CN113687530B - Silicon-based electro-optic modulator and preparation method thereof - Google Patents
Silicon-based electro-optic modulator and preparation method thereof Download PDFInfo
- Publication number
- CN113687530B CN113687530B CN202111017879.7A CN202111017879A CN113687530B CN 113687530 B CN113687530 B CN 113687530B CN 202111017879 A CN202111017879 A CN 202111017879A CN 113687530 B CN113687530 B CN 113687530B
- Authority
- CN
- China
- Prior art keywords
- layer
- silicon
- waveguide
- silicon dioxide
- buried
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Active
Links
Classifications
-
- 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
- G02F1/01—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 for the control of the intensity, phase, polarisation or colour
- G02F1/03—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 for the control of the intensity, phase, polarisation or colour based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect
- G02F1/035—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 for the control of the intensity, phase, polarisation or colour based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect in an optical waveguide structure
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B6/13—Integrated optical circuits characterised by the manufacturing method
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B6/13—Integrated optical circuits characterised by the manufacturing method
- G02B6/134—Integrated optical circuits characterised by the manufacturing method by substitution by dopant atoms
- G02B6/1347—Integrated optical circuits characterised by the manufacturing method by substitution by dopant atoms using ion implantation
-
- 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
- G02F1/365—Non-linear optics in an optical waveguide structure
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B2006/12083—Constructional arrangements
- G02B2006/12097—Ridge, rib or the like
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B2006/12133—Functions
- G02B2006/12142—Modulator
Landscapes
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Engineering & Computer Science (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Chemical & Material Sciences (AREA)
- Ceramic Engineering (AREA)
- Crystallography & Structural Chemistry (AREA)
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
- Optical Integrated Circuits (AREA)
Abstract
Description
技术领域Technical field
本发明涉及一种硅基电光调制器及其制备方法。The invention relates to a silicon-based electro-optical modulator and a preparation method thereof.
背景技术Background technique
硅基具有尺寸小、能耗低、CMOS工艺兼容以及便于与现有的电子器件和光子器件实现单片、微纳集成等优点,利用硅基实现光的产生、调制、传输、操控以及探测等功能的硅光子学,已被公认为突破计算机和通信超大容量、超高速信息传输和处理瓶颈的理想技术之一,硅光子学受到研究者的高度关注,成为近年光电子研究领域的热点。目前,基于硅基的关键器件,如拉曼激光器、电光调制器、光电探测器、波长转换、光逻辑门、码型转换、光滤波等已经被提出,促进了硅基光子学的发展,这些研究成果在光通信、光传感等领域获得广泛应用,并且还在光子集成、光互连以及光计算等方面呈现出诱人前景。Silicon base has the advantages of small size, low energy consumption, CMOS process compatibility, and ease of monolithic and micro-nano integration with existing electronic devices and photonic devices. Silicon base is used to achieve light generation, modulation, transmission, control, and detection. Functional silicon photonics has been recognized as one of the ideal technologies to break through the bottleneck of ultra-large capacity and ultra-high-speed information transmission and processing in computers and communications. Silicon photonics has attracted great attention from researchers and has become a hot spot in the field of optoelectronics research in recent years. At present, key devices based on silicon, such as Raman lasers, electro-optical modulators, photodetectors, wavelength conversion, optical logic gates, code conversion, optical filtering, etc., have been proposed, promoting the development of silicon-based photonics. Research results have been widely used in fields such as optical communications and optical sensing, and also present attractive prospects in photonic integration, optical interconnection, and optical computing.
硅电光调制器是硅基器件中最关键的器件,起到将电信号转换为光信号的重要作用。然而硅具有中心反演对称性晶体结构,其本身不具有二阶非线性极化率χ(2),因而硅不具有电光调制特性(Pockels效应)。硅电光调制器一般都是基于等离子色散效应,通过掺杂引起自由载流子的注入、积累或者耗尽,改变自由载流子浓度而使硅的折射率发生变化,从而起到调制的作用。基于等离子色散效应的硅电光调制器的带宽受限于载流子运输时间很难再提高,并且掺杂致使调制速度以及非线性下降以及带来插入损耗。Silicon electro-optical modulator is the most critical device among silicon-based devices, playing an important role in converting electrical signals into optical signals. However, silicon has a central inversion symmetry crystal structure and does not have a second-order nonlinear polarizability χ (2) . Therefore, silicon does not have electro-optical modulation properties (Pockels effect). Silicon electro-optical modulators are generally based on the plasma dispersion effect, which causes the injection, accumulation or depletion of free carriers through doping, changing the free carrier concentration to change the refractive index of silicon, thus playing a modulation role. The bandwidth of silicon electro-optical modulators based on the plasmon dispersion effect is limited by the carrier transport time and is difficult to increase, and doping causes the modulation speed and nonlinearity to decrease and causes insertion loss.
发明内容Contents of the invention
针对上述问题,本发明提供一种硅基电光调制器及其制备方法。To address the above problems, the present invention provides a silicon-based electro-optical modulator and a preparation method thereof.
本发明的一个方面,提供一种硅基电光调制器,包括:SOI晶圆,SOI 晶圆为多层结构,自下而上依次为硅衬底、第一二氧化硅埋层、顶部硅层;第二二氧化硅埋层,埋设于顶部硅层中,将顶部硅层分割为上下两层,上层为第一硅层,下层为波导层,其中,第二二氧化硅埋层一部分向上凸起,使得下方波导层形成脊形结构,脊形结构的向上凸起部分为硅波导,第二二氧化硅埋层内部存在压应力,向外挤压第一硅层及波导层;GSG单驱动共面波导行波电极,设置于第一硅层上,使得GSG单驱动共面波导行波电极施加的电场可以到达硅波导。One aspect of the present invention provides a silicon-based electro-optical modulator, including: an SOI wafer. The SOI wafer has a multi-layer structure, and from bottom to top is a silicon substrate, a first silicon dioxide buried layer, and a top silicon layer. ; The second buried silicon dioxide layer is buried in the top silicon layer. The top silicon layer is divided into upper and lower layers. The upper layer is the first silicon layer and the lower layer is the waveguide layer. Part of the second buried silicon dioxide layer protrudes upward. rise, causing the waveguide layer below to form a ridge structure. The upward convex part of the ridge structure is the silicon waveguide. There is compressive stress inside the second buried silicon dioxide layer, which squeezes the first silicon layer and the waveguide layer outward; GSG single drive The coplanar waveguide traveling wave electrode is disposed on the first silicon layer so that the electric field applied by the GSG single-driven coplanar waveguide traveling wave electrode can reach the silicon waveguide.
本发明的另一个方面,提供一种硅基电光调制器制备方法,包括:选择SOI晶圆,SOI晶圆为多层结构,自下而上依次为硅衬底、第一二氧化硅埋层、顶部硅层;在顶部硅层中制备第二二氧化硅埋层,将顶部硅层分割为上下两层,上层为第一硅层,下层为波导层,其中,第二二氧化硅埋层一部分向上凸起,使得下方波导层形成脊形结构,脊形结构的向上凸起部分为硅波导,第二二氧化硅埋层内部存在压应力,向外挤压第一硅层及波导层;在第一硅层上设置GSG单驱动共面波导行波电极,使得GSG 单驱动共面波导行波电极施加的电场可以到达硅波导。Another aspect of the present invention provides a method for preparing a silicon-based electro-optical modulator, which includes: selecting an SOI wafer. The SOI wafer has a multi-layer structure, and from bottom to top is a silicon substrate and a first buried silicon dioxide layer. , top silicon layer; prepare a second buried silicon dioxide layer in the top silicon layer, divide the top silicon layer into upper and lower layers, the upper layer is the first silicon layer, and the lower layer is the waveguide layer, wherein the second buried silicon dioxide layer A part of it bulges upward, causing the waveguide layer below to form a ridge structure. The upward bulge part of the ridge structure is a silicon waveguide. There is compressive stress inside the second buried silicon dioxide layer, which squeezes the first silicon layer and the waveguide layer outward; A GSG single-driven coplanar waveguide traveling wave electrode is arranged on the first silicon layer, so that the electric field applied by the GSG single-driven coplanar waveguide traveling wave electrode can reach the silicon waveguide.
进一步地,本发明的一种硅基电光调制器制备方法,制备第二二氧化硅埋层包括:在顶部硅层上表面进行热氧化反应,使得顶部硅层上部形成第一二氧化硅层;将掩膜版图案转移至第一二氧化硅层,按照掩膜版图案刻蚀第一二氧化硅层,得到二氧化硅波导;在二氧化硅波导及因刻蚀暴露出的顶部硅层表面沉积二氧化硅,形成厚度一定的第二二氧化硅层;自上向下将氧离子透过第二二氧化硅层及二氧化硅波导注入到顶部硅层中,形成富氧离子层,其中,富氧离子层在二氧化硅波导下方的部分向上凸起;高温退火使得富氧离子层中的氧离子与富氧离子层中的硅原子发生反应,生成第二二氧化硅埋层。Further, in the silicon-based electro-optical modulator preparation method of the present invention, preparing the second buried silicon dioxide layer includes: performing a thermal oxidation reaction on the upper surface of the top silicon layer, so that a first silicon dioxide layer is formed on the upper part of the top silicon layer; Transfer the mask pattern to the first silicon dioxide layer, and etch the first silicon dioxide layer according to the mask pattern to obtain a silicon dioxide waveguide; on the surface of the silicon dioxide waveguide and the top silicon layer exposed by etching Deposit silicon dioxide to form a second silicon dioxide layer with a certain thickness; inject oxygen ions from top to bottom through the second silicon dioxide layer and the silicon dioxide waveguide into the top silicon layer to form an oxygen ion-rich layer, where , the part of the oxygen-rich ion layer below the silicon dioxide waveguide bulges upward; high-temperature annealing causes the oxygen ions in the oxygen-rich ion layer to react with the silicon atoms in the oxygen-rich ion layer to generate a second buried silicon dioxide layer.
进一步地,本发明的一种硅基电光调制器制备方法,高温退火之前,包括:刻蚀第二二氧化硅层及二氧化硅波导,以使暴露出顶部硅层;在顶部硅层上沉积高密度二氧化硅保护层,以防止顶部硅层被氧化。Further, the method for preparing a silicon-based electro-optical modulator of the present invention, before high-temperature annealing, includes: etching the second silicon dioxide layer and the silicon dioxide waveguide to expose the top silicon layer; depositing on the top silicon layer High-density silicon dioxide protective layer to prevent the top silicon layer from being oxidized.
进一步地,本发明的一种硅基电光调制器制备方法,高温退火之后,刻蚀高密度二氧化硅保护层,以使暴露出第一硅层。Furthermore, according to a method for preparing a silicon-based electro-optical modulator of the present invention, after high-temperature annealing, the high-density silicon dioxide protective layer is etched to expose the first silicon layer.
进一步地,本发明的一种硅基电光调制器制备方法,顶部硅层厚度为 600nm。Further, according to the silicon-based electro-optical modulator preparation method of the present invention, the thickness of the top silicon layer is 600nm.
进一步地,本发明的一种硅基电光调制器制备方法,第一二氧化硅层厚度为100nm。Further, according to the silicon-based electro-optical modulator preparation method of the present invention, the thickness of the first silicon dioxide layer is 100 nm.
进一步地,本发明的一种硅基电光调制器制备方法,第二二氧化硅层厚度为50nm。Further, according to the silicon-based electro-optical modulator preparation method of the present invention, the thickness of the second silicon dioxide layer is 50 nm.
进一步地,本发明的一种硅基电光调制器制备方法,氧离子注入总剂量范围为2×1017~7×1017/cm2,氧离子注入能量范围为150-200KeV。Furthermore, according to the silicon-based electro-optical modulator preparation method of the present invention, the total dose of oxygen ion implantation ranges from 2×10 17 to 7×10 17 /cm 2 , and the energy range of oxygen ion injection ranges from 150 to 200KeV.
进一步地,本发明的一种硅基电光调制器制备方法,高温退火温度为 1200℃,时间为2~3小时。Furthermore, according to the silicon-based electro-optical modulator preparation method of the present invention, the high-temperature annealing temperature is 1200°C and the time is 2 to 3 hours.
本发明具有如下有益效果:The invention has the following beneficial effects:
(1)通过氧离子注入与高温退火,将波导图案转移至埋层,形成埋层脊形硅波导结构,通过高温退火温度与时间的控制,调节脊形硅波导中的应力水平,打破硅的中心反演对称结构,在脊形硅波导中诱导出二阶非线性极化率χ(2),从而使脊形硅波导具有电光调制特性,实现高速电光调制器,克服了常规硅电光调制器的带宽受限于载流子运输时间很难再提高的问题。(1) Through oxygen ion implantation and high-temperature annealing, the waveguide pattern is transferred to the buried layer to form a buried-layer ridge silicon waveguide structure. By controlling the high-temperature annealing temperature and time, the stress level in the ridge silicon waveguide is adjusted to break the silicon The central inversion symmetry structure induces a second-order nonlinear polarizability χ (2) in the ridge silicon waveguide, thereby giving the ridge silicon waveguide electro-optical modulation characteristics and realizing a high-speed electro-optic modulator, overcoming the conventional silicon electro-optic modulator. The bandwidth is limited by the problem that the carrier transport time is difficult to improve.
(2)利用埋层脊形硅波导结构中的二阶非线性极化率实现电光调制,埋层脊形硅波导结构通过将波导图案转移至埋层而形成,避免了常规硅电光调制器中制备硅波导方案刻蚀所带来的侧壁粗糙度高与离子注入而导致的插入损耗大的问题,因而插入损耗小。(2) Electro-optical modulation is achieved by utilizing the second-order nonlinear polarizability in the buried-layer ridge silicon waveguide structure. The buried-layer ridge silicon waveguide structure is formed by transferring the waveguide pattern to the buried layer, avoiding the problems encountered in conventional silicon electro-optical modulators. The problem of high sidewall roughness caused by etching and high insertion loss caused by ion implantation in preparing silicon waveguides, so the insertion loss is small.
(3)硅电光调制器处于埋层中,第一硅层可用于制备其它光电器件,从而可实现3D光子集成。(3) The silicon electro-optical modulator is in the buried layer, and the first silicon layer can be used to prepare other optoelectronic devices, thereby enabling 3D photonic integration.
附图说明Description of the drawings
图1是本发明的硅基电光调制器的结构示意图;Figure 1 is a schematic structural diagram of the silicon-based electro-optical modulator of the present invention;
图2是本发明的硅基电光调制器制备方法流程示意图;Figure 2 is a schematic flow chart of the silicon-based electro-optical modulator preparation method of the present invention;
图3是本发明一些实施例的硅基电光调制器制备方法在制备第二二氧化硅埋层时的流程示意图;Figure 3 is a schematic flow chart of the preparation method of the silicon-based electro-optical modulator in preparing the second silicon dioxide buried layer according to some embodiments of the present invention;
图4是本发明一个实施例的硅基电光调制器制备方法步骤示意图;Figure 4 is a schematic diagram of the steps of a silicon-based electro-optical modulator preparation method according to one embodiment of the present invention;
图5是本发明一个实施例的硅基电光调制器的光场与电场分布图。Figure 5 is a light field and electric field distribution diagram of a silicon-based electro-optical modulator according to an embodiment of the present invention.
图中:In the picture:
1-硅衬底;2-第一二氧化硅埋层;3-顶部硅层;4-第二二氧化硅埋层;5-第一硅层;6-波导层;7-硅波导;8-GSG单驱动共面波导行波电极;9- 第一二氧化硅层;10-二氧化硅波导;11-第二二氧化硅层;12-富氧离子层; 13-高密度二氧化硅保护层。1-Silicon substrate; 2-First buried silicon dioxide layer; 3-Top silicon layer; 4-Second buried silicon dioxide layer; 5-First silicon layer; 6-Waveguide layer; 7-Silicon waveguide; 8 -GSG single-driven coplanar waveguide traveling wave electrode; 9- first silicon dioxide layer; 10- silicon dioxide waveguide; 11- second silicon dioxide layer; 12- oxygen-rich ion layer; 13- high-density silicon dioxide The protective layer.
具体实施方式Detailed ways
为使本发明的目的、技术方案和优点更加清楚明白,以下结合具体实施例,并参照附图,对本发明进一步详细说明。In order to make the purpose, technical solutions and advantages of the present invention more clear, the present invention will be further described in detail below with reference to specific embodiments and the accompanying drawings.
如图1所示为本发明的硅基电光调制器结构示意图。Figure 1 shows a schematic structural diagram of the silicon-based electro-optical modulator of the present invention.
本发明的硅基电光调制器包括SOI(Silicon-On-Insulator,绝缘衬底上的硅)晶圆,该SOI晶圆为多层结构,自下而上依次为硅衬底1、第一二氧化硅埋层2、顶部硅层3。在顶部硅层3中埋设有第二二氧化硅埋层4,使得第二二氧化硅埋层4将顶部硅层3分割为上下两层,上层为第一硅层 5,下层为波导层6。其中,第二二氧化硅埋层4一部分向上凸起,使得下方波导层6形成脊形结构,脊形结构的向上凸起部分为硅波导7。The silicon-based electro-optical modulator of the present invention includes an SOI (Silicon-On-Insulator, silicon on an insulating substrate) wafer. The SOI wafer has a multi-layer structure. From bottom to top, there are silicon substrate 1, first and second Silicon oxide buried layer 2 and top silicon layer 3. A second buried silicon dioxide layer 4 is buried in the top silicon layer 3, so that the second buried silicon dioxide layer 4 divides the top silicon layer 3 into two upper and lower layers. The upper layer is the first silicon layer 5, and the lower layer is the waveguide layer 6. . Among them, a part of the second silicon dioxide buried layer 4 is convex upward, so that the lower waveguide layer 6 forms a ridge structure, and the upward convex part of the ridge structure is the silicon waveguide 7 .
第二二氧化硅埋层4内部存在压应力,向外挤压第一硅层5及波导层 6,使得硅波导7左上角及右上角因受挤压而引起原子排列结构改变,在硅波导7中诱导出二阶非线性极化率。There is compressive stress inside the second silicon dioxide buried layer 4, which squeezes the first silicon layer 5 and the waveguide layer 6 outward, so that the upper left corner and the upper right corner of the silicon waveguide 7 are squeezed, causing the atomic arrangement structure to change. In the silicon waveguide 7, the second-order nonlinear polarizability is induced.
GSG单驱动共面波导行波电极8设置于第一硅层5上,使得GSG单驱动共面波导行波电极8施加的电场可以到达硅波导7。The GSG single-driven coplanar waveguide traveling wave electrode 8 is disposed on the first silicon layer 5 so that the electric field applied by the GSG single-driven coplanar waveguide traveling wave electrode 8 can reach the silicon waveguide 7 .
下面介绍本发明的硅基电光调制器制备方法。如图2是本发明的硅基电光调制器制备方法流程示意图,包括:The preparation method of the silicon-based electro-optical modulator of the present invention is introduced below. Figure 2 is a schematic flow chart of the silicon-based electro-optical modulator preparation method of the present invention, which includes:
S201,选择SOI晶圆,SOI晶圆为多层结构,自下而上依次为硅衬底1、第一二氧化硅埋层2、顶部硅层3。顶部硅层3的厚度优选为600nm。S201, select an SOI wafer. The SOI wafer has a multi-layer structure, consisting of silicon substrate 1, first silicon dioxide buried layer 2, and top silicon layer 3 from bottom to top. The thickness of the top silicon layer 3 is preferably 600 nm.
S202,在顶部硅层3中制备第二二氧化硅埋层4,将顶部硅层3分割为上下两层,上层为第一硅层5,下层为波导层6。S202, prepare a second buried silicon dioxide layer 4 in the top silicon layer 3, and divide the top silicon layer 3 into upper and lower layers. The upper layer is the first silicon layer 5, and the lower layer is the waveguide layer 6.
在步骤S202,制备的第二二氧化硅埋层4一部分向上凸起,使得下方波导层6形成脊形结构,脊形结构的向上凸起部分为硅波导7。In step S202, a portion of the prepared second silicon dioxide buried layer 4 is convex upward, so that the lower waveguide layer 6 forms a ridge structure, and the upward convex part of the ridge structure is the silicon waveguide 7.
第二二氧化硅埋层4内部存在压应力,向外挤压第一硅层5及波导层 6,使得硅波导7左上角及右上角因受挤压而引起原子排列结构改变,在硅波导7中诱导出二阶非线性极化率。There is compressive stress inside the second silicon dioxide buried layer 4, which squeezes the first silicon layer 5 and the waveguide layer 6 outward, so that the upper left corner and the upper right corner of the silicon waveguide 7 are squeezed, causing the atomic arrangement structure to change. In the silicon waveguide 7, the second-order nonlinear polarizability is induced.
S203,在第一硅层5上设置GSG单驱动共面波导行波电极8,使得 GSG单驱动共面波导行波电极8施加的电场可以到达硅波导7。在一些实施例中,本发明采用蒸镀或电镀的方式将GSG单驱动共面波导行波电极8 连接到第一硅层5上。S203, set the GSG single-driven coplanar waveguide traveling wave electrode 8 on the first silicon layer 5, so that the electric field applied by the GSG single-driven coplanar waveguide traveling wave electrode 8 can reach the silicon waveguide 7. In some embodiments, the present invention uses evaporation or electroplating to connect the GSG single-driven coplanar waveguide traveling wave electrode 8 to the first silicon layer 5 .
如图3是本发明一些实施例的硅基电光调制器制备方法在制备第二二氧化硅埋层时的流程示意图。本发明的一些实施例,在制备第二二氧化硅埋层4时还包括:Figure 3 is a schematic flowchart of the preparation method of the silicon-based electro-optical modulator in preparing the second buried silicon dioxide layer according to some embodiments of the present invention. In some embodiments of the present invention, preparing the second buried silicon dioxide layer 4 also includes:
S2021,在顶部硅层3上表面进行热氧化反应,使得顶部硅层3上部形成第一二氧化硅层9。第一二氧化硅层9的厚度优选为100nm。S2021, perform a thermal oxidation reaction on the upper surface of the top silicon layer 3, so that the first silicon dioxide layer 9 is formed on the top of the top silicon layer 3. The thickness of the first silicon dioxide layer 9 is preferably 100 nm.
S2022,将掩膜版图案转移至第一二氧化硅层9,按照掩膜版图案刻蚀第一二氧化硅层9,得到二氧化硅波导10。刻蚀可采用等离子刻蚀、反应离子刻蚀等干法刻蚀,或者采用湿法刻蚀。S2022, transfer the mask pattern to the first silicon dioxide layer 9, and etch the first silicon dioxide layer 9 according to the mask pattern to obtain the silicon dioxide waveguide 10. Etching can use dry etching such as plasma etching, reactive ion etching, or wet etching.
S2023,在二氧化硅波导10及因刻蚀暴露出的顶部硅层3表面沉积二氧化硅,形成厚度一定的第二二氧化硅层11。沉积二氧化硅可采用等离子体增强化学(PECVD)的气相沉积,沉积厚度为50nm。S2023, deposit silicon dioxide on the surface of the silicon dioxide waveguide 10 and the top silicon layer 3 exposed by etching to form a second silicon dioxide layer 11 with a certain thickness. Silicon dioxide can be deposited using plasma enhanced chemical vapor deposition (PECVD) with a deposition thickness of 50nm.
S2024,自上向下将氧离子透过第二二氧化硅层11及二氧化硅波导10 注入到顶部硅层3中,形成富氧离子层12,其中,富氧离子层12在二氧化硅波导10下方的部分向上凸起。S2024, inject oxygen ions from top to bottom through the second silicon dioxide layer 11 and the silicon dioxide waveguide 10 into the top silicon layer 3 to form an oxygen ion-rich layer 12, wherein the oxygen ion-rich layer 12 is in the silicon dioxide layer. The lower part of the waveguide 10 is raised upward.
在步骤S2024,在注入氧离子时,由于第二二氧化硅层11及二氧化硅波导10在顶部硅层3上方形成的二氧化硅阻挡层厚度不一,使得注入氧离子时在二氧化硅波导10下方的部分位置比其他位置注入更浅,因此形成的富氧离子层12在二氧化硅波导10下方的部分向上凸起。In step S2024, when oxygen ions are implanted, since the thickness of the silicon dioxide barrier layer formed by the second silicon dioxide layer 11 and the silicon dioxide waveguide 10 above the top silicon layer 3 is different, the thickness of the silicon dioxide barrier layer is different when the oxygen ions are implanted. The portion below the waveguide 10 is implanted more shallowly than other locations, so the formed oxygen ion-rich layer 12 bulges upward in the portion below the silicon dioxide waveguide 10 .
在一些实施例中,氧离子注入的总剂量范围为2×1017~7×1017/cm2,氧离子注入能量范围为150-200KeV。In some embodiments, the total dose of oxygen ion implantation ranges from 2×10 17 to 7×10 17 /cm 2 , and the oxygen ion implantation energy ranges from 150-200KeV.
在一些实施例中,为了使得富氧离子层12中的氧离子分布均匀,每次注入总剂量的1/4,然后将SOI晶圆绕晶圆圆心向某一方向旋转90°,重复注入氧离子并向同一方向将SOI晶圆绕晶圆圆心旋转90°,直至将所有氧离子均匀注入到顶部硅层3中。In some embodiments, in order to make the distribution of oxygen ions in the oxygen-rich layer 12 uniform, 1/4 of the total dose is injected each time, and then the SOI wafer is rotated 90° in a certain direction around the center of the wafer, and oxygen is injected repeatedly. ions and rotate the SOI wafer 90° around the center of the wafer in the same direction until all oxygen ions are evenly implanted into the top silicon layer 3.
S2025,高温退火使得富氧离子层12中的氧离子与富氧离子层12中的硅原子发生反应,生成第二二氧化硅埋层4。S2025 , high-temperature annealing causes oxygen ions in the oxygen-ion-rich layer 12 to react with silicon atoms in the oxygen-ion-rich layer 12 to generate the second silicon dioxide buried layer 4 .
在步骤S2025,高温退火使得富氧离子层12中位于硅原子间隙中的氧离子与此位置处原本的硅原子发生反应,形成均匀的第二二氧化硅埋层4。由于富氧离子层12存在部分向上凸起,使得反应生成的第二二氧化硅埋层4也有相应的一部分向上凸起。此时下方波导层6形成脊形结构,脊形结构的向上凸起部分为硅波导7。In step S2025, high-temperature annealing causes the oxygen ions located in the gaps between silicon atoms in the oxygen ion-rich layer 12 to react with the original silicon atoms at the positions to form a uniform second silicon dioxide buried layer 4. Since the oxygen ion-rich layer 12 has a portion that bulges upward, a corresponding portion of the second silicon dioxide buried layer 4 generated by the reaction also bulges upward. At this time, the lower waveguide layer 6 forms a ridge structure, and the upward convex part of the ridge structure is the silicon waveguide 7 .
由于由于硅和二氧化硅具有不同的摩尔体积(molar volume),硅的摩尔体积是12.17cm3/mol,二氧化硅的摩尔体积是27.27cm3/mol,所以当富氧离子层12中的氧离子与硅原子发生反应,形成均匀的第二二氧化硅埋层4时,会使该处体积膨胀2.2倍。体积膨胀会使第二二氧化硅埋层4内部产生压应力,压缩周围物质,如压缩第一硅层5与波导层6。由于波导层6是脊形结构,第二二氧化硅埋层4的体积膨胀可以压缩硅波导7左上角与右上角,引起硅波导7内部原子排列结构改变,打破硅的中心反演对称结构,在硅中诱导出二阶非线性极化率。Since silicon and silicon dioxide have different molar volumes, the molar volume of silicon is 12.17cm 3 /mol and the molar volume of silicon dioxide is 27.27cm 3 /mol, so when the molar volume in the oxygen-rich layer 12 When oxygen ions react with silicon atoms to form a uniform second silicon dioxide buried layer 4, the volume there will expand 2.2 times. Volume expansion will generate compressive stress inside the second silicon dioxide buried layer 4 and compress surrounding materials, such as compressing the first silicon layer 5 and the waveguide layer 6 . Since the waveguide layer 6 has a ridge structure, the volume expansion of the second silicon dioxide buried layer 4 can compress the upper left corner and the upper right corner of the silicon waveguide 7, causing the internal atomic arrangement structure of the silicon waveguide 7 to change, breaking the central inversion symmetry structure of silicon. Second-order nonlinear polarizability is induced in silicon.
此外,在高温退火阶段,高温环境可以催化SiO2的形成,从而加速应力的产生,随着高温退火温度提高与时间增加,硅与二氧化硅介于固体与液体的状态,其粘性降低,应力逐渐释放,因而通过对高温退火温度与时间的控制,可以对硅波导7中的应力水平进行调节。In addition, during the high-temperature annealing stage, the high-temperature environment can catalyze the formation of SiO 2 , thereby accelerating the generation of stress. As the high-temperature annealing temperature increases and the time increases, silicon and silicon dioxide are in a state between solid and liquid, and their viscosity decreases, stress It is gradually released, so by controlling the high-temperature annealing temperature and time, the stress level in the silicon waveguide 7 can be adjusted.
为了使硅波导7中的应力尽量高,并且同时降低第一硅层5中的应力,在一些实施例中退火温度为1200℃,退火时间为2~3小时。In order to make the stress in the silicon waveguide 7 as high as possible and reduce the stress in the first silicon layer 5 at the same time, in some embodiments, the annealing temperature is 1200°C and the annealing time is 2 to 3 hours.
第一硅层5中由于氧离子注入带来的损伤在高温退火中被修复,可以用来制备其他的光电子器件,从而与所形成的超低损耗硅波导7进行垂直集成,实现3D集成,以适应未来大规模光电子集成。The damage caused by oxygen ion implantation in the first silicon layer 5 is repaired during high-temperature annealing, and can be used to prepare other optoelectronic devices, thereby vertically integrating with the formed ultra-low loss silicon waveguide 7 to achieve 3D integration. Adapt to future large-scale optoelectronics integration.
在一些实施例中,高温退火之前还包括:刻蚀第二二氧化硅层11及二氧化硅波导10,以使暴露出顶部硅层3,刻蚀可采用等离子刻蚀方法;在顶部硅层3上沉积高密度二氧化硅保护层13,以防止顶部硅层3在高温退火过程中被氧化。In some embodiments, the high-temperature annealing also includes: etching the second silicon dioxide layer 11 and the silicon dioxide waveguide 10 to expose the top silicon layer 3. The etching may use a plasma etching method; A high-density silicon dioxide protective layer 13 is deposited on 3 to prevent the top silicon layer 3 from being oxidized during the high-temperature annealing process.
在一些实施例中,沉积高密度二氧化硅保护层13采用感应耦合等离子体增强化学气相沉积(ICPECVD),沉积的高密度二氧化硅保护层13厚度为350nm。在完成高温退火之后,将高密度二氧化硅保护层13移除,如直接采用刻蚀方式移除。此时露出第一硅层5的上表面。In some embodiments, inductively coupled plasma enhanced chemical vapor deposition (ICPECVD) is used to deposit the high-density silicon dioxide protective layer 13, and the thickness of the deposited high-density silicon dioxide protective layer 13 is 350 nm. After completing the high-temperature annealing, the high-density silicon dioxide protective layer 13 is removed, for example, directly by etching. At this time, the upper surface of the first silicon layer 5 is exposed.
下面以一个具体的实施例来详细说明本发明的硅基电光调制器制备方法。如图4是本发明一个实施例的硅基电光调制器制备方法步骤示意图。The preparation method of the silicon-based electro-optical modulator of the present invention will be described in detail below with a specific embodiment. Figure 4 is a schematic diagram of the steps of a method for preparing a silicon-based electro-optical modulator according to one embodiment of the present invention.
(1)选择一个SOI晶圆,SOI晶圆包括三层结构,自下而上依次为硅衬底1、第一二氧化硅埋层2、顶部硅层3,其中顶部硅层3厚度为600nm。(1) Select an SOI wafer. The SOI wafer includes a three-layer structure, from bottom to top, silicon substrate 1, first buried silicon dioxide layer 2, and top silicon layer 3. The thickness of top silicon layer 3 is 600nm. .
(2)在顶部硅层3上表面进行热氧化反应,使得顶部硅层3上部形成第一二氧化硅层9,其中第一二氧化硅层9的厚度为100nm。(2) A thermal oxidation reaction is performed on the upper surface of the top silicon layer 3 to form a first silicon dioxide layer 9 on the top surface of the top silicon layer 3, where the thickness of the first silicon dioxide layer 9 is 100 nm.
(3)将掩膜版图案转移至第一二氧化硅层9,按照掩膜版图案,采用等离子刻蚀方法刻蚀第一二氧化硅层9,得到二氧化硅波导10。(3) Transfer the mask pattern to the first silicon dioxide layer 9, and use the plasma etching method to etch the first silicon dioxide layer 9 according to the mask pattern to obtain the silicon dioxide waveguide 10.
(4)在二氧化硅波导10及因刻蚀暴露出的顶部硅层3表面采用等离子体增强化学的气相沉积方法沉积二氧化硅,形成厚度为50nm的第二二氧化硅层11。(4) Use a plasma-enhanced chemical vapor deposition method to deposit silicon dioxide on the surface of the silicon dioxide waveguide 10 and the top silicon layer 3 exposed by etching to form a second silicon dioxide layer 11 with a thickness of 50 nm.
(5)自上向下将氧离子透过第二二氧化硅层11及二氧化硅波导10 注入到顶部硅层3中,形成富氧离子层12,其中,富氧离子层12在二氧化硅波导10下方的部分向上凸起。氧离子注入总剂量为2×1017/cm2,氧离子注入能量为150KeV。(5) Inject oxygen ions from top to bottom through the second silicon dioxide layer 11 and the silicon dioxide waveguide 10 into the top silicon layer 3 to form an oxygen ion-rich layer 12, wherein the oxygen ion-rich layer 12 is formed in the silicon dioxide layer 12. The lower part of the silicon waveguide 10 is raised upward. The total dose of oxygen ion implantation is 2×10 17 /cm 2 , and the oxygen ion implantation energy is 150KeV.
(6)采用等离子刻蚀方法刻蚀第二二氧化硅层11及二氧化硅波导10,以使暴露出顶部硅层3。(6) Use a plasma etching method to etch the second silicon dioxide layer 11 and the silicon dioxide waveguide 10 to expose the top silicon layer 3 .
(7)采用感应耦合等离子体增强化学气相沉积方法在顶部硅层3上沉积高密度二氧化硅保护层13,以防止顶部硅层3在高温退火过程中被氧化。(7) Use the inductively coupled plasma enhanced chemical vapor deposition method to deposit a high-density silicon dioxide protective layer 13 on the top silicon layer 3 to prevent the top silicon layer 3 from being oxidized during the high-temperature annealing process.
(8)高温退火使得富氧离子层12中的氧离子与富氧离子层12中的硅原子发生反应,生成第二二氧化硅埋层4。(8) High-temperature annealing causes the oxygen ions in the oxygen ion-rich layer 12 to react with the silicon atoms in the oxygen ion-rich layer 12 to form the second silicon dioxide buried layer 4 .
(9)采用等离子刻蚀方式将高密度二氧化硅保护层13移除,露出第一硅层5的上表面。(9) Use plasma etching to remove the high-density silicon dioxide protective layer 13 to expose the upper surface of the first silicon layer 5 .
(10)采用电镀的方式将GSG单驱动共面波导行波电极8连接到第一硅层5上。(10) Connect the GSG single-driven coplanar waveguide traveling wave electrode 8 to the first silicon layer 5 by electroplating.
至此,本实施例制得如本发明技术方案所述的硅基电光调制器。其光场与电场分布图如图5所示。So far, this embodiment has produced the silicon-based electro-optical modulator as described in the technical solution of the present invention. Its light field and electric field distribution diagram is shown in Figure 5.
以上所述的具体实施例,对本发明的目的、技术方案和有益效果进行了进一步详细说明,所应理解的是,以上所述仅为本发明的具体实施例而已,并不用于限制本发明,凡在本发明的精神和原则之内,所做的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。The above-mentioned specific embodiments further describe the purpose, technical solutions and beneficial effects of the present invention in detail. It should be understood that the above-mentioned are only specific embodiments of the present invention and are not intended to limit the present invention. Any modifications, equivalent substitutions, improvements, etc. made within the spirit and principles of the present invention shall be included in the protection scope of the present invention.
Claims (10)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202111017879.7A CN113687530B (en) | 2021-08-31 | 2021-08-31 | Silicon-based electro-optic modulator and preparation method thereof |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202111017879.7A CN113687530B (en) | 2021-08-31 | 2021-08-31 | Silicon-based electro-optic modulator and preparation method thereof |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN113687530A CN113687530A (en) | 2021-11-23 |
| CN113687530B true CN113687530B (en) | 2023-12-08 |
Family
ID=78585076
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN202111017879.7A Active CN113687530B (en) | 2021-08-31 | 2021-08-31 | Silicon-based electro-optic modulator and preparation method thereof |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN113687530B (en) |
Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN1323404A (en) * | 1998-10-15 | 2001-11-21 | 国际商业机器公司 | Optical waveguide device |
| CN102117820A (en) * | 2009-12-31 | 2011-07-06 | 中国科学院微电子研究所 | Silicon-based optoelectronic heterogeneous integration method and silicon-based optoelectronic heterogeneous integrated chip |
| CN103165663A (en) * | 2011-12-09 | 2013-06-19 | 英飞凌科技股份有限公司 | Anchoring and Engaging Structures |
| CN111610651A (en) * | 2020-07-10 | 2020-09-01 | 北京爱杰光电科技有限公司 | A silicon-based electro-optic modulator based on stressed silicon and its fabrication method |
| CN112269277A (en) * | 2020-10-09 | 2021-01-26 | 三明学院 | A kind of electro-optical modulator based on stress silicon and preparation method thereof |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CA2482724C (en) * | 2004-02-25 | 2011-05-17 | Dan-Xia Xu | Stress-induced control of polarization dependent properties in photonic devices |
-
2021
- 2021-08-31 CN CN202111017879.7A patent/CN113687530B/en active Active
Patent Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN1323404A (en) * | 1998-10-15 | 2001-11-21 | 国际商业机器公司 | Optical waveguide device |
| CN102117820A (en) * | 2009-12-31 | 2011-07-06 | 中国科学院微电子研究所 | Silicon-based optoelectronic heterogeneous integration method and silicon-based optoelectronic heterogeneous integrated chip |
| CN103165663A (en) * | 2011-12-09 | 2013-06-19 | 英飞凌科技股份有限公司 | Anchoring and Engaging Structures |
| CN111610651A (en) * | 2020-07-10 | 2020-09-01 | 北京爱杰光电科技有限公司 | A silicon-based electro-optic modulator based on stressed silicon and its fabrication method |
| CN112269277A (en) * | 2020-10-09 | 2021-01-26 | 三明学院 | A kind of electro-optical modulator based on stress silicon and preparation method thereof |
Also Published As
| Publication number | Publication date |
|---|---|
| CN113687530A (en) | 2021-11-23 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN111487793B (en) | Z-cut LNOI electro-optic modulator for improved modulation efficiency and its application | |
| CN100547456C (en) | Electro-optic modulator based on horizontal slit plate and photonic crystal line-defect waveguide | |
| US11543688B2 (en) | Waveguide component | |
| CN102763264B (en) | Phase shifter, coupler and methods for their production | |
| CN114995010B (en) | Silicon-based three-dimensional waveguide mode optical switch based on phase change material | |
| CN117908186B (en) | Monolithic integrated high-speed modulation silicon-based optical chip and preparation method thereof | |
| CN106653957A (en) | Surface plasmon polariton electro-excitation and electrical modulation integrated device and manufacturing method thereof | |
| JP6606631B6 (en) | Light modulator | |
| CN110780381A (en) | Polarization beam splitter with asymmetric three-waveguide structure and preparation method thereof | |
| CN115373163A (en) | On-chip multi-physical field regulation and control device | |
| CN113359330A (en) | Sinking electrode lithium niobate thin film electro-optical modulator and preparation method thereof | |
| CN114400236B (en) | Silicon photonic integrated chip integrating silicon photonic modulator and silicon germanium detector and preparation method thereof | |
| CN111812867A (en) | A kind of photonic crystal electro-optic modulator and its manufacturing method | |
| CN113687530B (en) | Silicon-based electro-optic modulator and preparation method thereof | |
| CN101718890B (en) | Preparation method of cross silt wave guide based on oxygen implantation technology | |
| CN116009284A (en) | A kind of miniature optical switch unit and its design method based on double hole GST phase change material | |
| CN115755444A (en) | Efficient electro-optic devices based on electro-optic polymers and thin-film lithium niobate waveguides | |
| CN111458909B (en) | Electro-optic modulator of silicon-based composite waveguide based on plasma structure and organic material | |
| CN113703093B (en) | Ultra-low loss silicon waveguide and its preparation method | |
| CN209707731U (en) | A three-dimensional silicon-based mode control device | |
| CN116990906A (en) | A kind of lithium silicon niobate hybrid integrated electro-optical modulator based on MZ structure and its preparation method | |
| CN119045120A (en) | Phase change material post-integrated processing method compatible with CMOS (complementary metal oxide semiconductor) process and device | |
| CN117706810A (en) | A hybrid non-etching scandium-doped aluminum nitride electro-optical modulator and preparation method | |
| CN113130696B (en) | Optical switch based on quantum-confined Stark effect | |
| CN113281921B (en) | First-order electro-optic effect silicon modulator and preparation process thereof |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PB01 | Publication | ||
| PB01 | Publication | ||
| SE01 | Entry into force of request for substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| GR01 | Patent grant | ||
| GR01 | Patent grant |