JPH02234105A - Hollow waveguide tube for ultraviolet wavelength range laser beam - Google Patents
Hollow waveguide tube for ultraviolet wavelength range laser beamInfo
- Publication number
- JPH02234105A JPH02234105A JP1054567A JP5456789A JPH02234105A JP H02234105 A JPH02234105 A JP H02234105A JP 1054567 A JP1054567 A JP 1054567A JP 5456789 A JP5456789 A JP 5456789A JP H02234105 A JPH02234105 A JP H02234105A
- Authority
- JP
- Japan
- Prior art keywords
- glass tube
- waveguide
- laser beam
- quartz glass
- ultraviolet
- 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 27
- 229910052751 metal Inorganic materials 0.000 claims description 16
- 239000002184 metal Substances 0.000 claims description 16
- 238000002834 transmittance Methods 0.000 claims description 13
- 239000000463 material Substances 0.000 claims description 7
- 239000012530 fluid Substances 0.000 claims description 5
- 230000007613 environmental effect Effects 0.000 claims description 4
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 abstract description 29
- 229910052782 aluminium Inorganic materials 0.000 abstract description 25
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 abstract description 25
- 230000005540 biological transmission Effects 0.000 abstract description 12
- 230000007423 decrease Effects 0.000 abstract description 10
- 230000003287 optical effect Effects 0.000 abstract description 3
- 238000005229 chemical vapour deposition Methods 0.000 abstract 1
- 230000003247 decreasing effect Effects 0.000 abstract 1
- 230000002542 deteriorative effect Effects 0.000 abstract 1
- 238000000034 method Methods 0.000 description 16
- 230000003746 surface roughness Effects 0.000 description 11
- 238000010586 diagram Methods 0.000 description 9
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 6
- 229910001873 dinitrogen Inorganic materials 0.000 description 6
- 230000000694 effects Effects 0.000 description 5
- 238000005498 polishing Methods 0.000 description 4
- 239000000126 substance Substances 0.000 description 4
- 239000007789 gas Substances 0.000 description 3
- 230000003647 oxidation Effects 0.000 description 3
- 238000007254 oxidation reaction Methods 0.000 description 3
- 230000002123 temporal effect Effects 0.000 description 3
- 238000007738 vacuum evaporation Methods 0.000 description 3
- 238000010521 absorption reaction Methods 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 2
- 238000005253 cladding Methods 0.000 description 2
- 238000001816 cooling Methods 0.000 description 2
- 239000003365 glass fiber Substances 0.000 description 2
- 230000031700 light absorption Effects 0.000 description 2
- 239000013307 optical fiber Substances 0.000 description 2
- 239000000377 silicon dioxide Substances 0.000 description 2
- 125000006850 spacer group Chemical group 0.000 description 2
- 241001062872 Cleyera japonica Species 0.000 description 1
- PXGOKWXKJXAPGV-UHFFFAOYSA-N Fluorine Chemical compound FF PXGOKWXKJXAPGV-UHFFFAOYSA-N 0.000 description 1
- 239000004809 Teflon Substances 0.000 description 1
- 229920006362 Teflon® Polymers 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000000354 decomposition reaction Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000000835 fiber Substances 0.000 description 1
- 229910052731 fluorine Inorganic materials 0.000 description 1
- 239000011737 fluorine Substances 0.000 description 1
- 125000002887 hydroxy group Chemical group [H]O* 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 238000001182 laser chemical vapour deposition Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- TWNQGVIAIRXVLR-UHFFFAOYSA-N oxo(oxoalumanyloxy)alumane Chemical compound O=[Al]O[Al]=O TWNQGVIAIRXVLR-UHFFFAOYSA-N 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- 238000001356 surgical procedure Methods 0.000 description 1
- 238000003786 synthesis reaction Methods 0.000 description 1
Landscapes
- Optical Fibers, Optical Fiber Cores, And Optical Fiber Bundles (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、高出力の紫外線波長域のレーザ光を高効率に
伝送し得る中空導波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 hollow waveguide that can transmit high-power laser light in the ultraviolet wavelength range with high efficiency.
紫外線域の波長を有するレーザ、例えばエキシマレーザ
などのレーザ光は高エネルギーであり、レーザCVD、
表面改質、光化学合成等その利用範囲は極めて広範囲で
ある。また、医療分野においては内視鏡と併用して体内
手術に用いたり、工業分野におい℃は微細加工に用いた
りしている。Laser light having a wavelength in the ultraviolet region, such as excimer laser, has high energy, and is used in laser CVD,
Its application range is extremely wide, including surface modification and photochemical synthesis. Furthermore, in the medical field, it is used in combination with an endoscope for internal surgery, and in the industrial field, it is used for microfabrication.
上記しーザ光の産業、医療分野への実用化においては、
それを効率よく目的場所に導く導波技術の確立が必須の
要件となる。エキシマレーザなどの短波長でビークパワ
ーの大きいレーザ光は生体に対して有害であり、それを
遠隔部に安全に伝送するには困難な問題があった。また
、この様なレーザ光を必要とする位置に容易に伝送でき
る導波路が特に医療分舒等から要望されていた。In the practical application of the above-mentioned Caesar light in the industrial and medical fields,
Establishing waveguide technology that efficiently guides it to its destination is an essential requirement. Laser light with a short wavelength and high peak power, such as excimer laser, is harmful to living organisms, and there are difficult problems in safely transmitting it to a remote location. Furthermore, there has been a demand for waveguides that can easily transmit such laser light to locations where it is needed, especially from medical distribution facilities and the like.
従来、紫外線域の波長を有するレーザ、例えばエキシマ
レーザ等の高エネルギーレーザ光を伝送する方法には、
下記(1)乃至(3)のような方法があった。Conventionally, methods for transmitting high-energy laser light such as a laser having a wavelength in the ultraviolet range, such as an excimer laser, include:
There were methods (1) to (3) below.
(1)石英系光ファイバによる方法
第6図に示すように、紫外域の光に対して透過率の良い
石英ガラスをコア51とし、それを取り巻くクラッド5
2にはフッ素等の不純物をドープした石英ガラスとし、
コア51よりも屈折率を小さくした2種のガラスからな
るガラスファイバを用い、ファ51とクラッド52の境
界面でレーザ光を反射させながら光Pを伝送する方法で
ある。(1) Method using silica-based optical fiber As shown in Figure 6, the core 51 is made of quartz glass that has good transmittance for light in the ultraviolet region, and the cladding 5 surrounding it
2 is made of quartz glass doped with impurities such as fluorine,
This method uses a glass fiber made of two types of glasses with a refractive index smaller than that of the core 51, and transmits the light P while reflecting the laser light at the interface between the fiber 51 and the cladding 52.
コアには特定波長の吸収を小さくするために水酸基など
をドーブしたものもある。なお、第6図(a)はガラス
ファイバの横断面図、同図(b)はその縦断面図である
。Some cores are doped with hydroxyl groups to reduce absorption at specific wavelengths. Note that FIG. 6(a) is a cross-sectional view of the glass fiber, and FIG. 6(b) is a vertical cross-sectional view thereof.
(2)アルミニウム管導波路による方法第7図に示すよ
うに、紫外域の光に対して高い反射率を有するアルミニ
ウムを管状にしたアルミニウム管53を用い、その内面
を研磨して内面反射率を上げ、アルミニウム管53の内
表面で反射させながら光!を伝送する所謂中空導波管を
用いる方法。なお、第7図(a)はアルミニウム管の横
断面図、同図(b)はその縦断面図である。(2) Method using an aluminum tube waveguide As shown in Figure 7, an aluminum tube 53 made of aluminum, which has a high reflectance for ultraviolet light, is used, and its inner surface is polished to increase the inner reflectance. Light is reflected on the inner surface of the aluminum tube 53! A method that uses a so-called hollow waveguide to transmit. Note that FIG. 7(a) is a cross-sectional view of the aluminum tube, and FIG. 7(b) is a longitudinal cross-sectional view thereof.
(3)アルミニウム板方形中空路による方法第8図に示
すように、光の進行方向に長い2枚の金属平板54 .
54を反射板として、その横方向の両端に誘電体のスペ
ーサ55を挾み、中空路の間隔を一定に保つ導波路を用
い、光!は2枚の金属平板54.54で反射しながら伝
送される。(3) Aluminum plate rectangular hollow path method As shown in FIG. 8, two metal flat plates 54.
54 is used as a reflector, dielectric spacers 55 are sandwiched between its lateral ends, and a waveguide is used in which the interval between the hollow paths is kept constant. is transmitted while being reflected by two flat metal plates 54, 54.
この金属平板54.54は紫外域の光に対して高い反射
率を有するアルミニウムであり、中空路の内側面は研磨
してある。また、スペーサである誘電体にはテフロンを
用いている.なお、第8図(a)はアルミニウム板方形
中空路の横断面図、同図(b)はその縦断面図である。The flat metal plates 54, 54 are made of aluminum having a high reflectance for light in the ultraviolet region, and the inner surfaces of the hollow passages are polished. Additionally, Teflon is used for the dielectric spacer. Note that FIG. 8(a) is a cross-sectional view of the rectangular hollow channel of an aluminum plate, and FIG. 8(b) is a longitudinal cross-sectional view thereof.
しかしながら、上記従来の(1)の石英系光ファイバに
よる方法は、伝送効率は良いが、入射端面の損傷しきい
値が低く、入射する光のエネルギー密度が大きいと入射
端面は破壊されてしまうという問題があった。又、コア
51の材料の原子間の結合エネルギーに対応する波長に
光の吸収が現れてしまい透過率の極端に低い波長もある
。そして、伝送率の時間的変化も大きくなり問題となる
。また、(2》のアルミニウム管導波路による方Y台
は、入射パワーは大きくできるが、導波管の径が細くな
るに従い内面研磨が難しく又酸化などによって時間とと
もに内面の反射率が低下し伝送効率が低下するという問
題がある。However, although the conventional method (1) using a silica-based optical fiber has good transmission efficiency, the damage threshold of the input end face is low, and if the energy density of the incident light is high, the input end face will be destroyed. There was a problem. Furthermore, there are wavelengths at which light absorption occurs at wavelengths corresponding to the bond energy between atoms of the material of the core 51, resulting in extremely low transmittance. Moreover, temporal changes in the transmission rate also become large, which poses a problem. In addition, although the incident power of (2) Y type using an aluminum tube waveguide can be increased, as the diameter of the waveguide becomes smaller, it is difficult to polish the inner surface, and the reflectance of the inner surface decreases over time due to oxidation etc. There is a problem that efficiency decreases.
また、〈3)のアルミニウム板方形中空路による方法は
、上記(2》と同様、入射パワーは大きくでき、反射板
の内面研磨は容易にできるが、小さい断面積のもの(例
えば1mm”程度のもの)は製作が困難である。また、
上記(2)と同様、酸化などにより内面の反射率が低下
して伝送効率が低下するという問題がある。In addition, the method (3) using an aluminum plate rectangular hollow channel allows the incident power to be increased and the inner surface of the reflector to be easily polished, as in (2) above, but the method is similar to (2) above. products) are difficult to produce.Also,
Similar to (2) above, there is a problem in that the reflectance of the inner surface decreases due to oxidation and the like, resulting in a decrease in transmission efficiency.
本発明は上述の点に鑑みてなされたもので上記問題点を
除去し、内面研磨等の困難な工程を必要とすることなく
、吸収や反射面の酸化等による反射率の低下による伝送
効率が低下することのない紫外線波長域レーザ光用中空
導波管を提供することにある。The present invention has been made in view of the above-mentioned points, and eliminates the above-mentioned problems, and eliminates the need for difficult processes such as internal polishing, and reduces transmission efficiency due to reduction in reflectance due to absorption and oxidation of the reflective surface. It is an object of the present invention to provide a hollow waveguide for laser light in the ultraviolet wavelength range that does not deteriorate.
上記課題を解決するため本発明は、石英等の紫外光に対
して高透過率であり且つ耐環境性に優れたガラス材から
なるガラス管を導波管内面とし、その外側に紫外光に対
して高反射率の金属膜を形成し、ガラス管内表面及び該
ガラス管と金着膜との境雰面にて紫外線波長域レーザ光
を反射させながら伝送させることを特徴とする。In order to solve the above problems, the present invention uses a glass tube made of a glass material such as quartz that has high transmittance to ultraviolet light and has excellent environmental resistance as the inner surface of the waveguide, and has a The present invention is characterized in that a metal film with a high reflectance is formed in the glass tube, and the laser light in the ultraviolet wavelength range is transmitted while being reflected on the inner surface of the glass tube and the interface between the glass tube and the gold-plated film.
また、ガラス管内の空間中を紫外光透過率の良い物質流
体を流しながら紫外線波長域レーザ光を伝送させるこ゜
とを特徴とする。Another feature is that a laser beam in the ultraviolet wavelength range is transmitted while flowing a material fluid with high ultraviolet light transmittance through the space inside the glass tube.
上記の如く構成することにより、ガラス管を用いるから
レーザ光の入射は導波管内表面であり入射面積が大きい
ため単位面積当りの損傷しきい値が上記(1)の場合の
端面と同じであったとしても、入射エネルギーの損傷し
きい値はトータルとして大きくなる。With the above configuration, since the glass tube is used, the laser beam is incident on the inner surface of the waveguide, and the incident area is large, so the damage threshold per unit area is the same as the end face in the case of (1) above. Even so, the damage threshold of the incident energy becomes larger in total.
また、ガラス管の外面に金属膜を形成するので、金属膜
の表面粗さはガラス管外面の表面粗さとなり、該表面粗
さは十分の数μm程度であるから、〒解研磨などの方法
による研磨面粗さ数μmより/J%さい優れた反射表面
を容易に得ることができる。In addition, since a metal film is formed on the outer surface of the glass tube, the surface roughness of the metal film becomes the surface roughness of the outer surface of the glass tube, and since this surface roughness is about several tenths of a micrometer, methods such as decomposition polishing are used. An excellent reflective surface with a polished surface roughness of less than a few μm/J% can be easily obtained.
また、金属膜の反射面はガラス管外面に密着しているた
め、該反射面が空気に触れることなく、表面が酸化被膜
に覆われ反射率が低下することもない。Further, since the reflective surface of the metal film is in close contact with the outer surface of the glass tube, the reflective surface does not come into contact with air, and the surface is not covered with an oxide film and the reflectance is not reduced.
また、導波管内空間に紫外光透過率の良い物質流体を流
すことができ、伝送効率が向上すると共に、冷却効果に
より伝送率の時間的低下は小さくなる。In addition, a material fluid with high ultraviolet light transmittance can be flowed into the waveguide interior space, improving transmission efficiency and reducing the temporal decrease in transmission rate due to the cooling effect.
以下、本発明の実施例を図面に基づいて説明する。 Embodiments of the present invention will be described below based on the drawings.
第1図は本発明に係る紫外線波長域レーザ光用中空導波
管の横断面図である。導波管3は同図に示すように石英
ガラス管2の外面にCVD,PVD或いは真空蒸着等の
適当な方法でアルミニウム膜1を形成した構成である。FIG. 1 is a cross-sectional view of a hollow waveguide for ultraviolet wavelength laser light according to the present invention. As shown in the figure, the waveguide 3 has a structure in which an aluminum film 1 is formed on the outer surface of a quartz glass tube 2 by an appropriate method such as CVD, PVD, or vacuum evaporation.
第2図はレーザ光が上記構成の導波管3の石英ガラス管
2内を伝送する様子を説明するための図であり、図示す
るように、入射したレーザ光!は石英ガラス管2の表面
及び石英ガラス管2とアルミニウム膜1との境界面で反
射しながら伝送される。FIG. 2 is a diagram for explaining how a laser beam is transmitted through the quartz glass tube 2 of the waveguide 3 having the above configuration.As shown in the figure, the incident laser beam! is transmitted while being reflected on the surface of the quartz glass tube 2 and the interface between the quartz glass tube 2 and the aluminum film 1.
第4図は上記導波管3にレーザ光Pを入射ずる様子を説
明するための図であり、レーザ装置5から出てきたレー
ザ光2は焦光レンズ4で焦光され導波管3内に導かれ、
上述のように導波管3を伝送していく。FIG. 4 is a diagram for explaining how the laser beam P is incident on the waveguide 3. The laser beam 2 coming out of the laser device 5 is focused by the focusing lens 4 and is inside the waveguide 3. Guided by
Transmission is carried out through the waveguide 3 as described above.
第4図は焦光するレーザ光!の焦点7と導波管3の位置
関係を示す図であり、レーザ光クの光軸8と導波管3の
中心軸6を一致させ、焦点7の位置は導波路の中心軸6
上であり、全てのレーザ光Pが導波管3の石英ガラス管
2内面に入則するようにする。これにより、入射された
レーザ光クは第2図に示すように、石英ガラス管2の表
面及び石英ガラス管2とアルミニウム膜1との境界面で
反射しながら伝送される.
導波管3を第1図に示す構成とすることにより、石英ガ
ラスは紫外光に対して高透過率であり且つ耐環境性に優
れたガラスであり、アルミニウムは紫外光に対して高反
射率の金属であるから、入射されたレーザ光eが石英ガ
ラス管2の表面及び石英ガラス管2とアルミニウム膜1
との境界面で反射しながら伝送する間の減衰は極めて小
さくなる。Figure 4 shows a focused laser beam! is a diagram showing the positional relationship between the focal point 7 and the waveguide 3, where the optical axis 8 of the laser beam and the central axis 6 of the waveguide 3 are aligned, and the position of the focal point 7 is aligned with the central axis 6 of the waveguide.
above, so that all the laser light P enters the inner surface of the quartz glass tube 2 of the waveguide 3. As a result, the incident laser beam is transmitted while being reflected at the surface of the quartz glass tube 2 and the interface between the quartz glass tube 2 and the aluminum film 1, as shown in FIG. By configuring the waveguide 3 as shown in Fig. 1, silica glass has a high transmittance to ultraviolet light and is a glass with excellent environmental resistance, and aluminum has a high reflectance to ultraviolet light. , the incident laser beam e hits the surface of the quartz glass tube 2 and the quartz glass tube 2 and the aluminum film 1.
The attenuation during transmission while being reflected at the interface with is extremely small.
また、石英ガラス管2を用いレーザ光Pの入射はこの石
英ガラス管2の内表面とするから、入射面積が大きいた
め入射エネルギーの損傷しきい値はトータルとして大き
くなる。Further, since the quartz glass tube 2 is used and the laser beam P is incident on the inner surface of the quartz glass tube 2, the incident area is large, so that the damage threshold of the incident energy becomes large in total.
また、石英ガラス管2の外面にアルミニウムをCVD,
PVD或いは真空蒸着等の適当な方法でアルミニウム膜
1を形成するので、アルミニウム膜1の表面粗さは石英
ガラス管2の外面の表面粗さとなり、その表面粗さは十
分の数μm程度であるから、電解研磨などの方法による
研磨面粗さ数μmより小さい優れた表面を容易に得るこ
とができる。In addition, aluminum is coated on the outer surface of the quartz glass tube 2 by CVD,
Since the aluminum film 1 is formed by an appropriate method such as PVD or vacuum evaporation, the surface roughness of the aluminum film 1 is the same as that of the outer surface of the quartz glass tube 2, and the surface roughness is about several tenths of a μm. Therefore, it is possible to easily obtain an excellent surface with a polished surface roughness of less than several μm by a method such as electrolytic polishing.
また、アルミニウムは紫外光に対して高反射率の金属で
あるが酸化され易い金属であり、空中においた場合、表
面は即座にレーザ光の反射効率の低下をもたらす酸化ア
ルミニウムを主成分とする被膜に覆われしまう。しかし
ながら本実施例では、アルミニウム膜1はCVD,PV
D或いは真空蒸着等の高真空雰囲気で行なわれると共に
、レーザ光の反射を行なう反射面は石英ガラス管2の外
面に密着して形成されるから空気に触れることは全くな
く、表面が酸化被膜に覆われ反射率が低下することもな
い。In addition, although aluminum is a metal with a high reflectance for ultraviolet light, it is a metal that is easily oxidized, and if it is placed in the air, the surface will immediately become coated with aluminum oxide as its main component, which will immediately reduce the laser beam reflection efficiency. covered in. However, in this embodiment, the aluminum film 1 is formed by CVD, PV
The process is carried out in a high vacuum atmosphere such as D or vacuum evaporation, and the reflective surface that reflects the laser beam is formed in close contact with the outer surface of the quartz glass tube 2, so it never comes into contact with air and the surface is coated with an oxide film. It will not be covered and the reflectance will not decrease.
第5図は導波管に窒素ガスN,を流しならレーザ光を伝
送する装置の概略構成を示す図である。FIG. 5 is a diagram showing a schematic configuration of an apparatus for transmitting laser light by flowing nitrogen gas N through a waveguide.
焦光レンズ4を装着する事具9にはガス流入口10が設
けられている。このガス流入口10から窒素ガスN,を
導波管3の石英ガラス管2内に流しながら、レーザ光!
を導波管3に入射(第4図参照)させると、窒素ガスは
紫外光透過率の良い物質であるから、紫外光吸収による
透過率の減衰を抑えるばかりか、導波管3に外部から物
質の流入を防ぐ作用や、導波管3を冷却する作用を果た
す。なお、上記実施例では導波管3のガラス管として石
英ガラス管2を用いたが、紫外光に対して高透過率であ
り、且つ耐環境性に優れたガラスであれば石英ガラスに
限定されるものではない。A gas inlet 10 is provided in the fixture 9 to which the focusing lens 4 is attached. While flowing nitrogen gas N from this gas inlet 10 into the quartz glass tube 2 of the waveguide 3, a laser beam is generated!
When entering the waveguide 3 (see Figure 4), since nitrogen gas is a substance with good ultraviolet light transmittance, it not only suppresses the attenuation of the transmittance due to ultraviolet light absorption, but also allows the waveguide 3 to be exposed to light from the outside. It functions to prevent the inflow of substances and to cool the waveguide 3. In the above embodiment, the quartz glass tube 2 was used as the glass tube of the waveguide 3, but any glass that has high transmittance to ultraviolet light and excellent environmental resistance may be used. It's not something you can do.
また、ガラス管外面の金属膜としてアルミニウム膜1と
したが、この膜の金属は紫外光に対して高反射率の金属
であればアルミニウムに限定されるものではない.
また、導波管3に流す物質として窒素ガスを用いたが、
紫外光透過率の良い物質からなる流体であれば窒素ガス
に限定されるものではない。Further, although the aluminum film 1 was used as the metal film on the outer surface of the glass tube, the metal of this film is not limited to aluminum as long as it has a high reflectance to ultraviolet light. In addition, nitrogen gas was used as the substance flowing into the waveguide 3, but
The fluid is not limited to nitrogen gas as long as it is made of a substance with good ultraviolet light transmittance.
以上説明したように本発明によれば下記のような優れた
効果が得られる.
(1)ガラス管を導波管内面とするから、レーザ光の入
射面はこのガラス管内表面であり入射面積が大きいため
入射エネルギーの損傷しきい値はトータルとして大きく
なる.
《2》ガラス管の外面に金属膜を形成するので、金属膜
の表面粗さはガラス管外面の表面粗さとなり、該表面粗
さは十分の数μm程度であるから、電解研磨などの方法
による研磨面粗さ数μmより小さい優れた反射表面を容
易に得ることができる。As explained above, according to the present invention, the following excellent effects can be obtained. (1) Since a glass tube is used as the inner surface of the waveguide, the incident surface of the laser beam is the inner surface of the glass tube, and since the incident area is large, the damage threshold of the incident energy becomes large in total. <<2>> Since a metal film is formed on the outer surface of the glass tube, the surface roughness of the metal film becomes the surface roughness of the outer surface of the glass tube, and since this surface roughness is about a few tenths of a micrometer, methods such as electrolytic polishing can be used. An excellent reflective surface with a polished surface roughness of less than a few μm can be easily obtained.
(3》金属膜の反射面はガラス管外面に密着しているた
め、該反射面は形成時及び形成後も空気に触れることな
く、表面が酸化被膜に覆われ反射率が低下することもな
い..
(4》導波管内空間に紫外光透過率の良い物質流体を流
すことにより、伝送効率が向上すると共に、その冷却効
果により伝送率の時間的低下は小さくなる.(3) Since the reflective surface of the metal film is in close contact with the outer surface of the glass tube, the reflective surface does not come into contact with air during or after formation, and the surface is not covered with an oxide film and the reflectance does not decrease. (4) By flowing a material fluid with good ultraviolet light transmittance into the waveguide interior space, transmission efficiency is improved, and its cooling effect reduces the temporal decrease in transmission rate.
第1図は本発明に係る紫外線波長域レーザ光用中空導波
管の横断面図、第2図はレーザ光の導波管を伝送して行
く様子を説明するための図、第3図は導波管にレーザ光
を入射する様子を説明するための図、第4図は焦光する
レーザ光の焦点と導波管の位置関係を示す図、第5図は
導波管に窒素ガスを流しならレーザ光を伝送する装置の
概略構成を示す図、第6図,第7図,第8図はそれぞれ
従来の高エネルギーレーザ光を伝送する装置の概略構成
を示す図である。
図中、1・・・・アルミニウム膜、2・・・・石英ガラ
ス管、3・・・・導波管、4・・・・焦光レンズ、5・
・・・レーザ装置、6・・・・中心軸、7・・・・焦点
、8・・・・光軸、9・・・・事具、10・・・・ガス
流入口。
第1図
出願人 株式会社榊←←解斥(外1名)代理人 弁理士
熊谷隆(外1名)
第2図
第3図
第5
図
【L:Lノ
(bノ
第6
図
第7
図
第8
図
tFigure 1 is a cross-sectional view of a hollow waveguide for laser light in the ultraviolet wavelength range according to the present invention, Figure 2 is a diagram for explaining how laser light is transmitted through the waveguide, and Figure 3 is Figure 4 is a diagram to explain how the laser beam is incident on the waveguide. Figure 4 is a diagram showing the positional relationship between the focal point of the laser beam and the waveguide. Figure 5 is a diagram showing how nitrogen gas is introduced into the waveguide. FIG. 6, FIG. 7, and FIG. 8 are diagrams each showing a schematic configuration of a device for transmitting conventional high-energy laser light. In the figure, 1...aluminum film, 2...quartz glass tube, 3...waveguide, 4...focusing lens, 5...
...Laser device, 6.. Central axis, 7.. Focus, 8.. Optical axis, 9.. Equipment, 10.. Gas inlet. Figure 1 Applicant Sakaki←←Kaiho Co., Ltd. (1 other person) Agent Patent attorney Takashi Kumagai (1 other person) Figure 2 Figure 5 Figure [L: Lノ (b No. 6 Figure 7) Figure 8 Figure t
Claims (2)
れたガラス材からなるガラス管を導波管内面とし、その
外側に紫外光に対して高反射率の金属膜を形成し、前記
ガラス管内表面及び該ガラス管と前記金属膜との境界面
にて紫外線波長域レーザ光を反射させながら伝送させる
ことを特徴とする紫外線波長域レーザ光用中空導波管。(1) The inner surface of the waveguide is a glass tube made of a glass material that has high transmittance to ultraviolet light and excellent environmental resistance, and a metal film with high reflectance to ultraviolet light is formed on the outside. A hollow waveguide for laser light in the ultraviolet wavelength range, characterized in that the laser light in the ultraviolet wavelength range is transmitted while being reflected at the inner surface of the glass tube and the interface between the glass tube and the metal film.
質流体を流しながら紫外線波長域レーザ光を伝送させる
ことを特徴とする請求項(1)記載の紫外線波長域レー
ザ光用中空導波管。(2) A hollow waveguide for ultraviolet wavelength laser light according to claim (1), characterized in that the ultraviolet wavelength laser beam is transmitted while flowing a material fluid with good ultraviolet light transmittance through the space inside the glass tube. tube.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1054567A JPH02234105A (en) | 1989-03-07 | 1989-03-07 | Hollow waveguide tube for ultraviolet wavelength range laser beam |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1054567A JPH02234105A (en) | 1989-03-07 | 1989-03-07 | Hollow waveguide tube for ultraviolet wavelength range laser beam |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02234105A true JPH02234105A (en) | 1990-09-17 |
Family
ID=12974268
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1054567A Pending JPH02234105A (en) | 1989-03-07 | 1989-03-07 | Hollow waveguide tube for ultraviolet wavelength range laser beam |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02234105A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR20010037798A (en) * | 1999-10-20 | 2001-05-15 | 이명일 | Light ray transmission tube using specular reflection |
-
1989
- 1989-03-07 JP JP1054567A patent/JPH02234105A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR20010037798A (en) * | 1999-10-20 | 2001-05-15 | 이명일 | Light ray transmission tube using specular reflection |
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