direction (width direction of the vacuum vessel), the electric field will concentrate only on the convex portion, causing a local discharge, and will spread over the entire width direction of the vacuum vessel. In some cases, it may not be possible to obtain a uniform discharge.

このため、本発明では、真空容器10対向する両生面外
表面に、スズ酸化物を混入した酸化インジウムからなる
透明導゛亀膜(ITO) 5A、5Bを1μm程度の厚
ざに被着しである。この透明4に膜5A 。
For this reason, in the present invention, transparent conductive films (ITO) 5A and 5B made of indium oxide mixed with tin oxide are deposited on the outer surfaces of the vacuum vessel 10 facing each other in a thickness of about 1 μm. be. A film 5A is applied to this transparent material 4.

5B は、両対向M、N2A、2B間の放電経路を完全
にカバーするように、端部が電極2A、2Bのエツジ部
4A、 4Bに重なるように設けである。
5B is provided so that its end overlaps the edge portions 4A, 4B of the electrodes 2A, 2B so as to completely cover the discharge path between the opposing M, N2A, 2B.

そこで、これらの透明導電膜5A、5Bに図示のように
トリガ電源6を接続し、約20KV程度のトリガ電圧を
印加することにより、電極2A、 2B間の放電経路全
体にわたり放電の誘導路が形成でれ、全体に均一な放電
が行なわれる。なお、電極のエツジ部4A、4Bは高電
圧に耐えるように白金を用いた。
Therefore, by connecting a trigger power source 6 to these transparent conductive films 5A and 5B as shown in the figure and applying a trigger voltage of approximately 20 KV, a discharge guiding path is formed over the entire discharge path between the electrodes 2A and 2B. This results in uniform discharge throughout the area. Note that platinum was used for the edge portions 4A and 4B of the electrodes so as to withstand high voltage.

このような励起用ランプは、例えば第2図のようにして
用いられる。すなわち第2図(&)は本発明の励起用ラ
ンプを用いたスラブ形固体レーザ装置の構成例を示す斜
視図、同図伽)はb−b断面図、同図(C)はc −c
 @面図である。
Such an excitation lamp is used, for example, as shown in FIG. That is, FIG. 2 (&) is a perspective view showing a configuration example of a slab-type solid-state laser device using the excitation lamp of the present invention, FIG.
@ side view.

同図において、レーザ活性媒体11はリン酸塩系ガラス
(I、KG−8:保谷硝子製)を傾斜角45.4嘔6喘
、幅30朋の偏平菱形断面形状−に加工したもので、特
に人出射面と、入射光が多重反射を繰り返す平行な上下
対向主面は、平滑研磨して損失を極力少なくしている。
In the figure, the laser active medium 11 is made of phosphate glass (I, KG-8, manufactured by Hoya Glass Co., Ltd.) processed into a flat rhombic cross-sectional shape with an inclination angle of 45.4 mm and a width of 30 mm. In particular, the human exit surface and the parallel upper and lower opposing principal surfaces, where incident light undergoes multiple reflections, are polished smooth to minimize loss.

このレーザ活性媒体11は、その両側面が支持具12.
13に固着されて支持されている。また、その上記対向
主面からそれぞれ1〜3H程度の間隔を萱いて、それぞ
れ仕切板14.15が、支持具16.17および18゜
19に固N’Gれ支持でれて平行に配置されており、そ
の外側に、第1図に示したような励起用ランプ20.2
1が、それぞれ支持具22.23および24.25によ
り長手方向両側面を固着支持でれて配置されている。さ
らに励起用ランプ20゜21の外側に上カバー26およ
び下カバー27が配置されている。仕切板14.15は
、励起用ランプ20.21の励起光を透光する物質、本
実施例では石英ガラスにより形成されている。励起用ラ
ンプ20.21は、内部にXeガスが封入され、±切板
14.15から2〜5M程度離間して、その透明導電膜
5A、 5Bを被着した両対向主面がレーザ活性媒体1
1の上下対向主面に平行になるように配置されている。
This laser active medium 11 has supports 12 on both sides thereof.
13 and is supported. Furthermore, partition plates 14 and 15 are arranged parallel to each other at a distance of about 1 to 3 H from the opposing main surfaces, and are firmly supported by supports 16, 17 and 18°19. and on the outside thereof an excitation lamp 20.2 as shown in FIG.
1 are fixedly supported on both longitudinal sides by supports 22, 23 and 24, 25, respectively. Further, an upper cover 26 and a lower cover 27 are arranged outside the excitation lamp 20°21. The partition plates 14.15 are made of a material that transmits the excitation light from the excitation lamps 20.21, and in this embodiment is made of quartz glass. The excitation lamp 20.21 is filled with Xe gas, is spaced from the cutting plate 14.15 by about 2 to 5M, and has both opposing main surfaces covered with transparent conductive films 5A and 5B serving as a laser active medium. 1
They are arranged parallel to the vertically opposing main surfaces of 1.

さらに上カバー26、下カバー27の内面は上記ランプ
20.21の主面に平行に形成されてランプ20.21
から1〜5閣程度離間して配置され、かつそこには光反
射率を高くするために金メッキが施されてリフレクタと
して作用するようKしてらる。
Further, the inner surfaces of the upper cover 26 and the lower cover 27 are formed parallel to the main surface of the lamp 20.21.
They are placed at a distance of about 1 to 5 squares from each other, and are plated with gold to increase the light reflectance so that they act as reflectors.

上記構成において、入射光28は、レーザ活性媒体11
の入射面に垂直に入射した後、上下対向主面での多重反
射と表面励起とにより増幅されながら伝搬し、出射面か
ら出射光29として出射される。なお、入射面および出
射面側の双方にミラー30および31を、光軸に垂直に
配置することにより、固体レーザ発振装置が構成できる
In the above configuration, the incident light 28 is transmitted to the laser active medium 11
After being perpendicularly incident on the incident surface, the light propagates while being amplified by multiple reflections and surface excitation on the upper and lower opposing principal surfaces, and is emitted as output light 29 from the output surface. Note that a solid-state laser oscillation device can be constructed by arranging mirrors 30 and 31 perpendicular to the optical axis on both the incident surface and the exit surface side.

ここで、前述したように励起用ランプ20゜21はその
主面全体にわたって均一な放電を行なうことから、当該
主面に平行に配置でれたレーザ活性媒体11は、主面全
体にわたって均一な分布σ励起光を受ける。この結果、
温度および屈折率の分布も均一となる。特に、本構成例
ではレーザ活性媒体11と仕切板14.15との間、仕
切板14.15と励起用ランプ20.21との間、励起
用ランプ20.21と上カバー26および下カバー27
の間の離間部に冷却様体止して冷却水(純水)を流すこ
とにより、上述した均一化の効果は一層大きくなり、高
出力化が可能上なる。
Here, as mentioned above, since the excitation lamps 20 and 21 produce a uniform discharge over the entire main surface, the laser active medium 11 disposed parallel to the main surface has a uniform distribution over the entire main surface. Receives σ excitation light. As a result,
The temperature and refractive index distributions also become uniform. In particular, in this configuration example, between the laser active medium 11 and the partition plate 14.15, between the partition plate 14.15 and the excitation lamp 20.21, between the excitation lamp 20.21 and the upper cover 26 and the lower cover 27.
By flowing cooling water (pure water) with a cooling body in the space between the two, the above-mentioned uniformity effect becomes even greater, and higher output becomes possible.

また、励起用ランプの外周を冷却すると七は。Also, if the outer circumference of the excitation lamp is cooled, 7.

透明導電膜5A、 5Bの経年変化を防止する点でも有
効である。
This is also effective in preventing aging of the transparent conductive films 5A and 5B.

なお、上述した構成例において、例えばレーザ活性媒体
11は、それを構成する物質をNd: YAG。
In the configuration example described above, for example, the laser active medium 11 is made of Nd:YAG.

Nd:GGGまたはYLF等にしてもよいし、その形状
を入射角をブリュースタ角にした偏平菱形断面形状にし
、入射光と出射光とを平行にするなどしてもよい。また
上カバー26および下カバー27の内面は金メッキの代
りに銀メッキに酸化防止膜を施したものや、BIL80
4等の膜を施してもよく、これらの変更によって、本発
明の外部トリガ用透明導電膜を備えた偏平形状の励起用
ランプによる効果は何ら損われることはない。
It may be Nd:GGG or YLF, or it may have a flat rhombic cross-sectional shape with the incident angle set to Brewster's angle so that the incident light and the outgoing light are parallel. In addition, the inner surfaces of the upper cover 26 and lower cover 27 may be silver plated with an oxidation prevention film instead of gold plating, or BIL80
4 or the like may be applied, and these changes do not impair the effect of the flat-shaped excitation lamp provided with the external trigger transparent conductive film of the present invention.

また、励起用ランプ20.21の外側にブらにレーザ活
性媒体を重ねて配置し、あるいはさらにその外側に励起
用ランプ、レーザ活性媒体を多重に配置した構造にも、
本発明の励起用ランプは同様に適用して同様の効果を得
ることができる。
In addition, a structure in which the laser active medium is arranged in a layered manner on the outside of the excitation lamp 20, 21, or in which the excitation lamp and the laser active medium are arranged in multiple layers on the outside thereof, may also be used.
The excitation lamp of the present invention can be similarly applied to obtain similar effects.

以上、いわゆるスラブ形固体レーザ装置に使用する場合
を例に説明したが、本発明はこれに限定されるものでは
なく、例えば近年核融合の分野等で利用されている、ス
ラブ形のようにジグザグの光路をとるものではないが、
やはり板状のレーザ活性媒体を用いるディスクレーザ装
置などにも有効に使用できる。
The above description has been made using the case where the laser is used in a so-called slab-type solid-state laser device, but the present invention is not limited to this. Although it does not take the optical path of
It can also be effectively used in a disk laser device using a plate-shaped laser active medium.

また、上述した実施例では透明導電膜を真空容器の対向
主面のそれぞれに別々に設けたが、両者を輪状につなぎ
外周をとり囲むように被着してもよく、また片面のみに
設けてもよい。
Further, in the above embodiment, the transparent conductive film was separately provided on each of the opposing main surfaces of the vacuum container, but the two may be connected in a ring shape and coated so as to surround the outer periphery, or the transparent conductive film may be provided on only one surface. Good too.

さらに、透明導電膜としてはITO膜に限定されず、例
えば、酸化インジウム(In20B)もしくはこれにタ
ングステン(W)を添加したもの、または酸化スズ(S
nOa )にストロンチウム(sb)、フッ素(F)等
を添加したもののような、少なくともレーザ活性媒体の
有効吸収帯の光に対して透光性を有し、また実用上ある
程度耐食性を有する導電性膜であればよい。
Furthermore, the transparent conductive film is not limited to an ITO film, but includes, for example, indium oxide (In20B) or a film to which tungsten (W) is added, or tin oxide (S
A conductive film, such as one in which strontium (sb), fluorine (F), etc. are added to nOa), is transparent to at least light in the effective absorption band of the laser active medium, and has a certain degree of corrosion resistance in practical use. That's fine.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明によれば、励起用ランプを
板状のレーザ活性媒体の主面にほぼ平行な主面を有する
偏平状として帯状の対向電極を設け、しかも当該対向電
極間の放電経路に沿って、真空容器の少なくとも一方の
主面外表面に透光性を有する外部トリガ用導電性膜を被
着したことにより、板状のレーザ活性媒体をその主面全
体にわたって均一に励起することが可能となる。
As explained above, according to the present invention, the excitation lamp is formed into a flat shape having a main surface substantially parallel to the main surface of the plate-shaped laser active medium, and the strip-shaped opposing electrodes are provided, and the discharge between the opposing electrodes is provided. A light-transmitting conductive film for an external trigger is deposited on the outer surface of at least one main surface of the vacuum container along the path, so that the plate-shaped laser active medium is uniformly excited over the entire main surface of the vacuum container. becomes possible.

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

第1図(−)は本発明の一実施例を示す固体レーザ励起
用ランプの平面図、同図0)は−4王面図、同図(c)
は側面図、第2図(a)はこのランプを用いた固体レー
ザ装置の斜視図、同図(b)はb−bIfr面図、同図
(c)はc −a Ur面図である。 1・・・・真空容器、2A、2B・・・・対向1!1.
極、4A、4B・・・・エツジ部、5A、 5B・・・
・透明導電膜、11・・・・レーザ活性媒体、20.2
1・・・・励起用ランプ。
Figure 1 (-) is a plan view of a solid-state laser excitation lamp showing an embodiment of the present invention, Figure 1 (0) is a -4 king side view, Figure 1 (c) is
2 is a side view, FIG. 2(a) is a perspective view of a solid-state laser device using this lamp, FIG. 2(b) is a bbIfr plane view, and FIG. 2(c) is a c-a Ur plane view. 1...Vacuum container, 2A, 2B...Opposing 1!1.
Pole, 4A, 4B...Edge part, 5A, 5B...
・Transparent conductive film, 11...Laser active medium, 20.2
1... Excitation lamp.

Claims (1)

【特許請求の範囲】[Claims] 真空容器の内部に対向電極を備えた放電管からなり、板
状のレーザ活性媒体に隣接して配置されて当該レーザ活
性媒体の表面を光励起する固体レーザ励起用ランプにお
いて、真空容器はレーザ活性媒体の主面にほぼ平行な主
面を有する偏平形状で上記主面に沿つてほぼ平行に延在
する帯状の対向電極を備え、かつ当該対向電極間の放電
経路に沿つて、上記真空容器の少なくとも一方の主面外
表面に、少なくともレーザ活性媒体の有効吸収帯の光に
対して透光性を有する導電性膜を被着したことを特徴と
する固体レーザ励起用ランプ。
In a solid-state laser excitation lamp consisting of a discharge tube equipped with a counter electrode inside a vacuum vessel and placed adjacent to a plate-shaped laser active medium to optically excite the surface of the laser active medium, the vacuum vessel is the laser active medium. a flat-shaped counter electrode having a main surface substantially parallel to the main surface of the vacuum container and extending substantially parallel to the main surface; 1. A solid-state laser excitation lamp, characterized in that a conductive film that transmits at least light in an effective absorption band of a laser active medium is coated on the outer surface of one main surface.
JP18033484A 1984-08-31 1984-08-31 Lamp for solid-state laser excitation Expired - Lifetime JPH06105810B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18033484A JPH06105810B2 (en) 1984-08-31 1984-08-31 Lamp for solid-state laser excitation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18033484A JPH06105810B2 (en) 1984-08-31 1984-08-31 Lamp for solid-state laser excitation

Publications (2)

Publication Number Publication Date
JPS6159787A true JPS6159787A (en) 1986-03-27
JPH06105810B2 JPH06105810B2 (en) 1994-12-21

Family

ID=16081402

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18033484A Expired - Lifetime JPH06105810B2 (en) 1984-08-31 1984-08-31 Lamp for solid-state laser excitation

Country Status (1)

Country Link
JP (1) JPH06105810B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62176180A (en) * 1986-01-29 1987-08-01 Toshiba Corp Solid state laser oscillator
JPH02201980A (en) * 1989-01-30 1990-08-10 Fuji Electric Co Ltd Slab type solid-state laser oscillator

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62176180A (en) * 1986-01-29 1987-08-01 Toshiba Corp Solid state laser oscillator
JPH02201980A (en) * 1989-01-30 1990-08-10 Fuji Electric Co Ltd Slab type solid-state laser oscillator

Also Published As

Publication number Publication date
JPH06105810B2 (en) 1994-12-21

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