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JP4640207B2 - Optical element manufacturing method - Google Patents
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JP4640207B2 - Optical element manufacturing method - Google Patents

Optical element manufacturing method Download PDF

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JP4640207B2
JP4640207B2 JP2006045412A JP2006045412A JP4640207B2 JP 4640207 B2 JP4640207 B2 JP 4640207B2 JP 2006045412 A JP2006045412 A JP 2006045412A JP 2006045412 A JP2006045412 A JP 2006045412A JP 4640207 B2 JP4640207 B2 JP 4640207B2
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substrate
optical element
crystal
wavelength conversion
manufacturing
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JP2007225786A (en
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勝彦 徳田
公資 東條
守 久光
一智 門倉
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Shimadzu Corp
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Description

本発明は、光学素子の製造方法に関し、さらに詳しくは、製造作業効率を向上できると共に安定した特性が得られる光学素子を製造できる光学素子の製造方法に関する。 The present invention relates to an optical element manufacturing method , and more particularly to an optical element manufacturing method capable of manufacturing an optical element that can improve manufacturing work efficiency and obtain stable characteristics.

レーザ結晶と波長変換結晶とを一体化した構造の光学素子およびその製造方法が知られている(特許文献1参照。)。
他方、内部に周期的分極反転構造を有する強誘電体結晶の製造方法が知られている(特許文献2参照。)。
特開2005−57043号公報 特開2005−208197号公報
An optical element having a structure in which a laser crystal and a wavelength conversion crystal are integrated and a manufacturing method thereof are known (see Patent Document 1).
On the other hand, a manufacturing method of a ferroelectric crystal having a periodic domain-inverted structure inside is known (see Patent Document 2).
JP 2005-57043 A JP-A-2005-208197

レーザ結晶と波長変換結晶とを一体化した構造の光学素子では、製造に際して、レーザ結晶のレーザ光出射面と波長変換結晶のレーザ光入射面とを貼り合わせて一体化する作業が必要になる。ここで、レーザ結晶のレーザ光出射面および波長変換結晶のレーザ光入射面の両方とも広い面積とすることが出来れば、貼り合わせる作業に困難はない。
しかし、波長変換結晶のレーザ光入射面が狭い面積となる場合がある。例えば、結晶内に周期的分極反転構造を形成する必要がある波長変換結晶では、周期的分極反転構造の分極反転の周期と分極方向の結晶厚のアスペクト比の制約により、結晶厚を大きくできないため、レーザ光入射面が狭い面積となってしまう。このような場合は、レーザ結晶のレーザ光出射面と波長変換結晶のレーザ光入射面とを貼り合わせて一体化する作業が困難になり、作業効率が悪くなる問題点がある。また、安定した品質で貼り合わせることが困難になり、貼り合わせた面内の場所によって特性が異なったり、光学素子間で特性がばらついたりする問題点がある。
そこで、本発明の目的は、製造作業効率を向上できると共に安定した特性が得られる光学素子を製造できる光学素子の製造方法を提供することにある。
In an optical element having a structure in which a laser crystal and a wavelength conversion crystal are integrated, it is necessary to attach and integrate the laser light emission surface of the laser crystal and the laser light incident surface of the wavelength conversion crystal during manufacture. Here, if both the laser light emitting surface of the laser crystal and the laser light incident surface of the wavelength conversion crystal can have a large area, there is no difficulty in bonding.
However, the laser light incident surface of the wavelength conversion crystal may have a narrow area. For example, in a wavelength conversion crystal that needs to form a periodic domain-inverted structure in the crystal, the crystal thickness cannot be increased due to restrictions on the aspect ratio of the period of domain inversion of the periodic domain-inverted structure and the crystal thickness in the polarization direction. The laser light incident surface becomes a small area. In such a case, it is difficult to attach and integrate the laser light emitting surface of the laser crystal and the laser light incident surface of the wavelength conversion crystal, and there is a problem that the working efficiency is deteriorated. Further, it is difficult to bond with a stable quality, and there are problems that the characteristics differ depending on the location within the bonded surface, and the characteristics vary between optical elements.
SUMMARY OF THE INVENTION An object of the present invention is to provide an optical element manufacturing method capable of improving the manufacturing work efficiency and manufacturing an optical element capable of obtaining stable characteristics.

第1の観点では、本発明は、板状体であって反転分極構造を有する複数の波長変換結晶基板(12)と板状体の複数のダミー材基板(13)とを、前記波長変換結晶基板(12)のレーザ光入射面(12i)以外の面(12a)において交互に貼り合わせて、第1複合基板(21)を生成する工程と、前記第1複合基板(21)の前記レーザ光入射面(12i)がある面と板状体であってその一面がレーザ光出射面(11o)であるレーザ結晶基板(11)の前記レーザ光出射面(11o)がある面とを貼り付けて第2複合基板(22)を生成する工程と、前記第2複合基板(22)を切断して複数の光学素子(10)を得る工程とを有することを特徴とする光学素子の製造方法を提供する。
上記第1の観点による光学素子の製造方法では、波長変換結晶基板(12)とダミー材基板(13)とを貼り合わせた後、レーザ結晶基板(11)に貼り付けるといった製造方法を採ることが出来る。ここで、周期的分極反転構造の分極反転の周期と分極方向の結晶厚のアスペクト比の制約がレーザ光入射面(2i)以外の面(12a)にはないため、波長変換結晶基板(12)とダミー材基板(13)の貼り合わせ面積を大きくすることができ、この貼り合わせ作業は容易である。また、波長変換結晶基板(12)とダミー材基板(13)とを貼り合わせた第1複合基板(21)をレーザ結晶基板(11)に貼り合わせるが、波長変換結晶基板(12)とダミー材基板(13)とを合わせた貼り合わせ面積になるため、貼り合わせ作業が容易になる。よって、製造の作業効率を向上することが出来る。さらに、安定した品質で貼り合わせることが出来るため、貼り合わせた面内の場所によって特性が異なったり、光学素子間で特性がばらついたりする問題点がなくなり、安定した特性の光学素子が得られる。
In a first aspect, the present invention provides a plurality of wavelength conversion crystal substrates (12) each having a plate-like body having an inverted polarization structure and a plurality of dummy material substrates (13) having a plate-like body. A step of alternately laminating on a surface (12a) other than the laser light incident surface (12i) of the substrate (12) to generate a first composite substrate (21), and the laser light of the first composite substrate (21) The surface having the incident surface (12i) and the surface having the laser light emitting surface (11o) of the laser crystal substrate (11), which is a plate-like body and one surface thereof is the laser light emitting surface (11o), are attached. Provided is a method for producing an optical element, comprising: a step of generating a second composite substrate (22); and a step of obtaining a plurality of optical elements (10) by cutting the second composite substrate (22). To do.
In the optical element manufacturing method according to the first aspect, the wavelength conversion crystal substrate (12 ) and the dummy material substrate (13 ) are bonded together, and then bonded to the laser crystal substrate ( 11). Can be taken. Since periodically poled polarization inversion period to the polarization direction of the crystal thickness aspect ratio limitations of structure is not the laser light entrance surface (1 2i) other surfaces (1 2a), the wavelength conversion crystal substrate ( 1 2) and can increase the bonding area of the dummy material substrate (1 3), the bonding work is easy. Further, attaching the first composite substrate (21) bonded to a wavelength conversion crystal substrate (1 2) and a dummy member substrate (1 3) to the laser crystal substrate (1 1), the wavelength conversion crystal substrate (1 2 ) and dummy material substrate (1 3) and order to become bonded area combined, the combined work becomes easy pasting Ri. Therefore, the work efficiency of manufacture can be improved. Furthermore, since it is possible to bond with stable quality, or different characteristics depending on the location in the bonding surface, there is no problem or variations in characteristics between the optical elements, the optical element with stable characteristics can be obtained.

上記第1の観点による光学素子の製造方法では、内部に周期的分極反転構造を有する強誘電体結晶を波長変換結晶(2)とするので、周期的分極反転構造の分極反転の周期と分極方向の結晶厚のアスペクト比の制約を受ける。従って、本発明が特に有用になる。 In the method of manufacturing an optical element according to the first aspect, since the ferroelectric crystal having a periodic polarization inversion structure is used as the wavelength conversion crystal (2), the period of polarization inversion of the periodic polarization inversion structure and the polarization direction The crystal thickness aspect ratio is limited. Therefore, the present invention is particularly useful.

前記強誘電体結晶として、定比組成(ストイキオメトリ)または定比組成に近いタンタル酸リチウムを用いる、周期的分極反転構造の形成が容易になる。 As the ferroelectric crystal, the use of lithium tantalate close to the stoichiometric composition (stoichiometric) or the stoichiometric composition, the formation of the periodically poled structure is facilitated.

前記タンタル酸リチウムとして、モル分率Li2O/(Ta25+Li2O)が0.490以上0.500未満のタンタル酸リチウムを用いる、周期的分極反転構造の形成が容易になる。 As the lithium tantalate, the mole fraction Li 2 O / (Ta 2 O 5 + Li 2 O) is a lithium tantalate less 0.500 or 0.490, formation of the periodically poled structure is facilitated .

前記タンタル酸リチウムとして、Mg,Zn,Sc,Inの少なくとも一種類をドープされたものであると、周期的分極反転構造の形成が容易になる。 When the lithium tantalate is doped with at least one of Mg, Zn, Sc, and In , the periodic domain-inverted structure can be easily formed.

の観点では、本発明は、前記レーザ結晶基板(11)に前記第1複合基板(21)を接着剤と同じ屈折率のスペーサ(5)を挟んで前記接着剤により貼り付けことを特徴とする光学素子の製造方法を提供する。
接着剤だけであれば、接着剤の厚さがほぼ決まってしまい、エタロン効果を生じることがある。
そこで、上記第の観点による光学素子の製造方法では、スペーサ(5)を挟んで光路長を調整し、エタロン効果を抑制できる。
In a second aspect, the present invention is that more pasted to the adhesive across the spacer having the same refractive index as the adhesive (5) the first composite substrate (21) to the laser crystal substrate (1 1) An optical element manufacturing method is provided.
If only the adhesive is used, the thickness of the adhesive is almost determined, and an etalon effect may occur.
Therefore, in the method for manufacturing an optical element according to the second aspect, by adjusting the optical path length across the spacer (5), Ru can be suppressed etalon effect.

の観点では、本発明は、前記第1の観点による光学素子の製造方法において、前記レーザ結晶基板(11)に前記第1複合基板(21)をオプチカルコンタクト(7)により貼り付けことを特徴とする光学素子の製造方法を提供する。
上記第の観点による光学素子の製造方法では、オプチカルコンタクト(7)を用いるため、エタロン効果を生じなくなる。
In a third aspect, the present invention provides a method for manufacturing an optical element according to the first aspect, the first composite substrate (21) that paste by Opti cull contact (7) in the laser crystal substrate (1 1) An optical element manufacturing method is provided.
In the optical element manufacturing method according to the third aspect , since the optical contact (7) is used, the etalon effect does not occur.

の観点では、本発明は、前記第1の観点による光学素子の製造方法において、前記波長変換結晶基板(12)と前記ダミー材基板(13)とを接着剤により貼り付けことを特徴とする光学素子の製造方法を提供する。
上記第の観点による光学素子の製造方法では、接着剤を用いるため、オプチカルコンタクト(7)を用いる場合より、作業が容易になる。
In a fourth aspect, the present invention provides a method for manufacturing an optical element according to the first aspect, the wavelength conversion crystal substrate (1 2) and the dummy material substrate (1 3) and that that adhered by an adhesive An optical element manufacturing method is provided.
In the method for manufacturing an optical element according to the fourth aspect , since an adhesive is used, the operation becomes easier than when the optical contact (7) is used.

上記第1の観点による光学素子の製造方法では、複数の光学素子(10)をまとめて製造できる。 The method for manufacturing an optical element according to the first aspect, can be produced together multiple optical elements (10).

本発明の光学素子の製造方法によれば、製造の作業効率を向上することが出来る。さらに、安定した特性の光学素子が得られる。 According to the manufacturing method of an optical element of the present invention, it is possible to improve the working efficiency of the production. Furthermore, an optical element having stable characteristics can be obtained.

以下、図に示す実施例により本発明をさらに詳細に説明する。なお、これにより本発明が限定されるものではない。   Hereinafter, the present invention will be described in more detail with reference to the embodiments shown in the drawings. Note that the present invention is not limited thereby.

図1は、実施例1に係る光学素子10を示す斜視図である。
この光学素子10は、半導体レーザからの励起レーザ光Liにより励起されて基本波レーザ光を出すレーザ結晶1と、基本波レーザ光の高調波である波長変換レーザ光Loを出す波長変換結晶2と、波長変換結晶2をサンドイッチ状に挟むダミー材3とを具備している。
FIG. 1 is a perspective view illustrating an optical element 10 according to the first embodiment.
The optical element 10 includes a laser crystal 1 that emits a fundamental laser beam by being excited by excitation laser light Li from a semiconductor laser, and a wavelength conversion crystal 2 that emits a wavelength conversion laser beam Lo that is a harmonic of the fundamental laser beam. And a dummy material 3 sandwiching the wavelength conversion crystal 2 in a sandwich shape.

図2は、光学素子10の分解斜視図である。
板状体のレーザ結晶1のレーザ光出射面1o一部に、板状体の波長変換結晶2のレーザ光入射面2iが貼り付けられる。また、レーザ結晶1のレーザ光出射面1oの別の一部に、板状体のダミー材3の一面3dが貼り付けられ且つダミー材3の別の一面3eが波長変換結晶2のレーザ光入射面2i以外の一面2aに貼り付けられる。
FIG. 2 is an exploded perspective view of the optical element 10.
The laser beam incident surface 2i of the plate-shaped wavelength conversion crystal 2 is attached to a part of the laser beam emitting surface 1o of the plate-shaped laser crystal 1. Further, one surface 3d of the plate-like dummy material 3 is attached to another part of the laser light emitting surface 1o of the laser crystal 1, and the other surface 3e of the dummy material 3 is incident on the laser light of the wavelength conversion crystal 2. Affixed to one surface 2a other than the surface 2i.

図3は、光学素子10の製造手順を示すフロー図である。
ステップS1では、図4に示すごとき波長変換結晶大基板32を作成する。
波長変換結晶大基板32は、例えば特許文献2に記載の製造方法により製造できる。すなわち、所定サイズの強誘電体結晶大基板32aの対向面に周期電極32bとベタ電極32cを形成し、電極間に電圧を印加し、強誘電体結晶大基板32aの内部に周期的分極反転構造を形成する。電極の対向方向が分極方向Dpになり、周期電極32bの形状の周期パターン方向が分極反転方向Drになる。電極は、そのまま残しておいてもよいし、除去してもよい。ダミー材との接着にオプチカルコンタクトを利用する場合には除去する方が望ましい。
FIG. 3 is a flowchart showing the manufacturing procedure of the optical element 10.
In step S1, a wavelength conversion crystal large substrate 32 as shown in FIG. 4 is formed.
The wavelength conversion crystal large substrate 32 can be manufactured by the manufacturing method described in Patent Document 2, for example. That is, the periodic electrode 32b and the solid electrode 32c are formed on the opposing surfaces of the ferroelectric crystal large substrate 32a having a predetermined size, a voltage is applied between the electrodes, and the periodic polarization inversion structure is formed inside the ferroelectric crystal large substrate 32a. Form. The opposing direction of the electrodes is the polarization direction Dp, and the periodic pattern direction of the shape of the periodic electrode 32b is the polarization inversion direction Dr. The electrode may be left as it is or may be removed. When using an optical contact for bonding to the dummy material, it is preferable to remove it.

強誘電体結晶大基板32aは、例えば、MgOをドープした、定比組成(ストイキオメトリ)または定比組成に近いタンタル酸リチウム基板(MgOドープ定比組成タンタル酸リチウムj基板)であり、そのモル分率Li2O/(Ta25+Li2O)は0.49以上0.5未満である。 The ferroelectric crystal large substrate 32a is, for example, a MgO-doped, stoichiometric composition or stoichiometric lithium tantalate substrate (MgO doped stoichiometric lithium tantalate j substrate), The molar fraction Li 2 O / (Ta 2 O 5 + Li 2 O) is 0.49 or more and less than 0.5.

図3に戻り、ステップS2では、分極反転方向Drの幅が所定の作用長Lになるように波長変換結晶大基板32をダイシング装置で切断し、図5に示すごとき波長変換結晶基板12を複数得る。例えば、波長変換結晶基板12の作用長Lは2mm、厚さdは0.4mm、分極方向Dpおよび分極反転方向Drに交差する方向の長さGは6mmである。
そして、ステップS5へ進む。
Returning to FIG. 3, in step S <b> 2, the wavelength conversion crystal large substrate 32 is cut with a dicing device so that the width of the polarization reversal direction Dr becomes a predetermined action length L, and a plurality of wavelength conversion crystal substrates 12 as shown in FIG. obtain. For example, the working length L of the wavelength conversion crystal substrate 12 is 2 mm, the thickness d is 0.4 mm, and the length G in the direction intersecting the polarization direction Dp and the polarization inversion direction Dr is 6 mm.
Then, the process proceeds to step S5.

ステップS3では、厚さWのダミー材大基板と厚さwのダミー材大基板とを作成する。
ステップS4では、波長変換結晶基板12の作用長Lと長さGに合わせたサイズにダミー材大基板を切断し、図6に示すごときダミー材基板13−1および13−2を複数得る。例えば、ダミー材基板13−1の厚さWは1mm、ダミー材基板13−2の厚さwは0.5mmである。
そして、ステップS5へ進む。
In step S3, a dummy material large substrate having a thickness W and a dummy material large substrate having a thickness w are formed.
In step S4, the dummy material large substrate is cut into a size that matches the working length L and length G of the wavelength conversion crystal substrate 12 to obtain a plurality of dummy material substrates 13-1 and 13-2 as shown in FIG. For example, the thickness W of the dummy material substrate 13-1 is 1 mm, and the thickness w of the dummy material substrate 13-2 is 0.5 mm.
Then, the process proceeds to step S5.

ダミー材は、熱膨張した時の悪影響を抑制するため、熱膨張係数がレーザ結晶1や波長変換結晶2と同程度の材料とするのが好ましい。例えばCLT基板である。   The dummy material is preferably made of a material having a thermal expansion coefficient comparable to that of the laser crystal 1 and the wavelength conversion crystal 2 in order to suppress adverse effects when thermally expanded. For example, a CLT substrate.

ステップS5では、図7に示すように波長変換結晶基板12とダミー材基板13−1とを交互に貼り合わせ、両端にはダミー材基板13−2を貼り合わせ、第1複合基板21を作成する。貼り合わせた方向の第1複合基板21の幅Zは例えば7mmである。
貼り合わせの方法は、接着剤を用いてもよいし、オプチカルコンタクトを用いてもよい。
In step S5, as shown in FIG. 7, the wavelength conversion crystal substrate 12 and the dummy material substrate 13-1 are alternately bonded, and the dummy material substrate 13-2 is bonded to both ends, thereby forming the first composite substrate 21. . The width Z of the first composite substrate 21 in the bonded direction is, for example, 7 mm.
As the bonding method, an adhesive may be used, or an optical contact may be used.

ステップS6では、分極反転方向Drに対向する第1複合基板21の2面に光学研磨を施し、必要なAR膜あるいはHR膜を成膜する。例えば、2面の一方に基本波に対するAR膜を成膜し、他方にHR膜を成膜する。
そして、ステップS10へ進む。
In step S6, the two surfaces of the first composite substrate 21 facing the polarization reversal direction Dr are optically polished to form a necessary AR film or HR film. For example, an AR film for the fundamental wave is formed on one of the two surfaces, and an HR film is formed on the other.
Then, the process proceeds to step S10.

ステップS7では、所定の厚さhを持つレーザ結晶大基板を作成する。
ステップS8では、第1複合基板21の長さGと幅Zに合わせたサイズにレーザ結晶大基板を切断し、図8に示すごときレーザ結晶基板11を得る。例えば、レーザ結晶基板11の厚さhは1mmである。
レーザ結晶大基板は、例えばYAG結晶大基板である。
In step S7, a laser crystal large substrate having a predetermined thickness h is formed.
In step S8, the large laser crystal substrate is cut to a size matching the length G and width Z of the first composite substrate 21 to obtain the laser crystal substrate 11 as shown in FIG. For example, the thickness h of the laser crystal substrate 11 is 1 mm.
The laser crystal large substrate is, for example, a YAG crystal large substrate.

ステップS9では、レーザ光が入射または出射するレーザ結晶基板11の2面に光学研磨を施し、必要なAR膜あるいはHR膜を成膜する。例えば、2面の一方に基本波に対するAR膜を成膜し、他方にHR膜を成膜する。
そして、ステップS10へ進む。
In step S9, the two surfaces of the laser crystal substrate 11 on which the laser beam is incident or emitted are optically polished to form a necessary AR film or HR film. For example, an AR film for the fundamental wave is formed on one of the two surfaces, and an HR film is formed on the other.
Then, the process proceeds to step S10.

ステップS10では、図8に示すように第1複合基板21のAR膜を成膜した面とレーザ結晶基板11のAR膜を成膜した面すなわちレーザ光出射面11aとを貼り合わせて第2複合基板22を作成する。
貼り合わせの方法は、接着剤を用いてもよいし、オプチカルコンタクトを用いてもよい。
In step S10, as shown in FIG. 8, the surface of the first composite substrate 21 on which the AR film is formed and the surface of the laser crystal substrate 11 on which the AR film is formed, that is, the laser light emitting surface 11a are bonded together. A substrate 22 is created.
As the bonding method, an adhesive may be used, or an optical contact may be used.

ステップS11では、図9に示すように切断線Cで第2複合基板22を切断し、複数の光学素子10を得る。   In step S11, as shown in FIG. 9, the 2nd composite substrate 22 is cut | disconnected by the cutting line C, and the some optical element 10 is obtained.

実施例1に係る光学素子10によれば、波長変換結晶2とダミー材3とを貼り合わせた後、レーザ結晶1に貼り付けるといった製造方法を採ることが出来るので、レーザ結晶1への貼り合わせ面積が波長変換結晶2とダミー材3とを合わせた面積になるため、貼り合わせ作業が容易になる。よって、製造の作業効率を向上することが出来る。また、安定した品質で貼り合わせることが出来るため、貼り合わせた面内の場所によって特性が異なったり、光学素子間で特性がばらついたりする問題点がなくなり、安定した特性が得られる。さらに、ダミー材3として、レーザ結晶1や波長変換結晶2よりも熱伝導のよい材料を用いれば、ダミー材3がない場合より温度制御がしやすくなる。   According to the optical element 10 according to the first embodiment, after the wavelength conversion crystal 2 and the dummy material 3 are bonded together, a manufacturing method in which the wavelength conversion crystal 2 and the dummy material 3 are bonded to the laser crystal 1 can be adopted. Since the area is the area where the wavelength conversion crystal 2 and the dummy material 3 are combined, the bonding operation is facilitated. Therefore, the work efficiency of manufacture can be improved. In addition, since it can be bonded with a stable quality, there is no problem that the characteristics are different depending on the location within the bonded surface or the characteristics vary between optical elements, and stable characteristics can be obtained. Furthermore, if a material having better thermal conductivity than the laser crystal 1 and the wavelength conversion crystal 2 is used as the dummy material 3, temperature control becomes easier than when the dummy material 3 is not provided.

また、実施例1に係る光学素子の製造方法によれば、複数の光学素子10をまとめて容易に製造できる。   Moreover, according to the manufacturing method of the optical element which concerns on Example 1, the some optical element 10 can be manufactured collectively easily.

図10および図11に示すように、レーザ結晶1のレーザ出射面1oと、波長変換結晶2のレーザ光入射面2iおよびダミー材3の面3dとの間に、スぺーサ5を挟んでもよい。
スぺーサ5は、基本波レーザ光を通し且つレーザ結晶1と同程度の熱膨張率を持つ材料とするのが好ましい。
As shown in FIGS. 10 and 11, a spacer 5 may be sandwiched between the laser emission surface 1 o of the laser crystal 1, the laser light incident surface 2 i of the wavelength conversion crystal 2, and the surface 3 d of the dummy material 3. .
The spacer 5 is preferably made of a material that transmits fundamental laser light and has a thermal expansion coefficient comparable to that of the laser crystal 1.

実施例2に係る光学素子10によれば、スぺーサ5の厚さを適切にすることで、接着剤によるエタロン効果を緩和することが出来る。   According to the optical element 10 according to the second embodiment, the etalon effect due to the adhesive can be reduced by making the thickness of the spacer 5 appropriate.

(1)波長変換結晶大基板32として、内部に周期的分極構造を有したLT基板やLN基板、MgOをドープしたLT基板やLN基板、KTP基板も使用できる。
(2)ダミー材大基板として、波長変換結晶2と同じ材料(周期的分極反転構造は必要ない)や、石英ガラス、BK−7なども使用できる。
(3)ダミー基板3を波長変換結晶2の片面だけに貼り合わせてもよい。
(1) As the wavelength conversion crystal large substrate 32, an LT substrate or LN substrate having a periodic polarization structure therein, an LT substrate or LN substrate doped with MgO, or a KTP substrate can also be used.
(2) As the dummy material large substrate, the same material as the wavelength conversion crystal 2 (periodic polarization inversion structure is not required), quartz glass, BK-7, or the like can be used.
(3) The dummy substrate 3 may be bonded to only one side of the wavelength conversion crystal 2.

本発明の光学素子およびその製造方法は、例えばSHG波長変換技術を用いた半導体励起固体レーザ等に利用できる。   The optical element and the manufacturing method thereof according to the present invention can be used for, for example, a semiconductor excitation solid-state laser using SHG wavelength conversion technology.

実施例1に係る光学素子を示す斜視図である。1 is a perspective view showing an optical element according to Example 1. FIG. 実施例1に係る光学素子を示す分解斜視図である。1 is an exploded perspective view showing an optical element according to Example 1. FIG. 実施例1に係る光学素子の製造手順を示すフロー図である。FIG. 3 is a flowchart showing a manufacturing procedure of the optical element according to Example 1. 波長変換結晶大基板を示す斜視図である。It is a perspective view which shows a wavelength conversion crystal large substrate. 波長変換結晶基板を示す斜視図である。It is a perspective view which shows a wavelength conversion crystal substrate. ダミー材基板を示す斜視図である。It is a perspective view which shows a dummy material board | substrate. 第1複合基板を示す斜視図である。It is a perspective view which shows a 1st composite substrate. 第1複合基板とレーザ結晶基板の貼り合わせ工程を示す斜視図である。It is a perspective view which shows the bonding process of a 1st composite substrate and a laser crystal substrate. 第2複合基板を示す斜視図である。It is a perspective view which shows a 2nd composite substrate. 実施例2に係る光学素子を示す斜視図である。6 is a perspective view showing an optical element according to Example 2. FIG. 実施例2に係る光学素子を示す分解斜視図である。6 is an exploded perspective view showing an optical element according to Embodiment 2. FIG.

符号の説明Explanation of symbols

1 レーザ結晶
1o レーザ光出射面
2 波長変換結晶
2i レーザ光入射面
3 ダミー材
5 スぺーサ
10 光学素子
21 第1複合基板
22 第2複合基板
DESCRIPTION OF SYMBOLS 1 Laser crystal 1o Laser beam emission surface 2 Wavelength conversion crystal 2i Laser beam incident surface 3 Dummy material 5 Spacer 10 Optical element 21 1st composite substrate 22 2nd composite substrate

Claims (4)

板状体であって反転分極構造を有する複数の波長変換結晶基板(12)と板状体の複数のダミー材基板(13)とを、前記波長変換結晶基板(12)のレーザ光入射面(12i)以外の面(12a)において交互に貼り合わせて、第1複合基板(21)を生成する工程と、前記第1複合基板(21)の前記レーザ光入射面(12i)がある面と板状体であってその一面がレーザ光出射面(11o)であるレーザ結晶基板(11)の前記レーザ光出射面(11o)がある面とを貼り付けて第2複合基板(22)を生成する工程と、前記第2複合基板(22)を切断して複数の光学素子(10)を得る工程とを有することを特徴とする光学素子の製造方法 A plurality of wavelength conversion crystal substrates (12) each having a plate-like body and an inverted polarization structure and a plurality of dummy material substrates (13) of the plate-like body are connected to a laser light incident surface (12) of the wavelength conversion crystal substrate (12). A step of alternately laminating on a surface (12a) other than 12i) to generate a first composite substrate (21), and a surface and a plate having the laser light incident surface (12i) of the first composite substrate (21) The second composite substrate (22) is generated by pasting the surface of the laser crystal substrate (11) having the laser light emitting surface (11o) and the surface having the laser light emitting surface (11o). A method of manufacturing an optical element, comprising: a step; and a step of cutting the second composite substrate (22) to obtain a plurality of optical elements (10) . 請求項1に記載の光学素子の製造方法において、前記レーザ結晶基板(11)に前記第1複合基板(21)を接着剤と同じ屈折率のスペーサ(5)を挟んで前記接着剤により貼り付けることを特徴とする光学素子の製造方法 2. The method of manufacturing an optical element according to claim 1, wherein the first composite substrate (21) is attached to the laser crystal substrate (11) with the adhesive having a spacer (5) having the same refractive index as that of the adhesive. A method for manufacturing an optical element . 請求項1に記載の光学素子の製造方法において、前記レーザ結晶基板(11)に前記第1複合基板(21)をオプチカルコンタクトにより貼り付けることを特徴とする光学素子の製造方法 The method of manufacturing an optical element according to claim 1, wherein the first composite substrate (21) is attached to the laser crystal substrate (11) by optical contact . 請求項1に記載の光学素子の製造方法において、前記波長変換結晶基板(12)と前記ダミー材基板(13)とを接着剤により貼り付けることを特徴とする光学素子の製造方法 2. The method of manufacturing an optical element according to claim 1, wherein the wavelength conversion crystal substrate (12) and the dummy material substrate (13) are attached with an adhesive .
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