JPS5863188A - Linearly polarizing laser tube - Google Patents
Linearly polarizing laser tubeInfo
- Publication number
- JPS5863188A JPS5863188A JP16227181A JP16227181A JPS5863188A JP S5863188 A JPS5863188 A JP S5863188A JP 16227181 A JP16227181 A JP 16227181A JP 16227181 A JP16227181 A JP 16227181A JP S5863188 A JPS5863188 A JP S5863188A
- Authority
- JP
- Japan
- Prior art keywords
- plate
- glass plate
- laser tube
- slit
- spring
- 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
- 239000011521 glass Substances 0.000 claims abstract description 32
- 241000218645 Cedrus Species 0.000 claims description 4
- 230000010287 polarization Effects 0.000 abstract description 8
- 230000003247 decreasing effect Effects 0.000 abstract 1
- 239000005357 flat glass Substances 0.000 abstract 1
- 239000002184 metal Substances 0.000 description 9
- 239000000463 material Substances 0.000 description 6
- 238000000034 method Methods 0.000 description 4
- 238000004519 manufacturing process Methods 0.000 description 3
- 239000000853 adhesive Substances 0.000 description 2
- 230000001070 adhesive effect Effects 0.000 description 2
- 238000005530 etching Methods 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 229910000679 solder Inorganic materials 0.000 description 2
- 238000004026 adhesive bonding Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005489 elastic deformation Effects 0.000 description 1
- 238000005304 joining Methods 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 238000003825 pressing Methods 0.000 description 1
- 238000003672 processing method Methods 0.000 description 1
- 230000008646 thermal stress Effects 0.000 description 1
- 238000003466 welding 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
- H01S3/034—Optical devices within, or forming part of, the tube, e.g. windows, mirrors
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】
本発明はガスレーザ管、特に内部ミラー形直線偏光レー
ザ管の管内にブリュースタ角を有するガラス板を取付け
るための保持構造に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a holding structure for mounting a glass plate having a Brewster angle in a gas laser tube, particularly an internally mirrored linearly polarized laser tube.
一般に、ガスレーザ管にはブリ、−スタ角を有するブリ
、−メタ窓が設けられることが多い。特に外部ミラー形
レーザ管では管端に窓が取付けられ、光学的共振器用ミ
ラーをレーザ管に独立に配置しであるので、管端に取付
けられた窓をブリュースタ角を有する様に取付けること
は容易である。Generally, a gas laser tube is often provided with a burr, a burr having a -star angle, and a -meta window. In particular, in external mirror type laser tubes, a window is attached to the tube end, and the optical resonator mirror is arranged independently on the laser tube, so it is difficult to install the window attached to the tube end so that it has Brewster's angle. It's easy.
しかしながら、内部ミラー形レーザ管では、両管端に光
学的共振器用ミラーが設けられているため、管端にブリ
ュースタ窓を設けることは不可能となる。ガスレーザ管
では、このブリュースタ窓を共振器内に設けることで発
振レーザ光の偏光方向を一方向に決めることが可能とな
る。又、He−Neガスレーザでは0.6328μmの
光の他に3.39μmの光が誘導放射をしてしまうが、
このブリ、−メタ窓を設けることで3.39μmの発振
を抑制することもで負る。この様な内部ミラー形ガスレ
ーザ管においてブリ、−メタ窓を設けた従来構成例を示
すのが第6〜7図である。第6図では、ガスレーザ管端
の一部を拡大した図であυ、101はガスを封入スるレ
ーザ管本体である。このレーザ管本体1の端部をブリュ
ースタ角を有する様に傾斜させその傾斜させた端面にブ
リュースタ窓用のガラス板102を接着固定させている
。更に、このガラス板102のレーザ管本体1と接着し
た側と反対側に、ブリュースタ角を有する様に端面を傾
斜させた管103をガラス板102に接着する。この管
103の他端にはミラー104をレーザ軸と垂直に設け
である。この様な構成の場合、ガラス板を接着する面を
ブリュースタ面に傾斜させねばならず製作が困難且つ高
価であり、接合部の気密性でも問題を生じることがある
。又、第7図では金属封入皿105を有するガスレーザ
管の一端を拡大した図であり、この金属外筒105に内
接する一端をブリュースタ角に傾斜させた一対の金属内
筒106.106’によりガラス板102を挟持する構
成となっている。し□
かし、この様な構成の場合、わずかな隙間が生じ易くガ
ラス板102が衝撃で移動して偏光度が狂ったわ、レー
ザ出力が低下することがあるため金属外筒105よ如金
属内筒106.106’の熱膨張率を低いものを選び、
高温で組立てることによって内外の収縮差による熱応力
によってガラス板102を強く挟持する方法が採られる
が、これとてガラス板102に内部歪が生じるため、レ
ーザ出力や偏光度が低下する難点がある。本発明はこれ
らの欠点を除き、価格・量産性に優れ、レーザ出力や偏
光度を損うことなくレーザ管内にブリュースタ窓をすべ
ての方向に移動しない様に保持した直線偏光レーザ管を
提供するものである。However, in an internal mirror type laser tube, since optical resonator mirrors are provided at both tube ends, it is impossible to provide a Brewster window at the tube ends. In a gas laser tube, by providing this Brewster window in the resonator, it becomes possible to determine the polarization direction of the oscillated laser light in one direction. Also, in the He-Ne gas laser, in addition to the 0.6328 μm light, 3.39 μm light is stimulated to emit light.
By providing this burr-metal window, 3.39 μm oscillation can also be suppressed. FIGS. 6 and 7 show examples of conventional configurations in which such an internal mirror type gas laser tube is provided with a burr-metal window. FIG. 6 is an enlarged view of a part of the end of the gas laser tube, and 101 is the laser tube body in which gas is sealed. The end of the laser tube body 1 is inclined to have a Brewster's angle, and a glass plate 102 for a Brewster window is adhesively fixed to the inclined end face. Further, on the opposite side of the glass plate 102 to the side bonded to the laser tube main body 1, a tube 103 whose end face is inclined to have Brewster's angle is bonded to the glass plate 102. At the other end of this tube 103, a mirror 104 is provided perpendicular to the laser axis. In the case of such a structure, the surface to which the glass plate is bonded must be inclined to the Brewster surface, which is difficult and expensive to manufacture, and there may be problems with the airtightness of the joint. FIG. 7 is an enlarged view of one end of the gas laser tube having a metal enclosure dish 105, and a pair of metal inner tubes 106 and 106', one end of which is inscribed in the metal outer tube 105, is inclined at Brewster's angle. It is configured to sandwich the glass plate 102. However, in such a configuration, a slight gap is likely to occur, and the glass plate 102 moves due to the impact, causing the degree of polarization to go awry.The laser output may also decrease, so it is important to avoid contact with the metal outer cylinder 105. Select the inner cylinder 106.106' with a low coefficient of thermal expansion,
A method is adopted in which the glass plate 102 is strongly clamped by thermal stress due to the difference in shrinkage inside and outside by assembling at a high temperature, but this creates internal distortion in the glass plate 102, which has the disadvantage of reducing laser output and polarization degree. . The present invention eliminates these drawbacks, provides a linearly polarized laser tube that is excellent in cost and mass production, and retains the Brewster window within the laser tube so as not to move in any direction without impairing the laser output or degree of polarization. It is something.
即ち、ブリュースタ角度にスリットを切ったコの字形弾
性形板材がガラス板を側面および端面よりバネ状突起に
よって固定すると共に、前記杉板材自体がレーザ管内に
弾性的にあるいは他の接合方法によシ保持される様にし
た構造を特徴とする。That is, a U-shaped elastic plate with a slit cut at the Brewster angle fixes the glass plate from the side and end surfaces by spring-like protrusions, and the cedar plate itself is inserted into the laser tube elastically or by other joining methods. It is characterized by a structure that allows it to be held in place.
以下に本発明について実施例を用いて詳細に説明する。The present invention will be described in detail below using examples.
第1図は本発明の一夾施例を示すガスレーザ管の断面図
であり、第2図は第1図の左端の分解図である。両図に
おいて1はブリ、−メタ窓用ガラス板であり、コの字形
弾性杉板10の対向する板の両側にレーザ軸線方向にブ
リュースタ角をなす様に形成されたスリット11に、矢
印Cで示す方向より挿入されている。スJy)110両
端にはガラス板1と平行にバネ状突起12が設けられ、
スリット11の中央部にはガラス板1と垂直にバネ状突
起13が設けられている。又、対向する板はレーザ光が
通過する穴14を具えた板で互いに接続されており、こ
の様な形板材10はプレスやエツチング等の容易な加工
法により安価にしかも一体構造として得られる。前記形
板の材料としては比較的高温でも弾性を失わぬ耐熱バネ
用金属等が使用される。9はガラス−金属等の庇付の円
筒であり一端はレーザ管本体4に接続されており、開放
した他端からガラス板1を保持したコの字形板材10が
挿入される。この詩形板材10の対向した板の部分は予
め円筒9の内径よシ僅かに大きく広げておき、形板材の
弾性を利用して円−筒9内に固定される様にすると共に
レーザ軸線方向に対しては円筒9の底とぐラー2によっ
て挟持され半田カラス・高気密接着剤等3で固定される
。FIG. 1 is a sectional view of a gas laser tube showing one embodiment of the present invention, and FIG. 2 is an exploded view of the left end of FIG. In both figures, reference numeral 1 denotes a glass plate for a Buri-meta window, and a slit 11 formed at a Brewster's angle in the direction of the laser axis is formed on both sides of the U-shaped elastic cedar plate 10 to form a Brewster's angle. It is inserted in the direction shown by . Spring-like protrusions 12 are provided at both ends of the glass plate 1 in parallel with the glass plate 1,
A spring-like protrusion 13 is provided in the center of the slit 11 perpendicularly to the glass plate 1. Further, the opposing plates are connected to each other by a plate having a hole 14 through which the laser beam passes, and such a shaped plate material 10 can be obtained as an inexpensive and integral structure by an easy processing method such as pressing or etching. As the material for the shape plate, a heat-resistant spring metal or the like that does not lose its elasticity even at relatively high temperatures is used. Reference numeral 9 is a cylinder made of glass-metal or the like with an eave, one end of which is connected to the laser tube main body 4, and a U-shaped plate member 10 holding the glass plate 1 is inserted from the open other end. The opposing plate portions of this poem-shaped plate material 10 are made in advance slightly wider than the inner diameter of the cylinder 9, so that they can be fixed inside the cylinder 9 by utilizing the elasticity of the shaped plate material, and in the direction of the laser axis. On the other hand, it is held between the bottom puller 2 of the cylinder 9 and fixed with a solder crow, high-tight adhesive, etc. 3.
5−
5は陰極、6はレーザ細管、7は陰極導入棒、8は陽極
である。5 - 5 is a cathode, 6 is a laser tube, 7 is a cathode introduction rod, and 8 is an anode.
M3.4.5図は、酊2図においてそれぞれ矢印A、B
、Cから見た矢視図である。これらの図を用いてガラス
板1が保持される形板材10の作用について説明する。Figure M3.4.5 shows arrows A and B in Figure 2, respectively.
, is a view seen from arrow C. The action of the plate material 10 on which the glass plate 1 is held will be explained using these figures.
第4図に示す様KCの方向から形板材10のスリ、ト1
1に挿入されたガラス板1は、スリットの両端に設けら
れたバネ状突起12a、12b、12c。As shown in FIG.
The glass plate 1 inserted into the slit has spring-like protrusions 12a, 12b, and 12c provided at both ends of the slit.
12dによってガラス板の側面を矢印りで示す4つの方
向から押付けられるため水平方向に固定されると同時に
、第5図で示す様にスリット巾より予め催かに出る様に
形成されたバネ状突起taaおよび13bにより垂直方
向にも固定される。こうしてガラス板1を保持した形板
材10は第3図に示す円筒9の内側に挿入される際前記
バネ状突起12a112b、 12c、 12dの反力
によシ対向する板が相互に広がろうとするため形板の有
する4本の稜線で円筒の内側に移動することなく正確な
ブリュースタ角で固定される。しかもガラス板1はレー
ザ光6−
が通過する中心部を避けた周辺部を線接触ないしは点接
触で保持されるためガラス板の内部歪の影響が少なくな
り出力や偏光度の低下が極めて少い。12d presses against the side surface of the glass plate from the four directions indicated by the arrows, so it is fixed in the horizontal direction, and at the same time, as shown in Figure 5, a spring-like protrusion is formed in advance to protrude from the slit width. It is also fixed in the vertical direction by taa and 13b. When the shaped plate 10 holding the glass plate 1 is inserted into the cylinder 9 shown in FIG. 3, the opposing plates tend to spread apart due to the reaction force of the spring-like protrusions 12a112b, 12c, and 12d. The four ridgelines of the retainer plate allow it to be fixed at an accurate Brewster's angle without moving inside the cylinder. Moreover, since the glass plate 1 is held in line contact or point contact in the peripheral area, avoiding the center area through which the laser beam 6- passes, the influence of internal distortion of the glass plate is reduced, and the decrease in output and polarization degree is extremely small. .
以上の方法によれば、偏光用プリー−メタ窓がレーザ管
内においてすべての方向に移動しない様な耐衝撃性をレ
ーザ出力や偏光度を損うことなく得られると共に、保持
用の形板材がプレス、エツチングなどで容易にでき、ガ
ラス板をレーザ管内に組込む作業が容易になる々ど製造
コストや量産性の面でも優れている。According to the above method, it is possible to obtain impact resistance that prevents the polarizing pre-metal window from moving in all directions within the laser tube without damaging the laser output or the degree of polarization, and the holding shape plate is pressed. This can be easily done by etching, etc., making it easier to assemble the glass plate into the laser tube, and is also superior in terms of manufacturing costs and mass productivity.
上記実施例においてコの字形弾性形板材は第2図〜第5
図の実施例の形状に留まらず、コの字の開放面の方向の
変形やスリットを有する板が円筒面や多角形の断面を有
するものであってもよいし、バネ状突起の数、位置、弾
性変形方向等も上記実施例に限らガい。又、形板材を保
持する相手は、円筒などの様に杉板全体を収納する形状
に限らず、。In the above embodiment, the U-shaped elastic plate material is shown in Figures 2 to 5.
The shape is not limited to the shape of the embodiment shown in the figure, and the U-shaped open surface may be deformed in the direction, the plate with slits may have a cylindrical surface or a polygonal cross section, and the number and position of the spring-like projections may be changed. , the elastic deformation direction, etc. are also limited to the above embodiments. Also, the object that holds the shaped board is not limited to a shape that accommodates the entire cedar board, such as a cylinder.
彫版の一部を溶接・接着等の方法でレーザ管の部品に固
定しても上記実施例と同様な効果が得られる。Even if a part of the engraving is fixed to a part of the laser tube by a method such as welding or gluing, the same effect as in the above embodiment can be obtained.
第1図は本発明の一実施例を示す内部ミラー形直線偏光
ガスレーザ管の断面図、嬉2図は第1図の左端にあるガ
ラス板保持部の分解図、第3図は第2図におけるA矢視
図、第4図は第2図におけるB矢視図、第り図は第2図
のC矢視部分断面図、第6図および第7図はそれぞれ従
来の実施例2種を示すレーザ管左端部の部分断面図であ
る。
1・・・・・・ガラス板、2・・・・・・きラー、3・
・・・・・半田ガラス、高気密接着剤、4・・・・・・
レーザ管本体、5・・・・・・陰極、6・・・・・・レ
ーザ細管、7・・・・・・陰極導入棒、8・・・・・・
陽極、9・・・・・・円筒、10・・・・・・コの字形
弾性形板材、11・・・・・・スIJ 、 )、12.
13・・・・・・バネ状突起、14・・・・・・穴。Fig. 1 is a cross-sectional view of an internal mirror type linearly polarized gas laser tube showing an embodiment of the present invention, Fig. 2 is an exploded view of the glass plate holder at the left end of Fig. 1, and Fig. 3 is an exploded view of the glass plate holder at the left end of Fig. 2. A view in the direction of the arrow A, FIG. 4 is a view in the direction of the B arrow in FIG. 2, a partial sectional view in the direction of the C arrow in FIG. FIG. 3 is a partial cross-sectional view of the left end of the laser tube. 1...Glass plate, 2...Killer, 3.
...Solder glass, high airtight adhesive, 4...
Laser tube body, 5... cathode, 6... laser thin tube, 7... cathode introduction rod, 8...
Anode, 9...Cylinder, 10...U-shaped elastic plate, 11...S IJ, ), 12.
13... Spring-like protrusion, 14... Hole.
Claims (1)
ラス板がブリュースタ角で配設される内部ミラー形直線
偏光レーザ管において、コの字形弾性杉板材の対向する
板のレーザ軸線方向にブリ、−スタ角度にスリットを設
けふと共に、ガラス板側面の少くとも2方向以上に働く
スリット端のバネ状突起およびガラス板の端面に垂直に
働くスリット中央部のバネ状突起とを有し、前記スリッ
トにガラス板を押えつけて保持することを特徴とする直
線偏光レーザ管。In an internal mirror type linearly polarized laser tube, in which a glass plate in addition to the laser thin tube is arranged at Brewster's angle between a pair of opposing mirrors, the laser axis direction of the opposing plates of U-shaped elastic cedar plates is used. In addition to providing a slit at a vertical angle, the glass plate has a spring-like protrusion at the end of the slit that acts in at least two directions on the side surface of the glass plate, and a spring-like protrusion at the center of the slit that acts perpendicularly to the end surface of the glass plate. . A linearly polarized laser tube, characterized in that a glass plate is pressed and held in the slit.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16227181A JPS5863188A (en) | 1981-10-12 | 1981-10-12 | Linearly polarizing laser tube |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16227181A JPS5863188A (en) | 1981-10-12 | 1981-10-12 | Linearly polarizing laser tube |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5863188A true JPS5863188A (en) | 1983-04-14 |
Family
ID=15751282
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP16227181A Pending JPS5863188A (en) | 1981-10-12 | 1981-10-12 | Linearly polarizing laser tube |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5863188A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60167353U (en) * | 1984-04-13 | 1985-11-06 | 日本電気株式会社 | Linearly polarized laser tube |
-
1981
- 1981-10-12 JP JP16227181A patent/JPS5863188A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60167353U (en) * | 1984-04-13 | 1985-11-06 | 日本電気株式会社 | Linearly polarized laser tube |
JPH0310682Y2 (en) * | 1984-04-13 | 1991-03-15 |
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