JP2003140214A - Method of manufacturing thin film substrate for wavelength conversion element and method of manufacturing wavelength conversion element - Google Patents
Method of manufacturing thin film substrate for wavelength conversion element and method of manufacturing wavelength conversion elementInfo
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- JP2003140214A JP2003140214A JP2001337313A JP2001337313A JP2003140214A JP 2003140214 A JP2003140214 A JP 2003140214A JP 2001337313 A JP2001337313 A JP 2001337313A JP 2001337313 A JP2001337313 A JP 2001337313A JP 2003140214 A JP2003140214 A JP 2003140214A
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- Prior art keywords
- substrate
- wavelength conversion
- conversion element
- thin film
- manufacturing
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- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
Abstract
(57)【要約】
【課題】 波長変換素子の製造に好適な薄膜基板(例え
ば3インチウエハの全面積にわたって均一な組成、膜厚
を持つようなニオブ酸リチウムの薄膜基板)の製造方法
を提供し、また、前記薄膜基板を用いて分極反転構造を
有する光導波路を作製し、もって高性能な波長変換素子
を提供する。
【解決手段】 二次の非線形効果を有し且つ非線形定数
が周期的に変調する構造をもつ第一の基板と、第二の基
板とを貼り合わせる第一の工程と、第一の基板の厚さを
薄くして光導波路を形成するための所定の厚さにする第
二の工程とを有する波長変換素子用薄膜基板の製造方法
において、前記第一の工程では第一の基板と第二の基板
とを、熱処理による拡散接合によって直接貼り合わせ
る。
PROBLEM TO BE SOLVED: To provide a method for producing a thin film substrate (for example, a lithium niobate thin film substrate having a uniform composition and film thickness over the entire area of a 3-inch wafer) suitable for producing a wavelength conversion element. Further, an optical waveguide having a domain-inverted structure is manufactured using the thin film substrate, thereby providing a high-performance wavelength conversion element. A first step of bonding a first substrate having a second-order nonlinear effect and having a structure in which a nonlinear constant is periodically modulated, a first step of bonding the second substrate, and a thickness of the first substrate. A second step of reducing the thickness to a predetermined thickness to form an optical waveguide, the method for manufacturing a thin film substrate for a wavelength conversion element, wherein the first substrate and the second substrate in the first step The substrate is directly bonded by diffusion bonding by heat treatment.
Description
【0001】[0001]
【発明の属する技術分野】本発明は、波長多重や時間多
重を利用した光通信システムにおける光駆動型光回路装
置、具体的には、非線形光学媒質中で生じる差周波発生
効果を用いて信号光の波長を別の波長に変換する波長変
換素子及び波長変換素子用薄膜基板に関するものであ
る。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical drive type optical circuit device in an optical communication system using wavelength division multiplexing or time division multiplexing, and more specifically, to signal light using a difference frequency generation effect generated in a nonlinear optical medium. The present invention relates to a wavelength conversion element and a thin film substrate for a wavelength conversion element for converting the wavelength of the above into another wavelength.
【0002】[0002]
【従来の技術】近年、光通信システムの通信容量の増大
を図るために、波長の異なる複数の光を多重化して伝送
する波長分割多重(WDM)通信システムが積極的に導
入されている。このようなWDM通信システムにおいて
は、限られた波長数を有効に利用するために、信号波長
を任意の信号波長に変換する波長変換デバイスの実用化
が求められている。2. Description of the Related Art In recent years, in order to increase the communication capacity of an optical communication system, a wavelength division multiplexing (WDM) communication system for multiplexing and transmitting a plurality of lights having different wavelengths has been actively introduced. In such a WDM communication system, in order to effectively use the limited number of wavelengths, it is required to put a wavelength conversion device that converts a signal wavelength into an arbitrary signal wavelength into practical use.
【0003】従来、光の波長を変換する波長変換素子と
しては、半導体光増幅器を用いるもの、四光波混合を利
用するもの等が知られている。しかしながら、これらの
波長変換素子においては光通信システムにおいて求めら
れる、高効率、高速、広帯域、低ノイズ、偏波無依存な
どの条件を満足させることはできていなかった。Conventionally, as a wavelength conversion element for converting the wavelength of light, one using a semiconductor optical amplifier, one using four-wave mixing, and the like are known. However, these wavelength conversion elements have not been able to satisfy the conditions required for optical communication systems, such as high efficiency, high speed, wide band, low noise, and polarization independence.
【0004】一方、二次非線形効果の一種である擬似位
相整合による差周波発生を利用した波長変換素子が知ら
れている。図8は、この種の擬似位相整合型の波長変換
素子の構成を示す概略図である。同図に示すように、比
較的小さな光強度を持つ信号光Aと、比較的大きな光強
度を持つ制御光Bは合波器1により合波されて、分極反
転構造をもった非線形光導波路2に入射される。光導波
路2中で信号光Aは、別の波長を持つ差周波光Cへと変
換され、制御光Bと共に導波路2から出射される。出射
された差周波光Cと制御光Bは、分波器3により分離さ
れる。例えば、制御光Bの波長λ1=0.77μmとし
た場合、波長λ2=1.55μmの信号光Aを波長λ3
=1.53μmの差周波光Cへと変換することができ
る。On the other hand, there is known a wavelength conversion element utilizing difference frequency generation by quasi phase matching which is a kind of second-order nonlinear effect. FIG. 8 is a schematic diagram showing the configuration of a quasi phase matching type wavelength conversion element of this type. As shown in the figure, the signal light A having a relatively small light intensity and the control light B having a relatively large light intensity are combined by the combiner 1 to form the nonlinear optical waveguide 2 having the polarization inversion structure. Is incident on. The signal light A is converted into the difference frequency light C having another wavelength in the optical waveguide 2, and is emitted from the waveguide 2 together with the control light B. The emitted difference frequency light C and control light B are separated by the demultiplexer 3. For example, when the control light B has a wavelength λ1 = 0.77 μm, the signal light A having a wavelength λ2 = 1.55 μm is converted into a wavelength λ3.
= 1.53 μm of the difference frequency light C can be converted.
【0005】このような擬似位相整合を利用した波長変
換素子を作製する従来の方法においては、ニオブ酸リチ
ウムなどの非線形光学結晶基板に周期分極反転構造を作
製した後、プロトン交換導波路を作製することによって
波長変換素子を作製していた。In the conventional method of producing a wavelength conversion element utilizing such quasi phase matching, a proton-exchanged waveguide is produced after producing a periodically poled structure on a nonlinear optical crystal substrate such as lithium niobate. Thus, the wavelength conversion element was manufactured.
【0006】これに対し、導波路中への光閉じ込めを改
善しバルクもしくはバルクに近い非線形効果を利用した
高効率な波長変換を実現するために、リッジ型の光導波
路構造をもった波長変換素子が提案されている。On the other hand, in order to improve the optical confinement in the waveguide and to realize highly efficient wavelength conversion utilizing the bulk or near-nonlinear effect, a wavelength conversion element having a ridge type optical waveguide structure. Is proposed.
【0007】リッジ型光導波路を持つような波長変換素
子を作製するための従来の方法は、液相エピタキシャル
法によって成長されたニオブ酸リチウムなどの単結晶膜
に、通常のフォトリソグラフィによってエッチングマス
クを作製し、それに続くドライエッチングプロセスにお
いて、マスク部以外の単結晶膜を除去することによって
リッジ型光導波路を作製していた。A conventional method for producing a wavelength conversion element having a ridge-type optical waveguide is that a single crystal film of lithium niobate or the like grown by a liquid phase epitaxial method is provided with an etching mask by ordinary photolithography. The ridge-type optical waveguide was manufactured by removing the single crystal film except the mask portion in the subsequent dry etching process.
【0008】一方、これとは別にリッジ型光導波路を作
製する方法として、Mg添加ニオブ酸リチウム基板に周
期分極反転構造を作製した後、別に用意したニオブ酸リ
チウム基板に接着剤を用いて接着し、Mg添加ニオブ酸
リチウム基板の基板厚さを平面研削加工によって薄くし
た後、ダイシングソーを用いた超精密研削加工によって
リッジ型導波路を作製することが行われている(レーザ
研究:第28巻第9号p601−603)。On the other hand, as another method for producing a ridge type optical waveguide, a periodically poled structure is formed on a Mg-added lithium niobate substrate and then bonded to a separately prepared lithium niobate substrate using an adhesive. , A Mg-added lithium niobate substrate is thinned by surface grinding to form a ridge-type waveguide by ultra-precision grinding using a dicing saw (Laser Research: Volume 28). No. 9, p601-603).
【0009】[0009]
【発明が解決しようとする課題】しかしながら、プロト
ン交換導波路は、拡散型の屈折率分布をもち導波モード
が非対称であること、また、プロトン交換処理によって
基板表面が変質するため、導波路部分の非線形光学効果
が劣化するなどが問題となっていた。However, since the proton exchange waveguide has a diffusion type refractive index distribution and the waveguide mode is asymmetric, and the surface of the substrate is altered by the proton exchange treatment, the waveguide portion is affected. There was a problem that the non-linear optical effect of was deteriorated.
【0010】また、液相エピタキシャル法による単結晶
膜の作製は大面積化が難しく、たとえば3インチのウエ
ハの全面積にわたって均一な組成あるいは膜厚を持つよ
うな単結晶膜の作製は難しかった。Further, it is difficult to form a single crystal film by the liquid phase epitaxial method, and it is difficult to form a single crystal film having a uniform composition or film thickness over the entire area of a 3-inch wafer, for example.
【0011】更に、単結晶膜と基板とを接着剤を用いて
貼り合わせる方法は、接着剤と単結晶膜の熱膨張係数が
異なるために温度が変化した時に単結晶膜に割れが生じ
ることが問題となることのほかに、導波路中で発生する
SHG光によって接着剤が劣化するために動作中に導波
路損失が増加し波長変換の効率が劣化することが問題と
なっていた。また、接着層の不均一性のために単結晶膜
の膜厚が不均一となり、波長変換素子の位相整合波長が
ずれることが問題となっていた。Further, in the method of bonding the single crystal film and the substrate using an adhesive, the single crystal film may be cracked when the temperature changes because the adhesive and the single crystal film have different thermal expansion coefficients. In addition to the problem, the SHG light generated in the waveguide deteriorates the adhesive, which increases the waveguide loss during operation and deteriorates the wavelength conversion efficiency. Further, the non-uniformity of the adhesive layer makes the film thickness of the single crystal film non-uniform, which causes a problem that the phase matching wavelength of the wavelength conversion element shifts.
【0012】本発明の目的は、上記問題を解決した波長
変換素子の製造に好適な薄膜基板の製造方法を提供する
ことであり、例えば3インチウエハの全面積にわたって
均一な組成、膜厚を持つようなニオブ酸リチウムの薄膜
基板を提供することである。また、本発明の目的は、前
記した薄膜基板を用いて分極反転構造を有する光導波路
を作製し、もって高性能な波長変換素子を提供すること
である。An object of the present invention is to provide a method of manufacturing a thin film substrate suitable for manufacturing a wavelength conversion device which solves the above problems, and has a uniform composition and film thickness over the entire area of a 3-inch wafer, for example. It is to provide such a thin film substrate of lithium niobate. Another object of the present invention is to provide an optical waveguide having a domain-inverted structure using the above-mentioned thin film substrate, and to provide a high-performance wavelength conversion element.
【0013】[0013]
【課題を解決するための手段】上記課題を解決するため
の請求項1に記載の発明は、二次の非線形効果を有し且
つ非線形定数が周期的に変調する構造をもつ第一の基板
と、第二の基板とを貼り合わせる第一の工程と、前記第
一の基板の厚さを薄くして光導波路を形成するための所
定の厚さにする第二の工程と、を有する波長変換素子用
薄膜基板の製造方法であって、前記第一の工程では前記
第一の基板と前記第二の基板とを、熱処理による拡散接
合によって直接貼り合わせることを特徴とする。According to a first aspect of the invention for solving the above-mentioned problems, a first substrate having a structure having a quadratic nonlinear effect and a nonlinear constant being periodically modulated, is provided. , A second step of laminating a second substrate, and a second step of reducing the thickness of the first substrate to a predetermined thickness for forming an optical waveguide A method of manufacturing a thin film substrate for a device, characterized in that in the first step, the first substrate and the second substrate are directly bonded by diffusion bonding by heat treatment.
【0014】また、請求項2に記載の発明は、請求項1
に記載の発明において、前記第一の工程における熱処理
は前記第一の基板のキュリー温度以下の温度で行うこと
を特徴とする。The invention described in claim 2 is the same as claim 1
In the invention described in (3), the heat treatment in the first step is performed at a temperature equal to or lower than the Curie temperature of the first substrate.
【0015】また、請求項3に記載の発明は、請求項1
又は2に記載の発明において、前記第二の工程では前記
第一の基板の厚さを20μm以下にすることを特徴とす
る。The invention according to claim 3 is the same as claim 1
Alternatively, in the invention described in 2, the thickness of the first substrate is set to 20 μm or less in the second step.
【0016】また、請求項4に記載の発明は、請求項1
〜3の何れか1項に記載の発明において、前記第一の基
板が、LiNbO3 、KNbO3 、LiTaO3 、Li
Nb (x) Ta(1-x) O3 (0≦x≦1)又はKTiOP
O4 、或いは、それらにMg、Zn、Sc、Inからな
る群から選ばれた少なくとも一種を添加物として含有し
ていることを特徴とする。The invention according to claim 4 is the same as claim 1
In the invention according to any one of claims 1 to 3, the first group
The plate is LiNbO3, KNbO3, LiTaO3, Li
Nb (x)Ta(1-x)O3(0 ≦ x ≦ 1) or KTiOP
OFourOr, if they are made of Mg, Zn, Sc, In
Containing at least one selected from the group
It is characterized by
【0017】また、請求項5に記載の発明は、請求項1
〜4の何れか1項に記載の発明において、前記第二の基
板の屈折率は前記第一の基板の屈折率よりも小さいこと
を特徴とする。The invention described in claim 5 is the same as claim 1.
The invention according to any one of claims 1 to 4, characterized in that the refractive index of the second substrate is smaller than the refractive index of the first substrate.
【0018】また、請求項6に記載の発明は、請求項5
に記載の発明において、前記第二の基板は水晶基板又は
ガラス基板であることを特徴とする。The invention described in claim 6 is the same as claim 5
In the invention described in (3), the second substrate is a quartz substrate or a glass substrate.
【0019】また、請求項7に記載の発明は、請求項1
〜4の何れか1項に記載の発明において、前記第二の基
板の前記第一の基板に接合する表面層の屈折率は、前記
第一の基板の屈折率よりも小さいことを特徴とする。The invention described in claim 7 is the same as claim 1.
The invention according to any one of claims 1 to 4, wherein the surface layer of the second substrate joined to the first substrate has a refractive index smaller than that of the first substrate. .
【0020】また、請求項8に記載の発明は、請求項7
に記載の発明において、前記第二の基板の表面層は低融
点ガラス膜又は低融点ガラス基板であることを特徴とす
る。The invention according to claim 8 is the same as claim 7
In the invention described in (3), the surface layer of the second substrate is a low melting point glass film or a low melting point glass substrate.
【0021】また、請求項9に記載の発明は、請求項1
〜4の何れか1項に記載の発明において、前記第一の基
板の第二の基板に接合する表面層の屈折率は、光導波路
を形成する前記第一の基板の本体層の屈折率よりも小さ
いことを特徴とする。The invention described in claim 9 is the same as claim 1.
In the invention according to any one of claims 1 to 4, the refractive index of the surface layer of the first substrate joined to the second substrate is greater than the refractive index of the main body layer of the first substrate forming the optical waveguide. Is also small.
【0022】また、請求項10に記載の発明は、請求項
9に記載の発明において、前記第一の基板の表面層は低
融点ガラス膜又は低融点ガラス基板であることを特徴と
する。The invention according to claim 10 is characterized in that, in the invention according to claim 9, the surface layer of the first substrate is a low melting point glass film or a low melting point glass substrate.
【0023】また、請求項11に記載の発明は、請求項
1〜4の何れか1項に記載の発明において、前記第一の
基板の第二の基板に接合する表面層の屈折率は、光導波
路を形成する前記第一の基板の本体部の屈折率よりも小
さく、且つ、前記第二の基板の前記第一の基板に接合す
る表面層の屈折率も、前記第一の基板の本体層の屈折率
よりも小さいことを特徴とする。The invention according to claim 11 is the invention according to any one of claims 1 to 4, wherein the surface layer bonded to the second substrate of the first substrate has a refractive index of The refractive index of the surface layer of the second substrate, which is smaller than the refractive index of the main body of the first substrate forming the optical waveguide, and which is joined to the first substrate, is also the main body of the first substrate. It is characterized by being smaller than the refractive index of the layer.
【0024】また、請求項12に記載の発明は、請求項
11に記載の発明において、前記第一の基板の表面層は
低融点ガラス膜又は低融点ガラス基板であり、前記第二
の基板の表面層も低融点ガラス膜又は低融点ガラス基板
であることを特徴とする。The invention according to claim 12 is the invention according to claim 11, wherein the surface layer of the first substrate is a low-melting glass film or a low-melting glass substrate, The surface layer is also a low melting point glass film or a low melting point glass substrate.
【0025】また、請求項13に記載の発明は、請求項
1〜12の何れか1項に記載の発明において、前記第二
の基板の熱膨張係数が、前記第一の基板の熱膨張係数に
ほぼ一致することを特徴とする。The invention according to claim 13 is the invention according to any one of claims 1 to 12, wherein the coefficient of thermal expansion of the second substrate is the coefficient of thermal expansion of the first substrate. It is characterized by almost matching.
【0026】また、請求項14に記載の発明の波長変換
素子の製造方法は、請求項1〜13の何れか1項に記載
の発明の波長変換素子用薄膜基板の製造方法によって波
長変換素子用薄膜基板を作製し、これに続く第三の工程
で、前記波長変換素子用薄膜基板における前記第一の基
板に光導波路を作製することを特徴とする。A method for manufacturing a wavelength conversion element according to a fourteenth aspect of the present invention is the method for manufacturing a thin film substrate for a wavelength conversion element according to any one of the first to thirteenth aspects. A thin film substrate is produced, and an optical waveguide is produced on the first substrate of the wavelength conversion element thin film substrate in a third step subsequent thereto.
【0027】[作用]擬似位相整合を利用した波長変換
素子の効率を改善するためには、変換効率が原理的に相
互作用長(周期分極反転構造を有する導波路長)の2乗
に比例することから、素子の長さを長くすること、即
ち、素子作製に用いる非線形光学結晶基板を大面積化す
ること、更には、光導波路中での信号光と制御光の光電
界の重なりを良くすることが重要である。このとき、光
導波路に入射された励起光と信号光は光導波路の基底モ
ードを励振することが望ましく、且つ、高いパワー密度
が光導波路中で得られるようにするためには、光導波層
すなわち非線形光学結晶膜の厚さがおよそ20μm以下
であることが望ましい。光導波層の厚さが20μm以上
である場合には、信号光と励起光とが多モード状態とな
って光電界の重なりを良くすることが難しい。[Operation] In order to improve the efficiency of the wavelength conversion element utilizing the quasi phase matching, the conversion efficiency is in principle proportional to the square of the interaction length (the length of the waveguide having the periodically poled structure). Therefore, increasing the length of the device, that is, increasing the area of the nonlinear optical crystal substrate used for manufacturing the device, and further improving the overlap of the optical fields of the signal light and the control light in the optical waveguide. This is very important. At this time, it is desirable that the excitation light and the signal light incident on the optical waveguide excite the fundamental mode of the optical waveguide, and in order to obtain a high power density in the optical waveguide, It is desirable that the thickness of the nonlinear optical crystal film is approximately 20 μm or less. When the thickness of the optical waveguide layer is 20 μm or more, it is difficult to improve the overlap of the optical electric fields because the signal light and the excitation light are in a multimode state.
【0028】本発明者らは、このような長尺の波長変換
素子の作製が可能となり、且つ、20μm以下の膜厚を
もつような、非線形光学結晶からなる薄膜基板の製造方
法について鋭意検討した結果、非線形効果を持つ光学結
晶からなる基板と熱膨張係数がおよそ一致するような、
同種の非線形光学結晶、異種の光学結晶或いはガラス基
板などを拡散による直接接合によって貼り合わせた後、
非線形光学結晶基板を研削、研磨あるいはエッチングな
どの方法によって20μm以下の膜厚になるように調整
して、光導波路の作製に好適な非線形単結晶薄膜基板を
製造する方法を見出した。The present inventors diligently studied a method of manufacturing a thin film substrate made of a non-linear optical crystal capable of producing such a long wavelength conversion element and having a film thickness of 20 μm or less. As a result, the coefficient of thermal expansion is approximately the same as that of a substrate made of an optical crystal having a nonlinear effect,
After bonding non-linear optical crystals of the same type, optical crystals of different types or glass substrates, etc. by direct bonding by diffusion,
The inventors have found a method for producing a nonlinear single crystal thin film substrate suitable for producing an optical waveguide by adjusting the nonlinear optical crystal substrate so as to have a film thickness of 20 μm or less by a method such as grinding, polishing or etching.
【0029】本発明において、周期分極反転構造が作製
された非線形光学結晶基板(第一の基板)は、その第一
の工程において別に用意された第二の基板にマイクロパ
ーティクルが極力存在しないような清浄雰囲気中で直接
重ね合わされた後、電気炉中で熱処理されることによっ
て拡散接合される。ここで基板を熱処理する温度は前記
第一の基板のキュリー温度以下であることが好ましい。
キュリー温度以上の温度で熱処理することは周期分極反
転構造が乱れる恐れがあるので好ましくない。特に非線
形光学結晶基板としてLiTaO3 を用いた場合におい
ては、キュリー温度が650℃であるので、650℃を
越える温度で熱処理することは分極反転構造が乱れる原
因となるので好ましくない。In the present invention, the non-linear optical crystal substrate (first substrate) on which the periodically poled structure is formed is such that microparticles are not present as much as possible on the second substrate prepared separately in the first step. After being directly laminated in a clean atmosphere, they are heat-treated in an electric furnace to be diffusion-bonded. Here, the temperature for heat-treating the substrate is preferably equal to or lower than the Curie temperature of the first substrate.
It is not preferable to perform the heat treatment at a temperature equal to or higher than the Curie temperature because the periodically poled structure may be disturbed. In particular, when LiTaO 3 is used as the nonlinear optical crystal substrate, the Curie temperature is 650 ° C., so heat treatment at a temperature higher than 650 ° C. is not preferable because it causes disorder of the domain-inverted structure.
【0030】貼り合わされた基板は、第二の工程におい
て非線形光学結晶基板の厚さが20μm以下になるまで
研磨・研削あるいはエッチングされることによって、波
長変換素子用の薄膜基板とすることができる。The bonded substrates can be used as a thin film substrate for a wavelength conversion element by polishing, grinding or etching until the thickness of the nonlinear optical crystal substrate becomes 20 μm or less in the second step.
【0031】本発明においては、基板の接合に接着剤を
用いておらず基板同士の直接接合である点が従来の方法
とは異なる。The present invention differs from the conventional method in that an adhesive is not used for joining the substrates and the substrates are directly joined.
【0032】また、引き続いて本発明の薄膜基板を用い
て波長変換素子を作製する場合は、続く第三の工程にお
いて、ダイシングソーを用いた超精密研削加工によって
リッジ型の光導波路を作製することもできるし、ドライ
エッチングあるいはウエットエッチング法によってリッ
ジ型の光導波路を作製することもできる。When a wavelength conversion element is subsequently manufactured using the thin film substrate of the present invention, in the subsequent third step, a ridge type optical waveguide is manufactured by ultraprecision grinding using a dicing saw. Alternatively, a ridge type optical waveguide can be produced by dry etching or wet etching.
【0033】以下、本発明を実施例を用いて詳細に説明
するが、本発明はこれらの実施例によって何ら制限され
るものではない。Hereinafter, the present invention will be described in detail with reference to examples, but the present invention is not limited to these examples.
【0034】[0034]
【発明の実施の形態】(実施例1)図1は本発明の実施
例1の波長変換素子用薄膜基板を作製する工程を示すフ
ロー図である。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS (Embodiment 1) FIG. 1 is a flow chart showing a process for producing a thin film substrate for a wavelength conversion element according to a first embodiment of the present invention.
【0035】図1に示すように、本実施例1において
は、第一の基板11としてあらかじめ1.5μm帯で位
相整合条件が満たされるように周期分極反転構造が作製
されているZカットZn添加LiNbO3 基板を用い、
第二の基板12としてZカットMg添加LiNbO3 基
板を用いて波長変換素子用薄膜基板を作製した。第一の
基板11と第二の基板12は、何れもLiNbO3 に添
加物を添加したものであり、熱膨張係数がほぼ一致して
いる。また、添加物の種類を変えることにより、第一の
基板11の屈折率よりも第二の基板12の屈折率のほう
が小さくなっている。なお、第一及び第二の基板11,
12は何れも両面が光学研磨されてある3インチウエハ
であり、基板厚さは300μmである。As shown in FIG. 1, in the present Example 1, Z-cut Zn was added as a first substrate 11 in which a periodically poled structure was prepared in advance so that the phase matching condition was satisfied in the 1.5 μm band. Using LiNbO 3 substrate,
A Z-cut Mg-added LiNbO 3 substrate was used as the second substrate 12 to prepare a thin film substrate for wavelength conversion element. Both the first substrate 11 and the second substrate 12 are made by adding an additive to LiNbO 3 and have substantially the same thermal expansion coefficient. In addition, the refractive index of the second substrate 12 is smaller than that of the first substrate 11 by changing the kind of the additive. The first and second substrates 11,
Reference numeral 12 is a 3-inch wafer whose both surfaces are optically polished, and has a substrate thickness of 300 μm.
【0036】第一の工程では、用意した第一及び第二の
基板11,12の表面を通常の酸洗浄あるいはアルカリ
洗浄によって親水性にした後、これら二つの基板11,
12をマイクロパーティクルが極力存在しない清浄雰囲
気中で重ね合わせた。そして、この重ね合わせた第一及
び第二の基板11,12を電気炉に入れ、400℃で3
時間熱処理することにより拡散接合を行った。接着され
た基板は接合面にマイクロパーティクル等の挟み込みが
なくてボイドフリーであり、室温に戻したときにおいて
もクラックなどは発生しなかった。In the first step, the surfaces of the prepared first and second substrates 11 and 12 are made hydrophilic by ordinary acid cleaning or alkali cleaning, and then these two substrates 11 and 12 are made hydrophilic.
12 was superposed in a clean atmosphere in which microparticles were not present as much as possible. Then, the superposed first and second substrates 11 and 12 are put into an electric furnace and heated at 400 ° C. for 3 hours.
Diffusion bonding was performed by heat treatment for a time. The bonded substrates were void-free, with no microparticles or the like sandwiched between the bonded surfaces, and no cracks or the like were generated even when returned to room temperature.
【0037】次に、第二の工程では、研磨定盤の平坦度
が管理された研磨装置を用いて、接着された基板の第一
の基板11の厚さが20μmになるまで研磨加工を施し
た。研磨加工の後に、ポリッシング加工を行うことによ
り鏡面の研磨表面を得ることができた。基板の平行度
(最大高さと最小高さとの差)を光学的な平行度測定機
を用いて測定したところ、3インチウエハの周囲を除
き、ほぼ全体にわたってサブミクロンの平行度が得ら
れ、波長変換素子の作製に好適な薄膜基板13を作製す
ることができた。この薄膜基板13は、接着剤を用い
ず、第一の基板11と第二の基板12とを熱処理による
拡散接合によって直接貼り合わせることにより作製した
ため、3インチウエハの全面積にわたって均一な組成、
膜厚を持つものであった。Next, in the second step, a polishing apparatus whose flatness of the polishing platen is controlled is used to perform polishing until the thickness of the first substrate 11 of the bonded substrates reaches 20 μm. did. After the polishing process, a polishing process could be performed to obtain a mirror-polished surface. When the parallelism of the substrate (difference between the maximum height and the minimum height) was measured using an optical parallelism measuring machine, submicron parallelism was obtained over almost the entire area except for the circumference of the 3-inch wafer, and The thin film substrate 13 suitable for producing the conversion element could be produced. Since this thin film substrate 13 was produced by directly bonding the first substrate 11 and the second substrate 12 by diffusion bonding by heat treatment without using an adhesive, a uniform composition over the entire area of the 3-inch wafer,
It had a film thickness.
【0038】なお、第一の基板11としてXカットZn
添加LiNbO3 基板を用い、第二の基板12としてX
カットMg添加LiNbO3 基板を用いた場合において
も、本実施例1と同様の方法によって波長変換素子用薄
膜基板13を作製することができた。As the first substrate 11, X-cut Zn
Using the added LiNbO 3 substrate, X is used as the second substrate 12.
Even when the cut Mg-added LiNbO 3 substrate was used, the thin film substrate 13 for a wavelength conversion element could be manufactured by the same method as in Example 1.
【0039】次に、第三の工程では、作製した薄膜基板
13を用い、また、光導波路の作製手段としてはドライ
エッチングプロセスを用いて波長変換素子を作製した。
即ち、薄膜基板13(第一の基板11)の表面に通常の
フォトリソグラフィのプロセスによって導波路パターン
を作製した後、ドライエッチング装置に基板をセット
し、CF4 ガスをエッチングガスとして薄膜基板13
(第一の基板11)の表面をエッチングすることにより
リッジ型光導波路を作製した。図2はエッチング後の基
板断面を示す図である。図2に示すように、高さ8μ
m、導波路幅およそ8μmのリッジ型光導波路14を、
薄膜基板13(第一の基板11)に作製することができ
た。図示されているように、ドライエッチングのプロセ
スにおいてはマスクと膜のエッチング選択比が大きくな
いために、光導波路14がメサ形状となる。Next, in the third step, the manufactured thin film substrate 13 was used, and a wavelength conversion element was manufactured using a dry etching process as a means for manufacturing an optical waveguide.
That is, after a waveguide pattern is formed on the surface of the thin film substrate 13 (first substrate 11) by a normal photolithography process, the substrate is set in a dry etching device and CF 4 gas is used as an etching gas to form the thin film substrate 13.
A ridge type optical waveguide was produced by etching the surface of the (first substrate 11). FIG. 2 is a view showing a cross section of the substrate after etching. As shown in Fig. 2, the height is 8μ
m, a ridge type optical waveguide 14 having a waveguide width of about 8 μm,
The thin film substrate 13 (first substrate 11) could be produced. As shown in the drawing, the optical waveguide 14 has a mesa shape because the etching selectivity between the mask and the film is not large in the dry etching process.
【0040】図3に示すように、光導波路14は3イン
チウエハである薄膜基板13に平行に複数本作製した。
そして、これらの各光導波路14ごとに基板13を短冊
状に切り出し、光導波路14の両端面14aを光学研磨
することによって長さ60mmの波長変換素子15を作
製した。作製した波長変換素子15に波長0.77μm
の制御光と波長1.55μmの信号光を入射したとこ
ろ、波長1.53μmの波長変換光が得られ高効率で波
長変換を実現できた。As shown in FIG. 3, a plurality of optical waveguides 14 were produced in parallel with the thin film substrate 13 which was a 3-inch wafer.
Then, the substrate 13 was cut into strips for each of the optical waveguides 14, and both end surfaces 14a of the optical waveguides 14 were optically polished to fabricate a wavelength conversion element 15 having a length of 60 mm. Wavelength of 0.77 μm in the manufactured wavelength conversion element 15
When the control light and the signal light with a wavelength of 1.55 μm were incident, wavelength-converted light with a wavelength of 1.53 μm was obtained, and wavelength conversion could be realized with high efficiency.
【0041】(実施例2)図4は本発明の実施例2の波
長変換素子用薄膜基板を作製する工程を示したフロー図
である。(Embodiment 2) FIG. 4 is a flow chart showing the steps for producing a thin film substrate for a wavelength conversion element according to Embodiment 2 of the present invention.
【0042】図4に示すように、本実施例2において
は、第一の基板21としてあらかじめ周期分極反転構造
が作製してあるLiNbO3 基板を用意し、第二の基板
22として水晶基板を用いて波長変換素子用薄膜基板を
作製した。水晶のZ軸に垂直な面内方向の熱膨張係数は
13.6×10-6/Kであり、LiNbO3 の熱膨張係
数に近く、また、LiNbO3 の屈折率が2.1である
のに対して、水晶の屈折率は1.53と小さいため、本
発明の実施態様の一例として好適である。As shown in FIG. 4, in the second embodiment, a LiNbO 3 substrate having a periodically poled structure is prepared as the first substrate 21, and a quartz substrate is used as the second substrate 22. Thus, a thin film substrate for wavelength conversion element was produced. Thermal expansion coefficient of the plane perpendicular to the Z axis of the crystal is 13.6 × 10 -6 / K, close to the thermal expansion coefficient of the LiNbO 3, also the refractive index of the LiNbO 3 is 2.1 On the other hand, since the refractive index of quartz is as small as 1.53, it is suitable as an example of the embodiment of the present invention.
【0043】そして、本実施例2においても実施例1と
同様の方法によって作製することにより、実施例1と同
様の波長変換素子用薄膜基板を作製することができた。
即ち、第一の工程では、用意した第一及び第二の基板2
1,22の表面を通常の酸洗浄あるいはアルカリ洗浄に
よって親水性にした後、これら二つの基板21,22を
マイクロパーティクルが極力存在しない清浄雰囲気中で
重ね合わせた。そして、この重ね合わせた第一及び第二
の基板11,12を電気炉に入れ、400℃で3時間熱
処理することにより拡散接合を行った。接着された基板
は接合面にマイクロパーティクル等の挟み込みがなくて
ボイドフリーであり、室温に戻したときにおいてもクラ
ックなどは発生しなかった。In the second embodiment as well, by the same method as in the first embodiment, the thin film substrate for the wavelength conversion element similar to that in the first embodiment can be manufactured.
That is, in the first step, the prepared first and second substrates 2
The surfaces of the substrates 1 and 22 were made hydrophilic by ordinary acid cleaning or alkali cleaning, and then these two substrates 21 and 22 were superposed in a clean atmosphere in which microparticles were not present as much as possible. Then, the stacked first and second substrates 11 and 12 were placed in an electric furnace and heat-treated at 400 ° C. for 3 hours to perform diffusion bonding. The bonded substrates were void-free, with no microparticles or the like sandwiched between the bonded surfaces, and no cracks or the like were generated even when returned to room temperature.
【0044】次に、第二の工程では、研磨定盤の平坦度
が管理された研磨装置を用いて、接着された基板の第一
の基板21の厚さが20μmになるまで研磨加工を施し
た。研磨加工の後に、ポリッシング加工を行うことによ
り鏡面の研磨表面を得ることができた。基板の平行度を
光学的な平行度測定機を用いて測定したところ、3イン
チウエハの周囲を除き、ほぼ全体にわたってサブミクロ
ンの平行度が得られ、波長変換素子の作製に好適な薄膜
基板23を作製することができた。この薄膜基板23
は、接着剤を用いず、第一の基板21と第二の基板22
とを熱処理による拡散接合によって直接貼り合わせるこ
とにより作製したため、3インチウエハの全面積にわた
って均一な組成、膜厚を持つものであった。Next, in the second step, a polishing apparatus in which the flatness of the polishing platen is controlled is used until the first substrate 21 of the bonded substrates has a thickness of 20 μm. did. After the polishing process, a polishing process could be performed to obtain a mirror-polished surface. When the parallelism of the substrate was measured by using an optical parallelism measuring instrument, a parallelism of submicron was obtained almost all over the periphery of the 3-inch wafer, and the thin film substrate 23 suitable for manufacturing the wavelength conversion element was obtained. Could be made. This thin film substrate 23
Is a first substrate 21 and a second substrate 22 without using an adhesive.
And 3 were directly bonded by diffusion bonding by heat treatment, and thus had a uniform composition and film thickness over the entire area of the 3-inch wafer.
【0045】このほか、第一の基板21としてZn添加
LiNbO3 の他、Mg添加LiNbO3 、Sc添加L
iNbO3 、In添加LiNbO3 、LiTaO3 、L
iNb(x) Ta(1-x) O3 (0≦x≦1)、KNb
O3 、KTiOPO4 などを用いた場合においても、同
様の波長変換素子用薄膜基板23を作製することができ
た。In addition to the Zn-added LiNbO 3 as the first substrate 21, Mg-added LiNbO 3 and Sc-added L
iNbO 3 , In-added LiNbO 3 , LiTaO 3 , L
iNb (x) Ta (1-x) O 3 (0 ≦ x ≦ 1), KNb
Even when O 3 , KTiOPO 4, or the like was used, a similar thin film substrate 23 for wavelength conversion element could be produced.
【0046】また、第二の基板として熱膨張係数の値が
第一の基板の値に近く、屈折率の値が第一の基板よりも
小さいようなガラス基板を用いた場合においても同様の
波長変換素子用薄膜基板を作製することができた。ここ
でガラス基板の材料としては多成分石英ガラス、リン酸
ガラス、フッ化物ガラス、テルライトガラスなどのガラ
ス材料を用いることができる。なお、このガラス材料の
組成を適宜調整することによって所望の熱膨張係数や屈
折率を持つようなガラス基板を作製することは、ガラス
材料を製造する当該業者が適宜なしうるものである。Also, when a glass substrate whose coefficient of thermal expansion is close to that of the first substrate and whose refractive index is smaller than that of the first substrate is used as the second substrate, the same wavelength is obtained. A thin film substrate for a conversion element could be produced. Here, as the material of the glass substrate, glass materials such as multi-component quartz glass, phosphate glass, fluoride glass, and tellurite glass can be used. It is possible for a person skilled in the art of manufacturing glass materials to appropriately prepare a glass substrate having a desired coefficient of thermal expansion or refractive index by appropriately adjusting the composition of the glass material.
【0047】次に、作製した波長変換素子用薄膜基板を
用いて実施例1と同様の方法によってリッジ型光導波路
をもつ波長変換素子を作製した。作製した波長変換素子
に波長0.77μmの制御光と波長1.55μmの信号
光とを入射したところ、波長1.53μmの波長変換光
が得られ、実施例1で作製した波長変換素子よりも高効
率で波長変換を実現できた。これは、本実施例2におい
ては第一の基板として水晶基板又はガラス基板を用いる
ことにより、第一の基板と第二の基板との比屈折率差を
大きくすることができるため、光導波路中への光電界の
閉じ込めを実施例1で作製した波長変換素子よりも強く
することができるためである。Next, a wavelength conversion element having a ridge type optical waveguide was manufactured by the same method as in Example 1 using the manufactured thin film substrate for wavelength conversion element. When the control light having a wavelength of 0.77 μm and the signal light having a wavelength of 1.55 μm were incident on the manufactured wavelength conversion element, wavelength converted light having a wavelength of 1.53 μm was obtained, which was higher than that of the wavelength conversion element manufactured in Example 1. We were able to achieve wavelength conversion with high efficiency. This is because in Example 2, by using a quartz substrate or a glass substrate as the first substrate, it is possible to increase the relative refractive index difference between the first substrate and the second substrate. This is because the confinement of the optical electric field in the light can be made stronger than that in the wavelength conversion element manufactured in the first embodiment.
【0048】(実施例3)図5は本発明の実施例3の波
長変換素子用薄膜基板を作製する工程を示したフロー図
である。(Embodiment 3) FIG. 5 is a flow chart showing the steps for producing a thin film substrate for a wavelength conversion element according to Embodiment 3 of the present invention.
【0049】図5に示すように、本実施例3において
は、第一の基板31としてあらかじめ分極反転構造が作
製されたMg添加LiNbO3 基板を用意し、第二の基
板32として基板厚さが300μmのLiNbO3 基板
32(本体層)の上に、厚さ50μmの低融点ガラス膜
34(表面層)を作製した複合基板を用いて波長変換素
子用薄膜基板を作製した。As shown in FIG. 5, in Example 3, a Mg-doped LiNbO 3 substrate having a domain-inverted structure prepared in advance was prepared as the first substrate 31, and the second substrate 32 had a substrate thickness of A thin film substrate for a wavelength conversion element was produced using a composite substrate in which a low melting point glass film 34 (surface layer) having a thickness of 50 μm was formed on a LiNbO 3 substrate 32 (main body layer) having a thickness of 300 μm.
【0050】低融点ガラス膜34の作製はガラスペース
トを用いて行った。即ち、LiNbO3 基板33上に膜
厚が均一になるようにガラスペーストを塗布したものを
電気炉中で焼成することによって透明な低融点ガラス膜
34を作製した。The low melting point glass film 34 was manufactured by using a glass paste. That is, a transparent low-melting-point glass film 34 was prepared by baking a LiNbO 3 substrate 33 coated with a glass paste so as to have a uniform film thickness in an electric furnace.
【0051】ここで低融点ガラスとしてはSiO2 −R
2 O−B2 O3 系、SiO2 −R2O−B2 O−PbO
系、SiO2 −B2 O−PbO系、SiO2 −PbO−
TeO2 系、B2 O3 −PbO系、SiO2 −B2 O3
−ZnO−PbO系、B2 O 3 −ZnO−PbO系、B
2 O3 −RO系、TeO2 −R2 O系、TeO2 −R 2
O−La2 O3 系、TeO2 −ZnO系(Rは1価また
は2価の元素)などのガラス材料を用いることができる
が、この限りではない。なお、これらのガラス材料の組
成を適宜調整することによって所望の熱膨張係数や屈折
率を持つような低融点ガラス膜を得ることができるが、
このようなガラス材料の組成の調整はガラスペーストを
製造する当該業者が適宜なしうるものである。Here, SiO is used as the low melting point glass.2-R
2OB2O3System, SiO2-R2OB2O-PbO
System, SiO2-B2O-PbO system, SiO2-PbO-
TeO2System, B2O3-PbO type, SiO2-B2O3
-ZnO-PbO system, B2O 3-ZnO-PbO system, B
2O3-RO system, TeO2-R2O type, TeO2-R 2
O-La2O3System, TeO2-ZnO system (R is monovalent or
Can be a glass material such as a divalent element)
However, this is not the case. In addition, a set of these glass materials
The desired coefficient of thermal expansion and
It is possible to obtain a low-melting-point glass film having a certain rate,
Glass paste is used to adjust the composition of such glass materials.
It can be appropriately done by the manufacturer concerned.
【0052】本実施例3の第二の基板32に用いた低融
点ガラスは、その熱膨張係数がLiNbO3 におよそ一
致し、且つ、屈折率はLiNbO3 の値より小さい値を
持つようにガラス組成が調整されているので本発明の実
施態様の一例として好適である。The low melting point glass used for the second substrate 32 of the third embodiment has a coefficient of thermal expansion substantially equal to that of LiNbO 3 and has a refractive index smaller than that of LiNbO 3. Since the composition is adjusted, it is suitable as an example of the embodiment of the present invention.
【0053】そして、本実施例3においても実施例1と
同様の方法によって作製することにより、実施例1と同
様の波長変換素子用薄膜基板を作製することができた。
即ち、第一の工程では、用意した第一及び第二の基板3
1,32の表面を通常の酸洗浄あるいはアルカリ洗浄に
よって親水性にした後、これら二つの基板31,32
を、第一の基板31の表面(下面)が第二の基板32の
低融点ガラス膜34の表面(上面)に重なるようにマイ
クロパーティクルが極力存在しない清浄雰囲気中で重ね
合わせた。そして、この重ね合わせた第一及び第二の基
板31,32を電気炉に入れ、400℃で3時間熱処理
することにより拡散接合を行った。接着された基板は接
合面にマイクロパーティクル等の挟み込みがなくてボイ
ドフリーであり、室温に戻したときにおいてもクラック
などは発生しなかった。In the third embodiment as well, by the same method as in the first embodiment, the same thin film substrate for wavelength conversion element as in the first embodiment can be manufactured.
That is, in the first step, the prepared first and second substrates 3
After the surfaces of the substrates 1, 32 are made hydrophilic by ordinary acid cleaning or alkaline cleaning, these two substrates 31, 32 are
Were superposed in a clean atmosphere in which microparticles were not present as much as possible so that the surface (lower surface) of the first substrate 31 overlaps the surface (upper surface) of the low melting point glass film 34 of the second substrate 32. Then, the stacked first and second substrates 31 and 32 were placed in an electric furnace and heat-treated at 400 ° C. for 3 hours to perform diffusion bonding. The bonded substrates were void-free, with no microparticles or the like sandwiched between the bonded surfaces, and no cracks or the like were generated even when returned to room temperature.
【0054】次に、第二の工程では、研磨定盤の平坦度
が管理された研磨装置を用いて、接着された基板の第一
の基板31の厚さが20μmになるまで研磨加工を施し
た。研磨加工の後に、ポリッシング加工を行うことによ
り鏡面の研磨表面を得ることができた。基板の平行度を
光学的な平行度測定機を用いて測定したところ、3イン
チウエハの周囲を除き、ほぼ全体にわたってサブミクロ
ンの平行度が得られ、波長変換素子の作製に好適な薄膜
基板35を作製することができた。この薄膜基板35
は、接着剤を用いず、第一の基板31と第二の基板32
とを熱処理による拡散接合によって直接貼り合わせるこ
とにより作製したため、3インチウエハの全面積にわた
って均一な組成、膜厚を持つものであった。Next, in the second step, a polishing apparatus in which the flatness of the polishing platen is controlled is used to perform polishing until the thickness of the first substrate 31 of the bonded substrates becomes 20 μm. did. After the polishing process, a polishing process could be performed to obtain a mirror-polished surface. When the parallelism of the substrate was measured using an optical parallelism measuring instrument, a parallelism of submicron was obtained over almost the entire area except for the periphery of the 3-inch wafer, and the thin film substrate 35 suitable for manufacturing the wavelength conversion element was obtained. Could be made. This thin film substrate 35
Is a first substrate 31 and a second substrate 32 without using an adhesive.
And 3 were directly bonded by diffusion bonding by heat treatment, and thus had a uniform composition and film thickness over the entire area of the 3-inch wafer.
【0055】このほか、第一の基板としてLiNbO3
の他、Zn添加LiNbO3 、Sc添加LiNbO3 、
In添加LiNbO3 、LiTaO3 、LiNb(x) T
a(1 -x) O3 (0≦x≦1)、KNbO3 、KTiOP
O4 などを用いた場合においても、同様の波長変換素子
用薄膜基板を作製することができた。Besides, LiNbO 3 is used as the first substrate.
In addition, Zn-added LiNbO 3 , Sc-added LiNbO 3 ,
In-added LiNbO 3 , LiTaO 3 , LiNb (x) T
a (1 -x) O 3 (0 ≦ x ≦ 1), KNbO 3 , KTiOP
Even when O 4 or the like was used, a similar thin film substrate for wavelength conversion element could be produced.
【0056】また、第二の基板上に作製する低融点ガラ
ス膜の作製方法として蒸着或いはスパッタを用いた場合
においても同様の第二の基板32を作製することができ
た。また、低融点ガラスからなる基板を用意し、この低
融点ガラス基板とLiNbO 3 基板とを重ね合わせた
後、熱処理による拡散接合によって貼り合わせることに
よっても第二の基板を用意することができた。Further, a low melting point glass formed on the second substrate
When vapor deposition or sputtering is used as the method for forming the film
The same second substrate 32 can be manufactured in
It was We also prepared a substrate made of low-melting glass,
Melting point glass substrate and LiNbO 3Overlaid with the substrate
Later, by bonding by diffusion bonding by heat treatment
Therefore, the second substrate could be prepared.
【0057】次に、作製した波長変換素子用薄膜基板を
用いて実施例1と同様の方法によってリッジ型光導波路
をもつ波長変換素子を作製した。作製した波長変換素子
に波長が0.77μmの制御光と波長が1.55μmの
信号光とを入射したところ、波長が1.53μmの波長
変換光が得られ、実施例1で作製した波長変換素子より
も高効率の波長変換を実現できた。これは、本実施例3
においては第一の基板31と第二の基板32との比屈折
率差を大きくすることができるため、即ち、第二の基板
32に低融点ガラス膜34を作製したことによりこの低
融点ガラス膜34の屈折率と第一の基板31の屈折率と
の差を大きくすることができるため、光導波路中への光
電界の閉じ込めを実施例1で作製した波長変換素子より
も強くすることができるためである。Next, a wavelength conversion element having a ridge type optical waveguide was manufactured by the same method as in Example 1 using the manufactured thin film substrate for wavelength conversion element. When the control light having a wavelength of 0.77 μm and the signal light having a wavelength of 1.55 μm were incident on the produced wavelength conversion element, wavelength converted light having a wavelength of 1.53 μm was obtained, and the wavelength conversion produced in Example 1 was performed. We were able to realize wavelength conversion with higher efficiency than the device. This is the third embodiment.
In this case, since the relative refractive index difference between the first substrate 31 and the second substrate 32 can be increased, that is, by forming the low melting point glass film 34 on the second substrate 32, the low melting point glass film Since the difference between the refractive index of 34 and the refractive index of the first substrate 31 can be increased, the confinement of the optical electric field in the optical waveguide can be made stronger than that of the wavelength conversion element manufactured in Example 1. This is because.
【0058】(実施例4)図6は本実施例の波長変換素
子用薄膜基板を作製する工程を示したフロー図である。(Embodiment 4) FIG. 6 is a flow chart showing the steps for producing the thin film substrate for a wavelength conversion element of this embodiment.
【0059】図6に示すように、本実施例4において
は、第一の基板41としてあらかじめ分極反転構造が作
製されたMg添加LiNbO3 基板43(本体層)の下
に、厚さ50μmの低融点ガラス膜44(表面層)を作
製した複合基板を用意し、第二の基板42として厚さが
300μmのLiNbO3 基板を用いて波長変換素子用
薄膜基板を作製した。As shown in FIG. 6, in Example 4, as the first substrate 41, a low-thickness 50 μm film was formed under the Mg-added LiNbO 3 substrate 43 (main body layer) in which the domain-inverted structure was prepared in advance. A composite substrate having a melting point glass film 44 (surface layer) was prepared, and a LiNbO 3 substrate having a thickness of 300 μm was used as the second substrate 42 to prepare a thin film substrate for wavelength conversion element.
【0060】本実施例4において第一の基板41に作製
した低融点ガラス膜44は、周期分極反転構造が作製さ
れた非線形光学結晶基板(Mg添加LiNbO3 基板4
3)の屈折率よりも小さい値の屈折率を持ち、非線形光
学結晶基板(Mg添加LiNbO3 基板43)の熱膨張
係数に近い値の熱膨張係数を持つことが必要である。低
融点ガラス膜44の屈折率が非線形光学結晶基板(Mg
添加LiNbO3 基板43)の屈折率よりも大きい場合
は、非線形光学結晶基板(Mg添加LiNbO 3 基板4
3)に入射した信号光と制御光が全反射条件を満たすこ
とができず低融点ガラス膜44中に散逸する結果となり
リッジ型光導波路を形成することができなくなる。ま
た、低融点ガラス膜44の熱膨張係数が非線形光学結晶
基板(Mg添加LiNbO3 基板43)の熱膨張係数と
大きく異なる場合は、第一の基板41にソリが発生する
原因となる他、温度変化に対して第一の基板41にクラ
ックが発生する原因となるので好ましくない。Fabrication on the first substrate 41 in Example 4
The low melting point glass film 44 thus formed has a periodic polarization inversion structure.
Nonlinear optical crystal substrate (Mg-doped LiNbO3Board 4
Non-linear light with a refractive index smaller than that of 3)
Scientific crystal substrate (Mg added LiNbO3Thermal expansion of substrate 43)
It is necessary to have a coefficient of thermal expansion close to the coefficient. Low
The refractive index of the melting point glass film 44 is a nonlinear optical crystal substrate (Mg
Added LiNbO3When it is larger than the refractive index of the substrate 43)
Is a nonlinear optical crystal substrate (Mg-doped LiNbO 3Board 4
The signal light and control light incident on 3) satisfy the condition of total reflection.
As a result, it is possible to dissipate in the low melting point glass film 44.
The ridge type optical waveguide cannot be formed. Well
In addition, the coefficient of thermal expansion of the low melting point glass film 44 is a nonlinear optical crystal.
Substrate (Mg added LiNbO3The coefficient of thermal expansion of the substrate 43)
When the difference is large, warpage occurs on the first substrate 41.
In addition to being a cause, the first substrate 41 is not affected by temperature changes.
It is not preferable because it may cause a crack.
【0061】また、本実施例で用意した第二の基板42
の熱膨張係数は第一の基板41に作製した低融点ガラス
膜44の熱膨張係数に近い値を持つことが望ましい。こ
れは、第一の基板41と第二の基板42とを熱処理によ
って貼り合わせたときにソリ或いはクラックを発生させ
ないためである。一方、第二の基板42の屈折率は、第
一の基板41に作製した低融点ガラス膜44の膜厚が5
μm以下である場合は第一の基板41の屈折率よりも小
さい値を持つことが好ましい。これは、周期反転分極構
造をもった非線形光学結晶基板(Mg添加LiNbO3
基板43)に入射された信号光と制御光の光電界のすそ
が低融点ガラス膜44との界面を越えて5μm程度低融
点ガラス膜44中に広がっているため、第二の基板42
の表面層の屈折率が低融点ガラス膜44よりも大きい場
合には光電界が低融点ガラス膜を越えて第二の基板中に
散逸する結果となるためである。一方、低融点ガラス膜
44の膜厚が5μm以上である場合は第二の基板42の
屈折率に関する制限はない。The second substrate 42 prepared in this embodiment is also used.
The coefficient of thermal expansion of is preferably close to the coefficient of thermal expansion of the low melting point glass film 44 formed on the first substrate 41. This is because warpage or cracks do not occur when the first substrate 41 and the second substrate 42 are bonded by heat treatment. On the other hand, the refractive index of the second substrate 42 is 5 when the film thickness of the low melting point glass film 44 formed on the first substrate 41 is 5
When it is less than or equal to μm, it preferably has a value smaller than the refractive index of the first substrate 41. This is a nonlinear optical crystal substrate (Mg-doped LiNbO 3 having a periodically inverted polarization structure).
Since the skirts of the optical fields of the signal light and the control light incident on the substrate 43) extend beyond the interface between the low melting point glass film 44 and about 5 μm into the low melting point glass film 44, the second substrate 42
This is because if the refractive index of the surface layer is larger than that of the low melting point glass film 44, the photo-electric field will dissipate into the second substrate beyond the low melting point glass film. On the other hand, when the thickness of the low melting point glass film 44 is 5 μm or more, there is no limitation on the refractive index of the second substrate 42.
【0062】第一の基板41に作製した低融点ガラス膜
44は実施例3と同様の方法によって作製した。即ち、
Mg添加LiNbO3 基板43上に膜厚が均一になるよ
うにガラスペーストを塗布したものを電気炉中で焼成す
ることによって厚さ50μmの透明な低融点ガラス膜4
4を作製した。The low melting point glass film 44 formed on the first substrate 41 was formed by the same method as in Example 3. That is,
A transparent low-melting-point glass film 4 having a thickness of 50 μm was obtained by coating a Mg-added LiNbO 3 substrate 43 with a glass paste applied so as to have a uniform film thickness, and firing it in an electric furnace.
4 was produced.
【0063】本実施例4に用いた低融点ガラスは、その
熱膨張係数がLiNbO3 におよそ一致し、且つ、屈折
率はLiNbO3 の値よりも小さい値を持つようにガラ
ス組成が調整されている。なお、ガラス組成を所望の熱
膨張係数と屈折率を持つように調整することは低融点ガ
ラスを製造している当該業者が適宜行うことができるも
のである。また、低融点ガラスとしては実施例3に記載
したようなガラス材料を用いることができる。The glass composition of the low melting point glass used in Example 4 was adjusted so that its thermal expansion coefficient was approximately equal to that of LiNbO 3 and that its refractive index was smaller than that of LiNbO 3. There is. The glass composition can be adjusted to have a desired coefficient of thermal expansion and a desired refractive index by a person skilled in the art of manufacturing low melting glass. Further, as the low melting point glass, the glass material as described in Example 3 can be used.
【0064】そして、図6に示すように、第一の工程で
は、用意した第一及び第二の基板41,42の表面を通
常の酸洗浄或いはアルカリ洗浄によって親水性にした。
次に、第一の基板41の低融点ガラス膜44が第二の基
板42の表面に重なるように二つの基板41,42をマ
イクロパーティクルが極力存在しない清浄雰囲気中で重
ね合わせた。そして、重ね合わせた第一及び第二の基板
41,42を電気炉にいれ400℃で3時間熱処理する
ことにより拡散接合を行った。接着された基板は接合面
にマイクロパーティクル等の挟み込みがなくてボイドフ
リーであり、室温に戻したときにおいてもクラックなど
は発生しなかった。Then, as shown in FIG. 6, in the first step, the surfaces of the prepared first and second substrates 41 and 42 were made hydrophilic by ordinary acid cleaning or alkali cleaning.
Next, the two substrates 41 and 42 were superposed in a clean atmosphere in which microparticles were not present as much as possible so that the low melting point glass film 44 of the first substrate 41 overlaps the surface of the second substrate 42. Then, the first and second substrates 41 and 42 that were overlapped were put in an electric furnace and heat-treated at 400 ° C. for 3 hours to perform diffusion bonding. The bonded substrates were void-free, with no microparticles or the like sandwiched between the bonded surfaces, and no cracks or the like were generated even when returned to room temperature.
【0065】次に、第二の工程では、研磨定盤の平坦度
が管理された研磨装置を用いて、接着された基板の分極
反転構造が形成された非線形光学結晶基板の厚さが10
μmになるまで研磨加工を施した。研磨加工の後に、ポ
リッシング加工を行うことにより鏡面の研磨表面を得る
ことができた。基板の平行度を光学的な平行度測定機を
用いて測定したところ、3インチウエハの周囲を除き、
ほぼ全体にわたってサブミクロンの平行度が得られ、波
長変換素子の作製に好適な薄膜基板45を作製すること
ができた。Next, in the second step, the thickness of the nonlinear optical crystal substrate in which the polarization inversion structure of the bonded substrate is formed is 10 by using the polishing apparatus in which the flatness of the polishing platen is controlled.
Polishing was performed until it became μm. After the polishing process, a polishing process could be performed to obtain a mirror-polished surface. When the parallelism of the substrate was measured using an optical parallelism measuring machine, except for the periphery of the 3 inch wafer,
Submicron parallelism was obtained over almost the entire area, and the thin film substrate 45 suitable for producing a wavelength conversion element could be produced.
【0066】このほか、第一の基板としてLiNbO3
の他、Zn添加LiNbO3 、Sc添加LiNbO3 、
In添加LiNbO3 、LiTaO3 、LiNb(x) T
a(1 -x) O3 (0≦x≦1)、KNbO3 、KTiOP
O4 などを用いた場合においても、同様の波長変換素子
用薄膜基板を作製することができた。In addition, LiNbO 3 is used as the first substrate.
In addition, Zn-added LiNbO 3 , Sc-added LiNbO 3 ,
In-added LiNbO 3 , LiTaO 3 , LiNb (x) T
a (1 -x) O 3 (0 ≦ x ≦ 1), KNbO 3 , KTiOP
Even when O 4 or the like was used, a similar thin film substrate for wavelength conversion element could be produced.
【0067】また、第一の基板上に作製する低融点ガラ
ス膜の作製方法として蒸着或いはスパッタを用いた場合
においても同様の第一の基板を作製することができた。
また、低融点ガラスからなる基板を用意し、この低融点
ガラス基板と分極反転構造が形成された非線形光学結晶
基板とを重ね合わせた後、熱処理によって貼り合わせる
ことによっても第一の基板を用意することができた。Also, when vapor deposition or sputtering was used as the method for producing the low melting point glass film to be produced on the first substrate, the same first substrate could be produced.
Further, a first substrate is also prepared by preparing a substrate made of low-melting glass, superposing this low-melting glass substrate and a nonlinear optical crystal substrate having a domain-inverted structure, and then bonding them by heat treatment. I was able to.
【0068】また、第二の基板として実施例3で用いた
ような低融点ガラス膜が表面に作製された複合基板を用
い、第一の基板として本実施例4の分極反転構造をもっ
た非線形光学結晶基板の下に低融点ガラス膜が作製され
ているような複合基板を用いて、これらの複合基板を各
基板の低融点ガラス膜同士が重なり合うようにして重ね
た後、熱処理による拡散接合によって貼り合わせた場合
においても同様の波長変換素子用薄膜基板を作製するこ
とができた。この場合には第一の基板と第二の基板のそ
れぞれに作製された低融点ガラス膜が薄い場合でも、こ
れらの低融点ガラス膜を貼り合わせることにより全体と
して低融点ガラス膜を厚くすることができる。Also, a composite substrate having a low melting point glass film as used in Example 3 formed on the surface is used as the second substrate, and a nonlinear substrate having the domain-inverted structure of Example 4 is used as the first substrate. By using a composite substrate in which a low-melting glass film is formed under the optical crystal substrate, stacking these composite substrates so that the low-melting glass films of the respective substrates overlap each other, and then performing diffusion bonding by heat treatment. A similar thin film substrate for a wavelength conversion element could be produced even when they were bonded together. In this case, even if the low-melting glass films formed on the first substrate and the second substrate are thin, it is possible to increase the thickness of the low-melting glass film as a whole by bonding these low-melting glass films. it can.
【0069】次に、作製した波長変換素子用薄膜基板を
用いて実施例1と同様の方法によってリッジ型光導波路
をもつ波長変換素子を作製した。作製した波長変換素子
に波長0.77μmの制御光と波長1.55μmの信号
光とを入射したところ、波長1.53μmの波長変換光
が得られ、実施例1で作製した波長変換素子よりも高効
率の波長変換を実現できた。これは、本実施例において
は第一の基板に低融点ガラス膜を作製したことにより、
第一の基板の本体層(Mg添加LiNbO3 基板)の屈
折率と表面層の低融点ガラス膜の屈折率との差を大きく
することができるため、光導波路中への光電界の閉じ込
めを実施例1で作製した波長変換素子よりも強くするこ
とができるためである。Next, a wavelength conversion element having a ridge type optical waveguide was manufactured by the same method as in Example 1 using the manufactured wavelength conversion element thin film substrate. When the control light having a wavelength of 0.77 μm and the signal light having a wavelength of 1.55 μm were incident on the manufactured wavelength conversion element, wavelength converted light having a wavelength of 1.53 μm was obtained, which was higher than that of the wavelength conversion element manufactured in Example 1. We were able to realize highly efficient wavelength conversion. This is because the low melting point glass film was formed on the first substrate in this example,
Since the difference between the refractive index of the main body layer of the first substrate (Mg-doped LiNbO 3 substrate) and the refractive index of the low melting point glass film of the surface layer can be increased, the optical electric field is confined in the optical waveguide. This is because it can be made stronger than the wavelength conversion element manufactured in Example 1.
【0070】(実施例5)図7は本実施例5によって加
工されたリッジ型導波路の断面図である。本実施例5に
おいては実施例1で作製した波長変換素子用薄膜基板1
3を用い、また、リッジ型光導波路16の作製手段とし
てダイシングソーによる超精密研削加工技術を用いて波
長変換素子17を作製した。リッジ部(光導波路16)
の幅は6μm、溝の深さは50μmであった。(Embodiment 5) FIG. 7 is a sectional view of a ridge type waveguide processed according to the present embodiment 5. In the fifth embodiment, the wavelength conversion element thin film substrate 1 manufactured in the first embodiment is used.
No. 3 was used, and the wavelength conversion element 17 was manufactured using the ultra-precision grinding processing technique using a dicing saw as a manufacturing means of the ridge type optical waveguide 16. Ridge part (optical waveguide 16)
Had a width of 6 μm and a groove depth of 50 μm.
【0071】作製された各光導波路16ごとに基板(3
インチウエハ)を短冊状に切りだし、導波路端面を光学
研磨することによって長さ60mmの波長変換素子17
を作製した。作製した波長変換素子に波長0.77μm
の制御光と波長1.55μmの信号光を入射したとこ
ろ、波長1.53μmの波長変換光が得られ、高効率の
波長変換が実現できた。このほか、実施例2,3及び4
で作製した波長変換素子用薄膜基板を用いても同様の波
長変換素子を作製することができた。The substrate (3
(Inch wafer) is cut into strips, and the end face of the waveguide is optically polished to obtain a wavelength conversion element 17 having a length of 60 mm.
Was produced. Wavelength 0.77 μm for the manufactured wavelength conversion element
When the control light and the signal light with a wavelength of 1.55 μm were incident, wavelength-converted light with a wavelength of 1.53 μm was obtained, and highly efficient wavelength conversion could be realized. In addition, Examples 2, 3 and 4
A similar wavelength conversion element could be manufactured using the thin film substrate for wavelength conversion element manufactured in.
【0072】[0072]
【発明の効果】以上説明したように、本発明によれば大
面積にわたって均一な組成と、膜厚を持つような波長変
換素子用薄膜基板を提供することができる。従って、本
発明の波長変換素子用薄膜基板を用いれば、長尺の波長
変換素子の製造が可能となり波長変換効率の向上に効果
がある。As described above, according to the present invention, it is possible to provide a thin film substrate for a wavelength conversion element having a uniform composition and a film thickness over a large area. Therefore, if the thin film substrate for wavelength conversion element of the present invention is used, a long wavelength conversion element can be manufactured, and it is effective in improving the wavelength conversion efficiency.
【図1】本発明の実施例1の波長変換素子用薄膜基板を
作製する工程を示すフロー図である。FIG. 1 is a flow chart showing a process of manufacturing a thin film substrate for a wavelength conversion element according to a first embodiment of the present invention.
【図2】本発明の実施例1の波長変換素子の断面を示す
図である。FIG. 2 is a diagram showing a cross section of the wavelength conversion element according to the first embodiment of the present invention.
【図3】本発明の実施例1の波長変換素子を切り出す様
子を示す図である。FIG. 3 is a diagram showing how the wavelength conversion element of Example 1 of the present invention is cut out.
【図4】本発明の実施例2の波長変換素子用薄膜基板を
作製する工程を示すフロー図である。FIG. 4 is a flow chart showing a process of manufacturing a thin film substrate for a wavelength conversion element according to a second embodiment of the present invention.
【図5】本発明の実施例3の波長変換素子用薄膜基板を
作製する工程を示すフロー図である。FIG. 5 is a flowchart showing steps of producing a thin film substrate for a wavelength conversion element according to Example 3 of the present invention.
【図6】本発明の実施例4の波長変換素子用薄膜基板を
作製する工程を示すフロー図である。FIG. 6 is a flowchart showing a process of manufacturing a thin film substrate for a wavelength conversion element according to Example 4 of the present invention.
【図7】本発明の実施例5の波長変換素子の断面を示す
図である。FIG. 7 is a diagram showing a cross section of a wavelength conversion element according to a fifth embodiment of the present invention.
【図8】擬似位相整合型の波長変換素子の構成を示す図
である。FIG. 8 is a diagram showing a configuration of a quasi phase matching type wavelength conversion element.
11 第一の基板(Zn添加LiNbO3 基板) 12 第二の基板(Mg添加LiNbO3 基板) 13 波長変換素子用薄膜基板 14 リッジ型光導波路 14a 導波路端面 15 波長変換素子 16 リッジ型光導波路 17 波長変換素子 21 第一の基板(LiNbO3 基板) 22 第二の基板(水晶基板) 23 波長変換素子用薄膜基板 31 第一の基板(Mg添加LiNbO3 基板) 32 第二の基板 33 LiNbO3 基板 34 低融点ガラス膜 35 波長変換素子用薄膜基板 41 第一の基板 42 第二の基板 43 Mg添加LiNbO3 基板 44 低融点ガラス膜 45 波長変換素子用薄膜基板Reference Signs List 11 First substrate (Zn-added LiNbO 3 substrate) 12 Second substrate (Mg-added LiNbO 3 substrate) 13 Thin film substrate for wavelength conversion element 14 Ridge type optical waveguide 14a Waveguide end face 15 Wavelength conversion element 16 Ridge type optical waveguide 17 Wavelength conversion element 21 First substrate (LiNbO 3 substrate) 22 Second substrate (crystal substrate) 23 Thin film substrate for wavelength conversion element 31 First substrate (Mg-added LiNbO 3 substrate) 32 Second substrate 33 LiNbO 3 substrate 34 low melting point glass film 35 thin film substrate for wavelength conversion element 41 first substrate 42 second substrate 43 Mg-added LiNbO 3 substrate 44 low melting point glass film 45 thin film substrate for wavelength conversion element
───────────────────────────────────────────────────── フロントページの続き (72)発明者 遊部 雅生 東京都千代田区大手町二丁目3番1号 日 本電信電話株式会社内 (72)発明者 忠永 修 東京都千代田区大手町二丁目3番1号 日 本電信電話株式会社内 (72)発明者 鈴木 博之 東京都千代田区大手町二丁目3番1号 日 本電信電話株式会社内 Fターム(参考) 2K002 AB12 BA03 CA02 CA03 EA07 FA27 FA29 GA04 HA21 ─────────────────────────────────────────────────── ─── Continued front page (72) Inventor Masao Yube 2-3-1, Otemachi, Chiyoda-ku, Tokyo Inside Telegraph and Telephone Corporation (72) Osamu Tadaga, inventor 2-3-1, Otemachi, Chiyoda-ku, Tokyo Inside Telegraph and Telephone Corporation (72) Inventor Hiroyuki Suzuki 2-3-1, Otemachi, Chiyoda-ku, Tokyo Inside Telegraph and Telephone Corporation F-term (reference) 2K002 AB12 BA03 CA02 CA03 EA07 FA27 FA29 GA04 HA21
Claims (14)
が周期的に変調する構造をもつ第一の基板と、第二の基
板とを貼り合わせる第一の工程と、前記第一の基板の厚
さを薄くして光導波路を形成するための所定の厚さにす
る第二の工程とを有する波長変換素子用薄膜基板の製造
方法であって、前記第一の工程では前記第一の基板と前
記第二の基板とを、熱処理による拡散接合によって直接
貼り合わせることを特徴とする波長変換素子用薄膜基板
の製造方法。1. A first step of bonding a first substrate having a structure having a quadratic nonlinear effect and a nonlinear constant being periodically modulated, and a second substrate, and the first substrate. A thin film substrate for a wavelength conversion element having a second step of reducing the thickness to a predetermined thickness for forming an optical waveguide, wherein the first step includes the first step. A method for manufacturing a thin film substrate for a wavelength conversion element, which comprises directly bonding the substrate and the second substrate by diffusion bonding by heat treatment.
基板の製造方法において、前記第一の工程における熱処
理は前記第一の基板のキュリー温度以下の温度で行うこ
とを特徴とする波長変換素子用薄膜基板の製造方法。2. The method for manufacturing a thin film substrate for a wavelength conversion element according to claim 1, wherein the heat treatment in the first step is performed at a temperature equal to or lower than the Curie temperature of the first substrate. Method for manufacturing thin film substrate for device.
薄膜基板の製造方法において、前記第二の工程では前記
第一の基板の厚さを20μm以下にすることを特徴とす
る波長変換素子用薄膜基板の製造方法。3. The method for manufacturing a thin film substrate for a wavelength conversion element according to claim 1, wherein the thickness of the first substrate is 20 μm or less in the second step. Method for manufacturing thin film substrate for device.
変換素子用薄膜基板の製造方法において、前記第一の基
板が、LiNbO3 、KNbO3 、LiTaO3 、Li
Nb(x) Ta(1-x) O3 (0≦x≦1)又はKTiOP
O4 、或いは、それらにMg、Zn、Sc、Inからな
る群から選ばれた少なくとも一種を添加物として含有し
ていることを特徴とする波長変換素子用薄膜基板の製造
方法。4. The method of manufacturing a thin film substrate for a wavelength conversion element according to claim 1, wherein the first substrate is LiNbO 3 , KNbO 3 , LiTaO 3 , Li.
Nb (x) Ta (1-x) O 3 (0 ≦ x ≦ 1) or KTiOP
A method of manufacturing a thin film substrate for a wavelength conversion element, which contains O 4 or at least one of them selected from the group consisting of Mg, Zn, Sc and In as an additive.
変換素子用薄膜基板の製造方法において、前記第二の基
板の屈折率は前記第一の基板の屈折率よりも小さいこと
を特徴とする波長変換素子用薄膜基板の製造方法。5. The method of manufacturing a thin film substrate for a wavelength conversion element according to claim 1, wherein the second substrate has a refractive index smaller than that of the first substrate. A method for manufacturing a thin film substrate for a wavelength conversion element, comprising:
基板の製造方法において、前記第二の基板は水晶基板又
はガラス基板であることを特徴とする波長変換素子用薄
膜基板の製造方法。6. The method for manufacturing a thin film substrate for a wavelength conversion element according to claim 5, wherein the second substrate is a quartz substrate or a glass substrate.
変換素子用薄膜基板の製造方法において、前記第二の基
板の前記第一の基板に接合する表面層の屈折率は、前記
第一の基板の屈折率よりも小さいことを特徴とする波長
変換素子用薄膜基板の製造方法。7. The method of manufacturing a thin film substrate for a wavelength conversion element according to claim 1, wherein a refractive index of a surface layer of the second substrate bonded to the first substrate is: A method for manufacturing a thin film substrate for a wavelength conversion element, which is smaller than the refractive index of the first substrate.
板の製造方法において、前記第二の基板の表面層は低融
点ガラス膜又は低融点ガラス基板であることを特徴とす
る波長変換素子用薄膜基板の製造方法。8. The wavelength conversion element according to claim 7, wherein the surface layer of the second substrate is a low melting point glass film or a low melting point glass substrate. Method for manufacturing thin film substrate.
変換素子用薄膜基板の製造方法において、前記第一の基
板の第二の基板に接合する表面層の屈折率は、光導波路
を形成する前記第一の基板の本体層の屈折率よりも小さ
いことを特徴とする波長変換素子用薄膜基板の製造方
法。9. The method of manufacturing a thin film substrate for a wavelength conversion element according to claim 1, wherein a refractive index of a surface layer of the first substrate bonded to the second substrate is A method of manufacturing a thin film substrate for a wavelength conversion element, which is smaller than a refractive index of a main body layer of the first substrate forming a waveguide.
基板の製造方法において、前記第一の基板の表面層は低
融点ガラス膜又は低融点ガラス基板であることを特徴と
する波長変換素子用薄膜基板の製造方法。10. The method of manufacturing a thin film substrate for a wavelength conversion element according to claim 9, wherein the surface layer of the first substrate is a low melting glass film or a low melting glass substrate. Method for manufacturing thin film substrate.
長変換素子用薄膜基板の製造方法において、前記第一の
基板の第二の基板に接合する表面層の屈折率は、光導波
路を形成する前記第一の基板の本体部の屈折率よりも小
さく、且つ、前記第二の基板の前記第一の基板に接合す
る表面層の屈折率も、前記第一の基板の本体層の屈折率
よりも小さいことを特徴とする波長変換素子用薄膜基板
の製造方法。11. The method for manufacturing a thin film substrate for a wavelength conversion element according to claim 1, wherein a refractive index of a surface layer of the first substrate bonded to the second substrate is The refractive index of the surface layer of the second substrate, which is smaller than the refractive index of the main body of the first substrate forming the waveguide, and which is bonded to the first substrate is also the main body layer of the first substrate. A method of manufacturing a thin film substrate for a wavelength conversion element, which is smaller than the refractive index of.
膜基板の製造方法において、前記第一の基板の表面層は
低融点ガラス膜又は低融点ガラス基板であり、前記第二
の基板の表面層も低融点ガラス膜又は低融点ガラス基板
であることを特徴とする波長変換素子用薄膜基板の製造
方法。12. The method of manufacturing a thin film substrate for a wavelength conversion element according to claim 11, wherein the surface layer of the first substrate is a low melting glass film or a low melting glass substrate, and the surface of the second substrate. A method for producing a thin film substrate for a wavelength conversion element, wherein the layer is also a low melting point glass film or a low melting point glass substrate.
波長変換素子用薄膜基板の製造方法において、前記第二
の基板の熱膨張係数が、前記第一の基板の熱膨張係数に
ほぼ一致することを特徴とする波長変換素子用薄膜基板
の製造方法。13. The method of manufacturing a thin film substrate for a wavelength conversion element according to claim 1, wherein the thermal expansion coefficient of the second substrate is the thermal expansion coefficient of the first substrate. A method for manufacturing a thin film substrate for a wavelength conversion element, which is characterized in that they are substantially identical.
波長変換素子用薄膜基板の製造方法によって波長変換素
子用薄膜基板を作製し、これに続く第三の工程で、前記
波長変換素子用薄膜基板における前記第一の基板に光導
波路を作製することを特徴とする波長変換素子の製造方
法。14. A thin film substrate for a wavelength conversion element is manufactured by the method for manufacturing a thin film substrate for a wavelength conversion element according to claim 1, and the wavelength conversion is performed in a subsequent third step. A method of manufacturing a wavelength conversion element, characterized in that an optical waveguide is formed on the first substrate of the element thin film substrate.
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