JPH02287520A - Laser device - Google Patents
Laser deviceInfo
- Publication number
- JPH02287520A JPH02287520A JP1110405A JP11040589A JPH02287520A JP H02287520 A JPH02287520 A JP H02287520A JP 1110405 A JP1110405 A JP 1110405A JP 11040589 A JP11040589 A JP 11040589A JP H02287520 A JPH02287520 A JP H02287520A
- Authority
- JP
- Japan
- Prior art keywords
- laser
- laser beam
- harmonic generation
- invisible
- light
- 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 abstract description 27
- 239000000835 fiber Substances 0.000 abstract description 3
- 239000002131 composite material Substances 0.000 abstract description 2
- 229920000642 polymer Polymers 0.000 abstract description 2
- 238000011282 treatment Methods 0.000 abstract description 2
- 230000004907 flux Effects 0.000 abstract 2
- 238000004040 coloring Methods 0.000 abstract 1
- 230000002093 peripheral effect Effects 0.000 abstract 1
- 238000010586 diagram Methods 0.000 description 6
- 239000000463 material Substances 0.000 description 5
- UHOVQNZJYSORNB-UHFFFAOYSA-N Benzene Chemical compound C1=CC=CC=C1 UHOVQNZJYSORNB-UHFFFAOYSA-N 0.000 description 3
- 239000013078 crystal Substances 0.000 description 3
- TYMLOMAKGOJONV-UHFFFAOYSA-N 4-nitroaniline Chemical compound NC1=CC=C([N+]([O-])=O)C=C1 TYMLOMAKGOJONV-UHFFFAOYSA-N 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000013532 laser treatment Methods 0.000 description 2
- 229920001610 polycaprolactone Polymers 0.000 description 2
- 230000001225 therapeutic effect Effects 0.000 description 2
- 230000000007 visual effect Effects 0.000 description 2
- 230000000903 blocking effect Effects 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 210000002615 epidermis Anatomy 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 239000002904 solvent Substances 0.000 description 1
- 210000001519 tissue Anatomy 0.000 description 1
Landscapes
- Laser Surgery Devices (AREA)
- Radiation-Therapy Devices (AREA)
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明はレーザ光を利用してレーザ治療を行なったり、
あるいはレーザ加工を行なうためのレーザ装置に関する
。[Detailed Description of the Invention] (Industrial Application Field) The present invention performs laser treatment using laser light,
Or it relates to a laser device for performing laser processing.
(従来の技術)
医療分野に用いられるレーザ装置のレーザ光としては、
Nd−Yag、CO2レーザ等が多く利用されている。(Prior art) Laser light from laser devices used in the medical field includes:
Nd-Yag, CO2 lasers, etc. are often used.
しかしながら、この杆のレーザは不1す視域のレーザで
あるため、実際にレーザ治療に用いるにはガイド光が必
要である。However, since this rod laser has a limited visual range, a guide light is required to actually use it for laser treatment.
一般に、ガイド光としては、可視光であるHe−Neレ
ーザが用いられている。また、不可視レーザ光から可視
領域の高調波を発生させる高調波発生素子(Secon
d l1arsonie Generation)を、
不可視レーザ光の光路上に設け、それによって可視レー
ザ光を発生させ、ガイド光とする手段も提案されている
(特開昭64−10224号公報参照)。Generally, a He-Ne laser that emits visible light is used as the guide light. In addition, a harmonic generation element (Second) that generates harmonics in the visible range from invisible laser light
d l1arsonie Generation),
There has also been proposed a means for providing a visible laser beam on the optical path of an invisible laser beam, thereby generating a visible laser beam and using it as a guide light (see Japanese Unexamined Patent Publication No. 10224/1983).
しかしながら、上記ガイド光として用いられるHe−N
eレーザは波長が638.2μlの赤色光であり、これ
は体腔内あるいは表皮下の部位の組織の色に近いため、
ガイド光であるにも拘らず、非常に見にくいものであっ
た。一方、高調波発生素子を設けて可視レーザ光を発生
させる場合は、非常に高価な単結晶素子(L i N
b 03−ニオブ酸リチウム−、KTP、KDP)が必
要であり、しかもガイド光用の光路を必要とし、レーザ
装置全体が煩雑となり、高価なものであった。However, the He-N used as the guide light
The e-laser emits red light with a wavelength of 638.2 μl, which is close to the color of tissues in body cavities or under the epidermis.
Even though it was a guide light, it was very difficult to see. On the other hand, when generating visible laser light by providing a harmonic generation element, a very expensive single crystal element (L i N
b 03-lithium niobate, KTP, KDP) is required, and an optical path for the guide light is required, making the entire laser device complicated and expensive.
本発明は上記事情に着目してなされたもので、その目的
とするところは、安価で取り扱いやすい高調波発生部材
を用いて、非常に簡略化された装置で可視レーザ光を発
生させることにより、小型かつ構造簡単で安価なレーザ
装置を提供することにある。The present invention was made in view of the above circumstances, and its purpose is to generate visible laser light with a very simplified device using a harmonic generation member that is inexpensive and easy to handle. The object of the present invention is to provide a small, simple, and inexpensive laser device.
〔課題を解決するための手段および作用〕上記目的を達
成するために、本発明のレーザ装置においては、結晶性
高分子と色素(単独では高調波を発生しない)を混合さ
せた複合系材料を具体的にはフィルム状とするとともに
、レーザ光源が発生する不可視レーザ光の光束径よりも
小径の通孔を6した高調波発生部材を形成し、この通孔
に不可視レーザ光の光軸部、つまりレーザ強度の強い部
分をそのまま通すとともに、光軸周囲、つまりレーザ強
度の弱い部分は高調波発生部材を透過させて=1J硯レ
ーザ光を発生させ、治療(加工)用レーザ光兼ガイド光
としてレーザ装置全体を小型かつ構造部tIXで安価な
ものとする。[Means and effects for solving the problem] In order to achieve the above object, the laser device of the present invention uses a composite material that is a mixture of a crystalline polymer and a dye (which does not generate harmonics when used alone). Specifically, a harmonic generation member is formed into a film and has a through hole with a diameter smaller than the beam diameter of the invisible laser beam generated by the laser light source, and the optical axis portion of the invisible laser beam is inserted into the through hole. In other words, the part with strong laser intensity passes through as it is, and the part around the optical axis, that is, the part with weak laser intensity, passes through the harmonic generation member to generate = 1J inkstone laser light, which is used as a treatment (processing) laser light and guide light. To make the entire laser device small and inexpensive with a structure part tIX.
以下、本発明の一実施例につき第1図ないし第3図を参
照して説明する。Hereinafter, one embodiment of the present invention will be described with reference to FIGS. 1 to 3.
第1図は本発明の基本構成を示す概略図であり、1は不
可視域のレーザ(例えばNd−Yag。FIG. 1 is a schematic diagram showing the basic configuration of the present invention, and 1 is a laser in an invisible range (for example, Nd-Yag).
CO2等)を発生するレーザ発振器である。そして、こ
のレーザ発振器1か発生する不可視レーザ光R1の光路
上には、手前側から順にカプラ2、高調波発生フィルム
3、集光レンズ4、導光ファイバ5および光学系6が配
設されている。また、高調波発生フィルム3と集光レン
ズ4との間の光路上にはレーザ光の遮断手段であるダイ
クロミラー7が開閉自在に設けられている。This is a laser oscillator that generates CO2, etc.). On the optical path of the invisible laser beam R1 generated by the laser oscillator 1, a coupler 2, a harmonic generation film 3, a condensing lens 4, a light guide fiber 5, and an optical system 6 are arranged in order from the front side. There is. Further, on the optical path between the harmonic generation film 3 and the condensing lens 4, a dichroic mirror 7 serving as a laser beam blocking means is provided so as to be openable and closable.
第2図に本発明による高調波発生材料でできた高調波発
生フィルム3の正面図を示す。この高調波発生フィルム
3は例えばパラニトロアニリン(P−NA)およびポリ
−ε−カプロラクトン(PCL :Mw=7.5X10
4)を、ベンゼンを溶媒としてキャストし、フィルム状
に形成したもので、その中央部にはレーザ発振器1から
射出された不可視レーザ光R1の光束径よりも若干小径
の通孔8が形成されている。すなわち、第3図(A)、
(B)に示すように、不可視レーザ光R,の光軸部すは
レーザ強度が高く、また光軸周囲a、Cはレーザ強度が
低くなっており、上記レーザ強度の高い光軸部すは高調
波発生フィルム3の通孔8にそのまま通され、レーザ強
度の低い光軸7.’j囲a、cは高調波発生フィルム3
を透過して可視領域の高調波を発生(可視化)するよう
になっている。FIG. 2 shows a front view of a harmonic generating film 3 made of a harmonic generating material according to the present invention. This harmonic generation film 3 is made of, for example, paranitroaniline (P-NA) and poly-ε-caprolactone (PCL: Mw=7.5×10
4) is cast into a film using benzene as a solvent, and a through hole 8 with a diameter slightly smaller than the beam diameter of the invisible laser beam R1 emitted from the laser oscillator 1 is formed in the center of the film. There is. That is, FIG. 3(A),
As shown in (B), the optical axis portion of the invisible laser beam R has high laser intensity, and the laser intensity is low around the optical axis a and C, and the optical axis portion with high laser intensity is The optical axis 7. is passed directly through the through hole 8 of the harmonic generation film 3, and has a low laser intensity. 'j Boxes a and c are harmonic generation films 3
It is designed to transmit (visualize) harmonics in the visible range.
このような構成のレーザ装置において、レーザ発振器l
より射出された不可視レーザ光R7はカブラ2を介して
高調波発生フィルム3に入射し、ここでレーザ強度の強
い光軸部すは通孔8にそのまま通され、またレーザ強度
の弱い光軸周囲a1Cは高調波発生フィルム3を透過す
る。したがって、レーザ強度の弱い部分のみが可視化さ
れ、全体として可視レーザ光R2となって集光レンズ4
で集光され、導光ファイバ5、光学系6を介して被照射
物9に照射される。このとき、被照射物9の所定の位置
をレーザ強度の弱い光輔周L!fJa%Cで照明するこ
とができ、同時にレーザ強度の強い光軸部すで被照射物
9をレーザ治療することができる。In a laser device with such a configuration, the laser oscillator l
The invisible laser beam R7 emitted from the lens enters the harmonic generation film 3 via the coupler 2, where it passes directly through the through hole 8 around the optical axis where the laser intensity is strong, and the area around the optical axis where the laser intensity is weak. a1C is transmitted through the harmonic generation film 3. Therefore, only the part where the laser intensity is weak is visualized, and the whole becomes visible laser light R2, which is transmitted to the condenser lens 4.
The light is focused and irradiated onto an irradiated object 9 via a light guide fiber 5 and an optical system 6. At this time, a predetermined position of the object 9 to be irradiated is illuminated by a light beam L with a weak laser intensity! It is possible to illuminate with fJa%C, and at the same time, the object 9 to be irradiated can be laser treated at the optical axis portion where the laser intensity is strong.
なお、可視レーザ光R2で被照射物9の所定の位置を照
明だけしたい場合は、ダイクロミラー′/を閉じて不可
視レーザを遮断すればよい。Incidentally, if it is desired to only illuminate a predetermined position of the object 9 to be irradiated with the visible laser beam R2, the dichroic mirror '/ may be closed to block the invisible laser beam.
このように、1つのレーザ発振器1が発生する不可視レ
ーザ光R1を、高調波発生材料をフィルム状に形成して
なる安価でシンプルな高調波発生フィルム3で可視レー
ザ光R2に変換し、これを治療用レーザ鳥兼ガイド光と
することができ、レーザ!;i!e置中にガイド光用の
光源および光路1手段を格別に用いる必要がなく、高価
で煩雑な単結晶素子を用いた高調波発生素子を設けた従
来に比べ、レーザ装置全体が簡略化され、小型かつシン
プルで取り扱いやすく、安価なものとなる。In this way, the invisible laser beam R1 generated by one laser oscillator 1 is converted into visible laser beam R2 using the inexpensive and simple harmonic generation film 3 made of a harmonic generation material formed into a film, and this is converted into visible laser beam R2. A laser that can be used as a therapeutic laser bird and guide light! ;i! There is no need to use a special light source and optical path means for the guide light during e-setting, and the entire laser device is simplified compared to the conventional system, which uses a harmonic generation element using an expensive and complicated single crystal element. It is small, simple, easy to handle, and inexpensive.
第4図は他の実施例を示すが、上記一実施例と同じ構成
要素については同一符号を付して説明を省略する。FIG. 4 shows another embodiment, and the same components as in the above embodiment are given the same reference numerals and the explanation thereof will be omitted.
すなわち、レーザ発振器1とダイクロミラー7との間の
光路上には上記一実施例で用いた高調波発生材料によっ
て形成された高調波発生シャッタ11が開閉自在に設け
られている。That is, on the optical path between the laser oscillator 1 and the dichroic mirror 7, a harmonic generating shutter 11 made of the harmonic generating material used in the above embodiment is provided so as to be openable and closable.
このような構成において、高調波発生シャッタ11を開
くと不可視レーザ光R,はそのまま被照射物9に照射さ
れ、高調波発生シャッタ11を閉じると11視レーザ光
に変換されて被照射物9の所定の位置を照明する。In such a configuration, when the harmonic generation shutter 11 is opened, the invisible laser beam R is directly irradiated onto the irradiated object 9, and when the harmonic generation shutter 11 is closed, it is converted into an 11-visible laser beam and is applied to the irradiated object 9. Illuminating a predetermined location.
第5図はさらに他の実施−1を示すが、この場合も上記
一実施例と同じ構成要素については同一符号を付して説
明を省略する。FIG. 5 shows still another embodiment-1, but in this case as well, the same components as in the above-mentioned embodiment are given the same reference numerals and the explanation thereof will be omitted.
すなわち、上記一実施例で用いた高調波発生材料は光学
系レンズの材料と混合することで、高調波発生レンズ1
2を作ることができ、レーザ発振器1とダイクロミラー
7との間の光路上には上記高調波発生レンズ12が通常
のレンズ13と任意に交換可能に設けられている。That is, the harmonic generation material used in the above embodiment can be mixed with the material of the optical system lens to form the harmonic generation lens 1.
On the optical path between the laser oscillator 1 and the dichroic mirror 7, the harmonic generation lens 12 is provided so as to be replaceable with a normal lens 13 as desired.
このような構成において、通常のレンズ13を用いると
不可視レーザ光R1はそのまま被照射物9に照射され、
高調波発生レンズ12を用いると可視レーザ光に変換さ
れて被照射物9の所定の位置を照明する。In such a configuration, when a normal lens 13 is used, the invisible laser beam R1 is directly irradiated onto the object 9,
When the harmonic generation lens 12 is used, the laser light is converted into visible laser light and illuminates a predetermined position of the object 9 to be irradiated.
なお、上記第4図および第5図に示した他の実施例は、
いずれも不可視レーザ光と可視レーザ光とを同時に発生
することができないため、やや取り扱いにくくなるが、
レーザ装置全体としては上記一実施例と同様、非常に簡
略化できる。Note that the other embodiments shown in FIGS. 4 and 5 above are as follows:
Both methods cannot generate invisible laser light and visible laser light at the same time, so they are somewhat difficult to handle.
The entire laser device can be extremely simplified as in the above embodiment.
以上説明したように、本発明のレーザ装置によれば、レ
ーザ装置中にガイド光用の光源および光路2手段を格別
に用いる必要がなく、また高1−6で煩雑な単結晶素子
を用いた高調波発生素子を設けることなく、1つのレー
ザ光源が発生する不可視レーザ光を安価でシンプルな高
調波発生部材でiiJ視レーザ光に変換し、これを治療
用レーザ光兼ガイド光としたから、レーザ装置全体が簡
略化され、小型かつシンプルで取り扱いやすく、安価な
ものとすることができる。As explained above, according to the laser device of the present invention, there is no need to use a light source for guiding light and two optical path means in the laser device, and a complicated single crystal element with a height of 1-6 is used. Without installing a harmonic generation element, invisible laser light generated by one laser light source is converted into IIJ visual laser light using an inexpensive and simple harmonic generation member, and this is used as a therapeutic laser light and guide light. The entire laser device is simplified, and can be made small, simple, easy to handle, and inexpensive.
第1図ないし第3図は本発明の一実施例を示し、第1図
はレーザ装置の概略構成図、第2図は高調波発生フィル
ムの正面図、第3図(A)は不可視レーザ光の正面図、
第3図(B)は不可視レーザ光の各部とレーザ強度との
関係を示す図、第4図は他の実施例を示すレーザ装置の
概略構成図、第5図はさらに他の実施例を示すレーザ装
置の概略構成図である。
1・・・レーザ発振器、3・・・高調波発生フィルム、
8・・・通孔、11・・・高調波発生シャッタ、12・
・・高調波発生レンズ。
11図
出願人代理人 弁理士 坪井 淳
第4図Figures 1 to 3 show an embodiment of the present invention, Figure 1 is a schematic diagram of a laser device, Figure 2 is a front view of a harmonic generation film, and Figure 3 (A) shows an invisible laser beam. front view of,
Fig. 3 (B) is a diagram showing the relationship between each part of the invisible laser beam and the laser intensity, Fig. 4 is a schematic configuration diagram of a laser device showing another embodiment, and Fig. 5 is a diagram showing still another embodiment. FIG. 1 is a schematic configuration diagram of a laser device. 1... Laser oscillator, 3... Harmonic generation film,
8... Through hole, 11... Harmonic generation shutter, 12.
...Harmonic generation lens. Figure 11 Applicant's agent Patent attorney Atsushi Tsuboi Figure 4
Claims (1)
不可視レーザ光から可視領域の高調波を発生させる高調
波発生部材を設けたレーザ装置において、上記高調波発
生部材はレーザ光源が発生する不可視レーザ光の光束径
よりも小径の通孔を有し、この通孔に不可視レーザ光の
光軸部をそのまま通すとともに、光軸周囲は高調波発生
部材を透過させて可視レーザ光を発生させることを特徴
とするレーザ装置。In a laser device, a harmonic generation member is provided on the optical path of invisible laser light generated by a laser light source, and the harmonic generation member generates harmonics in the visible range from the invisible laser light. It has a through hole with a diameter smaller than the beam diameter of the light, and allows the optical axis of the invisible laser beam to pass through this through hole as it is, while passing through a harmonic generation member around the optical axis to generate visible laser light. Characteristic laser equipment.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1110405A JPH02287520A (en) | 1989-04-28 | 1989-04-28 | Laser device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1110405A JPH02287520A (en) | 1989-04-28 | 1989-04-28 | Laser device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02287520A true JPH02287520A (en) | 1990-11-27 |
Family
ID=14534958
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1110405A Pending JPH02287520A (en) | 1989-04-28 | 1989-04-28 | Laser device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02287520A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2018038287A1 (en) * | 2016-08-24 | 2018-03-01 | 사단법인 원텍 단국 의광학 연구센터 | Lipodissolve apparatus using tunable laser apparatus |
-
1989
- 1989-04-28 JP JP1110405A patent/JPH02287520A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2018038287A1 (en) * | 2016-08-24 | 2018-03-01 | 사단법인 원텍 단국 의광학 연구센터 | Lipodissolve apparatus using tunable laser apparatus |
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