JPH03240284A - Ring type laser device - Google Patents
Ring type laser deviceInfo
- Publication number
- JPH03240284A JPH03240284A JP3632590A JP3632590A JPH03240284A JP H03240284 A JPH03240284 A JP H03240284A JP 3632590 A JP3632590 A JP 3632590A JP 3632590 A JP3632590 A JP 3632590A JP H03240284 A JPH03240284 A JP H03240284A
- Authority
- JP
- Japan
- Prior art keywords
- getter
- medium
- recess
- angle
- diameter
- 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
- 230000003287 optical effect Effects 0.000 claims description 17
- 230000001105 regulatory effect Effects 0.000 claims description 7
- 230000007423 decrease Effects 0.000 abstract description 3
- 230000004308 accommodation Effects 0.000 description 27
- 239000007789 gas Substances 0.000 description 8
- 230000002093 peripheral effect Effects 0.000 description 5
- 230000000694 effects Effects 0.000 description 3
- 238000010438 heat treatment Methods 0.000 description 3
- 239000012535 impurity Substances 0.000 description 2
- 239000003463 adsorbent Substances 0.000 description 1
- 229910052788 barium Inorganic materials 0.000 description 1
- DSAJWYNOEDNPEQ-UHFFFAOYSA-N barium atom Chemical compound [Ba] DSAJWYNOEDNPEQ-UHFFFAOYSA-N 0.000 description 1
- 230000035559 beat frequency Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000008020 evaporation Effects 0.000 description 1
- 238000001704 evaporation Methods 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 230000006698 induction Effects 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 230000010355 oscillation Effects 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
- H01S3/036—Means for obtaining or maintaining the desired gas pressure within the tube, e.g. by gettering, replenishing; Means for circulating the gas, e.g. for equalising the pressure within the tube
-
- 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
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/08—Construction or shape of optical resonators or components thereof
- H01S3/081—Construction or shape of optical resonators or components thereof comprising three or more reflectors
- H01S3/083—Ring lasers
-
- 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
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/08—Construction or shape of optical resonators or components thereof
- H01S3/081—Construction or shape of optical resonators or components thereof comprising three or more reflectors
- H01S3/083—Ring lasers
- H01S3/0835—Gas ring lasers
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】
[発明の目的]
(産業上の利用分野)
この発明はリングレーザジャイロなどに用いられるリン
グ型レーザ装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) The present invention relates to a ring-shaped laser device used in a ring laser gyro or the like.
(従来の技術)
たとえば、リングレーザジャイロに用いられるリング型
レーザ装置は、閉環状の光路内に互いに逆方向に進行す
るレーザ光を発振させ、装置全体が回転すると、その二
つのレーザ光に光路差が生じ(サニヤック効果)、この
光路差が互いに逆方向に進行する二つのレーザ光間に周
波数差を生じさせる。この二つのレーザ光を重ね合わせ
ると、ビート周波数をもった干渉縞ができることを利用
してその回転角速度を測定できるように構成されている
。(Prior art) For example, a ring laser device used in a ring laser gyro oscillates laser beams that travel in opposite directions within a closed annular optical path, and when the entire device rotates, the two laser beams are separated into two optical paths. A difference occurs (Sagnac effect), and this optical path difference causes a frequency difference between the two laser beams traveling in opposite directions. When these two laser beams are superimposed, interference fringes with a beat frequency are formed, which can be used to measure the rotational angular velocity.
従来、このようなリング型レーザ装置は第4図と第5図
とに示すように構成されていた。第4図中1は極めて低
い熱膨張係数をもった単体のガラスブロックでほぼ矩形
状に作られた本体である。Conventionally, such a ring-type laser device has been constructed as shown in FIGS. 4 and 5. Reference numeral 1 in FIG. 4 indicates a main body made of a single glass block having an extremely low coefficient of thermal expansion and having an approximately rectangular shape.
この本体1にはガスレーザ媒質が封入された矩形リング
状の細い光路2が穿設されている。この光路2のコーナ
部にはガス溜め用の収容凹部3が上記本体1の角部外面
に開口して形成され、この開口は反射ミラー4によって
気密に閉塞されている。This main body 1 has a narrow rectangular ring-shaped optical path 2 in which a gas laser medium is sealed. At the corner of this optical path 2, a housing recess 3 for a gas reservoir is formed by opening on the outer surface of the corner of the main body 1, and this opening is hermetically closed by a reflecting mirror 4.
また、本体1には、一端が上記光路2に連通し他端が本
体1の外周面に開口した第1の通孔5I!、、この第1
の通孔5に対して対称に一対の第2の通孔6とが穿設さ
れている。上記第1の通孔5の他端に対向する本体1の
外面には陰極7が気密に設けられ、第2の通孔6の他端
に対向する本体1の外面にはそれぞれ陽極8が気密に設
けられている。The main body 1 also has a first through hole 5I, which has one end communicating with the optical path 2 and the other end opening on the outer peripheral surface of the main body 1! ,,this first
A pair of second through holes 6 are bored symmetrically with respect to the through hole 5 . A cathode 7 is airtightly provided on the outer surface of the main body 1 facing the other end of the first through hole 5, and an anode 8 is airtightly provided on the outer surface of the main body 1 facing the other end of the second through hole 6. It is set in.
さらに、4つの収容凹部3のうちの2つにはゲッター9
が配置されている。このゲッター9は第5図に示すよう
に断面コ字状の部材によって収容凹部3よりも小径なリ
ング状に形成され、その溝部9aにはバリウム(Ba)
などの吸着剤からなるゲッター媒質11が充填されてい
る。そして、ゲッター9は溝部9aの開放端を反射ミラ
ー4と反対側である収容凹部3の底部3aに向けて保持
部材12により保持されている。Furthermore, getters 9 are provided in two of the four accommodation recesses 3.
is located. As shown in FIG. 5, the getter 9 is formed into a ring shape with a smaller diameter than the accommodation recess 3 by a member having a U-shaped cross section, and the groove 9a is filled with barium (Ba).
A getter medium 11 made of an adsorbent such as the like is filled. The getter 9 is held by a holding member 12 with the open end of the groove 9a facing the bottom 3a of the accommodation recess 3, which is the side opposite to the reflecting mirror 4.
このような構成においては、陰極7と陽極8との間に放
電電流を流すと、光路2に収容されたガスレーザ媒質が
光励起されて逆向きの2つのレーザ光が発生して光路2
内を走るから、これらレーザ光の光路差によって本体1
の回転を測定することができる。また、光路2内のガス
レーザ媒質の励起を繰返すことでその純度が低下すると
、1ノーザ光の出力も低下する。そのような状態を防ぐ
ために、レーザ媒質を導入する前に、ゲッター9をたと
えば高周波誘導加熱などの手段によって外部から加熱し
、ゲッター媒質11を蒸発飛散させて収容凹部3の底部
に蒸着させる。それによって、ガスレーザ媒質中の不純
物ガスを吸着することができるから、レーザ媒質の純度
を上げることができる。In such a configuration, when a discharge current is passed between the cathode 7 and the anode 8, the gas laser medium accommodated in the optical path 2 is optically excited, and two laser beams in opposite directions are generated, and the optical path 2
Because the laser beams run inside the main body 1, the optical path difference between these laser beams
rotation can be measured. Moreover, if the purity of the gas laser medium in the optical path 2 decreases due to repeated excitation, the output of one laser beam also decreases. In order to prevent such a situation, before introducing the laser medium, the getter 9 is heated from the outside by means such as high-frequency induction heating, and the getter medium 11 is evaporated and scattered to be deposited on the bottom of the accommodation recess 3. This allows impurity gases in the gas laser medium to be adsorbed, thereby increasing the purity of the laser medium.
しかしながら、ゲッター9の加熱が急速であったりする
と、蒸発飛散されたゲッター媒質11の蒸発速度が速く
なるから、第5図に矢印aで示すようにゲッター媒質1
1が収容凹部3の底部3aで反射してゲッター9の内径
部分を通過し、収容凹部3に対向して設けられた反射ミ
ラー4に衝突して付着することがある。ゲッター媒質1
1が反射ミラー4に付着すれば、レーザ光に対して散乱
などの損失原因となるばかりか、最悪の場合は1ノーザ
光の発振が停止することがある。However, if the getter 9 is heated rapidly, the evaporation rate of the evaporated getter medium 11 becomes faster.
1 may be reflected by the bottom 3a of the accommodation recess 3, pass through the inner diameter portion of the getter 9, and collide with and adhere to the reflection mirror 4 provided opposite to the accommodation recess 3. Getter medium 1
If 1 adheres to the reflecting mirror 4, it not only causes loss such as scattering of the laser beam, but in the worst case, the oscillation of the 1 noser light may stop.
(発明が解決しようとする課題)
このように、従来のリング型レーザ装置においては、ゲ
ッター媒質を蒸発飛散させたときに、収容凹部で反射し
たゲッター媒質が反射ミラーに付着するということがあ
った。(Problem to be Solved by the Invention) As described above, in the conventional ring-type laser device, when the getter medium is evaporated and scattered, the getter medium reflected at the accommodation recess may adhere to the reflection mirror. .
この発明は上記事情にもとずきなされたもので、その目
的とするところは、ゲッターを加熱することによって蒸
発飛散して収容凹部で反射したゲッター媒質が反射ミラ
ーに付着しずらいようにしたリング型レーザ装置を提供
することにある。This invention was made based on the above-mentioned circumstances, and its purpose is to make it difficult for the getter medium that is evaporated and scattered by heating the getter and reflected at the accommodation recess to adhere to the reflecting mirror. An object of the present invention is to provide a ring-type laser device.
[発明の構成]
(課題を解決するための手段及び作用)上記課題を解決
するためにこの発明は、複数の反射ミラーを光路の所定
位置に設けてリング状先路を形成した本体と、この本体
の上記反射ミラーの反射面と対向する部位に上記光路に
連通して形成された収容凹部と、この収容凹部内の上記
反射面と対向する位置に設けられたゲッターとを備え、
上記収容凹部の底部は上記ゲッターから蒸発飛散したゲ
ッター媒質を上記反射面以外の部位に反射させる規制部
に形成する。[Structure of the Invention] (Means and Effects for Solving the Problems) In order to solve the above problems, the present invention includes a main body in which a plurality of reflecting mirrors are provided at predetermined positions of an optical path to form a ring-shaped path; an accommodating recess formed in a portion of the main body facing the reflective surface of the reflective mirror so as to communicate with the optical path; and a getter provided in the accommodating recess at a position facing the reflective surface,
The bottom of the housing recess is formed as a regulating portion that reflects the getter medium evaporated and scattered from the getter to a portion other than the reflecting surface.
このような構成によれば、蒸発飛散したゲッター媒質が
収容凹部から出る方向へ反射するのを収容凹部の底部に
設けられた規制部によって防止できるから、ゲッター媒
質が収容凹部に対向して配置された反射ミラーに付着す
るのを防止できる。According to such a configuration, the regulating part provided at the bottom of the accommodation recess can prevent the evaporated and scattered getter medium from being reflected in the direction of exiting the accommodation recess, so that the getter medium is disposed facing the accommodation recess. This prevents the liquid from adhering to the reflective mirror.
(実施例)
以下、この発明の一実施例を第1図乃至第3図を参照し
て説明する。なお、第4図と第5図とに示す従来構成と
同一部分には同一記号を付して説明を省略する。(Embodiment) An embodiment of the present invention will be described below with reference to FIGS. 1 to 3. Note that the same parts as those in the conventional structure shown in FIGS. 4 and 5 are given the same symbols, and the description thereof will be omitted.
すなわち、この発明のリング型レーザ装置においては、
ゲッター9が保持された収容凹部3の底部3aに規制部
としての円錐状の凸部21が設けられている。第1図に
示すように凸部21の頂角をA1この凸部21の最大径
をC1ゲッター9の外径をD1内径をdとすると、D>
C>dの関係を満足するよう上記凸部21の最大径Cが
設定されている。また、上記凸部21の頂部から2本の
延長線gを、これら延長線gの挟角Xが上記頂角Aと等
しい角度となるよう延長したとき、これら延長線gの間
隔がゲッター9の外径りと等しくなるゲッター9の位置
をBとすると、ゲッター9はBの位置もしくはBの位置
と収容凹部3の底部3aとの間の位置に配置される。That is, in the ring laser device of the present invention,
A conical convex portion 21 as a regulating portion is provided at the bottom 3a of the accommodation recess 3 in which the getter 9 is held. As shown in FIG. 1, if the apex angle of the convex part 21 is A1, the maximum diameter of this convex part 21 is C1, the outer diameter of the getter 9 is D1, and the inner diameter is d, then D>
The maximum diameter C of the convex portion 21 is set so as to satisfy the relationship C>d. Further, when two extension lines g are extended from the top of the convex portion 21 so that the included angle X of these extension lines g is equal to the apex angle A, the interval between these extension lines g is Assuming that the position of the getter 9 that is equal to the outer diameter is B, the getter 9 is disposed at the position B or at a position between the position B and the bottom 3a of the accommodation recess 3.
このように、収容凹部3の底部3aに円錐状の凸部21
を設けるとともに、収容凹部3の軸方向におけるゲッタ
ー9の設置位置を上記Bの位置もしくはBの位置と底部
3aとの間にすれば、ゲッター9を加熱することによっ
て蒸発飛散するゲラター媒質11は、たとえば第1図に
矢印す、〜べ0−
す、で示すように収容凹部3″に==I6反射しても、
この収容凹部3から出る方向、つまりゲッター9の内径
部分を通過する方向に反射するのが防止される。In this way, the conical protrusion 21 is formed on the bottom 3a of the accommodation recess 3.
If the getter 9 is installed at the position B in the axial direction of the housing recess 3 or between the position B and the bottom 3a, the gelater medium 11 that evaporates and scatters by heating the getter 9 will be For example, even if ==I6 is reflected in the accommodation recess 3'' as shown by the arrows in Fig. 1,
This prevents the light from being reflected in the direction of exiting from the accommodation recess 3, that is, the direction of passing through the inner diameter portion of the getter 9.
すなわち、同図中矢印b1はゲッター9から蒸発飛散し
たゲッター媒質11が収容凹部3の径方向中心に向かっ
て進行した場合で、その場合には凸部21の表面に衝突
する。凸部21の表面は角度A/2で傾斜しているから
、ゲッター媒質11はその表面で入射角と等しい角度で
反射し、収容凹部3の内周面に衝突して付着する。That is, the arrow b1 in the figure indicates a case where the getter medium 11 evaporated and scattered from the getter 9 advances toward the radial center of the accommodation recess 3, in which case it collides with the surface of the convex portion 21. Since the surface of the convex portion 21 is inclined at an angle of A/2, the getter medium 11 is reflected from the surface at an angle equal to the incident angle, collides with the inner circumferential surface of the accommodation recess 3, and adheres thereto.
また、矢印b2はゲッター媒質11が収容凹部3の底面
3aの凸部21以外の部分に直接衝突した場合である。Further, arrow b2 indicates a case where the getter medium 11 directly collides with a portion of the bottom surface 3a of the accommodation recess 3 other than the convex portion 21.
上記凸部21の最大径Cはゲッター9の内径dよりも大
きく設定されているから、ゲッター媒質11は収容凹部
3の径方向外方に傾斜した角度で底部3aに衝突するか
ら、底部3aで反射したゲッター媒質11が上記ゲッタ
ー9の内径部分を通過することはなく、収容凹部3の内
周面や保持部材12に衝突して付着する。Since the maximum diameter C of the convex portion 21 is set larger than the inner diameter d of the getter 9, the getter medium 11 collides with the bottom portion 3a of the accommodation recess 3 at an angle inclined outward in the radial direction. The reflected getter medium 11 does not pass through the inner diameter portion of the getter 9, but collides with and adheres to the inner peripheral surface of the accommodation recess 3 and the holding member 12.
また、矢印Cはゲッター媒質11が収容凹部3の内周面
に直接衝突した場合で、その場合は収容凹部3の内周面
で反射したゲッター媒質11のほとんどは凸部21に表
面に衝突して付着する。Further, arrow C indicates a case where the getter medium 11 directly collides with the inner peripheral surface of the housing recess 3. In this case, most of the getter medium 11 reflected on the inner peripheral surface of the housing recess 3 collides with the surface of the convex portion 21. It sticks to the surface.
このように、ゲッター9から蒸発飛散するゲッター媒質
11のほとんどは、収容凹部3の内周面や凸部21の表
面に付着し、上記ゲッター9の内径部分を通過して反射
ミラー4に付着するということがない。したがって、ガ
スレーザ媒質に含まれる不純物ガスを吸着するために、
ゲッター媒質11を蒸発飛散させても、それによって反
射ミラー4の性能低下を招くのを防止できる。In this way, most of the getter medium 11 that evaporates and scatters from the getter 9 adheres to the inner peripheral surface of the accommodation recess 3 and the surface of the convex portion 21, passes through the inner diameter portion of the getter 9, and adheres to the reflection mirror 4. There is no such thing. Therefore, in order to adsorb impurity gas contained in the gas laser medium,
Even if the getter medium 11 is evaporated and scattered, it is possible to prevent the performance of the reflecting mirror 4 from being degraded.
この発明は上記一実施例に限定されず、その要旨を逸脱
しない範囲で種々変形可能である。たとえば、収容凹部
の底部に設けられる規制部を円錐状の凸部としたが、半
球状や半楕円状などの凸部であってもよく、さらには凸
部に代わり凹部であってもよく、要はゲッターから飛散
するゲッター媒質がゲッターの内径部分を通過する方向
に反射することがない形状であればよい。This invention is not limited to the one embodiment described above, and can be modified in various ways without departing from the gist thereof. For example, although the regulating portion provided at the bottom of the accommodation recess is a conical convex portion, it may be a hemispherical or semi-elliptical convex portion, or even a concave portion may be used instead of the convex portion. In short, any shape is sufficient as long as the getter medium scattered from the getter is not reflected in the direction of passing through the inner diameter portion of the getter.
また、この発明を適用することができるリング型レーザ
装置の光路は四角形に限られず、三角形のものであって
もよい。Furthermore, the optical path of a ring laser device to which the present invention can be applied is not limited to a rectangular shape, but may be triangular.
[発明の効果コ
以上述べたようにこの発明は、ゲッターが保持される収
容凹部の底部に、上記ゲッターから蒸発飛散したゲッタ
ー媒質が上記反射ミラーに付着する方向へ反射するのを
阻止する規制部を設けるようにした。したがって、ゲッ
ターから蒸発飛散したゲッター媒質が収容凹部に対向し
て配置された反射ミラーに付着するのを防止することが
できる。[Effects of the Invention] As described above, the present invention includes a regulating portion that prevents the getter medium evaporated and scattered from the getter from being reflected in the direction of adhering to the reflecting mirror, at the bottom of the accommodation recess in which the getter is held. . Therefore, it is possible to prevent the getter medium evaporated and scattered from the getter from adhering to the reflection mirror disposed opposite to the accommodation recess.
第1図はこの発明の一実施例を示す本体に形成された収
容凹部の部分の拡大図、第2図は同じくゲッター媒質の
飛散状態の説明図、第3図は全体構成の平面図、第4図
は従来の全体構成の平面図、第5図は同じく収容凹部に
おけるゲッター媒質の飛散状態の説明図である。
1・・・本体、2・・・光路、3・・・収容凹部、4・
・・反射ミラー 9・・・ゲッター 11・・・ゲッタ
ー媒質、21・・・円錐状の凸部(規制部)。FIG. 1 is an enlarged view of a housing recess formed in a main body showing an embodiment of the present invention, FIG. 2 is an explanatory view of the scattering state of the getter medium, and FIG. FIG. 4 is a plan view of the conventional overall configuration, and FIG. 5 is an explanatory diagram of the scattering state of the getter medium in the accommodation recess. DESCRIPTION OF SYMBOLS 1... Main body, 2... Optical path, 3... Accommodation recess, 4...
... Reflection mirror 9... Getter 11... Getter medium, 21... Conical convex part (regulating part).
Claims (1)
路を形成した本体と、この本体の上記反射ミラーの反射
面と対向する部位に上記光路に連通して形成された収容
凹部と、この収容凹部内の上記反射面と対向する位置に
設けられたゲッターとを備え、上記収容凹部の底部は上
記ゲッターから蒸発飛散したゲッター媒質を上記反射面
以外の部位に反射させる規制部に形成されたことを特徴
とするリング型レーザ装置。a main body in which a plurality of reflective mirrors are provided at predetermined positions of the optical path to form a ring-shaped optical path; a housing recess formed in a portion of the body facing the reflective surface of the reflective mirror so as to communicate with the optical path; a getter provided in a position facing the reflective surface within the recess, the bottom of the housing recess being formed as a regulating portion that reflects the getter medium evaporated and scattered from the getter to a portion other than the reflective surface; A ring-shaped laser device featuring:
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3632590A JPH03240284A (en) | 1990-02-19 | 1990-02-19 | Ring type laser device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3632590A JPH03240284A (en) | 1990-02-19 | 1990-02-19 | Ring type laser device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH03240284A true JPH03240284A (en) | 1991-10-25 |
Family
ID=12466688
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3632590A Pending JPH03240284A (en) | 1990-02-19 | 1990-02-19 | Ring type laser device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH03240284A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH07174912A (en) * | 1993-12-20 | 1995-07-14 | Agency Of Ind Science & Technol | Method for regenerating ultralow loss mirror used in high performance laser device |
CN105674973A (en) * | 2014-11-17 | 2016-06-15 | 中国航空工业第六八研究所 | Laser gyro built-in getter activation method |
-
1990
- 1990-02-19 JP JP3632590A patent/JPH03240284A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH07174912A (en) * | 1993-12-20 | 1995-07-14 | Agency Of Ind Science & Technol | Method for regenerating ultralow loss mirror used in high performance laser device |
CN105674973A (en) * | 2014-11-17 | 2016-06-15 | 中国航空工业第六八研究所 | Laser gyro built-in getter activation method |
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