WO2023209819A1 - Method for inspecting periodical polarization inversion structure - Google Patents
Method for inspecting periodical polarization inversion structure Download PDFInfo
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- WO2023209819A1 WO2023209819A1 PCT/JP2022/018939 JP2022018939W WO2023209819A1 WO 2023209819 A1 WO2023209819 A1 WO 2023209819A1 JP 2022018939 W JP2022018939 W JP 2022018939W WO 2023209819 A1 WO2023209819 A1 WO 2023209819A1
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/35—Non-linear optics
- G02F1/37—Non-linear optics for second-harmonic generation
Definitions
- the present invention relates to a method for inspecting a periodically poled structure of a dielectric material.
- Optical elements that can generate and modulate coherent light in the ultraviolet, visible, near-infrared, and terahertz wavelength bands play an important role.
- Such optical elements can be applied in a wide variety of fields such as wavelength conversion of optical signals, optical modulation, optical measurement, and optical processing in optical communication systems.
- optical elements that utilize nonlinear optical effects have excellent characteristics in terms of nonlinear optical effects such as wavelength conversion and electro-optic effects.
- Typical examples of optical materials having nonlinear optical effects and electro-optic effects are oxide-based compounds such as lithium niobate (LiNbO 3 :LN) and lithium tantalate (LiTaO 3 :LT).
- LiNbO 3 :LN lithium niobate
- LiTaO 3 :LT lithium tantalate
- PPLN Periodically Poled Lithium Niobate
- PPLT Periodically Poled Lithium Tantalate
- the periodically poled structure achieves high phase matching and high second-order nonlinear optical effects.
- a wavelength conversion element is known as an optical device that uses the high nonlinearity of PPLN and PPLT.
- the wavelength conversion element uses mechanisms of second harmonic generation (SHG), differential frequency generation (DFG), and sum frequency generation (SFG). Wavelength conversion elements that utilize these mechanisms are useful for building large-capacity optical communication networks, including the development of light sources in new wavelength bands, optical routing and wavelength collision avoidance through batch wavelength conversion, and signal distortion compensation using phase conjugate light. Supports core technology.
- Non-Patent Document 1 Quasi-phase matching technology becomes important for increasing wavelength conversion efficiency.
- the pseudo phase matching technique is a method of achieving pseudo phase matching in the light propagation direction by forming a structure in which the sign of nonlinear susceptibility is periodically inverted.
- quasi-phase matching will not be explained here, in order to periodically modulate the nonlinear optical coefficient in linear optical crystals, it is essential to fabricate with high precision a periodically poled structure that periodically reverses the crystal axis. It's technology.
- the conventional method for observing and inspecting periodically poled structures requires time and effort, and reduces the throughput of the manufacturing process when it is necessary to observe the vicinity of the waveguide.
- the present invention facilitates observation of periodic polarization structures near waveguides, improves throughput when it is necessary to inspect the vicinity of waveguides in the manufacturing process of optical devices including periodic polarization inversion structures, and improves the throughput of nonlinear optical elements.
- One aspect of the present invention is a method for inspecting a periodically poled structure created on a substrate, comprising the steps of fixing the substrate to a stage via an electrostatic chuck, and dry etching to form a capillary. selectively etching the inspection region of the periodically poled structure in the vicinity of the opening, and etching the periodically poled structure in the test region based on the unevenness formed in the dry etching according to the polarization direction. determining non-uniformities or defects in the wafer.
- FIG. 2 is a schematic diagram of the structure of a PPLN element having a periodic polarization inversion structure.
- FIG. 3 is a diagram illustrating various non-uniformity and defect patterns of a periodically poled structure.
- FIG. 3 is a diagram showing a region where a periodically poled structure is observed in an inspection process on a wafer.
- FIG. 2 is a diagram comparing inspection flows of a conventional technique and a periodic polarization inversion structure of the present disclosure.
- FIG. 1 is a diagram showing the configuration of a periodic polarization structure inspection device according to the present disclosure.
- FIG. 3 is a diagram showing a state of dry etching near the surface of a period-reversed polarization structure.
- FIG. 3 is a diagram illustrating a pattern of a periodically reversed polarization structure obtained by dry etching.
- FIG. 3 is a diagram illustrating inspection by local dry etching along a waveguide.
- the method for inspecting a periodically poled structure of the present disclosure fixes a sample using an electrostatic chuck and reveals a surface potential that depends on the polarization direction of the sample.
- dry etching it is possible to conduct a local inspection near where the waveguide is to be fabricated.
- complicated steps such as masking can be omitted, making it easier to inspect and observe the periodic polarization inversion structure in the vicinity of the waveguide. Since it is possible to locally inspect the vicinity of the waveguide, it is possible to more accurately discover non-uniformities and defects in the periodic structure.
- FIG. 1 is a schematic diagram of the structure of a PPLN element having a periodic polarization inversion structure.
- a ridge-type waveguide 13 having a periodic polarization inversion structure is formed in the PPLN element 10.
- the PPLN element 10 of FIG. 1 is constructed by directly bonding a first substrate 12 having a periodically polarized structure, which will be a core layer, and a second substrate 11, which will be a cladding layer, and forming a waveguide 13 by dry etching. It is obtained by processing it into the shape of.
- the ridge-type waveguide 13 is formed along the x direction, perpendicular to the boundary surface of each region of the periodically poled structure.
- the light 18 to be subjected to the nonlinear effect enters from one end of the ridge waveguide 13.
- the structure of the optical waveguide that is produced in the device that is finally obtained there are no limitations on the structure of the optical waveguide that is produced in the device that is finally obtained. Whether it is a ridge type optical waveguide as shown in Figure 1 or a diffused type optical waveguide in which ions or titanium are diffused, there are laser-drawn optical waveguides that form a structure using the change in refractive index caused by laser irradiation. But it's okay.
- a region 1a polarized downward (-z) and a region 1b polarized upward (+z) in the z-axis direction perpendicular to the substrate surface are arranged at a constant period (pitch). ) are repeated alternately.
- a structure in which the polarization direction is periodically reversed between upward and downward in this manner is a periodic polarization inversion structure.
- a polarization inversion structure is formed using an electric field application method.
- a high voltage is applied to invert the polarization of a ferroelectric material, and in particular, in LN, a very high electric field of about 21 kV/mm is used.
- Voltage application is performed by generating a voltage pulse with an arbitrary waveform generator, amplifying it with a high-voltage amplifier, and then applying it to the sample via a high-voltage cable.
- a metal electrode or a liquid electrode is in contact with the surface of the z-cut LN substrate, and the electric field is spatially modulated by the pattern shape of the electrode to form a periodic polarization inversion structure.
- various non-uniformities, variations, and defects may occur in the periodic structure.
- FIG. 2 is a diagram illustrating various defect patterns in a periodically poled structure. Both figures show a cross section (zx plane) perpendicular to the substrate surface (xy plane) of the periodically poled structure, and after the waveguide is fabricated, light propagates in the x-axis direction.
- FIG. 2(a) shows an ideal periodic polarization inversion structure in which there are no defects or non-uniformity, and downward polarized regions 1a and upward polarized regions 1b are regularly arranged at equal intervals.
- some areas 2-1 have a different pitch from other areas.
- the width 3a of the downward polarized region is different from the width 3b of the upward polarized region, resulting in non-uniformity of the structure.
- shape distortion in the z direction of each polarization region occurs in some regions 2-2.
- a defective region 3 in which polarization inversion is not formed occurs.
- FIG. 3 is a diagram showing a region where a periodically poled structure is observed in the inspection process.
- FIG. 3A shows a state in which a region 12 having a periodic polarization inversion structure is formed on, for example, an LN wafer 14.
- FIG. 3 shows the state before the waveguide is fabricated, and shows along the x direction a plurality of regions 13-1 to 13-5 where the waveguide is to be fabricated.
- FIG. 3 is a schematic diagram for explaining the region, and it should be noted that the period of the periodically poled structure and the width and spacing of the waveguides are not accurate. For example, in the actual manufacturing process of a PPLN element, it is possible to manufacture approximately several hundred waveguides within a 3-inch substrate.
- FIG. 4 is a diagram showing the flow of a method for inspecting a periodically poled structure according to the prior art and the present disclosure.
- FIG. 4A is a flow diagram illustrating an example of a conventional inspection method.
- FIG. 4B is a flowchart showing an example of a method for inspecting a periodically poled structure according to the present disclosure, and the details will be described later.
- FIG. 4 is shown as an inspection method in the manufacturing process of an optical element such as a wavelength conversion element, it should be noted that it also has aspects of an observation method and an evaluation method for a periodic polarization inversion structure.
- the flowchart 20 in FIG. 4(a) starts at step 21, in which a periodically poled structure is fabricated on, for example, an LN substrate, as in the wafer state shown in FIG. 3(a).
- the end region of FIG. A step 22 of masking the area where the other waveguides are to be fabricated except for the area 15 is required. This is to prevent the waveguide from being damaged by wet etching in the next step.
- a wet etching step 23 using hydrofluoric acid and hydrofluoric nitric acid the end region 15 is etched.
- the periodically poled structure there is a difference in etching rate between a region polarized in the z-direction of the crystal axis and a region polarized in the -z-axis direction. Non-uniformity and the presence of defects can be visualized by the step difference in the etched surface in the thickness direction of the substrate caused by the difference in etching rate.
- a masking removal step 24 is performed to observe the periodic polarization inversion structure.
- the observation step 25 if non-uniformity or defects in the periodic structure as shown in FIG. 2 are discovered, they are reflected in the next step, the waveguide structure fabrication step 26, according to certain criteria. For example, if more non-uniformities or defects are found than a certain standard, the wafer can be discarded.
- the wet etching step 23 is essential, so it is very difficult to observe the polarization inversion structure only in the vicinity of the crystal plane where the waveguide is actually created on the wafer.
- a solution such as hydrofluoric acid and hydrofluoronitric acid.
- a step 22 of masking the area outside the region to be wet etched and a step 24 of removing the masking are essential, as shown in FIG. 4(a).
- the inspection process shown in FIG. 4(a) involves inspecting the periodic polarization inversion structure near the waveguide before dicing and cutting out the optical circuit including the nonlinear optical element fabricated on the wafer as a chip. The case where this is implemented is shown. After dicing the wafer into chips, each chip may be inspected for a periodic polarization inversion structure similar to that shown in FIG. 4(a).
- the method for inspecting a periodically poled structure of the present disclosure greatly simplifies the process shown in FIG. 4(a) in the prior art, and more easily visualizes the periodically poled structure near the waveguide.
- optical elements such as wavelength conversion elements.
- the nonlinear optical material that can be used in the method of inspecting a periodically poled structure of the present disclosure may be any material as long as it is transparent at a light wavelength of 400 to 2000 nm. Further, the nonlinear optical material may have a second-order nonlinear optical effect or a third-order or higher nonlinear optical effect as long as it has a nonlinear optical effect. Examples include, in addition to the above-mentioned LN and LT, beta-barium bolite (BBO), potassium titanyl phosphate (KTiOPO 4 , KTP), and the like.
- the nonlinear optical material in the inspection method of the present disclosure is a material that can form a periodically poled structure to increase the nonlinear optical effect.
- FIG. 5 is a diagram showing the configuration of an inspection device that plays a part in the inspection method for a periodically inverted polarization structure of the present disclosure.
- the inspection device 40 is a dry etching device in which a sample 44 to be inspected is placed in a vacuum chamber 41 .
- the chamber 41 is evacuated to a vacuum state by a vacuum pump 50, and etching gas 47 is introduced into the chamber from a cylinder 46.
- etching gas argon or CF-based gas is mainly used, and the gas is used depending on the material to be etched.
- the sample 44 is fixed on a three-dimensionally movable stage 42 via an electrostatic chuck 43.
- the sample 44 is an insulating capillary 45 connected to a vacuum pump 50.
- the etching gas flows into the capillary due to the pressure difference between the chamber internal pressure (V2) and the capillary internal pressure (V1), and is exhausted by a vacuum pump.
- a high-frequency coil 48 is installed around the capillary outside the chamber, and by applying a high voltage to the high-frequency coil 48 from a high-frequency power source 49, plasma is generated from the capillary into the chamber.
- a part of the plasma is also generated on the entrance side (sample side) of the capillary 45, and the diameter of the plasma can be narrowed down to about several mm, for example.
- the diameter of this plasma depends on the inner diameter of the capillary and can be controlled by the shape and material conditions of the capillary.
- the inspection device 40 in FIG. 5 is a schematic diagram, and the length of the capillary, the relative position and distance to the high-frequency coil 48 and the sample 44 are different from the actual one.
- the plasma locally generated on the surface of the sample 44 makes it possible to perform local dry etching at any desired position on the periodically poled structure.
- the inspection device 40 shown in FIG. 5 uses an electrostatic chuck on the sample 44 to generate a surface potential on the sample that depends on the polarization direction of the sample, thereby realizing an etching rate that depends on the polarization direction. do.
- the sample 44 in FIG. 5 may be a wafer before waveguide fabrication, or a cut chip.
- FIG. 6 is a diagram showing the state of dry etching near the surface of the periodically reversed polarization structure.
- the cross section (xz plane) of the sample 44 fixed by the electrostatic chuck 43 is seen, and (a) in FIG. 6 is before the start of dry etching, and (b) is during dry etching, and the flow of the etching gas is schematically shown. It shows.
- the vertical position of the capillary 45 on the z-axis is away from the substrate surface, and the plasma is also away from the substrate surface.
- FIG. 6B when the capillary 45 descends to the vicinity of the substrate and the plasma limited to a certain area reaches the surface, local dry etching begins.
- Etching gas is constantly supplied from the outside to the inside of the capillary 45 due to the pressure difference (V 1 , V 2 ) between the inside and outside of the capillary 45 .
- FIG. 6(c) is a diagram illustrating the potential near the surface of the periodically reversed polarization structure during dry etching.
- regions where upward polarization in the z-axis direction (upward arrow) occurs and regions where downward polarization in the z-axis direction (downward arrow) occur are formed alternately along the x-axis.
- positively charged regions and negatively charged regions alternately appear on the outermost surface of the substrate. Therefore, the potential on the substrate surface changes periodically in the x-axis direction. Since the reactivity between the molecules of the etching gases 47a and 47b on the outermost surface of the substrate and the nonlinear optical material whose potential distribution varies, different etching rates are produced depending on the position on the x-axis.
- FIG. 7 is a diagram illustrating the pattern of a periodically reversed polarization structure obtained by dry etching.
- a region 12 having a periodically reversed polarization structure is formed on the wafer 14.
- the waveguide will be formed along the x-axis direction.
- an uneven pattern depending on the polarization direction is locally generated on the surface.
- dry etching can be performed continuously along the x-axis direction, an uneven pattern with a height at a periodic pitch of the polarization structure will appear in the x-axis direction, as shown in FIG. 7(b).
- FIG. 8 is a diagram illustrating inspection of a periodically reversed polarization structure by local dry etching along a waveguide.
- a stage 42 that holds a sample in the inspection apparatus 40 shown in FIG. 5 can move at least in the horizontal direction (x direction).
- local dry etching can be performed at any position on the substrate surface by a movable stage 42 that determines the position of the sample 44 in the horizontal plane.
- the stage 42 in the x-axis direction parallel to the light propagation direction 18 the generally circular etching region 16 is swept, making it possible to perform linear etching.
- the periodic polarization inversion structure can be visualized along the propagation direction of the light of the wavelength conversion element. . Although it depends on which places in the wafer are to be etched, the time required for local etching using the inspection apparatus 40 of FIG. 5 is about one hour at most.
- a flowchart 30 of the method of testing a periodically poled structure of the present disclosure is shown in contrast to the flowchart of the prior art testing method of FIG. 4(a).
- the method for inspecting a periodically poled structure of the present disclosure does not require a masking step before the local dry etching 32 or a masking removal step. Therefore, compared to the conventional inspection flow 20 using wet etching, complicated work steps are omitted, and throughput can be improved when it is necessary to observe the vicinity of the waveguide.
- the work time and cost for observing and inspecting the periodically poled structure are significantly reduced, and wavelength conversion elements can be evaluated and manufactured efficiently.
- the location and number of areas to be locally etched can be changed depending on the required quality level, and only good areas on the wafer can be used in the next process. It is also possible to provide such judgment information.
- the present invention can be used for manufacturing and developing optical devices.
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Abstract
Description
本発明は、誘電体材料の周期分極反転構造の検査方法に関する。 The present invention relates to a method for inspecting a periodically poled structure of a dielectric material.
紫外、可視、近赤外、テラヘルツの波長帯域においてコヒーレント光の発生や変調をすることが可能な光学素子は、重要な役割を果たしている。このような光学素子は、光通信システムにおける光信号の波長変換や光変調、光計測、光加工などの多岐にわたる分野において応用できる。なかでも非線形光学効果を利用する光学素子は、波長変換など生じる非線形光学効果や電気光学効果において優れた特性を有する。 Optical elements that can generate and modulate coherent light in the ultraviolet, visible, near-infrared, and terahertz wavelength bands play an important role. Such optical elements can be applied in a wide variety of fields such as wavelength conversion of optical signals, optical modulation, optical measurement, and optical processing in optical communication systems. Among them, optical elements that utilize nonlinear optical effects have excellent characteristics in terms of nonlinear optical effects such as wavelength conversion and electro-optic effects.
非線形光学効果および電気光学効果を有する光学材料の代表例は、ニオブ酸リチウム(LiNbO3:LN)やタンタル酸リチウム(LiTaO3:LT)等の酸化物系化合物である。LNやLTが室温で自発分極が可能な特性を生かして、周期的に分極反転された構造を有するPPLN(Periodically Poled Lithium Niobate)やPPLT(Periodically Poled Lithium Tantalate)が広く用いられている。周期分極反転構造によって、高い位相整合性と、高い二次非線形光学効果等を実現している。 Typical examples of optical materials having nonlinear optical effects and electro-optic effects are oxide-based compounds such as lithium niobate (LiNbO 3 :LN) and lithium tantalate (LiTaO 3 :LT). Taking advantage of the characteristic that LN and LT can spontaneously polarize at room temperature, PPLN (Periodically Poled Lithium Niobate) and PPLT (Periodically Poled Lithium Tantalate), which have a periodically polarized structure, are widely used. The periodically poled structure achieves high phase matching and high second-order nonlinear optical effects.
PPLN、PPLTの高い非線形性を用いた光デバイスとして、波長変換素子が知られている。波長変換素子は、第二次高調波発生(SHG: Second Harmonic Generation)、差周波発生(DFG: Differential Frequency Generation)、和周波発生(SFG:Sum Frequency generation)の各機構を利用する。これらの機構を利用する波長変換素子は、新しい波長帯域における光源の開発、一括波長変換による光のルーティングや波長衝突回避、位相共役光を利用した信号歪補償など、大容量光通信ネットワークを構築する根幹技術を支えている。 A wavelength conversion element is known as an optical device that uses the high nonlinearity of PPLN and PPLT. The wavelength conversion element uses mechanisms of second harmonic generation (SHG), differential frequency generation (DFG), and sum frequency generation (SFG). Wavelength conversion elements that utilize these mechanisms are useful for building large-capacity optical communication networks, including the development of light sources in new wavelength bands, optical routing and wavelength collision avoidance through batch wavelength conversion, and signal distortion compensation using phase conjugate light. Supports core technology.
上述の技術を実現するには、高効率な非線形光学素子の開発が必須である。波長変換効率の高効率化には、疑似位相整合技術が重要になってくる(非特許文献1)。疑似位相整合技術は、非線形感受率の符号を周期的に反転した構造を形成することにより、光の伝搬方向に対して疑似的に位相整合を達成する手法である。疑似位相整合についてここでは説明しないが、線形光学結晶において、非線形光学係数に対し周期的に変調を加えるため、結晶軸を周期的に反転させる周期分極反転構造を高い精度で作製することが必須の技術である。 In order to realize the above technology, it is essential to develop highly efficient nonlinear optical elements. Quasi-phase matching technology becomes important for increasing wavelength conversion efficiency (Non-Patent Document 1). The pseudo phase matching technique is a method of achieving pseudo phase matching in the light propagation direction by forming a structure in which the sign of nonlinear susceptibility is periodically inverted. Although quasi-phase matching will not be explained here, in order to periodically modulate the nonlinear optical coefficient in linear optical crystals, it is essential to fabricate with high precision a periodically poled structure that periodically reverses the crystal axis. It's technology.
高い二次非線形光学効果を発現させるためには、周期分極反転構造をできる限り最大効率が得られる理論値の構造で設計し、その構造で正確に作製する必要がある。実際には、設計値通りの周期分極反転構造を形成するのは非常に難しい。十分な性能を持つ周期分極反転構造を含むチップを作製するためには、周期分極反転構造の寸法精度や欠陥の有無を検査する工程が必須である。 In order to exhibit a high second-order nonlinear optical effect, it is necessary to design a periodically poled structure with a theoretical value that provides the maximum efficiency, and to precisely manufacture it with that structure. In reality, it is very difficult to form a periodically poled structure as designed. In order to manufacture a chip including a periodically poled structure with sufficient performance, a step of inspecting the dimensional accuracy of the periodically poled structure and the presence or absence of defects is essential.
しかしながら、従来技術の周期分極反転構造の観察、検査方法は、工程に時間と手間が掛かり、導波路近傍の観察をする必要がある場合の製造工程のスループットを低下させていた。本発明は、導波路近傍の周期分極構造の観察を容易とし、周期分極反転構造を含む光デバイスの製造工程で導波路近傍の検査をする必要がある場合のスループットを向上させ、非線形光学素子の開発の効率化を実現する光デバイスの検査手法を提供する。 However, the conventional method for observing and inspecting periodically poled structures requires time and effort, and reduces the throughput of the manufacturing process when it is necessary to observe the vicinity of the waveguide. The present invention facilitates observation of periodic polarization structures near waveguides, improves throughput when it is necessary to inspect the vicinity of waveguides in the manufacturing process of optical devices including periodic polarization inversion structures, and improves the throughput of nonlinear optical elements. We provide an optical device inspection method that improves development efficiency.
本発明の1つの態様は、基板上に作成された周期分極反転構造を検査する方法であって、前記基板を、静電チャックを介して、ステージに固定するステップと、ドライエッチングによって、キャピラリの開口部の近傍で、前記周期分極反転構造の検査領域を選択的にエッチングするステップと、前記ドライエッチングに形成された、分極方向に応じた凹凸に基づいて、前記検査領域における前記周期分極反転構造の不均一または欠陥を判定するステップとを備える方法である。 One aspect of the present invention is a method for inspecting a periodically poled structure created on a substrate, comprising the steps of fixing the substrate to a stage via an electrostatic chuck, and dry etching to form a capillary. selectively etching the inspection region of the periodically poled structure in the vicinity of the opening, and etching the periodically poled structure in the test region based on the unevenness formed in the dry etching according to the polarization direction. determining non-uniformities or defects in the wafer.
非線形光学素子の検査における煩雑な作業工程が省略され、導波路近傍の周期分極構造の観察が容易になる。 Complicated work steps in testing nonlinear optical elements are omitted, and the periodic polarization structure near the waveguide can be easily observed.
本開示の周期分極反転構造の検査方法は、静電チャックによって試料を固定して、試料の分極方向に依存した表面電位を顕在化する。ドライエッチングを組み合わせ得ることで、導波路の作製予定の近傍の局所的な検査を実現する。従来技術のウェットエッチングを使用した検査方法と比べて、マスキングなどの煩雑な工程を省略することができ、導波路近傍における周期分極反転構造の検査、観察を容易にする。導波路の近傍の局所的な検査ができるため、より正確に周期構造の不均一や欠陥を発見できる。 The method for inspecting a periodically poled structure of the present disclosure fixes a sample using an electrostatic chuck and reveals a surface potential that depends on the polarization direction of the sample. By combining this method with dry etching, it is possible to conduct a local inspection near where the waveguide is to be fabricated. Compared to the conventional inspection method using wet etching, complicated steps such as masking can be omitted, making it easier to inspect and observe the periodic polarization inversion structure in the vicinity of the waveguide. Since it is possible to locally inspect the vicinity of the waveguide, it is possible to more accurately discover non-uniformities and defects in the periodic structure.
以下の説明では、まず周期分極反転構造の構造とその作製工程について簡単に触れ、次に、周期分極反転構造における不均一や欠陥について述べる。さらに従来技術の周期分極反転構造の検査方法と対比させながら、本開示の周期分極反転構造の検査方法について説明する。 In the following explanation, first, the structure of the periodically poled structure and its manufacturing process will be briefly mentioned, and then non-uniformity and defects in the periodically poled structure will be described. Furthermore, a method for inspecting a periodically poled structure according to the present disclosure will be described in comparison with a conventional method for inspecting a periodically poled structure.
図1は、周期分極反転構造を有するPPLN素子の構造の模式図である。PPLN素子10には、周期分極反転構造を持つリッジ型導波路13が形成されている。図1のPPLN素子10は、一例として、コア層となる周期分極反転構造を作製した第1の基板12と、クラッド層となる第2の基板11とを直接接合し、ドライエッチングにより導波路13の形状に加工して得られる。リッジ型導波路13は、周期分極反転構造の各領域の境界面に垂直に、x方向に沿って形成される。非線形作用を受けることになる光18は、リッジ型導波路13の一端から入射する。本開示の周期分極反転構造の検査方法では、最終的に得られることになる素子において作製される光導波路の構造には、何ら限定はない。図1に示したようなリッジ型光導波路であっても、イオンやチタンを拡散させた拡散型光導波路であっても、レーザー照射による屈折率変化を利用し構造を形成するレーザー描画型光導波路でも良い。
FIG. 1 is a schematic diagram of the structure of a PPLN element having a periodic polarization inversion structure. A ridge-
リッジ型導波路13をx方向に見れば、基板面の垂直なz軸方向において下向き(-z)に分極した領域1aと、上向き(+z)に分極した領域1bとが、一定の周期(ピッチ)で交互に繰り返されている。このように分極方向が周期的に上向き、下向きの間を繰り返し反転している構造が、周期分極反転構造である。
Looking at the
LNに代表される強誘電体では、電界印加法を用いて分極反転構造が形成される。一般に、強誘電体の分極反転のために印加される電圧が高く、特にLNでは21kV/mm程度の非常に高い電界を用いられる。電圧印加は、任意波形発生器で電圧パルスを発生し、高圧アンプで増幅したのちに高圧ケーブルを介して試料に印加することで行われる。zカットのLN基板の表面には金属電極または液体電極が接しており、電極のパターン形状に電界が空間変調を受けて、周期分極反転構造が形成される。このような分極反転構造の作製方法では、周期構造に様々な不均一、ばらつき、欠陥が生じ得る。 In a ferroelectric material represented by LN, a polarization inversion structure is formed using an electric field application method. Generally, a high voltage is applied to invert the polarization of a ferroelectric material, and in particular, in LN, a very high electric field of about 21 kV/mm is used. Voltage application is performed by generating a voltage pulse with an arbitrary waveform generator, amplifying it with a high-voltage amplifier, and then applying it to the sample via a high-voltage cable. A metal electrode or a liquid electrode is in contact with the surface of the z-cut LN substrate, and the electric field is spatially modulated by the pattern shape of the electrode to form a periodic polarization inversion structure. In such a method for manufacturing a domain-inverted structure, various non-uniformities, variations, and defects may occur in the periodic structure.
図2は、周期分極反転構造における様々な欠陥パターンを説明する図である。いずれの図も周期分極反転構造の基板面(x-y面)に垂直な断面(z-x面)を示しており、導波路が作製された後で、光はx軸方向に伝搬する。図2の(a)は、欠陥や不均一が無く、下向きの分極領域1aと上向きの分極領域1bが等間隔で規則正しく並んだ、理想的な周期分極反転構造を示す。(b)は、一部の領域2-1で他の領域とは異なるピッチとなっている。(c)では、下向きの分極領域の幅3aと、上向きの分極領域の幅3bが異なっており、構造の不均一が生じている。(d)では、一部の領域2-2で、各分極領域のz方向の形状ひずみが生じている。(e)では、分極反転が形成されていない欠陥領域3が生じている。
FIG. 2 is a diagram illustrating various defect patterns in a periodically poled structure. Both figures show a cross section (zx plane) perpendicular to the substrate surface (xy plane) of the periodically poled structure, and after the waveguide is fabricated, light propagates in the x-axis direction. FIG. 2(a) shows an ideal periodic polarization inversion structure in which there are no defects or non-uniformity, and downward polarized
図2に示したような周期分極反転構造の不均一や欠陥の存在は、反転周期の不均一が生じており、光の伝搬方向(x方向)に、疑似位相整合条件の異なる構造が分布していることを意味する。これは、動作予定の波長の光を非線形光学素子に入力したときに、疑似位相整合条件が完全には満たされない構造部分があり、実効的な変換効率が低下することを意味する。 The presence of non-uniformity and defects in the periodically poled structure shown in Figure 2 is due to non-uniformity of the period of inversion, and structures with different quasi-phase matching conditions are distributed in the light propagation direction (x direction). means that This means that when light of the wavelength intended for operation is input to the nonlinear optical element, there are structural parts where the quasi-phase matching condition is not completely satisfied, and the effective conversion efficiency is reduced.
波長変換素子において、疑似位相整合による波長変換効率の最大化を目指すには、設計通りに周期分極反転構造を作製し、その構造を精度よく評価・検査する技術が必須となる。また、周期分極反転構造は基板(ウェファ)面内において、均一に形成することが難しいため、不均一や欠陥3a、3bの分布を正確に予測することも難しい。したがって、周期分極反転構造を作製した基板上で、後工程で導波路が作製されることになる領域のできる限り近傍で、その構造を精度よく評価・検査するのが好ましい。
In order to maximize the wavelength conversion efficiency through quasi-phase matching in wavelength conversion elements, it is essential to have the technology to fabricate a periodically polarized structure as designed and to evaluate and inspect that structure with precision. Further, since it is difficult to form the periodically poled structure uniformly within the plane of the substrate (wafer), it is also difficult to accurately predict the distribution of non-uniformity and
図3は、検査工程において周期分極反転構造を観察する領域を示す図である。図3の(a)は、例えばLNウェファ14上に、周期分極反転構造の領域12が作製された状態を示している。図3では導波路が作製される前の状態を示しており、x方向に沿って、導波路が作製される予定の複数の領域13-1~13-5が示されている。図3は領域の説明のための模式図であって、周期分極反転構造の周期および導波路の幅、間隔は、正確でないことに留意されたい。例えば、実際のPPLN素子の作製工程では、3インチ基板内に数100本程度の導波路の作製が可能である。
FIG. 3 is a diagram showing a region where a periodically poled structure is observed in the inspection process. FIG. 3A shows a state in which a
上述のように、ウェファ上の周期分極反転構造に多数の導波路が作製される場合、できるだけ導波路の近傍で周期分極反転構造の評価・検査が実施されるのが好ましい。しかしながら、従来技術の周期分極反転構造の評価・検査では、後述するように破壊検査を伴うため、ウェファ上の周期分極反転構造の領域12の端部領域15でしか評価ができなかった。本来であれば、図3の(b)の周期分極反転構造の拡大図で示したように、欠陥部3c、3dなどの存在やその密度を観察可能として、周期分極反転構造の局所的な品質判断を容易にするのが好ましい。したがって、導波路の作製予定領域13-1の出来る限り近傍の検査領域15で評価ができることが望まれる。
As described above, when a large number of waveguides are fabricated in a periodically poled structure on a wafer, it is preferable to evaluate and inspect the periodically poled structure as close to the waveguide as possible. However, in the evaluation and inspection of the periodically poled structure in the prior art, since destructive testing is involved as will be described later, it was possible to evaluate only the
図4は、従来技術と本開示の周期分極反転構造の検査方法のフローを示す図である。図4の(a)は、従来技術の検査方法の一例を示すフロー図である。図4の(b)は、本開示の周期分極反転構造の検査方法の一例を示すフロー図であって、詳細は後述する。図4は、波長変換素子などの光学素子の製造工程における検査方法として示しているが、周期分極反転構造の観察方法、評価方法の側面も持っている点に留意されたい。図4の(a)のフロー図20は、図3の(a)に示したウェファの状態のように、例えばLN基板上に周期分極反転構造が作製された段階21から始まる。
FIG. 4 is a diagram showing the flow of a method for inspecting a periodically poled structure according to the prior art and the present disclosure. FIG. 4A is a flow diagram illustrating an example of a conventional inspection method. FIG. 4B is a flowchart showing an example of a method for inspecting a periodically poled structure according to the present disclosure, and the details will be described later. Although FIG. 4 is shown as an inspection method in the manufacturing process of an optical element such as a wavelength conversion element, it should be noted that it also has aspects of an observation method and an evaluation method for a periodic polarization inversion structure. The
LN結晶の周期分極反転構造を観察するためには、まず、導波路が作製される領域から離れた、ウェファ上の周期分極反転構造領域12のエッジにある図3の(a)の端部領域15を残して、他の導波路の作製予定の領域をマスキングする工程22が必要である。次工程におけるウェットエッチングによって、導波路を損傷させないためである。次に、フッ酸およびフッ硝酸を用いたウェットエッチング工程23において、端部領域15に対してエッチングを行う。周期分極反転構造では、結晶軸z方向の分極領域と-z軸方向の分極領域との間で、エッチングレートに差がある。エッチングレート差で生じた、基板厚さ方向におけるエッチング面の段差によって、不均一や欠陥の存在を可視化することができる。
In order to observe the periodically poled structure of the LN crystal, first, the end region of FIG. A
ウェットエッチング工程23が終了すると、マスキングの除去工程24を実施して、周期分極反転構造を観察する。観察工程25において、図2に示したような周期構造の不均一や欠陥が発見されれば、一定の基準によって、次工程である導波路構造の作製工程26に反映させる。例えば、一定基準よりも多い不均一や欠陥が発見されれば、そのウェファを破棄することもできる。
After the
図4の(a)に示した検査フローではウェットエッチング工程23が必須であるため、ウェファ上で実際に導波路を作製する結晶面の近傍のみで分極反転構造を観察することが非常に難しい。ウェットエッチング時には、検査する領域のみをフッ酸およびフッ硝酸に代表される溶液に浸漬する。導波路を作製する結晶面の近傍のみ選択的にエッチングするには、図4の(a)のようにウェットエッチングする領域より外をマスキングする工程22およびマスキングを除去する工程24が必須である。ウェットエッチングに伴うこれらの必須の工程は、周期分極反転構造の検査工程で大きな時間を占め、作業内容も煩雑で、コストと時間がかかってしまう。
In the inspection flow shown in FIG. 4(a), the
尚、図4の(a)に示した検査工程は、ウェファ上に作製された非線形光学素子を含む光回路をチップとしてダイシングして切り出す前に、導波路の近傍で周期分極反転構造の検査を実施する場合を示した。ウェファをチップ状にダイシングした後で、個々のチップに対して図4の(a)と同等の周期分極反転構造の検査を行う場合もある。 The inspection process shown in FIG. 4(a) involves inspecting the periodic polarization inversion structure near the waveguide before dicing and cutting out the optical circuit including the nonlinear optical element fabricated on the wafer as a chip. The case where this is implemented is shown. After dicing the wafer into chips, each chip may be inspected for a periodic polarization inversion structure similar to that shown in FIG. 4(a).
本開示の周期分極反転構造の検査方法では、従来技術における図4の(a)に示したような工程を大幅に簡略化して、より簡単に、導波路近傍の周期分極反転構造を可視化する。導波路近傍の観察をする必要がある場合に、波長変換素子などの光学素子の製造工程のスループットを向上させることもできる。 The method for inspecting a periodically poled structure of the present disclosure greatly simplifies the process shown in FIG. 4(a) in the prior art, and more easily visualizes the periodically poled structure near the waveguide. When it is necessary to observe the vicinity of a waveguide, it is also possible to improve the throughput of the manufacturing process of optical elements such as wavelength conversion elements.
[対象とする非線形光学材料]
本開示の周期分極反転構造の検査方法を利用できる非線形光学材料は、光波長400~2000nmにおいて透明である材料であればどのような材料でも良い。また、非線形光学材料は、非線形光学効果を有している限り、二次非線形光学効果であっても三次以上の非線形光学効果であっても良い。例として、前述のLN、LTの他に、ベータバリウムボライト(BBO)、リン酸チタニルカリウム(KTiOPO4、KTP)等が挙げられる。本開示の検査方法における非線形光学材料は、非線形光学効果増大のために周期分極反転構造を形成できる材料である。
[Target nonlinear optical materials]
The nonlinear optical material that can be used in the method of inspecting a periodically poled structure of the present disclosure may be any material as long as it is transparent at a light wavelength of 400 to 2000 nm. Further, the nonlinear optical material may have a second-order nonlinear optical effect or a third-order or higher nonlinear optical effect as long as it has a nonlinear optical effect. Examples include, in addition to the above-mentioned LN and LT, beta-barium bolite (BBO), potassium titanyl phosphate (KTiOPO 4 , KTP), and the like. The nonlinear optical material in the inspection method of the present disclosure is a material that can form a periodically poled structure to increase the nonlinear optical effect.
[周期分極反転構造の検査装置]
図5は、本開示の周期反転分極構造の検査方法の一部を担う検査装置の構成を示す図である。検査装置40は、真空チャンバー41内に、検査対象の試料44を配置したドライエッチング装置である。チャンバー41は、真空ポンプ50によって真空状態へ排気するとともに、ボンベ46から、エッチングガス47がチャンバー内に導入される。エッチングガスとしては主にアルゴンやCF系のガスが用いられ、エッチング対象の材料に応じたガスが用いられる。試料44は、3次元に駆動可能なステージ42上に、静電チャック43を介して固定される。試料44の上方には、真空ポンプ50に接続された絶縁物のキャピラリ45がある。エッチングガスは、チャンバー内圧力(V2)とキャピラリ内圧力(V1)の差圧によりキャピラリ内部へと流入し、真空ポンプで排気される。
[Inspection device for periodically polarized structure]
FIG. 5 is a diagram showing the configuration of an inspection device that plays a part in the inspection method for a periodically inverted polarization structure of the present disclosure. The
チャンバーの外のキャピラリの周囲には高周波コイル48が設置されており、高周波電源49から高周波コイル48へ高電圧を印可することで、キャピラリからチャンバー内にかけてプラズマを発生させる。プラズマの一部はキャピラリ45の入り口側(試料側)にも発生しており、例えば、数mm程度までプラズマの径を絞ることができる。このプラズマの径はキャピラリの内径に依存し、キャピラリの形状や材料条件によって制御可能である。また図5の検査装置40は模式図であって、におけるキャピラリの長さや、高周波コイル48、試料44との相対位置、距離は実際とは異なることに留意されたい。
A high-
図5の構成の検査装置40における、試料44の表面で局所的に発生したプラズマにより、周期分極反転構造上の任意の所望の位置で、局所的にドライエッチングをすることが可能になる。図5に示した検査装置40では、試料44に対して静電チャックを用いることで、試料の分極方向に依存した表面電位を、試料に発生させることで、分極方向に依存したエッチングレートを実現する。図5における試料44は、導波路作製の前のウェファでも良いし、切断されたチップであっても良い。
In the
図6は、周期反転分極構造の表面近傍におけるドライエッチングの様子を示した図である。静電チャック43で固定された試料44の断面(x-z面)を見ており、図6の(a)はドライエッチング開始前、(b)はドライエッチング中で、エッチングガスの流れを模式的に示している。図6の(a)のドライエッチング開始前では、z軸におけるキャピラリ45の垂直位置が基板表面から離れており、プラズマも基板表面から離れている。図6の(b)のようにキャピラリ45が基板近傍まで下り、一定範囲に制限されたプラズマが表面に達すると、局所的なドライエッチングが始まる。エッチングガスは、キャピラリ45の内外の圧力差(V1、V2)によって、キャピラリの外から内側へ常に供給される。
FIG. 6 is a diagram showing the state of dry etching near the surface of the periodically reversed polarization structure. The cross section (xz plane) of the
図6の(c)は、ドライエッチング時の周期反転分極構造の表面近傍の電位を説明する図である。周期反転分極構造では、z軸方向の上向きの分極(上向き矢印)が生じる領域と、z軸方向の下向きの分極(下向き矢印)が生じる領域とが、x軸に沿って交互に形成されている。このとき、基板の最表面において、正の電荷を持つ領域と、負の電荷を持つ領域とが交互に現れる。したがって、基板表面の電位は、x軸方向に周期的に変動することになる。基板の最表面にあるエッチングガス47a、47bの分子と、電位分布が変動する非線形光学材料との反応性が変化するため、x軸の位置によって異なるエッチングレートが生まれる。
FIG. 6(c) is a diagram illustrating the potential near the surface of the periodically reversed polarization structure during dry etching. In a periodically reversed polarization structure, regions where upward polarization in the z-axis direction (upward arrow) occurs and regions where downward polarization in the z-axis direction (downward arrow) occur are formed alternately along the x-axis. . At this time, positively charged regions and negatively charged regions alternately appear on the outermost surface of the substrate. Therefore, the potential on the substrate surface changes periodically in the x-axis direction. Since the reactivity between the molecules of the
図7は、ドライエッチングで得られる周期反転分極構造の模様を説明する図である。図7の(a)に示したように、ウェファ14上に周期反転分極構造の領域12が形成されている。導波路は、x軸方向に沿って形成されることになる。図6で説明した、分極方向に依存したエッチングレートでエッチングガスとの反応が進むと、分極方向に依存した凹凸パターンが表面に局所的に発生する。x軸方向に沿って連続的にドライエッチングをできれば、図7の(b)に示したように、x軸方向に分極構造の周期ピッチで高さの凹凸パターンが現れる。分極方向に依存したこの凹凸パターンを光学顕微鏡や段差測定系に代表される各種測定器で観察することにより、局所的に周期分極反転構造を可視化することができる。
FIG. 7 is a diagram illustrating the pattern of a periodically reversed polarization structure obtained by dry etching. As shown in FIG. 7(a), a
[周期分極反転構造の検査方法の手順]
図8は、導波路に沿った局所的ドライエッチングによる周期反転分極構造の検査を説明する図である。図5に示した検査装置40で試料を保持するステージ42は、少なくとも水平方向(x方向)に対して移動することができる。装置40に固定されたキャピラリ45に対して、試料44の水平面内の位置を決定する移動可能なステージ42によって、基板面上の任意の位置で局所的なドライエッチングを実施できる。例えば図8において、光の伝搬方向18と平行なx軸方向に、ステージ42を移動(掃引、スキャン)させることで、概ね円形のエッチング領域16が掃引され、ライン状にエッチングが可能となる。ライン状に加工する領域17を、波長変換素子の導波路を作製予定の領域13-1に対して平行にすることで、波長変換素子の光の伝搬方向に沿って周期分極反転構造を可視化できる。ウェファ内において何か所のエッチングを行うかにも依るが、図5の検査装置40で局所エッチングに掛かる時間は長くても1時間程度である。
[Procedure of inspection method for periodically poled structure]
FIG. 8 is a diagram illustrating inspection of a periodically reversed polarization structure by local dry etching along a waveguide. A
図4の(b)を再び参照すれば、本開示の周期分極反転構造の検査方法のフロー図30が、(a)の従来技術の検査方法のフロー図と対比して示されている。フロー図30から明らかなように、本開示の周期分極反転構造の検査方法では、局所ドライエッチング32の前のマスキング工程も、マスキングの除去工程も不要である。したがって、従来技術のウェットエッチングを用いた検査フロー20と比べて、煩雑な作業工程が省略されて、導波路近傍の観察をする必要がある場合にスループットを向上させることができる。周期分極反転構造を観察・検査する作業時間、コストが大幅に短縮され、波長変換素子の評価、製造を効率的に行うことができる。
Referring again to FIG. 4(b), a
また、図4の(b)の検査方法では、要求される品質レベルに応じて、局所エッチングを行う箇所の位置や数を変更可能であり、ウェファ上の良好な部分だけを次工程に利用するような判断情報も提供できる。 In addition, in the inspection method shown in FIG. 4(b), the location and number of areas to be locally etched can be changed depending on the required quality level, and only good areas on the wafer can be used in the next process. It is also possible to provide such judgment information.
導波路近傍の周期分極構造の観察を容易とし、周期分極反転構造を含む光デバイスの製造工程で導波路近傍の検査をする必要がある場合のスループットを向上させ、非線形光学素子の開発の効率化を実現する。 Easily observe periodic polarization structures near waveguides, improve throughput when it is necessary to inspect the vicinity of waveguides in the manufacturing process of optical devices that include periodic polarization inversion structures, and improve efficiency in the development of nonlinear optical elements. Realize.
本発明は、光デバイスの製造や開発に利用できる。 The present invention can be used for manufacturing and developing optical devices.
Claims (3)
前記基板を、静電チャックを介して、ステージに固定するステップと、
ドライエッチングによって、キャピラリの開口部の近傍で、前記周期分極反転構造の検査領域を選択的にエッチングするステップと、
前記ドライエッチングに形成された、分極方向に応じた凹凸に基づいて、前記検査領域における前記周期分極反転構造の不均一または欠陥を判定するステップと
を備える方法。 A method for inspecting a periodically poled structure created on a substrate, the method comprising:
fixing the substrate to a stage via an electrostatic chuck;
selectively etching the inspection region of the periodically poled structure near the opening of the capillary by dry etching;
and determining non-uniformity or defects in the periodically poled structure in the inspection area based on the unevenness formed in the dry etching that corresponds to the polarization direction.
前記基板上で、導波路の作製予定領域に平行に前記検査領域を掃引するステップ
をさらに備える請求項1に記載の方法。 The stage is movable in a horizontal direction with respect to the opening of the capillary,
2. The method according to claim 1, further comprising: sweeping the inspection area on the substrate in parallel to a region where a waveguide is to be formed.
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Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6211999B1 (en) * | 1998-10-30 | 2001-04-03 | The Regents Of The University Of California | Lithium tantalate single-crystal and photo-functional device |
| WO2011045893A1 (en) * | 2009-10-16 | 2011-04-21 | パナソニック株式会社 | Method for manufacturing optical element |
| JP2017134110A (en) * | 2016-01-25 | 2017-08-03 | 株式会社島津製作所 | Polarization reversing element, method for manufacturing polarization reversing element, and device for manufacturing polarization reversing element |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6211999B1 (en) * | 1998-10-30 | 2001-04-03 | The Regents Of The University Of California | Lithium tantalate single-crystal and photo-functional device |
| WO2011045893A1 (en) * | 2009-10-16 | 2011-04-21 | パナソニック株式会社 | Method for manufacturing optical element |
| JP2017134110A (en) * | 2016-01-25 | 2017-08-03 | 株式会社島津製作所 | Polarization reversing element, method for manufacturing polarization reversing element, and device for manufacturing polarization reversing element |
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