JP2751119B2 - Parallel light creation device - Google Patents

Parallel light creation device

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Publication number
JP2751119B2
JP2751119B2 JP1206381A JP20638189A JP2751119B2 JP 2751119 B2 JP2751119 B2 JP 2751119B2 JP 1206381 A JP1206381 A JP 1206381A JP 20638189 A JP20638189 A JP 20638189A JP 2751119 B2 JP2751119 B2 JP 2751119B2
Authority
JP
Japan
Prior art keywords
light
parallel light
concave cylindrical
reflection surface
harmonic
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.)
Expired - Lifetime
Application number
JP1206381A
Other languages
Japanese (ja)
Other versions
JPH0369926A (en
Inventor
伸和 田中
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.)
Nippon Columbia Co Ltd
Original Assignee
Nippon Columbia Co Ltd
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 Nippon Columbia Co Ltd filed Critical Nippon Columbia Co Ltd
Priority to JP1206381A priority Critical patent/JP2751119B2/en
Publication of JPH0369926A publication Critical patent/JPH0369926A/en
Application granted granted Critical
Publication of JP2751119B2 publication Critical patent/JP2751119B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、非線形光学効果を用いて光波長変換を行う
非線形光学素子に関するものである。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a nonlinear optical element that performs light wavelength conversion using a nonlinear optical effect.

〔従来の技術〕[Conventional technology]

光導波路を利用したチェレンコフ放射型の第2高調波
発生(以下SHGと呼ぶ)素子によって発生する第2高調
波ビームは、発光点が導波路という細長い領域である。
A second harmonic beam generated by a Cerenkov radiation type second harmonic generation (hereinafter, referred to as SHG) element using an optical waveguide has a light emitting point in an elongated region called a waveguide.

そのため、第3図に示す概略構成図のように、SHG素
子31の導波路32に入射したレーザ光1は、第2高調波ビ
ーム33がチェレンコフ放射角を有して放射される。この
第2高調波ビーム33は、一方向にのみコリメートされ、
直交するもう一方向では発散光となってSHG素子31の端
面34から出射される。このようにして出射した第2高調
波ビーム33は、シリンドリカルレンズ35等の非対称レン
ズを使用してビーム整形を行うことにより、扱いやすい
コリメート光に変換していた。
Therefore, as shown in the schematic configuration diagram of FIG. 3, the laser beam 1 incident on the waveguide 32 of the SHG element 31 is emitted with the second harmonic beam 33 having a Cherenkov radiation angle. This second harmonic beam 33 is collimated in only one direction,
In the other orthogonal direction, the divergent light is emitted from the end face 34 of the SHG element 31. The second harmonic beam 33 emitted in this manner has been converted into collimated light that is easy to handle by performing beam shaping using an asymmetric lens such as a cylindrical lens 35.

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

チェレンコフ放射型SHG素子の導波路の入射端から放
射される第2高調波ビームと、出射端近くから放射され
る第2高調波ビームは、広がり角は一定であるが、発光
点が異なるため、弓状に湾曲した複雑なビームパターン
になり、従来の技術で述べたような方法では、コリメー
ト性の十分良い光ビームを得ることは難しい。また、光
波長変換素子としての小型化を考える上で、ビーム整形
用の光学系を必要とすることは問題である。
The second harmonic beam emitted from the entrance end of the waveguide of the Cherenkov radiation type SHG element and the second harmonic beam emitted from the vicinity of the exit end have a constant divergence angle but different emission points. A complicated beam pattern curved in an arc shape is obtained, and it is difficult to obtain a light beam having sufficiently good collimation by the method described in the related art. Further, when considering miniaturization as an optical wavelength conversion element, it is problematic to require an optical system for beam shaping.

そこで、本発明の目的は、新たにビーム整形用の光学
部品を用いずに、第2高調波ビームを品質の良い平行光
に変換する装置を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide an apparatus for converting a second harmonic beam into high-quality parallel light without newly using a beam shaping optical component.

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

そのため本発明では、入射光の高調波を出射する導波
路型非線形光学素子と、該導波路型非線形光学素子の出
射光を平行光に変換する凹シリンドリカル反射面とで構
成したもので、前記凹シリンドリカル反射部を、前記導
波路型非線形光学素子に設けたり、略等しい屈折率の光
学部材で構成した前記導波路型非線形光学素子の高調波
出射端面に設けたものである。さらに前記凹シリンドリ
カル反射部と、前記出射光の光軸と直交する断面との形
状を略円弧状にするとともに、前記凹シリンドリカル反
射面が、前記入射光の光軸と平行をなすようにしたこと
を特徴としたものである。
Therefore, in the present invention, the waveguide-type nonlinear optical element that emits a harmonic of the incident light, and a concave cylindrical reflection surface that converts the output light of the waveguide-type nonlinear optical element into parallel light, wherein the concave A cylindrical reflection portion is provided on the waveguide type nonlinear optical element, or provided on a harmonic emission end face of the waveguide type nonlinear optical element formed of an optical member having substantially the same refractive index. Further, the concave cylindrical reflecting portion and the cross section orthogonal to the optical axis of the outgoing light have a substantially arc shape, and the concave cylindrical reflecting surface is parallel to the optical axis of the incident light. It is characterized by.

〔作用〕[Action]

チェレンコフ放射型のSHG素子による第2高調波は、
ある程度の長さを持った導波路から、チェレンコフ角の
方向で一方向のみにコリメートされた発散光として発光
される。この第2高調波を導波路の形成されている素子
面と、平行に対向する素子面に照射した場合、その照射
面上の第2高調波は発光点から同じ距離にある。そこ
で、発散光の方向と直交する照射面の断面を略円弧状の
反射面として構成することにより、この略円弧状の反射
面で反射した第2高調波は、発散方向を整形してコリメ
ート光にすることができる。
The second harmonic of the Cherenkov radiation type SHG element is
Light is emitted from a waveguide having a certain length as divergent light collimated in only one direction in the direction of the Cherenkov angle. When this second harmonic is applied to the element surface in parallel with the element surface on which the waveguide is formed, the second harmonic on the irradiated surface is at the same distance from the light emitting point. Therefore, by forming the cross section of the irradiation surface perpendicular to the direction of the diverging light as a substantially arc-shaped reflecting surface, the second harmonic reflected by the substantially arc-shaped reflecting surface is shaped in the diverging direction to form the collimated light. Can be

〔実施例〕〔Example〕

第1図は本発明の一実施例を示す概略構成図である。 FIG. 1 is a schematic configuration diagram showing one embodiment of the present invention.

図において、高出力の基本波となるレーザ光1が集光
レンズ2によりニオブ酸リチウム結晶基板によるSHG素
子3の上に形成された光導波路4の端面に収束される。
このレーザ光1は、光導波路4を通るときに、非線形光
学効果により、光導波路4に対してある角度の方向に第
2高調波5を発生させる。この第2高調波5は1方向の
みコリメートされた発散光なので、この発散光となる方
向成分に対し、コリメート光の得られる曲率を有する反
射曲面7で反射させることにより、品質の良いコリメー
ト光6を得ることができる。そしてSHG素子3の端面8
から放射されることになる。
In the figure, a laser beam 1 serving as a high-output fundamental wave is converged by a condenser lens 2 on an end face of an optical waveguide 4 formed on a SHG element 3 made of a lithium niobate crystal substrate.
When the laser light 1 passes through the optical waveguide 4, a second harmonic 5 is generated in a direction at a certain angle with respect to the optical waveguide 4 by a nonlinear optical effect. Since the second harmonic 5 is divergent light that is collimated in only one direction, the directional component that becomes the divergent light is reflected by a reflection curved surface 7 having a curvature at which the collimated light is obtained, so that a high-quality collimated light 6 is obtained. Can be obtained. And the end face 8 of the SHG element 3
Will be radiated from

また第1図のような導波路方向に十分長い素子を使用
する代わりに第2図(a)の他の実施例に示すように、
SHG素子3の端面に略等しい屈折率を有する光学部材9
にビーム整形を行う反射曲面10を形成して、接合する構
成でもよい。この構成を用いればSHG素子3とは別に反
射曲面10を光学部材9で作成できるので、SHG素子31を
傷付ける心配がなくなる。そして反射曲面10を有する光
学部材9だけの量産化が可能となり、品質が安定し、コ
ストを低下させることができる。
Also, instead of using a sufficiently long element in the waveguide direction as shown in FIG. 1, as shown in another embodiment of FIG.
Optical member 9 having a refractive index substantially equal to the end face of SHG element 3
A reflection curved surface 10 for shaping the beam may be formed and joined. If this configuration is used, the reflection curved surface 10 can be formed by the optical member 9 separately from the SHG element 3, so that there is no fear of damaging the SHG element 31. Then, it becomes possible to mass-produce only the optical member 9 having the reflection curved surface 10, so that the quality can be stabilized and the cost can be reduced.

さらに第2図(b)に示すように、光学部材9からの
出射端面11と、コリメート光6の出射方向に直交する面
で構成して、コリメート光6を屈折させないようにして
もよい。
Further, as shown in FIG. 2 (b), the collimated light 6 may be prevented from being refracted by comprising an exit end face 11 from the optical member 9 and a surface orthogonal to the exit direction of the collimated light 6.

〔発明の効果〕〔The invention's effect〕

SHG素子自体もしくは、並設してコリメート光形成用
の反射曲面をつくることにより、新たにビーム整形用の
光学部品を使用せずに質のよいコリメート光を作成する
ことができる。また、発散の初期の段階で整形を行うの
で、第2高調波ビームのけられが少なく、ビーム効率を
高めることができる。
By forming a reflective curved surface for forming a collimated light in parallel with the SHG element itself, high-quality collimated light can be created without newly using an optical component for beam shaping. In addition, since shaping is performed at an early stage of divergence, the second harmonic beam is less eccentric and the beam efficiency can be increased.

【図面の簡単な説明】[Brief description of the drawings]

第1図は本発明の一実施例を示す概略構成図、第2図
(a)(b)は本発明の他の実施例を示す概略構成図、
第3図は従来例を示す概略構成図である。 1……レーザ光 2……集光レンズ 3,31……SHG素子 4,32……光導波路 5,33……第2高調波ビーム 6……コリメート光 7,10……反射曲面 8,11,34……端面 9……光学部材
FIG. 1 is a schematic configuration diagram showing one embodiment of the present invention, FIGS. 2 (a) and 2 (b) are schematic configuration diagrams showing another embodiment of the present invention,
FIG. 3 is a schematic configuration diagram showing a conventional example. 1 laser light 2 condensing lens 3,31 SHG element 4,32 optical waveguide 5,33 second harmonic beam 6 collimated light 7,10 reflection curved surface 8,11 , 34 …… End face 9 …… Optical member

Claims (4)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】入射光の高調波を出射する導波路型非線形
光学素子と、該導波路型非線形光学素子の出射光を平行
光に変換する凹シリンドリカル反射面とで構成した平行
光作成装置。
1. A parallel light generating apparatus comprising: a waveguide type nonlinear optical element for emitting harmonics of incident light; and a concave cylindrical reflection surface for converting light emitted from the waveguide type nonlinear optical element into parallel light.
【請求項2】前記凹シリンドリカル反射面を、前記導波
路型非線形光学素子に設けたことを特徴とする請求項
(1)記載の平行光作成装置。
2. The parallel light generating apparatus according to claim 1, wherein said concave cylindrical reflection surface is provided in said waveguide type nonlinear optical element.
【請求項3】前記凹シリンドリカル反射面を、前記導波
路型非線形光学素子と略等しい屈折率の光学部材の一面
に構成したことを特徴とする請求項(1)記載の平行光
作成装置。
3. The parallel light generating apparatus according to claim 1, wherein said concave cylindrical reflection surface is formed on one surface of an optical member having a refractive index substantially equal to that of said waveguide type nonlinear optical element.
【請求項4】前記凹シリンドリカル反射面と、前記出射
光の光軸と直交する断面との形状を略円弧状にするとと
もに、前記凹シリンドリカル反射面が前記入射光の光軸
と平行をなすようにしたことを特徴とする請求項(1)
記載の平行光作成装置。
4. The concave cylindrical reflection surface and a cross section orthogonal to the optical axis of the outgoing light are formed in a substantially arc shape, and the concave cylindrical reflection surface is parallel to the optical axis of the incident light. Claim (1) characterized in that:
The collimated light producing device as described in the above.
JP1206381A 1989-08-09 1989-08-09 Parallel light creation device Expired - Lifetime JP2751119B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1206381A JP2751119B2 (en) 1989-08-09 1989-08-09 Parallel light creation device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1206381A JP2751119B2 (en) 1989-08-09 1989-08-09 Parallel light creation device

Publications (2)

Publication Number Publication Date
JPH0369926A JPH0369926A (en) 1991-03-26
JP2751119B2 true JP2751119B2 (en) 1998-05-18

Family

ID=16522400

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1206381A Expired - Lifetime JP2751119B2 (en) 1989-08-09 1989-08-09 Parallel light creation device

Country Status (1)

Country Link
JP (1) JP2751119B2 (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE69938845D1 (en) 1998-07-13 2008-07-10 Daikin Ind Ltd FINE POWDER OF MODIFIED POLYTETRAFLUOROETHYLENE AND METHOD FOR THE PRODUCTION THEREOF
ATE404597T1 (en) 2002-12-19 2008-08-15 Asahi Glass Co Ltd TETRAFLUORETHYLENE COPOLYMER
KR100700606B1 (en) * 2004-10-23 2007-03-28 엘지전자 주식회사 Method for restricting ptt service
US9650479B2 (en) 2007-10-04 2017-05-16 W. L. Gore & Associates, Inc. Dense articles formed from tetrafluoroethylene core shell copolymers and methods of making the same

Also Published As

Publication number Publication date
JPH0369926A (en) 1991-03-26

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