JP2005241813A - Optical path converting optical waveguide and its manufacturing method - Google Patents
Optical path converting optical waveguide and its manufacturing method Download PDFInfo
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本発明は、光路変換光導波路の作製方法に関するもので、光を拡散させることなく90°もしくはそれに近い角度で光路を変換する光導波路を提供するものである。 The present invention relates to a method for manufacturing an optical path conversion optical waveguide, and provides an optical waveguide that converts an optical path at an angle of 90 ° or close to it without diffusing light.
レーザーの集光照射により、ガラスのような透明材料の内部を局所的に高屈折率化し、高屈折率化した領域を連続的に形成させることでガラス内部に導波路が形成できることが知られている(特許文献1参照)。 It is known that a waveguide can be formed inside the glass by locally forming a high refractive index inside a transparent material such as glass and continuously forming a high refractive index region by condensing laser irradiation. (See Patent Document 1).
前記、導波路形成方法を利用して、まず、レーザーにより基材に第1の導波路を形成させ、次に基材を90°回転させて先に形成した導波路と直交するように第2の導波路を形成させ、その後、直交部分を45°反射面がでるように切断除去することで光路変換導波路を作製する方法や、基材を予め45°研磨した後に、まず、第一の導波路を形成させ、次に基材を90°回転させて先に形成した導波路と45°研磨面で接触するように第二の導波路を形成させることで光路変換導波路を作製する方法(特許文献2、3参照)が知られている。 Using the above-described waveguide formation method, first, a first waveguide is formed on a substrate by a laser, and then the substrate is rotated by 90 ° so that the second waveguide is orthogonal to the previously formed waveguide. After that, a method for producing an optical path conversion waveguide by cutting and removing an orthogonal portion so that a 45 ° reflection surface appears, or after polishing the substrate in advance by 45 °, first, Method of forming an optical path conversion waveguide by forming a waveguide and then forming a second waveguide so that the substrate is rotated 90 ° to contact the previously formed waveguide at a 45 ° polished surface (See Patent Documents 2 and 3).
しかしながら、前記方法においては、反射部での僅かな位置ずれが損失の増大に繋がることから、第一の導波路と第二の導波路との位置合わせを高精度で行う必要があり、特に、コア径が10ミクロン以下のシングルモードタイプの光路変換光導波路作製においては、低伝送損失化及び複数の光路変換導波路間での伝送損失のバラツキ抑制が容易ではない。
光路変換光導波路の作製方法において、光路変換部分の導波路同士の位置合わせが不要で、低伝送損失かつ導波路間のバラツキがない光路変換導波路の作製方法を提供することを課題とする。 An object of the present invention is to provide a method for manufacturing an optical path conversion waveguide that does not require alignment between the waveguides in the optical path conversion portion, has a low transmission loss, and does not vary between the waveguides.
本発明は、レーザーの集光照射により、基材の内部を高屈折率化し、高屈折率化した領域を連続的に形成させることで光路変換導波路を作製する方法において、反射面前後で光軸の方向が変化した第一の光導波路と第二の光導波路を連続して一体的に形成することを特徴とする光路変換素子の製造方法であり、レーザーの光軸に対して、少なくとも1面以上がレーザー光を全反射する面を有している基材内部にレーザーを集光照射し、レーザーの集光レンズもしくは基材を、基材入射前のレーザーの光軸に対して平行に直線移動させることで、第一の光路を形成し、続いて全反射面でレーザー光の方向を変換することで、第二の光路部分にレーザー集光点に移動し、反射面前後の第一の光導波路と第二の光導波路を連続して形成することを特徴とする光路変換導波路の製造方法である。本方法と逆に第二の導波路を先に形成し続いて第一の導波路を形成することも有効である。 The present invention relates to a method for producing an optical path conversion waveguide by continuously forming a region having a high refractive index by increasing the refractive index inside a substrate by condensing irradiation of a laser. A method of manufacturing an optical path conversion element, characterized in that a first optical waveguide and a second optical waveguide whose axis directions are changed are continuously and integrally formed, and at least 1 with respect to the optical axis of the laser. The laser beam is focused and irradiated inside the base material that has a surface that totally reflects the laser beam, and the laser condensing lens or base material is parallel to the laser optical axis before the base material is incident. By moving in a straight line, the first optical path is formed, and then the direction of the laser beam is changed at the total reflection surface, so that the laser beam is moved to the second optical path portion, and the first optical path before and after the reflection surface. The optical waveguide and the second optical waveguide are formed continuously. It is a manufacturing method of the optical path conversion waveguide to. In contrast to this method, it is also effective to form the second waveguide first and then form the first waveguide.
また、複数の反射面をもつ光路変換導波路において、これらの方法を繰り返すことにより複数の部分で光路を変換する特徴とする多段光路変換素子の製造方法に関するものであり、これらの方法で作製された光路変換光導波路を含む光デバイスに関するものである。 The present invention also relates to a method of manufacturing a multistage optical path conversion element characterized by converting an optical path at a plurality of portions by repeating these methods in an optical path conversion waveguide having a plurality of reflecting surfaces. The present invention relates to an optical device including an optical path conversion optical waveguide.
本発明の光導波路の作製方法は、レーザーの集光照射により、基材の内部を高屈折率化し、高屈折率化した領域を連続的に形成させることで導波路を作製する方法において、導波路を形成させようとする基材の構成面の内、レーザーの光軸に対して少なくとも1面以上がレーザー光を全反射する入射角となるような面を有している状態でレーザーを基材内部に集光照射することで、レーザーの集光レンズもしくは基材をレーザーの光軸に対して平行に直線移動させるだけで、進行方向が異なる2本以上の直線導波路を反射面上で結合させることができることから、導波路特性にバラツキが無く、伝送損失が低い光路変換導波路を作製することができる。 The optical waveguide manufacturing method of the present invention is a method of manufacturing a waveguide by continuously forming a region having a high refractive index by increasing the refractive index inside the substrate by condensing laser irradiation. Of the constituent surfaces of the base material on which the waveguide is to be formed, at least one surface with respect to the optical axis of the laser has a surface that has an incident angle that totally reflects the laser light. By focusing and irradiating the inside of the material, it is possible to create two or more linear waveguides with different traveling directions on the reflecting surface simply by linearly moving the laser condensing lens or base material parallel to the optical axis of the laser. Since they can be coupled, it is possible to produce an optical path conversion waveguide with no variation in waveguide characteristics and low transmission loss.
以下、本発明について、図面を参照して実施の形態(実施例)とともに詳細に説明する。 Hereinafter, the present invention will be described in detail together with embodiments (examples) with reference to the drawings.
(実施例1) 図は、本発明による実施例1の光路変換光導波路の製造方法を示す模式図であり、図1の基材に図3に示す、1列が8本の直角に曲がった高屈折率ラインLを2列、図2の方法で形成する。まず、図1に示す形状に石英ガラスよりなる基材1を加工・研磨する。サイズは図1中、Aが20mm、B及びCが10mmでDの角度は45°である。表面は全面を光学研磨してある。 (Example 1) The figure is a schematic diagram showing a method of manufacturing an optical path converting optical waveguide of Example 1 according to the present invention, and one row shown in FIG. Two rows of high refractive index lines L are formed by the method shown in FIG. First, the substrate 1 made of quartz glass is processed and polished into the shape shown in FIG. In FIG. 1, A is 20 mm, B and C are 10 mm, and the angle of D is 45 °. The entire surface is optically polished.
次に、図2(a)に示すように基材1をガラス基盤4上に置き、基材1の下部より対物レンズ2を通して、全反射面5で反射してレーザー光3の最初の焦点位置がE点になるように基材1と対物レンズ2の位置を調節する。この際、レーザー3が対物レンズ2に入射される前のビーム径は5mmで、レーザーには波長:800nm、パルス幅:150fs、パルスエネルギー:2μJ、繰り返し周波数:200kHzのパルスレーザーを使用した。
次に、図2(b)のように基材1を図の上方向に直線移動させることで、図2(a)の集光点Eを連続的に図2(b)のF点まで移動させた。その際、集光点の奇跡は点線Gをたどり、集光点の奇跡が周囲に比べ高屈折率化している直角ラインが形成されていることを確認した。
Next, as shown in FIG. 2A, the base material 1 is placed on the glass substrate 4, reflected from the lower surface of the base material 1 through the objective lens 2, the total reflection surface 5, and the initial focal position of the laser light 3. The positions of the base material 1 and the objective lens 2 are adjusted so that becomes an E point. At this time, the beam diameter before the laser 3 was incident on the objective lens 2 was 5 mm, and a pulse laser having a wavelength of 800 nm, a pulse width of 150 fs, a pulse energy of 2 μJ, and a repetition frequency of 200 kHz was used.
Next, as shown in FIG. 2 (b), the base 1 is linearly moved upward in the figure, so that the condensing point E in FIG. 2 (a) is continuously moved to the point F in FIG. 2 (b). I let you. At that time, the miracle of the condensing point followed the dotted line G, and it was confirmed that a right-angle line was formed in which the miracle of the condensing point had a higher refractive index than the surroundings.
その後、レーザー光3を遮断し、基材1と対物レンズ2の位置関係を図2(a)の状態に戻し、更に基材1のみをY軸方向に250μm移動させ、図2(a)〜(b)の操作を再び繰り返しおこなった。この操作を、高屈折率化している直角ラインが8本形成されるまで繰り返した。
次に、基材1をX軸方向に250μm移動させ、同様に図2(a)〜(b)の操作を行い、更に−Y軸方向に250μm間隔で、(a)〜(b)の操作を繰り返しながら移動させることで、図3に示すような、基材1中に、1列が8本の直角に曲がった高屈折率ラインLを2列形成した。図3のH方向より各ラインに波長1300nmのレーザー光を入射し、I方向への出射光を測定することで、直角ライン内を透過した光の損失を調べたところ、16本の導波路の内部損失はいずれも0.2dB以下であり、95%以上の効率で光路を直角に変換できる光導波路が形成されていることを確認した。また、導波路のモードフィールド径は8μm、開口数は0.1であり、各導波路間におけるバラツキは認められなかった。
Thereafter, the laser beam 3 is blocked, the positional relationship between the base material 1 and the objective lens 2 is returned to the state shown in FIG. 2A, and only the base material 1 is moved by 250 μm in the Y-axis direction. The operation of (b) was repeated again. This operation was repeated until eight right-angle lines having a high refractive index were formed.
Next, the substrate 1 is moved 250 μm in the X-axis direction, and the operations shown in FIGS. 2A to 2B are performed in the same manner. Further, the operations shown in FIGS. As shown in FIG. 3, two rows of high refractive index lines L in which one row is bent at a right angle are formed as shown in FIG. When laser light having a wavelength of 1300 nm is incident on each line from the H direction in FIG. 3 and the outgoing light in the I direction is measured, the loss of light transmitted through the right angle line is examined. All internal losses were 0.2 dB or less, and it was confirmed that an optical waveguide capable of converting the optical path to a right angle with an efficiency of 95% or more was formed. Further, the mode field diameter of the waveguide was 8 μm, the numerical aperture was 0.1, and no variation was observed between the waveguides.
本実施例1では基材に石英ガラスを使用し、1列が8本で2列からなる16本の直角光路変換導波路を取り上げたが、基材は使用するレーザーで高屈折率化が生じる、いわゆる光誘起屈折率変化が起きる材料であれば特に限定されるものでは無く、他の酸化物ガラスやハロゲン化物ガラス、カルコゲナイドガラスや無機単結晶材料、あるいは有機高分子を使用することもできる。また、紫外線レーザーを使用することで、光硬化性樹脂内に光路変換光導波路を形成することも可能である。また、本実施例1の内容を逸脱しない範囲であれば、全反射面への入射角度は任意で構わない。また、導波路数として16本の例を取り上げたが、本実施例1の内容を逸脱しない範囲であれば、列数や導波路数は任意で構わず、さらに、隣り合う光導波路の間隔や距離は必ずしも一定である必要はない。 In the first embodiment, quartz glass is used as a base material, and 16 right-angle optical path conversion waveguides each consisting of two rows and eight rows are taken up. However, the base material has a high refractive index due to the laser used. The material is not particularly limited as long as it is a material in which a so-called photoinduced refractive index change occurs, and other oxide glass, halide glass, chalcogenide glass, inorganic single crystal material, or organic polymer can also be used. Moreover, it is also possible to form an optical path conversion optical waveguide in the photocurable resin by using an ultraviolet laser. Moreover, as long as it does not deviate from the content of the first embodiment, the incident angle on the total reflection surface may be arbitrary. Further, although the example of 16 waveguides has been taken up, the number of columns and the number of waveguides may be arbitrary as long as they do not deviate from the contents of the first embodiment. The distance does not necessarily have to be constant.
更に、基材と周囲との屈折率差を大きくしたり、反射面に多層膜コーティングを予め施したりすることで、全反射条件を満足するレーザーの入射角を45°より小さくすることも可能であり、この場合は鋭角で光路を変換する導波路の作製も可能である。本方法とは逆に基材入射前のレーザー光軸に平行な導波路を先に形成し、続いて光路を変換した導波路を形成することも有効である。 Furthermore, by increasing the difference in refractive index between the base material and the surroundings, or by applying a multilayer coating on the reflective surface in advance, it is possible to make the laser incident angle satisfying the total reflection condition smaller than 45 ° In this case, it is also possible to produce a waveguide that converts the optical path at an acute angle. Contrary to this method, it is also effective to first form a waveguide parallel to the laser optical axis before incidence on the substrate, and then form a waveguide obtained by converting the optical path.
また、実施例1では1つの全反射面のみを有する基材を使用しているが、基材へのレーザー入射後、レーザーの第1全反射面以降の面が、連続してレーザーの光軸に対して全反射条件を満足する角度になっていることで、各全反射面により連続的に複数回折り曲げられた光導波路を形成させることも可能である。 In Example 1, a base material having only one total reflection surface is used. However, after the laser is incident on the base material, the surfaces after the first total reflection surface of the laser are continuously connected to the optical axis of the laser. In contrast, since the angle satisfies the total reflection condition, it is possible to form an optical waveguide that is continuously bent a plurality of times by each total reflection surface.
1 基材
2 対物レンズ
3 レーザ光
4 ガラス基盤
5 反射面
E 最初のレーザ集光点
F 最終のレーザ集光点
G レーザー集光点の軌跡
DESCRIPTION OF SYMBOLS 1 Base material 2 Objective lens 3 Laser beam 4 Glass substrate 5 Reflective surface E First laser condensing point F Final laser condensing point G Laser condensing point locus
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