WO2016090534A1 - Waveguide device and chip comprising same - Google Patents

Waveguide device and chip comprising same Download PDF

Info

Publication number
WO2016090534A1
WO2016090534A1 PCT/CN2014/093294 CN2014093294W WO2016090534A1 WO 2016090534 A1 WO2016090534 A1 WO 2016090534A1 CN 2014093294 W CN2014093294 W CN 2014093294W WO 2016090534 A1 WO2016090534 A1 WO 2016090534A1
Authority
WO
WIPO (PCT)
Prior art keywords
waveguide
straight
straight waveguide
coupling
curved
Prior art date
Application number
PCT/CN2014/093294
Other languages
French (fr)
Chinese (zh)
Inventor
刘万元
Original Assignee
华为技术有限公司
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by 华为技术有限公司 filed Critical 华为技术有限公司
Priority to PCT/CN2014/093294 priority Critical patent/WO2016090534A1/en
Priority to CN201480081835.2A priority patent/CN106687836A/en
Publication of WO2016090534A1 publication Critical patent/WO2016090534A1/en

Links

Images

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/26Optical coupling means

Definitions

  • Embodiments of the present invention relate to the field of optics and, in particular, to a waveguide device.
  • the high refractive index contrast of silicon light makes it suitable for large-scale and high-density integration. At the same time, it can also utilize the mature complementary metal oxide semiconductor process of the electric chip, which makes silicon light unique. However, the optical path does not have the flexibility of the circuit. In large-scale switching matrices, the intersection of waveguides is unavoidable. In a silicon light platform, the cross-waveguide is an extremely core device. If the loss value of a cross-waveguide is 0.3 dB, if the number of cross-waveguides is 100 in one switch matrix, the loss caused by only the cross-waveguide reaches 30 dB, which is a very serious loss. Therefore, it is necessary to reduce the loss of the cross-waveguide.
  • the direct crossover structure of the waveguide is adopted. Due to the direct straddle of the waveguide, the abrupt change of the spatial structure of the device causes the divergence of the beam, and still generates a large cross-wave loss.
  • Embodiments of the present invention provide a waveguide device capable of effectively reducing transmission loss in a waveguide.
  • a waveguide device comprising: a first waveguide structure composed of a first straight waveguide, a first curved waveguide, and a second straight waveguide, the first straight waveguide and the second straight waveguide passing through The first curved waveguide is connected; the second waveguide structure is composed of a third straight waveguide, a second curved waveguide, and a fourth straight waveguide, and the third straight waveguide and the fourth straight waveguide pass through the second curved waveguide Connected; wherein the first waveguide structure and the second waveguide structure are coupled.
  • the second straight waveguide and the fourth straight waveguide are parallel in a first direction, the second straight waveguide and the fourth The distance between the straight waveguides in the second direction is greater than zero and less than the wavelength of the light beam transmitted at the waveguide device, the first direction being perpendicular to the second direction, the first waveguide structure and the first The coupling portion between the two waveguide structures has an odd multiple of the coupling length.
  • the length of the coupling portion between the first waveguide structure and the second waveguide structure is a coupling length .
  • the first straight waveguide, the second straight waveguide, the third straight waveguide, The fourth straight waveguide, the first curved waveguide, and the second curved waveguide are all single mode waveguides.
  • any one of the first to third possible implementations of the first aspect in a fourth possible implementation of the first aspect, the first light beam input from the first straight waveguide Output from the third straight waveguide.
  • any one of the first to third possible implementations of the first aspect in a fifth possible implementation of the first aspect, the second light beam input from the second straight waveguide Output from the fourth straight waveguide.
  • any one of the first to third possible implementations of the first aspect in a sixth possible implementation of the first aspect, the third light beam input from the third straight waveguide Output from the second straight waveguide.
  • any one of the first to third possible implementations of the first aspect in a seventh possible implementation of the first aspect, the fourth beam input from the fourth straight waveguide Output from the first straight waveguide.
  • any one of the first to seventh possible implementations of the first aspect, in the eighth possible implementation of the first aspect, the first straight waveguide and the second straight waveguide are mutually Vertically, the third straight waveguide and the fourth straight waveguide are perpendicular to each other.
  • a chip comprising the waveguide device provided by the first aspect.
  • the waveguide device of the embodiment of the present invention adopts a structure based on the waveguide coupling principle, the direct straddle of the waveguide is avoided to cause a sudden change in the spatial structure of the device, so that the transmission loss is effectively reduced at the time of transmission.
  • FIG. 1 is a schematic structural view of a waveguide device in accordance with an embodiment of the present invention.
  • FIG. 2 is a structural schematic view of a waveguide device in accordance with another embodiment of the present invention.
  • FIG. 2A is a structural schematic view of a waveguide device in accordance with another embodiment of the present invention.
  • FIG. 3 is a structural schematic view of a waveguide device in accordance with still another embodiment of the present invention.
  • FIG. 4 is a schematic diagram showing the power distribution of a transmission beam according to still another embodiment of the present invention.
  • FIG. 5 is a schematic diagram showing a power distribution of a transmission beam according to still another embodiment of the present invention.
  • Figure 6 is a schematic illustration of the relationship between exit end loss and beam wavelength in accordance with yet another embodiment of the present invention.
  • the waveguide device 100 of FIG. 1 includes a first waveguide structure 150 composed of a first straight waveguide 110, a first curved waveguide 101, and a second straight waveguide 120, the first straight waveguide 110 and the second straight waveguide 120 passing through the first curved waveguide 101 phase connection;
  • the second waveguide structure 160 is composed of a third straight waveguide 130, a second curved waveguide 102, and a fourth straight waveguide 140, and the third straight waveguide 130 and the fourth straight waveguide 140 are connected by the second curved waveguide 102; The waveguide structure 150 and the second waveguide structure 160 are coupled.
  • the first straight waveguide and the second straight waveguide may be perpendicular to each other or may be other angles; similarly, the third straight waveguide and the fourth straight waveguide may be perpendicular to each other or may be at other angles.
  • the straight waveguide and the curved waveguide appearing herein may be single mode waveguides or multimode waveguides. Preferably, all of the waveguides are single mode waveguides.
  • the waveguide in the text can be made of any waveguide material, for example, the core layer is made of silicon and the cladding layer is made of silicon dioxide. High refractive index contrast of silicon light It can be applied to large-scale high-density integration; at the same time, it can also utilize the mature complementary metal oxide semiconductor process of the electric chip, which makes silicon light unique.
  • the first waveguide structure and the second waveguide structure are coupled, and the waveguide device may have different functions based on the length of the coupling portion.
  • the function of the cross-waveguide can be achieved when the beam is ultimately coupled to the second waveguide structure for output, or when the second waveguide structure is ultimately coupled to the first waveguide structure for output.
  • the beam is coupled between the two waveguide structures, it is still coupled back to the input waveguide structure, for example, from the first waveguide structure input, still output from the first waveguide structure;
  • the second waveguide structure input is still output from the second waveguide structure, where the waveguide can be used to change the direction of the light.
  • the waveguide device of the embodiment of the present invention adopts a structure based on the waveguide coupling principle, the direct straddle of the waveguide avoids abrupt changes in the spatial structure of the device, and thus the transmission loss is effectively reduced when the beam is transmitted.
  • the waveguide device 200 of FIG. 2 includes a first waveguide structure 250 composed of a first straight waveguide 210, a first curved waveguide 201, and a second straight waveguide 220, and the first straight waveguide 210 and the second straight waveguide 220 pass through the first curved waveguide 201 connected;
  • the second waveguide structure 260 is composed of a third straight waveguide 230, a second curved waveguide 202, and a fourth straight waveguide 240.
  • the third straight waveguide 230 and the fourth straight waveguide 240 are connected by the second curved waveguide 202;
  • the waveguide structure 250 is coupled to the second waveguide structure 260,
  • the second straight waveguide 220 and the fourth straight waveguide 240 are parallel in the first direction, and the distance between the second straight waveguide 220 and the fourth straight waveguide 240 in the second direction is greater than zero and less than
  • the wavelength of the light beam transmitted by the waveguide device is perpendicular to the first direction and the second direction, and the coupling portion between the first waveguide structure 250 and the second waveguide structure 260 has an odd multiple of the coupling length.
  • the waveguide device of the embodiment of the present invention adopts a structure based on the waveguide coupling principle, the direct straddle of the waveguide avoids abrupt changes in the spatial structure of the device, and thus the transmission loss is effectively reduced when the beam is transmitted as a cross-waveguide.
  • the waveguide device of the embodiment of the present invention utilizes the principle of mode coupling to form a parallel structure of the waveguide in the intersection region instead of directly straddle, thereby avoiding abrupt changes in the spatial structure of the waveguide, suppressing the divergence of the beam, and making it more Low transmission loss.
  • the waveguide device of the embodiment of the present invention has a simple structure and is easy to manufacture.
  • the coupling portion has an odd multiple coupling length, the light beam input from the A terminal in Fig. 2 can be output from the C terminal, and the light beam input from the B terminal can be from the D terminal. Output.
  • the coupling length is the distance between the start of the coupling of the light beam from a certain waveguide structure (ie, the position at which the light intensity begins to decrease) to the position at which the light beam first becomes zero in the waveguide structure, or
  • the distance between where a waveguide beam begins to appear at the coupled beam (ie, where the intensity of the light appears) to where the intensity first reaches its maximum, for example, L1 in Figure 2A corresponding to the embodiment of Figure 2 is the coupling length.
  • the coupling portion refers to the portion of the beam between a coupling coupling and an ending coupling within a waveguide structure.
  • the length of the coupling portion is the distance between the position at which the light intensity changes from the start of the coupling to the position at which the light intensity at the end of the coupling is constant.
  • it mainly depends on the distance between the second straight waveguide and the second straight waveguide in the first direction, that is, mainly depends on the connection between the first curved waveguide and the second straight waveguide in the fourth straight waveguide and the second bending The distance between the waveguides in the first direction.
  • the distance can be approximately considered to be the length of the coupling portion.
  • L2 in Fig. 2A is the length of the coupling portion, and the width of the light beam indicates the light intensity.
  • the length of the coupling portion is three times the length of the coupling, and the light beam couples the light beam into the second waveguide structure through the coupling portion in the first waveguide structure.
  • the length of the coupling portion is one time the coupling length.
  • the coupling portion in the figure has a coupling length of three times. From the intensity of the light indicated by the width of the beam, it is known that the beam is coupled from the second straight waveguide to the fourth straight waveguide at a one-time coupling length in the coupling portion, and from the fourth straight waveguide to the second straight waveguide at the double coupling length And coupling from the second straight waveguide to the fourth straight waveguide at the triple coupling length.
  • the length of the coupling portion is equal to an odd multiple of the coupling length between the second straight waveguide and the fourth straight waveguide, the function of the ideal cross-waveguide can be achieved with very little energy loss. Even when the length and coupling of the coupling part When there is a tolerance within the engineering margin between the odd multiples of the length, the function of the cross-waveguide can still be well realized.
  • the second straight waveguide is adjacent to the fourth straight waveguide to maximize the coupling effect while reducing the size of the waveguide.
  • the distance between the first connection and the second connection in the first direction is equal to the coupling length between the second straight waveguide and the fourth straight waveguide, so that the loss of energy can be minimized.
  • the size of the cross waveguide can be reduced.
  • the coupling length between the second input straight waveguide and the second input straight waveguide is used to generate coupling.
  • the transmission beam may be passed from the second straight waveguide into the fourth straight waveguide, or From the fourth straight waveguide to the second straight waveguide, in other words, when the odd-numbered coupling length is double the coupling length, it is possible to manufacture a smaller coupling length to reduce the size of the waveguide device.
  • the light beam in the second straight waveguide is alternately transmitted between the two parallel waveguides multiple times, eventually entering the fourth waveguide, or vice versa.
  • the waveguide device 300 of FIG. 3 includes a first waveguide structure 350 composed of a first straight waveguide 310, a first curved waveguide 301, and a second straight waveguide 320, and the first straight waveguide 310 and the second straight waveguide 320 pass through the first curved waveguide 301 connected;
  • the second waveguide structure 360 is composed of a third straight waveguide 330, a second curved waveguide 302, and a fourth straight waveguide 340, and the third straight waveguide 330 and the fourth straight waveguide 340 are connected by the second curved waveguide 302;
  • first waveguide structure 350 and the second waveguide structure 360 are coupled, the second straight waveguide 320 and the fourth straight waveguide 340 are parallel in the first direction, and the second straight waveguide 320 and the fourth straight waveguide 340 are in the second
  • the distance in the direction is greater than zero and less than the wavelength of the beam transmitted at the waveguide, the first direction being perpendicular to the second direction.
  • the coupling portion between the first waveguide structure 350 and the second waveguide structure 360 has an odd multiple of the coupling length.
  • first straight waveguide and the second straight waveguide are perpendicular to each other, and the third straight waveguide and the fourth straight waveguide are perpendicular to each other.
  • the first straight waveguide and the second straight waveguide are perpendicular to each other, and the third straight waveguide and the fourth straight waveguide are perpendicular to each other. Therefore, the problem of the intersection between the transmitted beams when used as a cross-waveguide can be solved to the utmost.
  • the waveguide can be of any waveguide material, such as a core.
  • the layer is made of silicon and the cladding is made of silicon dioxide.
  • the second straight waveguide is adjacent to the fourth straight waveguide to maximize the coupling effect while reducing the size of the waveguide.
  • the coupling length between the second input straight waveguide and the second input straight waveguide is used to generate coupling.
  • the transmission beam may be from the second straight waveguide into the fourth straight waveguide, or from the fourth straight
  • the waveguide is routed into the second straight waveguide such that a smaller coupling length can be made to reduce the size of the waveguide. It is also possible that the light beam in the second straight waveguide is alternately transmitted between the two parallel waveguides multiple times, eventually entering the fourth waveguide, or vice versa.
  • the waveguide device of the embodiment of the present invention employs a structure based on the waveguide coupling principle, the direct straddle of the waveguide avoids abrupt changes in the spatial structure of the device, and thus the transmission loss is effectively reduced when transmitted as a cross-waveguide.
  • the first light beam input from the first straight waveguide may be output from the third straight waveguide.
  • the second beam input from the second straight waveguide may be output from the fourth straight waveguide.
  • the third beam input from the third straight waveguide may be output from the second straight waveguide.
  • the fourth beam input from the fourth straight waveguide may be output from the first straight waveguide.
  • FIG. 4 is a schematic diagram of the power distribution of the transmitted beam in the embodiment according to FIG. 3.
  • Fig. 4 shows the power transmission distribution state of light when light is input from the left end to the first straight waveguide.
  • the light transmitted in the horizontal direction passes through the ninety-degree curved waveguide, the propagation direction is deflected, and the second straight waveguide is coupled with the straight waveguide of the fourth waveguide, and the optical power is fully coupled at this time.
  • the light After entering the fourth waveguide, the light is again transmitted in the horizontal direction after passing through the third straight waveguide.
  • Figure 5 is a schematic illustration of the power distribution of another transmitted beam in accordance with the embodiment of Figure 3.
  • Fig. 5 shows the power transmission distribution state of light when the second straight waveguide is input from the upper end of the device.
  • the light is transmitted in the vertical direction at the second straight waveguide to be mode-coupled with the fourth straight waveguide, at which time the optical power is fully coupled into the fourth straight waveguide and continues to be transmitted.
  • Figure 6 is a schematic illustration of the relationship between exit end loss and beam wavelength in accordance with yet another embodiment of the present invention.
  • the device loss is about 0.0036 dB, which is about an order of magnitude lower than the loss of the prior art cross-waveguide.
  • the coupled mode theory is wavelength dependent, and both the coupling length and the coupling efficiency vary with wavelength.
  • the exit end loss is about 0.006 dB.
  • the loss of the device is wavelength dependent, its loss is still lower than the current technology at a wavelength change of 4 nanometers.
  • the ultra-low loss structure of this patent can be applied to Dense Wavelength Division Multiplexing (DWDM) systems.
  • DWDM Dense Wavelength Division Multiplexing

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Integrated Circuits (AREA)

Abstract

A waveguide device and a chip comprising same. The waveguide device comprises a first waveguide structure (150, 250, 350) and a second waveguide structure (160, 260, 360) which are coupled. The first waveguide structure (150, 250, 350) is constituted by a first straight waveguide (110, 210, 310), a first bent waveguide (101, 201, 301) and a second straight waveguide (120, 220, 320), and the first straight waveguide (110, 210, 310) and the second straight waveguide (120, 220, 320) are connected via the first bent waveguide (101, 201, 301). The second waveguide structure (160, 260, 360) is constituted by a third straight waveguide (130, 230, 330), a second bent waveguide (102, 202, 302) and a fourth straight waveguide (140, 240, 340), and the third straight waveguide (130, 230, 330) and the fourth straight waveguide (140, 240, 340) are connected via the second bent waveguide (102, 202, 302). The waveguide device avoids the mutation of the spatial structure of the device resulting from the direct crossing of the waveguides, thus reducing the transmission loss effectively when the light beam is transmitting.

Description

波导装置Waveguide 技术领域Technical field
本发明的实施例涉及光学领域,并尤其涉及一种波导装置。Embodiments of the present invention relate to the field of optics and, in particular, to a waveguide device.
背景技术Background technique
自第一台激光器问世以后,人类的通信发生了深刻的变革。光作为信息的载体,以其高速、稳定的特性,使人们的沟通变得及时而便捷。随着科技的发展,传统的模块光学逐渐显示出其在功耗、占空比方面的缺点。光路设计曾在多种材料中尝试过集成,但多受制于工艺而发展有限。而硅光由于其与电路工艺的兼容而备受关注,人们期望集成光学能在硅基上走过和电学同样的道路。Since the advent of the first laser, human communication has undergone profound changes. As a carrier of information, light makes people's communication timely and convenient with its high speed and stable characteristics. With the development of technology, traditional module optics gradually show its shortcomings in power consumption and duty cycle. Optical path design has tried to integrate in a variety of materials, but limited by the process and limited development. While silicon light has received much attention due to its compatibility with circuit processes, it is expected that integrated optical energy will travel the same way as electricity on silicon.
硅光高的折射率对比度,使得其可以应用于大规模高密度的集成;同时,它还可以利用电芯片成熟的互补金属氧化物半导体工艺,这些使得硅光独具优势。然而,光路却不具有电路的灵活性。在大规模的开关矩阵中,波导的交叉不可避免。在硅光平台中,交叉波导是一个极为核心的器件。若一个交叉波导的损耗值为0.3dB,若在一个开关矩阵中,交叉波导的数量为100个,则仅仅由交叉波导造成的损耗就达到30dB,这是很严重的损耗。所以,减小交叉波导的损耗就显得十分必要。The high refractive index contrast of silicon light makes it suitable for large-scale and high-density integration. At the same time, it can also utilize the mature complementary metal oxide semiconductor process of the electric chip, which makes silicon light unique. However, the optical path does not have the flexibility of the circuit. In large-scale switching matrices, the intersection of waveguides is unavoidable. In a silicon light platform, the cross-waveguide is an extremely core device. If the loss value of a cross-waveguide is 0.3 dB, if the number of cross-waveguides is 100 in one switch matrix, the loss caused by only the cross-waveguide reaches 30 dB, which is a very serious loss. Therefore, it is necessary to reduce the loss of the cross-waveguide.
在众多的交叉波导设计中,都采用了波导直接交叉的结构,由于波导的直接横跨导致器件空间结构的突变,会导致光束的发散,仍然会产生较大的交叉波导损耗。In many cross-waveguide designs, the direct crossover structure of the waveguide is adopted. Due to the direct straddle of the waveguide, the abrupt change of the spatial structure of the device causes the divergence of the beam, and still generates a large cross-wave loss.
发明内容Summary of the invention
本发明的实施例提供了一种波导装置,能够有效地减少波导中的传输损耗。Embodiments of the present invention provide a waveguide device capable of effectively reducing transmission loss in a waveguide.
第一方面,提供了一种波导装置,包括:第一波导结构,由第一直波导、第一弯曲波导和第二直波导构成,所述第一直波导和所述第二直波导通过所述第一弯曲波导相连接;第二波导结构,由第三直波导、第二弯曲波导和第四直波导构成,所述第三直波导和所述第四直波导通过所述第二弯曲波导相连接;其中,所述第一波导结构和所述第二波导结构耦合。 In a first aspect, a waveguide device is provided, comprising: a first waveguide structure composed of a first straight waveguide, a first curved waveguide, and a second straight waveguide, the first straight waveguide and the second straight waveguide passing through The first curved waveguide is connected; the second waveguide structure is composed of a third straight waveguide, a second curved waveguide, and a fourth straight waveguide, and the third straight waveguide and the fourth straight waveguide pass through the second curved waveguide Connected; wherein the first waveguide structure and the second waveguide structure are coupled.
结合第一方面,在第一方面的第一种可能的实现方式中,所述第二直波导与所述第四直波导在第一方向上平行,所述第二直波导与所述第四直波导之间的在第二方向上的距离大于零并且小于在所述波导装置传输的光束的波长,所述第一方向和所述第二方向垂直,所述第一波导结构和所述第二波导结构之间的耦合部分具有奇数倍的耦合长度。In conjunction with the first aspect, in a first possible implementation manner of the first aspect, the second straight waveguide and the fourth straight waveguide are parallel in a first direction, the second straight waveguide and the fourth The distance between the straight waveguides in the second direction is greater than zero and less than the wavelength of the light beam transmitted at the waveguide device, the first direction being perpendicular to the second direction, the first waveguide structure and the first The coupling portion between the two waveguide structures has an odd multiple of the coupling length.
结合第一方面的第一种可能的实现方式,在第一方面的第二种可能的实现方式中,所述第一波导结构和所述第二波导结构之间的耦合部分的长度为耦合长度。In conjunction with the first possible implementation of the first aspect, in a second possible implementation of the first aspect, the length of the coupling portion between the first waveguide structure and the second waveguide structure is a coupling length .
结合第一方面、第一方面的第一种或第二种可能的实现方式,在第一方面的第三种可能的实现方式中,第一直波导、第二直波导、第三直波导、第四直波导、第一弯曲波导和第二弯曲波导均为单模波导。With reference to the first aspect, the first or second possible implementation manner of the first aspect, in a third possible implementation manner of the first aspect, the first straight waveguide, the second straight waveguide, the third straight waveguide, The fourth straight waveguide, the first curved waveguide, and the second curved waveguide are all single mode waveguides.
结合第一方面、第一方面的第一种至第三种中的任一种可能的实现方式,在第一方面的第四种可能的实现方式中,从第一直波导输入的第一光束从第三直波导输出。With reference to the first aspect, any one of the first to third possible implementations of the first aspect, in a fourth possible implementation of the first aspect, the first light beam input from the first straight waveguide Output from the third straight waveguide.
结合第一方面、第一方面的第一种至第三种中的任一种可能的实现方式,在第一方面的第五种可能的实现方式中,从第二直波导输入的第二光束从第四直波导输出。With reference to the first aspect, any one of the first to third possible implementations of the first aspect, in a fifth possible implementation of the first aspect, the second light beam input from the second straight waveguide Output from the fourth straight waveguide.
结合第一方面、第一方面的第一种至第三种中的任一种可能的实现方式,在第一方面的第六种可能的实现方式中,从第三直波导输入的第三光束从第二直波导输出。With reference to the first aspect, any one of the first to third possible implementations of the first aspect, in a sixth possible implementation of the first aspect, the third light beam input from the third straight waveguide Output from the second straight waveguide.
结合第一方面、第一方面的第一种至第三种中的任一种可能的实现方式,在第一方面的第七种可能的实现方式中,从第四直波导输入的第四光束从第一直波导输出。In conjunction with the first aspect, any one of the first to third possible implementations of the first aspect, in a seventh possible implementation of the first aspect, the fourth beam input from the fourth straight waveguide Output from the first straight waveguide.
结合第一方面、第一方面的第一种至第七种中的任一种可能的实现方式,在第一方面的第八种可能的实现方式中,第一直波导和第二直波导互相垂直,第三直波导和第四直波导互相垂直。With reference to the first aspect, any one of the first to seventh possible implementations of the first aspect, in the eighth possible implementation of the first aspect, the first straight waveguide and the second straight waveguide are mutually Vertically, the third straight waveguide and the fourth straight waveguide are perpendicular to each other.
第二方面、提供了一种芯片,包括第一方面提供的波导装置。In a second aspect, a chip is provided, comprising the waveguide device provided by the first aspect.
本发明的实施例的波导装置由于采用了基于波导耦合原理的结构,避免了波导的直接横跨导致器件空间结构的突变,因此在进行传输时有效地减少了传输损耗。 Since the waveguide device of the embodiment of the present invention adopts a structure based on the waveguide coupling principle, the direct straddle of the waveguide is avoided to cause a sudden change in the spatial structure of the device, so that the transmission loss is effectively reduced at the time of transmission.
附图说明DRAWINGS
为了更清楚地说明本发明实施例的技术方案,下面将对本发明实施例中所需要使用的附图作简单地介绍,显而易见地,下面所描述的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to more clearly illustrate the technical solutions of the embodiments of the present invention, the drawings to be used in the embodiments of the present invention will be briefly described below. It is obvious that the drawings described below are only some embodiments of the present invention, Those skilled in the art can also obtain other drawings based on these drawings without paying any creative work.
图1为根据本发明的一个实施例的波导装置的结构性示意图。1 is a schematic structural view of a waveguide device in accordance with an embodiment of the present invention.
图2为根据本发明的另一实施例的波导装置的结构性示意图。2 is a structural schematic view of a waveguide device in accordance with another embodiment of the present invention.
图2A为根据本发明的另一实施例的波导装置的结构性示意图。2A is a structural schematic view of a waveguide device in accordance with another embodiment of the present invention.
图3为根据本发明的再一实施例的波导装置的结构性示意图。3 is a structural schematic view of a waveguide device in accordance with still another embodiment of the present invention.
图4为根据本发明的再一实施例的传输光束的功率分布示意图。4 is a schematic diagram showing the power distribution of a transmission beam according to still another embodiment of the present invention.
图5为根据本发明的再一实施例的传输光束的功率分布示意图。FIG. 5 is a schematic diagram showing a power distribution of a transmission beam according to still another embodiment of the present invention.
图6为根据本发明的又一实施例的出射端损耗和光束波长之间关系的示意图。Figure 6 is a schematic illustration of the relationship between exit end loss and beam wavelength in accordance with yet another embodiment of the present invention.
具体实施方式detailed description
下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例是本发明的一个实施例,而不是全部实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动的前提下所获得的所有其他实施例,都应属于本发明保护的范围。The technical solutions in the embodiments of the present invention are clearly and completely described in conjunction with the accompanying drawings in the embodiments of the present invention. It is obvious that the described embodiments are an embodiment of the present invention, and not all embodiments. All other embodiments obtained by those skilled in the art based on the embodiments of the present invention without creative efforts shall fall within the scope of the present invention.
图1为根据本发明的一个实施例的波导装置的结构性示意图。图1的波导装置100包括:第一波导结构150,由第一直波导110、第一弯曲波导101和第二直波导120构成,第一直波导110和第二直波导120通过第一弯曲波导101相连接;1 is a schematic structural view of a waveguide device in accordance with an embodiment of the present invention. The waveguide device 100 of FIG. 1 includes a first waveguide structure 150 composed of a first straight waveguide 110, a first curved waveguide 101, and a second straight waveguide 120, the first straight waveguide 110 and the second straight waveguide 120 passing through the first curved waveguide 101 phase connection;
第二波导结构160,由第三直波导130、第二弯曲波导102和第四直波导140构成,第三直波导130和第四直波导140通过第二弯曲波导102相连接;其中,第一波导结构150和第二波导结构160耦合。The second waveguide structure 160 is composed of a third straight waveguide 130, a second curved waveguide 102, and a fourth straight waveguide 140, and the third straight waveguide 130 and the fourth straight waveguide 140 are connected by the second curved waveguide 102; The waveguide structure 150 and the second waveguide structure 160 are coupled.
应理解,对于波导装置,第一直波导和第二直波导可以互相垂直,也可以是成其他的角度;相似地,第三直波导和第四直波导互相垂直,也可以是成其他角度。文中出现的直波导和弯曲波导可以为单模波导也可以为多模波导,优选地,所有的波导均为单模波导。文中的波导可以采用任何波导材料,例如芯层采用硅制成,包层采用二氧化硅制成。硅光高的折射率对比度,使 得其可以应用于大规模高密度的集成;同时,它还可以利用电芯片成熟的互补金属氧化物半导体工艺,这些使得硅光独具优势。It should be understood that for the waveguide device, the first straight waveguide and the second straight waveguide may be perpendicular to each other or may be other angles; similarly, the third straight waveguide and the fourth straight waveguide may be perpendicular to each other or may be at other angles. The straight waveguide and the curved waveguide appearing herein may be single mode waveguides or multimode waveguides. Preferably, all of the waveguides are single mode waveguides. The waveguide in the text can be made of any waveguide material, for example, the core layer is made of silicon and the cladding layer is made of silicon dioxide. High refractive index contrast of silicon light It can be applied to large-scale high-density integration; at the same time, it can also utilize the mature complementary metal oxide semiconductor process of the electric chip, which makes silicon light unique.
还应理解,第一波导结构和第二波导结构耦合,基于耦合部分的长度的不同,该波导装置可以具有不同的功能。例如,光束从第一波导结构最终耦合至第二波导结构而输出,或者从第二波导结构最终耦合至第一波导结构而输出时,可以实现交叉波导的功能。对于有些的耦合部分的特定的长度,当光束在两个波导结构之间耦合时,仍然耦合回输入时的波导结构,例如,从第一波导结构输入,仍然从第一波导结构输出;或者从第二波导结构输入,仍然从第二波导结构输出,这时该波导装置可以用于改变光线的方向。It should also be understood that the first waveguide structure and the second waveguide structure are coupled, and the waveguide device may have different functions based on the length of the coupling portion. For example, the function of the cross-waveguide can be achieved when the beam is ultimately coupled to the second waveguide structure for output, or when the second waveguide structure is ultimately coupled to the first waveguide structure for output. For a particular length of some coupling portions, when the beam is coupled between the two waveguide structures, it is still coupled back to the input waveguide structure, for example, from the first waveguide structure input, still output from the first waveguide structure; The second waveguide structure input is still output from the second waveguide structure, where the waveguide can be used to change the direction of the light.
本发明的实施例的波导装置由于采用了基于波导耦合原理的结构,避免了波导的直接横跨导致器件空间结构的突变,因此在进行光束的传输时有效地减少了传输损耗。Since the waveguide device of the embodiment of the present invention adopts a structure based on the waveguide coupling principle, the direct straddle of the waveguide avoids abrupt changes in the spatial structure of the device, and thus the transmission loss is effectively reduced when the beam is transmitted.
图2为根据本发明的另一实施例的波导装置的结构性示意图。图2的波导装置200包括:第一波导结构250,由第一直波导210、第一弯曲波导201和第二直波导220构成,第一直波导210和第二直波导220通过第一弯曲波导201相连接;2 is a structural schematic view of a waveguide device in accordance with another embodiment of the present invention. The waveguide device 200 of FIG. 2 includes a first waveguide structure 250 composed of a first straight waveguide 210, a first curved waveguide 201, and a second straight waveguide 220, and the first straight waveguide 210 and the second straight waveguide 220 pass through the first curved waveguide 201 connected;
第二波导结构260,由第三直波导230、第二弯曲波导202和第四直波导240构成,第三直波导230和第四直波导240通过第二弯曲波导202相连接;其中,第一波导结构250和第二波导结构260耦合,The second waveguide structure 260 is composed of a third straight waveguide 230, a second curved waveguide 202, and a fourth straight waveguide 240. The third straight waveguide 230 and the fourth straight waveguide 240 are connected by the second curved waveguide 202; The waveguide structure 250 is coupled to the second waveguide structure 260,
在本实施例中,第二直波导220与第四直波导240在第一方向上平行,第二直波导220与第四直波导240之间的在第二方向上的距离大于零并且小于在波导装置传输的光束的波长,第一方向和第二方向垂直,第一波导结构250和第二波导结构260之间的耦合部分具有奇数倍的耦合长度。In this embodiment, the second straight waveguide 220 and the fourth straight waveguide 240 are parallel in the first direction, and the distance between the second straight waveguide 220 and the fourth straight waveguide 240 in the second direction is greater than zero and less than The wavelength of the light beam transmitted by the waveguide device is perpendicular to the first direction and the second direction, and the coupling portion between the first waveguide structure 250 and the second waveguide structure 260 has an odd multiple of the coupling length.
本发明的实施例的波导装置由于采用了基于波导耦合原理的结构,避免了波导的直接横跨导致器件空间结构的突变,因此在作为交叉波导进行光束的传输时有效地减少了传输损耗。Since the waveguide device of the embodiment of the present invention adopts a structure based on the waveguide coupling principle, the direct straddle of the waveguide avoids abrupt changes in the spatial structure of the device, and thus the transmission loss is effectively reduced when the beam is transmitted as a cross-waveguide.
换句话说,本发明实施例的波导装置利用模式耦合的原理,在交叉区域形成波导的平行结构而不是直接横跨,避免了波导空间结构的突变,在抑制了光束的发散,使其具有更低的传输损耗。另外,本发明实施例的波导装置结构简单,制作容易。另外,由于耦合部分具有奇数倍的耦合长度使得从图2中A端输入的光束可以从C端输出,同时从B端输入的光束可以从D端 输出。In other words, the waveguide device of the embodiment of the present invention utilizes the principle of mode coupling to form a parallel structure of the waveguide in the intersection region instead of directly straddle, thereby avoiding abrupt changes in the spatial structure of the waveguide, suppressing the divergence of the beam, and making it more Low transmission loss. In addition, the waveguide device of the embodiment of the present invention has a simple structure and is easy to manufacture. In addition, since the coupling portion has an odd multiple coupling length, the light beam input from the A terminal in Fig. 2 can be output from the C terminal, and the light beam input from the B terminal can be from the D terminal. Output.
应理解,耦合长度定义为L=π/2K,其中K为第一波导结构和第二波导结构之间的耦合系数,耦合长度与波长以及第二直波导与第四直波导之间的在第二方向上的距离相关。换句话说,耦合长度为光束从某一波导结构开始耦合(即光强开始减少的位置)到该光束第一次在该波导结构中的光强变为零的位置之间的距离,或者,在某一波导结构开始出现耦合光束处(即出现光强的位置)到光强第一次达到最大处之间的距离,例如与图2的实施例对应的图2A中的L1即为耦合长度。应理解,当第二直波导与第四直波导之间的在第二方向上的距离大于零并且小于在波导装置传输的光束的波长时,可以获得比较理想的耦合效果。It should be understood that the coupling length is defined as L=π/2K, where K is the coupling coefficient between the first waveguide structure and the second waveguide structure, the coupling length and the wavelength, and the second between the second straight waveguide and the fourth straight waveguide. The distance in the two directions is related. In other words, the coupling length is the distance between the start of the coupling of the light beam from a certain waveguide structure (ie, the position at which the light intensity begins to decrease) to the position at which the light beam first becomes zero in the waveguide structure, or The distance between where a waveguide beam begins to appear at the coupled beam (ie, where the intensity of the light appears) to where the intensity first reaches its maximum, for example, L1 in Figure 2A corresponding to the embodiment of Figure 2 is the coupling length. . It should be understood that a better coupling effect can be obtained when the distance between the second straight waveguide and the fourth straight waveguide in the second direction is greater than zero and less than the wavelength of the beam transmitted by the waveguide.
还应理解,耦合部分是指光束在某一波导结构内从开始耦合处到结束耦合处之间的部分。换句话说,耦合部分的长度为由开始耦合引起光强变化的位置到由耦合结束时的光强不变的位置之间的距离。通常情况下,主要取决于第二直波导和第二直波导在第一方向上的距离,即主要取决于第一弯曲波导与第二直波导之间的连接处于第四直波导和第二弯曲波导之间的连接处在第一方向上的距离。因此,对于图2以及图2A的实施例,可以近似地认为该距离为耦合部分的长度。It should also be understood that the coupling portion refers to the portion of the beam between a coupling coupling and an ending coupling within a waveguide structure. In other words, the length of the coupling portion is the distance between the position at which the light intensity changes from the start of the coupling to the position at which the light intensity at the end of the coupling is constant. Generally, it mainly depends on the distance between the second straight waveguide and the second straight waveguide in the first direction, that is, mainly depends on the connection between the first curved waveguide and the second straight waveguide in the fourth straight waveguide and the second bending The distance between the waveguides in the first direction. Thus, for the embodiment of Figures 2 and 2A, the distance can be approximately considered to be the length of the coupling portion.
在光束绝大部分从一个波导结构耦合到另一波导结构中的情况下,可以使得实现较理想的交叉波导的功能。In the case where most of the beam is coupled from one waveguide structure to another, a better function of the cross-waveguide can be achieved.
如图2A中的L2为耦合部分的长度,光束的宽度指示光强。在该图中,耦合部分的长度为耦合长度的三倍,光束在第一波导结构中通过耦合部分使光束耦合到第二波导结构中,实际上,由于光束绝大部分都是在直波导之间耦合的,因此当第一波导结构和第二波导结构之间的耦合部分具有奇数倍的耦合长度时,可以使传输带的损耗达到最小。优选地,耦合部分的长度为一倍的耦合长度。L2 in Fig. 2A is the length of the coupling portion, and the width of the light beam indicates the light intensity. In the figure, the length of the coupling portion is three times the length of the coupling, and the light beam couples the light beam into the second waveguide structure through the coupling portion in the first waveguide structure. In fact, since most of the light beam is in the straight waveguide Inter-coupled, so that when the coupling portion between the first waveguide structure and the second waveguide structure has an odd multiple of the coupling length, the loss of the transmission belt can be minimized. Preferably, the length of the coupling portion is one time the coupling length.
仍以图2A为例进行说明,图中的耦合部分具有三倍的耦合长度。从光束的宽度指示的光强,可知光束在耦合部分中的一倍耦合长度处从第二直波导耦合到第四直波导,在二倍耦合长度处从第四直波导耦合到第二直波导,在三倍耦合长度处再从第二直波导耦合到第四直波导。事实上,只要耦合部分的长度等于第二直波导和第四直波导之间的耦合长度的奇数倍,都可以以极小的能量损耗实现理想的交叉波导的功能。即使当耦合部分的长度与耦合 长度的奇数倍之间存在工程余量内允许的偏差时,仍然可以很好的实现交叉波导的功能。Still taking FIG. 2A as an example, the coupling portion in the figure has a coupling length of three times. From the intensity of the light indicated by the width of the beam, it is known that the beam is coupled from the second straight waveguide to the fourth straight waveguide at a one-time coupling length in the coupling portion, and from the fourth straight waveguide to the second straight waveguide at the double coupling length And coupling from the second straight waveguide to the fourth straight waveguide at the triple coupling length. In fact, as long as the length of the coupling portion is equal to an odd multiple of the coupling length between the second straight waveguide and the fourth straight waveguide, the function of the ideal cross-waveguide can be achieved with very little energy loss. Even when the length and coupling of the coupling part When there is a tolerance within the engineering margin between the odd multiples of the length, the function of the cross-waveguide can still be well realized.
应理解,作为优选的实施例,第二直波导与第四直波导靠近,以使耦合的效果最好,同时可以减小波导装置的尺寸。另外,作为优选的实施例,第一连接处和第二连接处在第一方向上的距离等于第二直波导和第四直波导之间的耦合长度,这样可以使能量的损失降到最小,同时可以减小交叉波导的尺寸。It should be understood that as a preferred embodiment, the second straight waveguide is adjacent to the fourth straight waveguide to maximize the coupling effect while reducing the size of the waveguide. In addition, as a preferred embodiment, the distance between the first connection and the second connection in the first direction is equal to the coupling length between the second straight waveguide and the fourth straight waveguide, so that the loss of energy can be minimized. At the same time, the size of the cross waveguide can be reduced.
还应理解,第二输入直波导与第二输入直波导之间的耦合长度用于产生耦合,作为优选的实施例,可以是使传输光束从第二直波导进入到第四直波导中,或者从第四直波导到第二直波导中,换句话说,当奇数倍的耦合长度为一倍的耦合长度时,可以使得制造较小的耦合长度以减小波导装置的尺寸。也可以是第二直波导中的光束在两个平行的波导之间交替传输多次,最终进入第四波导,或是相反。It should also be understood that the coupling length between the second input straight waveguide and the second input straight waveguide is used to generate coupling. As a preferred embodiment, the transmission beam may be passed from the second straight waveguide into the fourth straight waveguide, or From the fourth straight waveguide to the second straight waveguide, in other words, when the odd-numbered coupling length is double the coupling length, it is possible to manufacture a smaller coupling length to reduce the size of the waveguide device. It is also possible that the light beam in the second straight waveguide is alternately transmitted between the two parallel waveguides multiple times, eventually entering the fourth waveguide, or vice versa.
图3为根据本发明的再一实施例的波导装置的结构性示意图。图3的波导装置300包括:第一波导结构350,由第一直波导310、第一弯曲波导301和第二直波导320构成,第一直波导310和第二直波导320通过第一弯曲波导301相连接;3 is a structural schematic view of a waveguide device in accordance with still another embodiment of the present invention. The waveguide device 300 of FIG. 3 includes a first waveguide structure 350 composed of a first straight waveguide 310, a first curved waveguide 301, and a second straight waveguide 320, and the first straight waveguide 310 and the second straight waveguide 320 pass through the first curved waveguide 301 connected;
第二波导结构360,由第三直波导330、第二弯曲波导302和第四直波导340构成,第三直波导330和第四直波导340通过第二弯曲波导302相连接;The second waveguide structure 360 is composed of a third straight waveguide 330, a second curved waveguide 302, and a fourth straight waveguide 340, and the third straight waveguide 330 and the fourth straight waveguide 340 are connected by the second curved waveguide 302;
其中,第一波导结构350和第二波导结构360耦合,第二直波导320与第四直波导340在第一方向上平行,第二直波导320与第四直波导340之间的在第二方向上的距离大于零并且小于在波导装置传输的光束的波长,第一方向与第二方向垂直。第一波导结构350和第二波导结构360之间的耦合部分具有奇数倍的耦合长度.Wherein, the first waveguide structure 350 and the second waveguide structure 360 are coupled, the second straight waveguide 320 and the fourth straight waveguide 340 are parallel in the first direction, and the second straight waveguide 320 and the fourth straight waveguide 340 are in the second The distance in the direction is greater than zero and less than the wavelength of the beam transmitted at the waveguide, the first direction being perpendicular to the second direction. The coupling portion between the first waveguide structure 350 and the second waveguide structure 360 has an odd multiple of the coupling length.
在本实施例中,第一直波导和第二直波导互相垂直,第三直波导和第四直波导互相垂直。In this embodiment, the first straight waveguide and the second straight waveguide are perpendicular to each other, and the third straight waveguide and the fourth straight waveguide are perpendicular to each other.
应理解,由于在本实施例的波导装置中,第一直波导和第二直波导互相垂直,第三直波导和第四直波导互相垂直。因此可以最大限度地解决了作为交叉波导使用时传输光束之间交叉的问题。It should be understood that, in the waveguide device of the present embodiment, the first straight waveguide and the second straight waveguide are perpendicular to each other, and the third straight waveguide and the fourth straight waveguide are perpendicular to each other. Therefore, the problem of the intersection between the transmitted beams when used as a cross-waveguide can be solved to the utmost.
还应理解,与图1的实施例相似,波导可以采用任何波导材料,例如芯 层采用硅制成,包层采用二氧化硅制成。与图2的实施例相似,作为优先的实施例,第二直波导与第四直波导靠近,以使耦合的效果最好,同时可以减小波导装置的尺寸。第二输入直波导与第二输入直波导之间的耦合长度用于产生耦合,作为优选的实施例,可以是使传输光束从第二直波导进入到第四直波导中,或者从第四直波导到第二直波导中,这样可以使得制造较小的耦合长度以减小波导装置的尺寸。也可以是第二直波导中的光束在两个平行的波导之间交替传输多次,最终进入第四波导,或是相反。It should also be understood that similar to the embodiment of Figure 1, the waveguide can be of any waveguide material, such as a core. The layer is made of silicon and the cladding is made of silicon dioxide. Similar to the embodiment of Fig. 2, as a preferred embodiment, the second straight waveguide is adjacent to the fourth straight waveguide to maximize the coupling effect while reducing the size of the waveguide. The coupling length between the second input straight waveguide and the second input straight waveguide is used to generate coupling. As a preferred embodiment, the transmission beam may be from the second straight waveguide into the fourth straight waveguide, or from the fourth straight The waveguide is routed into the second straight waveguide such that a smaller coupling length can be made to reduce the size of the waveguide. It is also possible that the light beam in the second straight waveguide is alternately transmitted between the two parallel waveguides multiple times, eventually entering the fourth waveguide, or vice versa.
本发明的实施例的波导装置由于采用了基于波导耦合原理的结构,避免了波导的直接横跨导致器件空间结构的突变,因此在作为交叉波导进行传输时有效地减少了传输损耗。Since the waveguide device of the embodiment of the present invention employs a structure based on the waveguide coupling principle, the direct straddle of the waveguide avoids abrupt changes in the spatial structure of the device, and thus the transmission loss is effectively reduced when transmitted as a cross-waveguide.
根据本发明的实施例,从第一直波导输入的第一光束可以从第三直波导输出。从第二直波导输入的第二光束可以从第四直波导输出。从第三直波导输入的第三光束可以从第二直波导输出。从第四直波导输入的第四光束可以从第一直波导输出。According to an embodiment of the invention, the first light beam input from the first straight waveguide may be output from the third straight waveguide. The second beam input from the second straight waveguide may be output from the fourth straight waveguide. The third beam input from the third straight waveguide may be output from the second straight waveguide. The fourth beam input from the fourth straight waveguide may be output from the first straight waveguide.
具体地,图4为根据图3的实施例中的传输光束的功率分布示意图。针对图3中的波导,图4示出了光从左端输入第一直波导时光的功率传输分布状态。当光从左端输入时,在水平方向传输的光经九十度弯曲波导,传播方向发生偏折,在第二直波导处与第四波导的直波导发生模式耦合,此时的光功率完全耦合进第四波导,并经第三直波导后光重新在水平方向传输。Specifically, FIG. 4 is a schematic diagram of the power distribution of the transmitted beam in the embodiment according to FIG. 3. With respect to the waveguide in Fig. 3, Fig. 4 shows the power transmission distribution state of light when light is input from the left end to the first straight waveguide. When light is input from the left end, the light transmitted in the horizontal direction passes through the ninety-degree curved waveguide, the propagation direction is deflected, and the second straight waveguide is coupled with the straight waveguide of the fourth waveguide, and the optical power is fully coupled at this time. After entering the fourth waveguide, the light is again transmitted in the horizontal direction after passing through the third straight waveguide.
图5为根据图3的实施例的另一传输光束的功率分布示意图。针对图3中的波导,图5示出了从器件上端输入第二直波导时光的功率传输分布状态。当光从上端输入时,光在垂直方向上传输在第二直波导处与第四直波导发生模式耦合,此时的光功率完全耦合进第四直波导,并继续传输。Figure 5 is a schematic illustration of the power distribution of another transmitted beam in accordance with the embodiment of Figure 3. With respect to the waveguide of Fig. 3, Fig. 5 shows the power transmission distribution state of light when the second straight waveguide is input from the upper end of the device. When light is input from the upper end, the light is transmitted in the vertical direction at the second straight waveguide to be mode-coupled with the fourth straight waveguide, at which time the optical power is fully coupled into the fourth straight waveguide and continues to be transmitted.
图6为根据本发明的又一实施例的出射端损耗和光束波长之间关系的示意图。从图6中可以看出,在1.55um的最佳波长时,器件损耗为0.0036dB左右,这一损耗值比现有技术交叉波导的损耗值大约低一个数量级左右。耦合模理论是和波长相关的,耦合长度和耦合效率均会随波长的改变而变化。从图上可以看出,当波长大约变化4个nm的时候,出射端损耗大约为0.006dB左右。尽管器件的损耗与波长相关,但在4个纳米的波长改变下,其损耗仍旧比当下的技术低。本专利的超低损耗结构,可应用于密集型光波复用(Dense Wavelength Division Multiplexing,DWDM)系统。 Figure 6 is a schematic illustration of the relationship between exit end loss and beam wavelength in accordance with yet another embodiment of the present invention. As can be seen from Figure 6, at an optimum wavelength of 1.55 um, the device loss is about 0.0036 dB, which is about an order of magnitude lower than the loss of the prior art cross-waveguide. The coupled mode theory is wavelength dependent, and both the coupling length and the coupling efficiency vary with wavelength. As can be seen from the figure, when the wavelength changes by about 4 nm, the exit end loss is about 0.006 dB. Although the loss of the device is wavelength dependent, its loss is still lower than the current technology at a wavelength change of 4 nanometers. The ultra-low loss structure of this patent can be applied to Dense Wavelength Division Multiplexing (DWDM) systems.
以上仅为本发明技术方案的较佳实施例而已,并非用于限定本发明的保护范围。凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。 The above is only a preferred embodiment of the technical solution of the present invention, and is not intended to limit the scope of the present invention. Any modifications, equivalent substitutions, improvements, etc. made within the spirit and scope of the present invention are intended to be included within the scope of the present invention.

Claims (10)

  1. 一种波导装置,其特征在于,包括:第一波导结构,由第一直波导、第一弯曲波导和第二直波导构成,所述第一直波导和所述第二直波导通过所述第一弯曲波导相连接;A waveguide device, comprising: a first waveguide structure composed of a first straight waveguide, a first curved waveguide, and a second straight waveguide, wherein the first straight waveguide and the second straight waveguide pass the first a curved waveguide connected;
    第二波导结构,由第三直波导、第二弯曲波导和第四直波导构成,所述第三直波导和所述第四直波导通过所述第二弯曲波导相连接;a second waveguide structure, which is composed of a third straight waveguide, a second curved waveguide, and a fourth straight waveguide, wherein the third straight waveguide and the fourth straight waveguide are connected by the second curved waveguide;
    其中,所述第一波导结构和所述第二波导结构耦合。Wherein the first waveguide structure and the second waveguide structure are coupled.
  2. 根据权利要求1所述的装置,其特征在于,所述第二直波导与所述第四直波导在第一方向上平行,所述第二直波导与所述第四直波导之间的在第二方向上的距离大于零并且小于在所述波导装置传输的光束的波长,所述第一方向和所述第二方向垂直,所述第一波导结构和所述第二波导结构之间的耦合部分具有奇数倍的耦合长度。The apparatus according to claim 1, wherein said second straight waveguide is parallel to said fourth straight waveguide in a first direction, and wherein said second straight waveguide and said fourth straight waveguide The distance in the second direction is greater than zero and less than the wavelength of the beam transmitted at the waveguide device, the first direction being perpendicular to the second direction, between the first waveguide structure and the second waveguide structure The coupling portion has an odd multiple of the coupling length.
  3. 根据权利要求2所述的装置,其特征在于,所述第一波导结构和所述第二波导结构之间的耦合部分的长度为耦合长度。The apparatus according to claim 2, wherein a length of the coupling portion between the first waveguide structure and the second waveguide structure is a coupling length.
  4. 根据权利要求1-3中的任一项所述的装置,其特征在于,所述第一直波导、所述第二直波导、所述第三直波导、所述第四直波导、所述第一弯曲波导和所述第二弯曲波导均为单模波导。The apparatus according to any one of claims 1 to 3, wherein the first straight waveguide, the second straight waveguide, the third straight waveguide, the fourth straight waveguide, the The first curved waveguide and the second curved waveguide are both single mode waveguides.
  5. 根据权利要求1-4中的任一项所述的装置,其特征在于,从所述第一直波导输入的第一光束从所述第三直波导输出。The apparatus according to any one of claims 1 to 4, wherein the first light beam input from the first straight waveguide is output from the third straight waveguide.
  6. 根据权利要求1-4中的任一项所述的装置,其特征在于,从所述第二直波导输入的第二光束从所述第四直波导输出。The apparatus according to any one of claims 1 to 4, wherein the second light beam input from the second straight waveguide is output from the fourth straight waveguide.
  7. 根据权利要求1-4中的任一项所述的装置,其特征在于,从所述第三直波导输入的第三光束从所述第二直波导输出。The apparatus according to any one of claims 1 to 4, characterized in that the third light beam input from the third straight waveguide is output from the second straight waveguide.
  8. 根据权利要求1-4中的任一项所述的装置,其特征在于,从所述第四直波导输入的第四光束从所述第一直波导输出。The apparatus according to any one of claims 1 to 4, characterized in that the fourth light beam input from the fourth straight waveguide is output from the first straight waveguide.
  9. 根据权利要求1-8中的任一项所述的装置,其特征在于,所述第一直波导和所述第二直波导互相垂直,所述第三直波导和所述第四直波导互相垂直。The apparatus according to any one of claims 1-8, wherein the first straight waveguide and the second straight waveguide are perpendicular to each other, and the third straight waveguide and the fourth straight waveguide are mutually vertical.
  10. 一种芯片,其特征在于,包括根据权利要求1-9所述的波导装置。 A chip characterized by comprising the waveguide device according to claims 1-9.
PCT/CN2014/093294 2014-12-08 2014-12-08 Waveguide device and chip comprising same WO2016090534A1 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
PCT/CN2014/093294 WO2016090534A1 (en) 2014-12-08 2014-12-08 Waveguide device and chip comprising same
CN201480081835.2A CN106687836A (en) 2014-12-08 2014-12-08 Waveguide device and chip comprising same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
PCT/CN2014/093294 WO2016090534A1 (en) 2014-12-08 2014-12-08 Waveguide device and chip comprising same

Publications (1)

Publication Number Publication Date
WO2016090534A1 true WO2016090534A1 (en) 2016-06-16

Family

ID=56106403

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/CN2014/093294 WO2016090534A1 (en) 2014-12-08 2014-12-08 Waveguide device and chip comprising same

Country Status (2)

Country Link
CN (1) CN106687836A (en)
WO (1) WO2016090534A1 (en)

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5255334A (en) * 1991-06-03 1993-10-19 The Furukawa Electric Co., Ltd. Directional coupler type optical device and a driving method therefor
CN1353826A (en) * 1999-03-31 2002-06-12 布里斯托尔大学 Optical crosspoint switch using vertical coupled waveguide structure
CN101248379A (en) * 2004-03-24 2008-08-20 斯欧普迪克尔股份有限公司 Optical crossover in thin silicon
CN101963734A (en) * 2009-07-21 2011-02-02 日本电气株式会社 Optical mixer
CN101971415A (en) * 2008-03-17 2011-02-09 日本电气株式会社 Waveguide coupler
CN103424810A (en) * 2012-05-14 2013-12-04 鸿富锦精密工业(深圳)有限公司 Optical waveguide directional coupler

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5504476B2 (en) * 2010-02-19 2014-05-28 独立行政法人産業技術総合研究所 Optical waveguide crossing structure

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5255334A (en) * 1991-06-03 1993-10-19 The Furukawa Electric Co., Ltd. Directional coupler type optical device and a driving method therefor
CN1353826A (en) * 1999-03-31 2002-06-12 布里斯托尔大学 Optical crosspoint switch using vertical coupled waveguide structure
CN101248379A (en) * 2004-03-24 2008-08-20 斯欧普迪克尔股份有限公司 Optical crossover in thin silicon
CN101971415A (en) * 2008-03-17 2011-02-09 日本电气株式会社 Waveguide coupler
CN101963734A (en) * 2009-07-21 2011-02-02 日本电气株式会社 Optical mixer
CN103424810A (en) * 2012-05-14 2013-12-04 鸿富锦精密工业(深圳)有限公司 Optical waveguide directional coupler

Also Published As

Publication number Publication date
CN106687836A (en) 2017-05-17

Similar Documents

Publication Publication Date Title
CN108885307B (en) Optical edge coupler with controllable mode field for photonic chips
CN105116491B (en) A kind of silicon substrate groove waveguides integrated-type optical power distributor
US9335472B2 (en) Planar optical waveguide device and DP-QPSK modulator
US9696498B2 (en) Three-dimensional (3D) photonic chip-to-fiber interposer
WO2015096070A1 (en) Waveguide polarization splitter and polarization rotator
US20180059324A1 (en) Polarization rotator and optical signal processing method
CN103513333B (en) A kind of silica-based nanowire mixing right-angled intersection device
JP2013524262A (en) Multi-mode optical coupler interface
CN105866885B (en) Polarization beam splitting rotator
CN106471410A (en) Double ends photo-coupler
CN106959485B (en) Directional coupling type TM polarizer and beam splitter based on sub-wavelength grating
US9354394B2 (en) Optical components having a common etch depth
US10605988B2 (en) Optical beam spot size converter
WO2017147773A1 (en) Optocoupler and light processing method
JP2017090575A (en) Optical multiplexing/demultiplexing element and optical modulator
JP5596825B1 (en) Photonic crystal resonator
JP2015169766A (en) polarization rotation circuit
CN106680933B (en) A kind of asymmetrical areflexia period waveguide microcavity bandpass filter of transverse direction
CN203311029U (en) An integrated device which realizes light polarization splitting and rotation
CN110989080B (en) Grating auxiliary polarizer based on reverse coupling principle
CN101881859A (en) Optical delayer coupled through adopting multiple-mode interference
CN115494586B (en) Double-waveguide adiabatic coupler
WO2016090534A1 (en) Waveguide device and chip comprising same
JP4549949B2 (en) Optical element
Urino et al. Demonstration of 30-Tbps/cm 2 bandwidth density by silicon optical interposers fully integrated with optical components

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application

Ref document number: 14907956

Country of ref document: EP

Kind code of ref document: A1

NENP Non-entry into the national phase

Ref country code: DE

122 Ep: pct application non-entry in european phase

Ref document number: 14907956

Country of ref document: EP

Kind code of ref document: A1