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CN101546014A - Large-bandwidth Y-branch power splitter based on mode gradual change principle - Google Patents

Large-bandwidth Y-branch power splitter based on mode gradual change principle Download PDF

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CN101546014A
CN101546014A CN200910097875A CN200910097875A CN101546014A CN 101546014 A CN101546014 A CN 101546014A CN 200910097875 A CN200910097875 A CN 200910097875A CN 200910097875 A CN200910097875 A CN 200910097875A CN 101546014 A CN101546014 A CN 101546014A
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optical waveguide
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戴道锌
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Zhejiang University ZJU
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Abstract

本发明的基于模式渐变原理的大带宽Y分支功分器,包括一条输入光波导和两条输出光波导;输入光波导包括相连接的直波导和锥形光波导,每条输出光波导包括相连的直波导和S型锥形光波导,输入光波导的锥形光波导平行插入两条输出光波导的S型锥形光波导之间,输入光波导的锥形光波导与两条输出光波导的S型锥形光波导的交叠区域为模式渐变区,形成Y状复合光波导。通过模式渐变区,输入光波导的基模逐渐转变为具有两个峰的场分布,这两个峰各自从输出光波导输出,实现低损耗的功率分配。本发明结构简单,在1.2μm~1.8μm带宽范围都具备超低损耗。

Figure 200910097875

The large-bandwidth Y-branch power splitter based on the mode gradient principle of the present invention includes an input optical waveguide and two output optical waveguides; the input optical waveguide includes connected straight waveguides and tapered optical waveguides, and each output optical waveguide includes connected The straight waveguide and S-shaped tapered optical waveguide, the tapered optical waveguide of the input optical waveguide is inserted between the S-shaped tapered optical waveguides of the two output optical waveguides in parallel, the tapered optical waveguide of the input optical waveguide and the two output optical waveguides The overlapping region of the S-shaped tapered optical waveguide is a mode gradient region, forming a Y-shaped composite optical waveguide. Through the mode transition region, the fundamental mode of the input optical waveguide is gradually transformed into a field distribution with two peaks, which are respectively output from the output optical waveguide, realizing low-loss power distribution. The invention has a simple structure and has ultra-low loss in the bandwidth range of 1.2 μm to 1.8 μm.

Figure 200910097875

Description

一种基于模式渐变原理的大带宽Y分支功分器 A Large Bandwidth Y-branch Power Splitter Based on Mode Gradual Principle

技术领域 technical field

本发明涉及一种Y分支功分器,尤其涉及一种基于模式渐变原理的大带宽Y分支功分器。The invention relates to a Y-branch power splitter, in particular to a large-bandwidth Y-branch power splitter based on the principle of mode gradual change.

背景技术 Background technique

除骨干网和城域网,光纤到户接入网逐渐成为光通信的重要发展建设方向。光纤到户(FTTH)可向用户提供极丰富的带宽,是一种理想的接入模式,是未来光纤通信系统解决“最后一公里”的最好方式,并将成为新一代宽带网络的标志。这对光器件提出了新的技术要求并为之开辟了一个崭新的应用领域。In addition to the backbone network and the metropolitan area network, the fiber-to-the-home access network has gradually become an important development and construction direction of optical communication. Fiber-to-the-home (FTTH) can provide users with extremely rich bandwidth. It is an ideal access mode and the best way to solve the "last mile" for future optical fiber communication systems, and will become a symbol of a new generation of broadband networks. This puts forward new technical requirements for optical devices and opens up a new application field for them.

在光纤到户接入网系统中,功分器是一种必需基本元器件。对于应用于FTTH的功分器,最重要特性是具有超大带宽(1250nm~1700nm)。相对于其它分立型器件来说,集成型Y分支功分器具有集成度高、尺寸小、稳定性高、大批量生产等突出优势。普通的集成型Y分支功分器的结构(如图1所示),包括依次相连的一条输入波导1、一个锥形区50和两条S型输出光波导2、3。然而,这种传统结构设计中包含一个尖角51。由于制备工艺的限制,这个尖角51在实际器件中难以实现,这将引起较大的损耗。为了克服尖角问题,有人提出了基于三条平行光波导耦合的功分器(Journal of Lightwave Technology,8(10):1621,1990),如图2所示,其中两条输出光波导具有均匀的宽度,其工作原理是基于倏逝波耦合。然而,输入光波导1与输出光波导2、3之间的倏逝波耦合具有波长敏感性,因而限制了这种功分器的带宽。也有人采用多模干涉(MMI)功分器结构,如图3所示。尽管可以避免普通Y分支功分器中的尖角,但由于MMI耦合器中的自成像对波长敏感,MMI功分器带宽仍然是受限。In the fiber-to-the-home access network system, the power splitter is a necessary basic component. For the power divider applied to FTTH, the most important feature is to have a super wide bandwidth (1250nm ~ 1700nm). Compared with other discrete devices, the integrated Y-branch power divider has outstanding advantages such as high integration, small size, high stability, and mass production. The structure of a common integrated Y-branch power splitter (as shown in FIG. 1 ) includes an input waveguide 1 , a tapered region 50 and two S-shaped output optical waveguides 2 and 3 connected in sequence. However, this conventional structural design includes a sharp corner 51 . Due to the limitation of the manufacturing process, it is difficult to realize the sharp corner 51 in the actual device, which will cause a large loss. In order to overcome the sharp angle problem, someone proposed a power splitter based on the coupling of three parallel optical waveguides (Journal of Lightwave Technology, 8(10): 1621, 1990), as shown in Figure 2, in which two output optical waveguides have uniform width, its working principle is based on evanescent wave coupling. However, the evanescent coupling between the input optical waveguide 1 and the output optical waveguides 2, 3 is wavelength sensitive, thus limiting the bandwidth of this power splitter. Some people also use multi-mode interference (MMI) power divider structure, as shown in Figure 3. Although the sharp corners in common Y-branch power splitters can be avoided, the MMI power splitter bandwidth is still limited due to the wavelength sensitivity of the self-imaging in the MMI coupler.

发明内容 Contents of the invention

本发明的目的是针对现有技术的不足,提出一种基于模式渐变原理的大带宽Y分支功分器,以解决普通Y分支功分器带宽过小的问题。The purpose of the present invention is to address the deficiencies in the prior art, and propose a large-bandwidth Y-branch power divider based on the principle of mode gradual change, so as to solve the problem of too small bandwidth of a common Y-branch power divider.

本发明的基于模式渐变原理的大带宽Y分支功分器,包括一条输入光波导和两条输出光波导;输入光波导包括相连接的直波导和锥形光波导,锥形光波导自与直波导的连接处到端部的宽度缓慢变化,满足模式渐变条件,每条输出光波导包括相连的直波导和S型锥形光波导,S型锥形光波导自与直波导的连接处到端部的宽度缓慢变化,满足模式渐变条件,输入光波导的锥形光波导平行插入两条输出光波导的S型锥形光波导之间,输入光波导的锥形光波导与两条输出光波导的S型锥形光波导的交叠区域为模式渐变区,形成Y状复合光波导。The large-bandwidth Y-branch power splitter based on the mode gradient principle of the present invention includes an input optical waveguide and two output optical waveguides; the input optical waveguide includes straight waveguides and tapered optical waveguides connected, and the tapered optical waveguide is connected with the straight waveguide. The width from the junction to the end of the waveguide changes slowly to meet the mode gradient condition. Each output optical waveguide includes a connected straight waveguide and an S-shaped tapered optical waveguide. The S-shaped tapered optical waveguide is from the junction with the straight waveguide to the end. The width of the part changes slowly to meet the mode gradient condition. The tapered optical waveguide of the input optical waveguide is inserted between the S-shaped tapered optical waveguides of the two output optical waveguides in parallel, and the tapered optical waveguide of the input optical waveguide and the two output optical waveguides The overlapping region of the S-shaped tapered optical waveguide is a mode gradient region, forming a Y-shaped composite optical waveguide.

本发明具有的有益效果是:The beneficial effects that the present invention has are:

1.在很大带宽(1.2μm~1.8μm)都具备超低损耗;1. Ultra-low loss in a large bandwidth (1.2μm ~ 1.8μm);

2.结构简单、设计方便,且制作工艺要求低。2. The structure is simple, the design is convenient, and the manufacturing process requirements are low.

附图说明 Description of drawings

图1是普通Y分支功分器结构示意图;Fig. 1 is a schematic diagram of the structure of a common Y branch power divider;

图2是基于三条平行光波导耦合的功分器结构示意图;Figure 2 is a schematic structural diagram of a power splitter based on the coupling of three parallel optical waveguides;

图3是多模干涉(MMI)功分器结构示意图;Fig. 3 is a schematic structural diagram of a multimode interference (MMI) power divider;

图4是本发明功分器结构示意图;Fig. 4 is a schematic structural diagram of a power divider of the present invention;

图5是本发明在1.2μm~1.8μm范围内的损耗特性;Fig. 5 is the loss characteristics of the present invention in the range of 1.2 μm to 1.8 μm;

具体实施方式 Detailed ways

下面结合附图和实施例对本发明作进一步说明。The present invention will be further described below in conjunction with drawings and embodiments.

参照图4,本发明的基于模式渐变原理的大带宽Y分支功分器,包括一条输入光波导1和两条输出光波导2、3;输入光波导1包括相连接的宽度均匀的直波导10和锥形光波导11,锥形光波导11自与直波导等宽度的连接处到端部12的宽度缓慢变化,满足模式渐变条件,每条输出光波导包括相连的宽度均匀的直波导20和S型锥形光波导21,S型锥形光波导21自与直波导20等宽度的连接处到端部23的宽度缓慢变化,满足模式渐变条件,输入光波导1的锥形光波导11平行插入两条输出光波导2、3的S型锥形光波导21之间,即相互之间没有交叉,输入光波导1的锥形光波导11与两条输出光波导2、3的S型锥形光波导21的交叠区域为模式渐变区43,在模式渐变区43中,输入光波导和两条输出光波导形成Y状复合光波导。With reference to Fig. 4, the large-bandwidth Y-branch power splitter based on the mode gradual change principle of the present invention comprises an input optical waveguide 1 and two output optical waveguides 2, 3; the input optical waveguide 1 comprises straight waveguides 10 connected with uniform width And the tapered optical waveguide 11, the width of the tapered optical waveguide 11 changes slowly from the connection with the straight waveguide equal width to the end 12, and satisfies the mode gradient condition, and each output optical waveguide includes a connected straight waveguide 20 with uniform width and S-shaped tapered optical waveguide 21, the width of S-shaped tapered optical waveguide 21 changes slowly from the connection with the straight waveguide 20 equal width to the end 23, satisfying the mode gradient condition, the tapered optical waveguide 11 of the input optical waveguide 1 is parallel Insert between the S-shaped tapered optical waveguides 21 of the two output optical waveguides 2, 3, that is, there is no intersection between each other, the tapered optical waveguide 11 of the input optical waveguide 1 and the S-shaped tapered optical waveguides of the two output optical waveguides 2, 3 The overlapping region of the shaped optical waveguides 21 is the mode transition region 43, and in the mode transition region 43, the input optical waveguide and the two output optical waveguides form a Y-shaped composite optical waveguide.

在模式渐变区输入位置,此复合光波导的模式与输入光波导的基模几乎相同;在模式渐变区输出位置,此复合光波导的模式与两条输出光波导的复合基模几乎相同。通过模式渐变区,输入光波导1的基模逐渐转变为具有两个峰的场分布,这两个峰各自从输出光波导2、3输出,实现低损耗的功率分配功能。At the input position of the mode transition area, the mode of the composite optical waveguide is almost the same as the fundamental mode of the input optical waveguide; at the output position of the mode transition area, the mode of the composite optical waveguide is almost the same as the complex fundamental modes of the two output optical waveguides. Through the mode gradient region, the fundamental mode of the input optical waveguide 1 gradually transforms into a field distribution with two peaks, and the two peaks are respectively output from the output optical waveguides 2 and 3, realizing a low-loss power distribution function.

两条输出光波导2、3关于输入光波导1可以对称分布,也可以非对称分布,相应地,获得均匀或非均匀的功率分配比率。The two output optical waveguides 2, 3 can be distributed symmetrically or asymmetrically with respect to the input optical waveguide 1, correspondingly, a uniform or non-uniform power distribution ratio can be obtained.

下面给出本发明的一个具体实施例。所有光波导为折射率差Δ=0.75%的SiO2-on-Si掩埋型光波导,此例中,两条输出光波导为对称分布。其几何尺寸参数如下:A specific embodiment of the present invention is given below. All optical waveguides are SiO 2 -on-Si buried optical waveguides with a refractive index difference Δ=0.75%. In this example, two output optical waveguides are distributed symmetrically. Its geometric parameters are as follows:

输入光波导1的直波导10宽度为3.5μm,锥形光波导11端部的宽度12为1.0μm、长度14为1300μm。The straight waveguide 10 of the input optical waveguide 1 has a width of 3.5 μm, the width 12 of the end of the tapered optical waveguide 11 is 1.0 μm, and the length 14 is 1300 μm.

输出光波导的直波导20宽度为6.0μm,S型锥形光波导21端部的宽度23为1.0μm、S型弯曲部分的长度24为2600μm、横向偏移26为6μm。The straight waveguide 20 of the output optical waveguide has a width of 6.0 μm, the width 23 of the end of the S-shaped tapered optical waveguide 21 is 1.0 μm, the length 24 of the S-shaped curved part is 2600 μm, and the lateral offset 26 is 6 μm.

图5给出了在1200~1800nm整个带宽内从输出光波导中输出的光功率。由此可见,本发明可以实现1200~1800nm超大带宽内的低损耗功率分配。Figure 5 shows the optical power output from the output optical waveguide within the entire bandwidth of 1200-1800nm. It can be seen that the present invention can realize low-loss power distribution within a super large bandwidth of 1200-1800nm.

上述实施例用来解释说明本发明,而不是对本发明进行限制,在本发明的精神和权利要求的保护范围内,对本发明作出的任何修改和改变,都落入本发明的保护范围。The above-mentioned embodiments are used to illustrate the present invention, rather than to limit the present invention. Within the spirit of the present invention and the protection scope of the claims, any modification and change made to the present invention will fall into the protection scope of the present invention.

Claims (1)

1. the large-bandwidth Y-branch power splitter based on mode gradual change principle is characterized in that comprising an input waveguide (1) and two output optical waveguides (2,3); Input waveguide (1) comprises straight wave guide (10) and the conical optical waveguide (11) that is connected, conical optical waveguide (11) is Zi slowly changing with the junction of the straight wave guide width to the end, satisfy the mode gradual change condition, every output optical waveguide comprises continuous straight wave guide (20) and S type conical optical waveguide (21), S type conical optical waveguide (21) is Zi slowly changing with the junction of straight wave guide (20) width to the end, satisfy the mode gradual change condition, two output optical waveguides (2 of the parallel insertion of conical optical waveguide (11) of input waveguide (1), 3) between the S type conical optical waveguide (21), the conical optical waveguide (11) of input waveguide (1) and two output optical waveguides (2, the overlapping region of S type conical optical waveguide (21) 3) is mode gradual change district (43), forms Y shape composite optical wave guide.
CN200910097875A 2009-04-20 2009-04-20 Large-bandwidth Y-branch power splitter based on mode gradual change principle Pending CN101546014A (en)

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Cited By (11)

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CN102866457A (en) * 2011-07-05 2013-01-09 上海圭光科技有限公司 Ridge waveguide coupled Y type branching device and 1*N branching device constituted thereby
US20150104130A1 (en) * 2013-10-14 2015-04-16 Cisco Technology, Inc. Optical power splitter
CN102866457B (en) * 2011-07-05 2016-12-14 上海圭光科技有限公司 The y-branch device of ridge waveguide-coupled and the 1 × N splitter being made up of it
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WO2019205918A1 (en) * 2018-04-26 2019-10-31 Huawei Technologies Co., Ltd. Optical splitter including a trident structure
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Cited By (16)

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CN102866457A (en) * 2011-07-05 2013-01-09 上海圭光科技有限公司 Ridge waveguide coupled Y type branching device and 1*N branching device constituted thereby
CN102866457B (en) * 2011-07-05 2016-12-14 上海圭光科技有限公司 The y-branch device of ridge waveguide-coupled and the 1 × N splitter being made up of it
US20150104130A1 (en) * 2013-10-14 2015-04-16 Cisco Technology, Inc. Optical power splitter
CN107924026A (en) * 2015-09-09 2018-04-17 日东电工株式会社 Fiber waveguide and the position sensor and photoelectricity base board using the fiber waveguide
WO2019205918A1 (en) * 2018-04-26 2019-10-31 Huawei Technologies Co., Ltd. Optical splitter including a trident structure
JP7163478B2 (en) 2019-02-25 2022-10-31 京セラ株式会社 Optical waveguides, planar optical circuits and light source modules
WO2020175236A1 (en) * 2019-02-25 2020-09-03 京セラ株式会社 Optical waveguide, planar optical circuit, and light source module
JPWO2020175236A1 (en) * 2019-02-25 2021-10-07 京セラ株式会社 Optical waveguide, planar optical circuit and light source module
CN112666653A (en) * 2019-10-16 2021-04-16 住友电气工业株式会社 Optical modulator
CN110658586A (en) * 2019-11-19 2020-01-07 华进半导体封装先导技术研发中心有限公司 End face coupler and preparation method thereof
CN110658586B (en) * 2019-11-19 2024-01-26 华进半导体封装先导技术研发中心有限公司 End face coupler and preparation method thereof
CN112596156A (en) * 2020-12-18 2021-04-02 海南师范大学 GOI or SOI based beam splitting/combining waveguide and preparation method thereof
CN113376740A (en) * 2021-06-18 2021-09-10 南京刻得不错光电科技有限公司 Light splitting/combining element and photonic device
CN113376740B (en) * 2021-06-18 2022-11-22 南京刻得不错光电科技有限公司 Light splitting/combining element and photonic device
WO2022262407A1 (en) * 2021-06-18 2022-12-22 南京刻得不错光电科技有限公司 Optical power distribution element and photonic device
CN113917685A (en) * 2021-09-30 2022-01-11 中航光电科技股份有限公司 A Design Method of Spectroscopic Optical Waveguide Based on Energy Directional Coupling

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