CN107634801A - Transverse SAM and OAM tunable photon emitting/receiving chip and its preparation method - Google Patents
Transverse SAM and OAM tunable photon emitting/receiving chip and its preparation method Download PDFInfo
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Abstract
本发明涉及一种横向SAM与OAM可调的光子发射/接收芯片,包括片上集成的氮化硅微环波导,及片上集成的设置在氮化硅微环波导两侧的氮化硅锥形耦合波导结构,所述氮化硅微环波导内侧的倏逝波区设置有角向光栅阵列。
The invention relates to a photon emitting/receiving chip with adjustable lateral SAM and OAM, comprising a silicon nitride microring waveguide integrated on the chip, and silicon nitride tapered couplings arranged on both sides of the silicon nitride microring waveguide integrated on the chip In the waveguide structure, the evanescent wave region inside the silicon nitride microring waveguide is provided with an angular grating array.
Description
技术领域technical field
本发明涉及光通信或量子信息处理领域,更具体地,涉及一种横向SAM与OAM可调的光子发射/接收芯片及其制备方法。The invention relates to the field of optical communication or quantum information processing, and more specifically, to a photon emitting/receiving chip with adjustable lateral SAM and OAM and a preparation method thereof.
背景技术Background technique
光携带本征自旋角动量和轨道角动量,它们分别由光的偏振和空间自由度决定。光子轨道角动量(OAM)由于其无限多的本征模式,理论上可以无限拓展信息容量。因此光子轨道角动量正在被广泛的用在光通信和量子信息处理等应用中。而光子自旋角动量也在量子纠缠、光的偏振复用中应用广泛。实际上,光子的自旋角动量和轨道角动量的相互作用(SOI)在非均匀介质、光学折射/反射界面上被发现,并通过现代光学理论进行了解释。SOI现象具有非常大的新型应用潜力,比如光学微操控,超高分辨成像,光束整形,分束等。Light carries intrinsic spin angular momentum and orbital angular momentum, which are determined by the polarization and spatial degrees of freedom of the light, respectively. Due to its infinite number of eigenmodes, photon orbital angular momentum (OAM) can theoretically expand the information capacity infinitely. Therefore, photon orbital angular momentum is being widely used in applications such as optical communication and quantum information processing. Photon spin angular momentum is also widely used in quantum entanglement and polarization multiplexing of light. In fact, the spin angular momentum and orbital angular momentum interactions (SOI) of photons are found in inhomogeneous media, optical refraction/reflection interfaces, and explained by modern optical theory. The SOI phenomenon has great potential for new applications, such as optical micro-manipulation, ultra-high resolution imaging, beam shaping, beam splitting, etc.
另一方面,光子自旋角动量SAM按照其旋转轴与光束传播方向的关系(垂直或平行)分为横向自旋角动量和纵向自旋角动量。相比自然界中普遍存在的纵向自旋角动量,横向自旋角动量主要发生在非均匀光场中,比如表面等离子激元,波导/非波导模式的倏逝波区以及强聚焦光束中。携带横向自旋角动量的光场在纳米光子学、生物传感中具有非常多的新应用。特别地,倏逝波中横向自旋角动量在波导模式的边界引起强烈的SOI现象,或被称为光的量子自旋霍尔效应。并在光的界面上引起横向自旋-方向性耦合,也即打破界面上由倏逝波参与的激发模式方向性。横向自旋角动量的这一特性在光学二极管、手性自旋光网络、量子信息处理等应用中发展出了非常多的功能器件。On the other hand, the photon spin angular momentum SAM is divided into transverse spin angular momentum and longitudinal spin angular momentum according to the relationship between its rotation axis and the beam propagation direction (perpendicular or parallel). Compared with the longitudinal spin angular momentum ubiquitous in nature, the transverse spin angular momentum mainly occurs in inhomogeneous optical fields, such as surface plasmons, evanescent wave regions of waveguide/non-waveguide modes, and strongly focused beams. Light fields carrying transverse spin angular momentum have many new applications in nanophotonics and biosensing. In particular, the transverse spin angular momentum in the evanescent wave induces a strong SOI phenomenon at the boundary of the waveguide mode, or known as the quantum spin Hall effect of light. And cause lateral spin-directional coupling on the interface of light, that is, break the directionality of the excitation mode participated by the evanescent wave on the interface. This characteristic of transverse spin angular momentum has developed a lot of functional devices in applications such as optical diodes, chiral spin-optical networks, and quantum information processing.
因此,同时对光子的横向自旋角动量和轨道角动量进行操控将会在整个角动量域中展现更加多样性的应用前景。并将带来新型功能器件,比如用于SAM-OAM空间中的光子态编/解码。Therefore, simultaneously manipulating the lateral spin angular momentum and orbital angular momentum of photons will open up more diverse application prospects in the entire angular momentum domain. And it will bring new functional devices, such as photon state encoding/decoding in SAM-OAM space.
发明内容Contents of the invention
本发明提供了一种横向SAM与OAM可调的光子发射/接收芯片,该芯片能够对光子的横向自旋角动量、轨道角动量进行调整,因此具备十分宽广的应用前景。The invention provides a photon emitting/receiving chip with adjustable lateral SAM and OAM. The chip can adjust the lateral spin angular momentum and orbital angular momentum of the photon, so it has very broad application prospects.
为实现以上发明目的,采用的技术方案是:For realizing above-mentioned purpose of the invention, the technical scheme that adopts is:
横向SAM与OAM可调的光子发射/接收芯片,包括片上集成的氮化硅微环波导,及片上集成的设置在氮化硅微环波导一侧的氮化硅锥形耦合波导结构,所述氮化硅微环波导内侧的倏逝波区设置有角向光栅阵列。A photon emitting/receiving chip with adjustable lateral SAM and OAM, including an on-chip silicon nitride microring waveguide, and an on-chip silicon nitride tapered coupling waveguide structure arranged on one side of the silicon nitride microring waveguide, said The evanescent wave region inside the silicon nitride microring waveguide is provided with an angular grating array.
上述方案中,芯片作为发射器时,氮化硅微环波导的折射率特性使得光场在波导倏逝波区中的径向分量强度和角向分量强度可比拟,产生横向自旋角动量,因此通过改变氮化硅微环波导的尺寸可以调控波导倏逝波区的两个电场分量大小,进而达到调控横向自旋角动量的目的。而氮化硅微环波导用于对发射光谱进行波长选择和轨道角动量的拓扑荷调控,进而达到调控轨道角动量的目的,然后通过倏逝波区的角向光栅阵列使氮化硅微环波导中的模式被垂直发射到自由空间中,同时携带横向自旋角动量和轨道角动量。In the above scheme, when the chip is used as the emitter, the refractive index characteristics of the silicon nitride microring waveguide make the intensity of the radial component and the intensity of the angular component of the light field in the evanescent wave region of the waveguide comparable, generating transverse spin angular momentum, Therefore, by changing the size of the silicon nitride microring waveguide, the magnitudes of the two electric field components in the evanescent wave region of the waveguide can be adjusted, thereby achieving the purpose of adjusting the lateral spin angular momentum. The silicon nitride microring waveguide is used to select the wavelength of the emission spectrum and the topological charge regulation of the orbital angular momentum, and then achieve the purpose of regulating the orbital angular momentum, and then make the silicon nitride microring waveguide through the angular grating array in the evanescent wave region Modes in the waveguide are launched vertically into free space, carrying both lateral spin angular momentum and orbital angular momentum.
当芯片作为接收器时,只有波长满足氮化硅微环波导的谐振条件且携带相应OAM阶数的入射光束能够被耦合进入氮化硅微环波导内,并通过横向自旋角动量的单向耦合特性,将分别携带左旋/右旋两种SAM的光束输出到氮化硅锥形耦合波导结构的左/右两个相反的方向,实现OAM-SAM两个空间的选择性接收。When the chip is used as a receiver, only the incident light beams whose wavelength satisfies the resonance condition of the silicon nitride microring waveguide and carry the corresponding OAM order can be coupled into the silicon nitride microring waveguide, and pass through the unidirectional spin angular momentum Coupling characteristics, the light beams carrying left-handed/right-handed SAMs are output to the left/right opposite directions of the silicon nitride tapered coupling waveguide structure, and the selective reception of the two spaces of OAM-SAM is realized.
同时,本发明还提供了一种以上芯片的制备方法,其具体的内容如下:Simultaneously, the present invention also provides more than a kind of preparation method of chip, and its specific content is as follows:
一种以上发射/接收芯片的制备方法,包括以下步骤:A method for preparing more than one transmitting/receiving chip, comprising the following steps:
S1.在晶向硅衬底上生长氧化硅层,然后通过化学气相方法在氧化硅层上沉积氮化硅层;S1. growing a silicon oxide layer on a crystalline silicon substrate, and then depositing a silicon nitride layer on the silicon oxide layer by a chemical vapor phase method;
S2.在氮化硅层上进行旋涂光刻胶、曝光、热回流、等离子体刻蚀步骤,制备氮化硅微环波导、氮化硅锥形耦合波导结构和角向光栅阵列。S2. Spin-coat photoresist, exposure, thermal reflow, and plasma etching steps on the silicon nitride layer to prepare silicon nitride microring waveguides, silicon nitride tapered coupling waveguide structures, and angular grating arrays.
与现有技术相比,本发明的有益效果是:Compared with prior art, the beneficial effect of the present invention is:
本发明结合了硅基集成光子轨道角动量发射器件的优点和对倏逝波区中横向自旋角动量的深入研究,给出一种横向自旋角动量与轨道角动量可调的光子发射/接收芯片。在这个方案中,氮化硅微环波导被设计成具有横向自旋角动量在较大范围内可调,而轨道角动量通过改变输入波长而改变拓扑荷数,再由输入光的激发方向决定发射到自由空间中的自旋角动量和轨道角动量方向。三种情况共同起作用,最终该器件产生的光束能够同时携带可调横向自旋和轨道角动量。而作为接收器件时,将入射到器件上的OAM光束通过倏逝波的横向自旋进行选择性耦合到两个不同的方向,实现OAM-SAM的同时选择性耦合。该设计具有耦合选择比高,产生的SAM-OAM纯度高等优点,且采用本发明中的加工工艺,该芯片可以在通用的半导体微加工平台上大规模流片生产,具有较大的应用前景。The invention combines the advantages of silicon-based integrated photon orbital angular momentum emitting devices and the in-depth study of lateral spin angular momentum in the evanescent wave region, and provides a photon emission/ Receive chip. In this scheme, the silicon nitride microring waveguide is designed to have a large range of adjustable lateral spin angular momentum, while the orbital angular momentum changes the topological charge by changing the input wavelength, which is determined by the excitation direction of the input light. Directions of spin angular momentum and orbital angular momentum emitted into free space. The three conditions work together, and finally the device produces a beam capable of simultaneously carrying tunable lateral spin and orbital angular momentum. When used as a receiving device, the OAM beam incident on the device is selectively coupled to two different directions through the transverse spin of the evanescent wave, realizing the simultaneous selective coupling of OAM-SAM. The design has the advantages of high coupling selection ratio and high purity of the generated SAM-OAM, and adopts the processing technology in the present invention, and the chip can be produced on a general semiconductor microprocessing platform in a large scale, and has great application prospects.
附图说明Description of drawings
图1为芯片的结构示意图。Figure 1 is a schematic diagram of the structure of the chip.
图2(a)、(b)、(c)为芯片的制备流程图。Figure 2 (a), (b), (c) is the flow chart of chip preparation.
具体实施方式detailed description
附图仅用于示例性说明,不能理解为对本专利的限制;The accompanying drawings are for illustrative purposes only and cannot be construed as limiting the patent;
以下结合附图和实施例对本发明做进一步的阐述。The present invention will be further elaborated below in conjunction with the accompanying drawings and embodiments.
实施例1Example 1
如图1所示,本发明提供的横向自旋角动量、轨道角动量可调的光子发射/接收芯片包括片上集成的氮化硅微环波导1,及片上集成的设置在氮化硅微环波导1一侧的氮化硅锥形耦合波导结构3,所述氮化硅微环波导1内侧的倏逝波区设置有角向光栅阵列2。As shown in Figure 1, the photon emitting/receiving chip with adjustable lateral spin angular momentum and orbital angular momentum provided by the present invention includes an on-chip silicon nitride microring waveguide 1, and an on-chip integrated silicon nitride microring waveguide 1 The silicon nitride tapered coupling waveguide structure 3 on one side of the waveguide 1 is provided with an angular grating array 2 in the evanescent wave region inside the silicon nitride microring waveguide 1 .
上述方案中,芯片作为发射器时,氮化硅微环波导1的折射率特性使得光场在波导倏逝波区中的径向分量强度和角向分量强度可比拟,产生横向自旋角动量,因此通过改变氮化硅微环波导1的尺寸可以调控波导倏逝波区的两个电场分量大小,进而达到调控横向自旋角动量的目的。而氮化硅微环波导1用于对发射光谱进行波长选择和轨道角动量的拓扑荷调控,进而达到调控轨道角动量的目的,然后通过倏逝波区的角向光栅阵列2使氮化硅微环波导1中的模式被垂直发射到自由空间中,并携带横向自旋角动量和轨道角动量。In the above scheme, when the chip is used as the emitter, the refractive index characteristics of the silicon nitride microring waveguide 1 make the intensity of the radial component and the intensity of the angular component of the light field in the evanescent wave region of the waveguide comparable, generating transverse spin angular momentum , so by changing the size of the silicon nitride microring waveguide 1, the magnitude of the two electric field components in the evanescent wave region of the waveguide can be regulated, thereby achieving the purpose of regulating the lateral spin angular momentum. The silicon nitride microring waveguide 1 is used to select the wavelength of the emission spectrum and the topological charge regulation of the orbital angular momentum, and then achieve the purpose of regulating the orbital angular momentum, and then through the angular grating array 2 in the evanescent wave region, the silicon nitride The modes in the microring waveguide 1 are launched vertically into free space and carry transverse spin angular momentum and orbital angular momentum.
当芯片作为接收器时,只有波长满足氮化硅微环波导1的谐振条件且携带相应OAM阶数的入射光束能够被耦合进入氮化硅微环波导1内,并通过横向自旋角动量的单向耦合特性,将分别携带左旋/右旋两种SAM的光束输出到氮化硅锥形耦合波导结构3的左/右两个相反的方向,实现OAM-SAM两个空间的选择性接收。When the chip is used as a receiver, only incident light beams with a wavelength that satisfies the resonance condition of the silicon nitride microring waveguide 1 and carries the corresponding OAM order can be coupled into the silicon nitride microring waveguide 1 and passed through the lateral spin angular momentum The one-way coupling feature outputs the light beams respectively carrying two kinds of left-handed and right-handed SAMs to the left/right two opposite directions of the silicon nitride tapered coupling waveguide structure 3, so as to realize the selective reception of the two spaces of OAM-SAM.
在具体的实施过程中,所述氮化硅微环波导1、氮化硅锥形耦合波导结构3的折射率为2.0。所述氮化硅微环波导1、氮化硅锥形耦合波导结构3的设置高度为0.6微米,其氮化硅微环波导1的宽度范围为0.8-1.6微米。所述氮化硅微环波导1的半径为80微米,与氮化硅锥形耦合波导结构的耦合间隔为200纳米,外层SU8波导的高度和宽度为3.5微米。In a specific implementation process, the refractive index of the silicon nitride microring waveguide 1 and the silicon nitride tapered coupling waveguide structure 3 is 2.0. The installation height of the silicon nitride microring waveguide 1 and the silicon nitride tapered coupling waveguide structure 3 is 0.6 microns, and the width range of the silicon nitride microring waveguide 1 is 0.8-1.6 microns. The radius of the silicon nitride microring waveguide 1 is 80 microns, the coupling interval with the silicon nitride tapered coupling waveguide structure is 200 nanometers, and the height and width of the outer SU8 waveguide are 3.5 microns.
上述方案中,所述角向光栅阵列2包括有517个周期性布置的角向光栅。所述角向光栅的高度和宽度均为100纳米。In the above solution, the angular grating array 2 includes 517 periodically arranged angular gratings. The height and width of the angular grating are both 100 nanometers.
在具体的实施过程中,所述氮化硅锥形耦合波导结构3包括直波导31和设置在直波导31两端的与直波导连接的锥形波导32,锥形波导32细处的宽度为140纳米,锥形波导32的长度为350微米。所述锥形波导32的外层设置有SU8直波导03,SU8直波导03的高度为3.5微米,宽度为3.5微米。In a specific implementation process, the silicon nitride tapered coupling waveguide structure 3 includes a straight waveguide 31 and a tapered waveguide 32 connected to the straight waveguide arranged at both ends of the straight waveguide 31. The width of the tapered waveguide 32 is 140 The length of the tapered waveguide 32 is 350 micrometers. The outer layer of the tapered waveguide 32 is provided with a SU8 straight waveguide 03, the height of the SU8 straight waveguide 03 is 3.5 microns, and the width is 3.5 microns.
实施例2Example 2
本实施例提供了一种实施例1的芯片的制备方法,如图2(a)、(b)、(c)所示,其具体的方案如下:This embodiment provides a method for preparing the chip of Embodiment 1, as shown in Figure 2 (a), (b) and (c), the specific scheme is as follows:
S1.在400微米厚的晶向硅衬底02上生长5微米厚的氧化硅层01,然后通过化学气相方法在氧化硅层01上沉积600纳米厚的氮化硅层00;S1. A 5-micron-thick silicon oxide layer 01 is grown on a 400-micron-thick crystalline silicon substrate 02, and then a 600-nm-thick silicon nitride layer 00 is deposited on the silicon oxide layer 01 by a chemical vapor phase method;
S2.在氮化硅层00上进行旋涂光刻胶、曝光、热回流、等离子体刻蚀步骤,制备氮化硅微环波导1、直波导31、锥形波导32和角向光栅阵列2。S2. Spin-coat photoresist, exposure, thermal reflow, and plasma etching steps on the silicon nitride layer 00 to prepare silicon nitride microring waveguides 1, straight waveguides 31, tapered waveguides 32, and angular grating arrays 2 .
S3.通过套刻和图形化转移得到锥形波导32外层的SU8直波导结构03;S3. Obtain the SU8 straight waveguide structure 03 on the outer layer of the tapered waveguide 32 by overlaying and pattern transfer;
显然,本发明的上述实施例仅仅是为清楚地说明本发明所作的举例,而并非是对本发明的实施方式的限定。对于所属领域的普通技术人员来说,在上述说明的基础上还可以做出其它不同形式的变化或变动。这里无需也无法对所有的实施方式予以穷举。凡在本发明的精神和原则之内所作的任何修改、等同替换和改进等,均应包含在本发明权利要求的保护范围之内。Apparently, the above-mentioned embodiments of the present invention are only examples for clearly illustrating the present invention, rather than limiting the implementation of the present invention. For those of ordinary skill in the art, other changes or changes in different forms can be made on the basis of the above description. It is not necessary and impossible to exhaustively list all the implementation manners here. All modifications, equivalent replacements and improvements made within the spirit and principles of the present invention shall be included within the protection scope of the claims of the present invention.
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Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN111399117A (en) * | 2020-04-30 | 2020-07-10 | 中国科学院半导体研究所 | Hybrid integrated silicon nitride micro-ring resonant cavity and preparation method thereof |
| CN113359233A (en) * | 2021-04-27 | 2021-09-07 | 中国科学院上海微系统与信息技术研究所 | Optical splitter based on silicon nitride photonic crystal and preparation method thereof |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101325313A (en) * | 2008-07-15 | 2008-12-17 | 浙江大学 | High-speed modulation of semiconductor lasers |
| WO2013179023A1 (en) * | 2012-06-01 | 2013-12-05 | The University Of Bristol | Orbital angular momentum |
-
2017
- 2017-07-25 CN CN201710614113.4A patent/CN107634801A/en active Pending
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101325313A (en) * | 2008-07-15 | 2008-12-17 | 浙江大学 | High-speed modulation of semiconductor lasers |
| WO2013179023A1 (en) * | 2012-06-01 | 2013-12-05 | The University Of Bristol | Orbital angular momentum |
Non-Patent Citations (2)
| Title |
|---|
| 余思远: ""涡旋光场的集成光子学操控方法"", 《光学学报》 * |
| 徐延海: ""集成 OAM 光束发射器模式纯度仿真分析"", 《电子测试》 * |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN111399117A (en) * | 2020-04-30 | 2020-07-10 | 中国科学院半导体研究所 | Hybrid integrated silicon nitride micro-ring resonant cavity and preparation method thereof |
| CN113359233A (en) * | 2021-04-27 | 2021-09-07 | 中国科学院上海微系统与信息技术研究所 | Optical splitter based on silicon nitride photonic crystal and preparation method thereof |
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