JPH02163723A - Optical system for making laser light intensity distribution uniform - Google Patents

Optical system for making laser light intensity distribution uniform

Info

Publication number
JPH02163723A
JPH02163723A JP63318503A JP31850388A JPH02163723A JP H02163723 A JPH02163723 A JP H02163723A JP 63318503 A JP63318503 A JP 63318503A JP 31850388 A JP31850388 A JP 31850388A JP H02163723 A JPH02163723 A JP H02163723A
Authority
JP
Japan
Prior art keywords
mirror
laser
laser beam
reflected
laser 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
Application number
JP63318503A
Other languages
Japanese (ja)
Inventor
Makoto Tani
誠 谷
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.)
NEC Corp
Original Assignee
NEC 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 NEC Corp filed Critical NEC Corp
Priority to JP63318503A priority Critical patent/JPH02163723A/en
Publication of JPH02163723A publication Critical patent/JPH02163723A/en
Pending legal-status Critical Current

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  • Laser Beam Processing (AREA)
  • Lasers (AREA)

Abstract

PURPOSE:To obtain a laser working spot which has a uniform laser light intensity distribution by combining half mirrors having specific reflectivity, total reflecting mirrors and a condensing lens. CONSTITUTION:Laser light L is reflected by the half mirror 1 at 90 deg. reflection angle with the specific reflectivity of the mirror and is made incident to the total reflecting mirror 2. The laser light passes the mirror 2 and the total reflecting mirror 3 at 90 deg. reflection angle, is reflected by the half mirror 4 at 90 deg. reflection angle with the specific reflectivity so as to be made incident in parallel with the laser light L to the mirror 1. On the other hand, the light transmitted through the mirror 4 is reflected by the total reflecting mirror 5 at 90 deg. reflecting angle and is made incident in parallel with the laser light L to the mirror 1. The light rays reflected from the mirrors 4, 5 are fed back again to the mirrors 4, 5 through the mirrors 1, 2, 3. The number of feedback times and the diameter of the incident light beam to the condenser lens 6 are regulated by the sizes of the mirrors 1 to 5 and the perpendicular distance between the mirrors 4 and 5. The laser beam working spot having the uniform intensity distribution is obtd. in this way.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はレーザ光強度分布が均一なレーザ加工スポツト
を形成するレーザ光強度分布均一光学系に関シ、%にマ
ルチモードレーザの光学系に関するものである。
Detailed Description of the Invention [Field of Industrial Application] The present invention relates to an optical system with uniform laser beam intensity distribution for forming a laser processing spot with uniform laser beam intensity distribution, and particularly relates to an optical system of a multimode laser. It is something.

〔従来の技術〕[Conventional technology]

従来、この種のマルチモードレーザ光強度分布均一光学
系は、レーザ発撫器から発射されたマルチモードレーザ
光をビームエキスパンダにより拡大し、レーザ光強度分
布の均一な部分をアパーチャにより取シ出す方法がとら
れてい友。
Conventionally, this type of multimode laser light intensity distribution uniform optical system expands the multimode laser light emitted from a laser oscillating device using a beam expander, and extracts the uniform part of the laser light intensity distribution using an aperture. The method is being taken my friend.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上述した従来のマルチモードレーザ光強度分布均一光学
系は、レーザ発振器から発射されたマルチモードレーザ
光をビームエキスパンダによす拡大し、レーザ光強度分
布の均一な部分をアパーチャにより取り出す方法となっ
ているので、発振レーザエネルギ値に比べて取り出せる
有効レーザエネルギ値は減少するという問題があった。
The conventional multimode laser light intensity distribution uniform optical system described above is a method in which the multimode laser light emitted from a laser oscillator is expanded using a beam expander, and the uniform part of the laser light intensity distribution is extracted using an aperture. Therefore, there is a problem in that the effective laser energy value that can be extracted is reduced compared to the oscillation laser energy value.

〔課題を解決するための手段〕[Means to solve the problem]

本発明は、前述した従来の問題を改善するためになされ
たものであシ、レーザ発振器から発振したレーザ光を特
定の反射率で90度反射角にて反射する第1のハーフミ
ラ−と、第1のハーフミラ−からの反射レーザ光を90
度反射角にて全反射する第1の全反射ミラーと、第1の
全反射ミラーからの反射レーザ光を90度反射角にて全
反射する第2の全反射ミラーと、第2の全反射ミラーか
らの反射レーザ光を特定の反射率で90度反射角にて反
射する第2のハーフミラ−と、第2の71−7ミラー透
過後の透過レーザ光を90度反射角にて全反射する第3
の全反射ミラーと、第1のハーフミラ−から透過するレ
ーザ光を集光する集光レンズとによシレーザ光強度分布
均一光学系を構成するものである。
The present invention was made in order to improve the above-mentioned conventional problems, and includes a first half mirror that reflects a laser beam oscillated from a laser oscillator at a reflection angle of 90 degrees with a specific reflectance; The reflected laser beam from the half mirror of 1 is 90
a first total reflection mirror that totally reflects the reflected laser beam from the first total reflection mirror at a 90 degree reflection angle; A second half mirror that reflects the laser beam reflected from the mirror at a 90-degree reflection angle with a specific reflectance, and a second 71-7 mirror that totally reflects the transmitted laser beam after passing through the mirror at a 90-degree reflection angle. Third
The total reflection mirror and the condenser lens that condenses the laser beam transmitted from the first half mirror constitute an optical system with uniform laser light intensity distribution.

〔作用〕[Effect]

本発明においては、レーザ発振器から発振したレーザ光
を反射角90度のノ・−7ミラーと、全反射ミ2−との
組合せ光学系によシ、基本発振レーザ光のし・−ザ光強
度分布を重ね合せ、第1のハーフミラ−から透過するレ
ーザ光強度分布の重ね合されたレーザ光を集光レンズに
より集光し、レーザ光強度分布が均一なレーザ加工スポ
ツトを形成できる。
In the present invention, the laser beam oscillated from the laser oscillator is reflected by a combination optical system consisting of a No. 7 mirror with a reflection angle of 90 degrees and a total reflection mirror. By superimposing the distributions and condensing the laser beams with the superimposed laser beam intensity distributions transmitted from the first half mirror by a condenser lens, it is possible to form a laser processing spot with a uniform laser beam intensity distribution.

〔実施例〕〔Example〕

次に、本発明について図面を参照して説明する。 Next, the present invention will be explained with reference to the drawings.

第1図は本発明の一実施例によるレーザ光強度分布均一
光学系を示す構成図である。同図において、図示しない
レーザ発振器から出射されたレーザ光りは、第1のハー
フミラ−1に入射し、この第1のハーフミラ−1によシ
特定の反射率で90度反射角にて反射し、第1の全反射
ミラー2に入射する。このレーザ光は90度反射角にて
第1の全反射ミラー2および第2の全反射ミラー3を通
過し第2のハーフミニ)−4によ)%定の反射率で90
度反射角にて反射し、レーザ発振器から出射されたレー
ザ光りと平行に第1のハーフミラ−IK入射される。一
方、第2のハーフミラ−4を透過したレーザ光は第3の
全反射ミラー5により90度反射角にて反射し、レーザ
発振器から出射されたレーザ光りと平行に第1のハーフ
ミラ−1に入射される。1回目の第2のハーフミラ−4
および第3の全反射ミラー5から反射されるレーザ光は
、第1のハーフミラ−IKよフ特定の反射率で90度反
射角にて反射し、第1の全反射ミラー2.第2の全反射
ミラー3を通過し、再び第2の7・−フミラー4.第3
の全反射ミラー5に入射される。
FIG. 1 is a configuration diagram showing an optical system with uniform laser light intensity distribution according to an embodiment of the present invention. In the same figure, laser light emitted from a laser oscillator (not shown) enters a first half mirror 1, and is reflected by this first half mirror 1 at a 90 degree reflection angle with a specific reflectance. The light is incident on the first total reflection mirror 2. This laser beam passes through the first total reflection mirror 2 and the second total reflection mirror 3 at a reflection angle of 90 degrees, and is reflected at a constant reflectance of 90% by the second half mini-4).
The laser beam is reflected at a degree reflection angle and is incident on the first half mirror IK in parallel with the laser beam emitted from the laser oscillator. On the other hand, the laser beam transmitted through the second half mirror 4 is reflected by the third total reflection mirror 5 at a reflection angle of 90 degrees, and enters the first half mirror 1 in parallel with the laser beam emitted from the laser oscillator. be done. 1st second half mirror 4
The laser beam reflected from the third total reflection mirror 5 is reflected from the first half mirror IK at a 90 degree reflection angle with a specific reflectance, and is reflected from the first total reflection mirror 2. It passes through the second total reflection mirror 3 and returns to the second 7-f mirror 4. Third
The light is incident on the total reflection mirror 5.

ここで、このフィードバックされるし・−ザ光の回数お
よび集光レンズ6への入射レーザ光のビーム径は、ハー
フミラ−1,4と、全反射ばラー2゜3.5との大きさ
および第2のハーフミラ−4と、第3の全反射ミラー5
との垂直距離によシ規定される。
Here, the number of times the laser beam is fed back and the beam diameter of the laser beam incident on the condensing lens 6 are determined by the size of the half mirrors 1 and 4 and the total reflection mirror 2°3.5. Second half mirror 4 and third total reflection mirror 5
It is defined by the vertical distance between

第2図(a)はレーザ発振器から発振したレーザ光りの
強度分布を示す図で、第1図の集光レンズ6の中心を通
る光軸に対して点線の斜線部分で示す上部側レーザ光強
度分布が強くなっている。第2図(′b)はレーザ発振
器から発振したレーザ光りがし一ザ光強度分布均−光学
系を通過し、フィードバック回数が1回の時の集光レン
ズ6への入射前のレーザ光束と、レーザ光強度分布との
関係を示す図で、レーザ光の光束間の距離dは第2のハ
ーフミラ−4と第3の全反射ミラー5との垂直距離によ
り規定される。
FIG. 2(a) is a diagram showing the intensity distribution of the laser beam oscillated from the laser oscillator, and the upper laser beam intensity is indicated by the dotted line with respect to the optical axis passing through the center of the condenser lens 6 in FIG. The distribution is getting stronger. Figure 2 ('b) shows the laser beam emitted from the laser oscillator, passes through the laser beam intensity distribution uniform optical system, and shows the laser beam before entering the condenser lens 6 when the number of feedback is one. , a diagram showing the relationship between laser beam intensity distribution and the distance d between the laser beam beams is defined by the vertical distance between the second half mirror 4 and the third total reflection mirror 5.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明は、特定の反射率のハーフミ
ラ−と、全反射ミラーと、集光レンズとを組合せること
Kより、レーザ光強度分布が均一なレーザ加工スポツト
を形成できる効果がある。
As explained above, the present invention has the effect of forming a laser processing spot with a uniform laser beam intensity distribution by combining a half mirror with a specific reflectance, a total reflection mirror, and a condensing lens. .

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

第1図は本発明の実施例によるレーザ光強度分布均一光
学系の光学系構成図、第2図(al 、 (b)は第1
図の光学系で得られる集光レンズ入射前レーザ光束位置
とレーザ光強度分布との関係を示す図である0 1 a@ψ・第1のハーフミラ−21I・・拳第1の全
反射ミラー 3−・1111第2の全反射ミラ4@11
#@第2のハーフミラ−511eIIII第3の全反射
ミラー ・集光レンズ。
FIG. 1 is an optical system configuration diagram of an optical system with uniform laser light intensity distribution according to an embodiment of the present invention, and FIG.
01 a@ψ・First half mirror 21I・・Fist first total reflection mirror 3 -・1111 Second total reflection mirror 4@11
#@Second half mirror-511eIII Third total reflection mirror/condensing lens.

Claims (1)

【特許請求の範囲】[Claims] マルチモードレーザ発振器と、前記レーザ発振器から出
射したレーザ光を反射角90度で反射する第1のハーフ
ミラーと、前記第1のハーフミラーからの反射レーザ光
を反射角90度で全反射する第1の全反射ミラーと、前
記第1の全反射ミラーからの反射レーザ光を反射角90
度で全反射する第2の全反射ミラーと、前記第2の全反
射ミラーからの反射レーザ光を反射角90度で反射する
第2のハーフミラーと、前記第2のハーフミラーからの
透過レーザ光を反射角90度で全反射する第3の全反射
ミラーと、前記第2のハーフミラーからの反射レーザ光
および第3の全反射ミラーからの反射レーザ光ならびに
前記レーザ発振器からのレーザ光が前記第1のハーフミ
ラーに入射し透過レーザ光を集光する集光レンズとを備
え、レーザ強度分布が均一なレーザ加工スポツトを形成
することを特徴としたレーザ光強度分布均一光学系。
a multi-mode laser oscillator; a first half mirror that reflects the laser beam emitted from the laser oscillator at a reflection angle of 90 degrees; and a first half mirror that totally reflects the reflected laser beam from the first half mirror at a reflection angle of 90 degrees. 1 total reflection mirror and the reflected laser beam from the first total reflection mirror at a reflection angle of 90
a second total reflection mirror that totally reflects the laser beam from the second total reflection mirror at a reflection angle of 90 degrees, and a second half mirror that reflects the reflected laser beam from the second total reflection mirror at a reflection angle of 90 degrees; A third total reflection mirror that totally reflects light at a reflection angle of 90 degrees, a laser beam reflected from the second half mirror, a laser beam reflected from the third total reflection mirror, and a laser beam from the laser oscillator. 1. A uniform laser beam intensity distribution optical system, comprising a condenser lens for condensing transmitted laser beams incident on the first half mirror, and forming a laser processing spot with a uniform laser intensity distribution.
JP63318503A 1988-12-19 1988-12-19 Optical system for making laser light intensity distribution uniform Pending JPH02163723A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63318503A JPH02163723A (en) 1988-12-19 1988-12-19 Optical system for making laser light intensity distribution uniform

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63318503A JPH02163723A (en) 1988-12-19 1988-12-19 Optical system for making laser light intensity distribution uniform

Publications (1)

Publication Number Publication Date
JPH02163723A true JPH02163723A (en) 1990-06-25

Family

ID=18099851

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63318503A Pending JPH02163723A (en) 1988-12-19 1988-12-19 Optical system for making laser light intensity distribution uniform

Country Status (1)

Country Link
JP (1) JPH02163723A (en)

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