CN114859470A - Optical path structure and method for increasing return loss and optical device - Google Patents

Optical path structure and method for increasing return loss and optical device Download PDF

Info

Publication number
CN114859470A
CN114859470A CN202210545447.1A CN202210545447A CN114859470A CN 114859470 A CN114859470 A CN 114859470A CN 202210545447 A CN202210545447 A CN 202210545447A CN 114859470 A CN114859470 A CN 114859470A
Authority
CN
China
Prior art keywords
lens
chip
return loss
optical fiber
optical
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN202210545447.1A
Other languages
Chinese (zh)
Inventor
丁晓亮
田桂霞
甘飞
李量
汪军
窦佳迪
包苓暄
徐菽晗
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Suzhou Zhuoyu Photon Technology Co ltd
Original Assignee
Suzhou Zhuoyu Photon Technology Co ltd
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 Suzhou Zhuoyu Photon Technology Co ltd filed Critical Suzhou Zhuoyu Photon Technology Co ltd
Priority to CN202210545447.1A priority Critical patent/CN114859470A/en
Publication of CN114859470A publication Critical patent/CN114859470A/en
Pending legal-status Critical Current

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
    • G02B6/262Optical details of coupling light into, or out of, or between fibre ends, e.g. special fibre end shapes or associated optical elements
    • 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
    • G02B6/42Coupling light guides with opto-electronic elements
    • G02B6/4201Packages, e.g. shape, construction, internal or external details
    • G02B6/4204Packages, e.g. shape, construction, internal or external details the coupling comprising intermediate optical elements, e.g. lenses, holograms
    • 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
    • G02B6/42Coupling light guides with opto-electronic elements
    • G02B6/4201Packages, e.g. shape, construction, internal or external details
    • G02B6/4204Packages, e.g. shape, construction, internal or external details the coupling comprising intermediate optical elements, e.g. lenses, holograms
    • G02B6/4206Optical features
    • 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
    • G02B6/42Coupling light guides with opto-electronic elements
    • G02B6/4201Packages, e.g. shape, construction, internal or external details
    • G02B6/4204Packages, e.g. shape, construction, internal or external details the coupling comprising intermediate optical elements, e.g. lenses, holograms
    • G02B6/4214Packages, e.g. shape, construction, internal or external details the coupling comprising intermediate optical elements, e.g. lenses, holograms the intermediate optical element having redirecting reflective means, e.g. mirrors, prisms for deflecting the radiation from horizontal to down- or upward direction toward a device
    • 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
    • G02B6/42Coupling light guides with opto-electronic elements
    • G02B6/4201Packages, e.g. shape, construction, internal or external details
    • G02B6/4204Packages, e.g. shape, construction, internal or external details the coupling comprising intermediate optical elements, e.g. lenses, holograms
    • G02B6/4215Packages, e.g. shape, construction, internal or external details the coupling comprising intermediate optical elements, e.g. lenses, holograms the intermediate optical elements being wavelength selective optical elements, e.g. variable wavelength optical modules or wavelength lockers
    • 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
    • G02B6/42Coupling light guides with opto-electronic elements
    • G02B6/4201Packages, e.g. shape, construction, internal or external details
    • G02B6/4285Optical modules characterised by a connectorised pigtail

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Couplings Of Light Guides (AREA)

Abstract

The invention relates to an optical path structure, a method and an optical device for increasing return loss, which comprise an optical fiber insertion component, a collimating lens, a converging lens and a PD chip; the optical fiber insertion assembly is provided with an optical fiber channel which is used for transmitting incident light; the outlet of the optical fiber channel is obliquely arranged and faces the collimating lens; the collimating lens is used for converting incident light into collimated light; the converging lens is used for converging collimated light and enabling the collimated light to be incident to the PD chip, the optical axis of the converging lens is parallel to the axis of the PD chip and arranged in an off-axis mode, and an inclined surface is arranged on one side, opposite to the PD chip, of the converging lens. A convergent lens in front of a PD chip is arranged in an off-axis mode and is designed to be a tilted convex lens, off-axis offset of the convergent lens can be small, and coupling efficiency is not affected; and reflected light on the surface of the PD reversely passes through the two lenses and is coupled and mismatched with the fiber core of the optical fiber channel, so that most of the reflected light cannot be coupled into the optical fiber channel, return loss parameters of the optical path are improved, and the performance of the optical device is ensured.

Description

Optical path structure and method for increasing return loss and optical device
Technical Field
The invention relates to the technical field of optical communication, in particular to an optical path structure, a method and an optical device for increasing return loss.
Background
At present, the optical communication industry enters a rapid development stage, an optical module plays a central role in the optical communication industry, and is widely applied to wireless equipment and transmission equipment, and an optical device is taken as a core component of the optical module and must meet technical indexes of the optical module in different application scenes.
The return loss is an important parameter of the performance of the optical device, and means that when an optical signal is transmitted inside the optical device and meets an optical element, part of the optical signal is reflected back to the transmitting end, thereby causing interference with the operation of the laser or influencing the transmission performance of the optical fiber.
At present, a collimated light path is widely applied to optical devices, and particularly, a single-fiber bidirectional optical device has a small return loss of the light path and does not meet a general return loss index.
Among the prior art, some schemes will receive the slope of optical signal's PD chip and place and increase the return loss, but the difficult control of inclination uniformity has reduced production efficiency, has reduced structural stability, has brought the reliability risk, and coupling efficiency also has certain loss simultaneously. In addition, as shown in chinese patent CN111650701A, a structure and an application for improving return loss are disclosed, in which the off-axis of the focusing lens in front of the PD chip is placed to expect to increase return loss, which seems to be feasible theoretically, but actually, in order to increase return loss, the off-axis offset of the focusing lens in front of the PD chip needs to be larger, which results in a great reduction in coupling efficiency.
Disclosure of Invention
The technical problem to be solved by the invention is to provide a light path structure, a method and an optical device for increasing return loss, wherein a convergent lens in front of a PD chip is arranged in an off-axis manner and is designed into a tilted convex lens, the off-axis offset of the convergent lens can be smaller, and the coupling efficiency is not influenced; incident light is reflected by the surface of the PD chip, and reflected light is mismatched with the fiber core of the optical fiber channel after passing through the two lenses again, so that most of the reflected light cannot be coupled into the optical fiber channel, return loss parameters of a light path are improved, and the performance of an optical device is further ensured.
In order to solve the technical problem, the invention provides an optical path structure for increasing return loss, which comprises an optical fiber insertion component, a collimating lens, a converging lens and a PD chip; the optical fiber insertion assembly is internally provided with an optical fiber channel for transmitting incident light; the outlet of the optical fiber channel is obliquely arranged and faces the collimating lens; the collimating lens is used for converting incident light into collimated light; the converging lens is used for converging the collimated light and enabling the collimated light to be incident to the PD chip, the optical axis of the converging lens is parallel to the axis of the PD chip and is arranged in an off-axis mode, and an inclined surface is arranged on one side, opposite to the PD chip, of the converging lens.
Preferably, the outlet of the optical fiber channel is inclined at an angle of 4-8 °.
Preferably, the inclined surface is inclined at an angle of not more than 10 °.
Preferably, the PD chip is a photodetection chip; the receiving surface of the photoelectric detection chip faces the convergent lens and is used for receiving the optical signal converged by the convergent lens.
Preferably, the filter also comprises a full-anti-wave plate and a filter plate; the full-reflection wave plate is arranged on one side of the collimating lens, which is far away from the optical fiber insertion assembly, and is used for deflecting the collimated light output by the collimating lens; the filter plate is arranged between the full-reflection wave plate and the collimating lens and used for filtering the collimated light after deflection.
Preferably, the collimating lens is a biconvex lens or a plano-convex lens, and the convex surface of the collimating lens is a spherical surface or an aspheric surface.
Preferably, the convex surface of the converging lens is spherical or aspherical.
Preferably, the optical fiber insertion assembly includes a ferrule having the optical fiber passage disposed therein.
A method of increasing return loss, comprising the steps of: s1, emitting incident light, and inputting the incident light to a preset collimating lens; s2, converting the incident light into collimated light based on the collimating lens, and inputting the collimated light to a preset converging lens; s3, converging the collimated light based on the converging lens, and inputting the converged collimated light to a PD chip in an inclined manner; and one part of the collimated light after being converged is absorbed by the PD chip, and the other part of the collimated light is reflected on the surface of the PD chip to form a return loss optical path.
An optical device comprising the above optical path structure for increasing return loss.
Compared with the prior art, the technical scheme of the invention has the following advantages:
the outlet of the optical fiber channel is obliquely arranged and faces the collimating lens, the optical axis of the converging lens is parallel to the axis of the PD chip and is arranged in an off-axis manner, and the inclined surface is arranged on one side of the converging lens, which is opposite to the PD chip. Compared with the prior art, the off-axis offset of the convergent lens can be smaller, and the coupling efficiency is not influenced. Incident light is reflected by the surface of the PD chip, reflected light is not collimated light after reversely passing through the converging lens, and is obviously mismatched with the fiber core of the optical fiber channel when reversely passing through the collimating lens and converging to the end face of the optical fiber channel, so that most of the reflected light cannot be coupled into the optical fiber channel, and the return loss value is increased.
Drawings
In order that the present disclosure may be more readily and clearly understood, reference is now made to the following detailed description of the present disclosure taken in conjunction with the accompanying drawings, in which:
FIG. 1 is a schematic diagram of the optical path structure of the present invention;
FIG. 2 is a schematic diagram of the return loss optical path structure of the present invention;
FIG. 3 is a diagram illustrating a second embodiment of the optical path structure according to the present invention;
fig. 4 is a third schematic view of an embodiment of an optical path structure of the present invention.
The specification reference numbers indicate: the optical fiber coupler comprises a 10-optical fiber insertion component, a 20-collimating lens, a 30-converging lens, a 40-PD chip, a 50-full-reflection wave plate, a 60-filter plate, a 501-second full-reflection wave plate and a 502-first full-reflection wave plate.
Detailed Description
The present invention is further described below in conjunction with the following figures and specific examples so that those skilled in the art may better understand the present invention and practice it, but the examples are not intended to limit the present invention.
Example one
The invention discloses an optical path structure for increasing return loss, which is shown in figure 1 and comprises the following components:
a fiber insertion assembly 10, a collimating lens 20, a converging lens 30, and a PD chip 40.
The center of the optical fiber insertion assembly 10 is provided with a ferrule, and a fiber channel is provided in the ferrule and is used for transmitting incident light.
The light outlet port of the optical fiber channel faces the collimating lens 20, the outlet of the optical fiber channel is arranged in an inclined manner, the inclination angle of the outlet of the optical fiber channel is 4-8 degrees, the inclination angle of the outlet of the optical fiber channel can be selected to be 4 degrees, 5 degrees, 6 degrees, 7 degrees, 8 degrees and the like according to actual conditions, so that the return loss of an optical path is increased, and the inclination angle of the outlet of the optical fiber channel can also be designed to be 0 degree according to requirements. Preferably, in this embodiment, the outlet of the fiber channel gradually increases in distance from the collimating lens 20 from top to bottom.
The above collimator lens 20 converts incident light into collimated light, which is condensed by the condenser lens 30 and is incident on the PD chip 40. The optical axis of the converging lens 30 is parallel to the axis of the PD chip 40 and is arranged off-axis, the off-axis offset of the converging lens 30 may be small, the coupling efficiency is not affected, the off-axis offset may be 0, and if the off-axis offset is not 0, the return loss value of the optical path may be greatly increased.
Further preferably, the collimating lens 20 may be a simple plano-convex lens as shown in fig. 1, or may be a biconvex lens, and the convex surface may be a spherical surface or an aspherical surface.
The side of the convergent lens 30 facing the PD chip 40 is provided with an inclined surface, and the convex surface of the convergent lens 30 is spherical or aspherical. The inclined surface of the condensing lens 30 is inclined at an angle of not more than 10 deg. to increase the return loss of the optical path. Preferably, in the present embodiment, the distance from the inclined surface of the condensing lens 30 to the PD chip 40 decreases gradually from top to bottom.
One part of the converged collimated light is absorbed by the PD chip 40, the proportion of the absorbed part in the incident light is the coupling efficiency, and the other part is reflected on the surface of the PD chip 40 to form a return loss optical path.
Incident light is reflected by the surface of the PD chip 40, reflected light is not collimated light after reversely passing through the converging lens 30, and is obviously coupled and mismatched with a fiber core of the optical fiber channel when being converged to the end face of the optical fiber channel through the collimating lens 20, so that most of the reflected light cannot be coupled into the optical fiber channel, return loss parameters of the optical path are improved, and production efficiency is not influenced.
The PD chip 40 is a photo detection chip, and a receiving surface of the photo detection chip is disposed toward the converging lens 30, and is configured to receive the optical signal converged by the lens assembly and convert the optical signal into an electrical signal.
Further, referring to fig. 2, it is a schematic view of the return loss optical path of the present invention.
The incident light is reflected by the surface of the PD chip 40, the reflected light is reflected by the condensing lens 30 in a reverse direction and is not collimated, and then is condensed by the collimating lens 20 in a reverse direction to the end surface of the optical fiber channel, so that the incident light is obviously mismatched with the fiber core of the optical fiber channel in a coupling manner, and the return loss value is increased.
Example two
Referring to fig. 3, the present invention discloses an optical path structure for increasing return loss, including:
a fiber insertion assembly 10, a collimating lens 20, a converging lens 30, and a PD chip 40.
The center of the optical fiber insertion assembly 10 is provided with a ferrule, and an optical fiber channel is disposed in the ferrule and used for transmitting incident light.
The light outlet port of the optical fiber channel faces the collimating lens 20, the outlet of the optical fiber channel is obliquely arranged, and the distance from the outlet of the optical fiber channel to the collimating lens 20 from top to bottom is gradually increased. Preferably, the inclination angle of the outlet of the optical fiber channel is 4-8 degrees to increase the return loss of the optical path, and the inclination angle of the outlet of the optical fiber channel can also be designed to be 0 degree according to actual requirements.
The above-described collimator lens 20 converts incident light into collimated light, which is condensed by the condenser lens 30 and is incident on the PD chip 40. The optical axis of the converging lens 30 is parallel to the axis of the PD chip 40 and is arranged off-axis, the off-axis offset of the converging lens 30 may be small, the coupling efficiency is not affected, the off-axis offset may be 0, and if the off-axis offset is not 0, the return loss value of the optical path may be greatly increased.
The side of the convergent lens 30 facing the PD chip 40 is provided with an inclined surface, and the convex surface of the convergent lens 30 is spherical or aspherical. Preferably, the distance from the inclined surface of the condensing lens 30 to the PD chip 40 decreases gradually from top to bottom; the inclined plane has an inclination angle of not more than 10 deg. to increase the return loss of the optical path.
In the first embodiment, there is no other optical device between the collimating lens 20 and the converging lens 30, and the whole optical path structure is arranged in a straight line.
In contrast to the first embodiment, in the present embodiment, a full-reflection wave plate 50 and a filter 60 are further disposed between the collimating lens 20 and the converging lens 30.
Specifically, the above-mentioned full-anti wave plate 50 is disposed on a side of the collimating lens 20 away from the fiber insertion assembly 10, and is used for deflecting the collimated light output by the collimating lens 20.
Preferably, the total reflection wave plate 50 is a 45 ° total reflection wave plate, and deflects the optical path by 90 °.
The filter 60 is disposed between the full-wave plate 50 and the collimator lens 20, and is used for filtering the collimated light after deflection.
Specifically, the light output by the optical fiber channel is converted into collimated light through the first collimating lens 20, is deflected through the 45-degree full-reflection wave plate, and is reflected to the filter 60, the filter 60 filters the collimated light after deflection, and the filtered collimated light is converged and incident on the PD chip 40 through the converging lens 30.
EXAMPLE III
The third embodiment is different from the second embodiment in that it includes a first full-anti-wave plate 501 and a second full-anti-wave plate 502. The first full-reflection wave plate 501 is a 13 ° full-reflection wave plate, and the second full-reflection wave plate 502 is a +32 ° full-reflection wave plate.
As shown in fig. 4, light output by the optical fiber channel is converted into collimated light through the first collimating lens 20, and then deflected through the first full-wave-plate 502 and the second full-wave-plate 501 in sequence, so that the collimated light is reflected to the filter 60, and the filter 60 filters the deflected collimated light. The filtered collimated light is condensed by the condensing lens 30 and is incident on the PD chip 40.
Example four
The invention also discloses a method for increasing return loss, which corresponds to the optical path structure for increasing return loss, and specifically comprises the following steps:
step one, emitting incident light from the optical fiber channel, and inputting the incident light to a preset collimating lens 20.
Wherein the light exit ports of the fiber channels are obliquely arranged and face the collimating lens 20.
In the second step, the collimating lens 20 converts the incident light into collimated light, and inputs the collimated light into the preset converging lens 30.
Step three, the condensing lens 30 condenses the collimated light, and the condensed collimated light is obliquely input to the PD chip 40. Part of the collimated light after being converged is absorbed by the PD chip 40, and the other part is reflected on the surface of the PD chip 40, thereby forming a return loss optical path.
The optical axis of the converging lens 30 is parallel to the axis of the PD chip 40 and is disposed off-axis, and an inclined surface is disposed on a side of the converging lens 30 facing the PD chip 40. The off-axis offset of the convergent lens 30 can be small, coupling efficiency is not affected, incident light is reflected by the surface of the PD chip 40, reflected light is not collimated light after reversely passing through the convergent lens 30, and when the reflected light is converged to the end face of the optical fiber channel through the collimating lens 20 reversely, the reflected light is obviously mismatched with the fiber core coupling of the optical fiber channel, most of the reflected light cannot be coupled into the optical fiber channel, return loss parameters of the optical path are improved, and production efficiency is not affected.
EXAMPLE five
The invention also discloses an optical device which comprises the optical path structure for increasing return loss.
The optical device is preferably a single-fiber bidirectional optical device.
It should be understood that the above examples are only for clarity of illustration and are not intended to limit the embodiments. Other variations and modifications will be apparent to persons skilled in the art in light of the above description. And are neither required nor exhaustive of all embodiments. And obvious variations or modifications of the invention may be made without departing from the spirit or scope of the invention.

Claims (10)

1. An optical path structure for increasing return loss, comprising: the optical fiber insertion component, the collimating lens, the converging lens and the PD chip;
the optical fiber insertion assembly is internally provided with an optical fiber channel for transmitting incident light;
the light outlet of the optical fiber channel is obliquely arranged and faces the collimating lens; the collimating lens is used for converting incident light into collimated light;
the convergent lens is used for converging the collimated light and enabling the collimated light to be incident to the PD chip, the optical axis of the convergent lens is parallel to the axis of the PD chip and arranged in an off-axis mode, and an inclined surface is arranged on one side, opposite to the PD chip, of the convergent lens.
2. The return loss-increasing optical path structure according to claim 1, wherein the outlet of the optical fiber channel is inclined at an angle of 4 ° to 8 °.
3. The return loss-increasing optical path structure according to claim 1, wherein the inclined surface is inclined at an angle of not more than 10 °.
4. The return loss increasing optical path structure according to claim 3, wherein the PD chip is a photodetection chip;
the receiving surface of the photoelectric detection chip faces the convergent lens and is used for receiving the optical signal converged by the convergent lens.
5. The return loss increasing optical path structure according to claim 1, further comprising a full-inverse wave plate and a filter plate;
the full-reflection wave plate is arranged on one side of the collimating lens, which is far away from the optical fiber insertion assembly, and is used for deflecting the collimated light output by the collimating lens;
the filter plate is arranged between the full-wave-reflecting plate and the collimating lens and used for filtering the collimated light after deflection.
6. The return loss increasing optical path structure according to claim 1, wherein the collimating lens is a biconvex lens or a plano-convex lens, and a convex surface of the collimating lens is a spherical surface or an aspherical surface.
7. The return loss increasing optical path structure according to claim 1, wherein the convex surface of the converging lens is spherical or aspherical.
8. The return loss increased optical circuit structure according to claim 1, wherein the optical fiber insertion assembly includes a ferrule, and the optical fiber passage is disposed in the ferrule.
9. A method of increasing return loss, comprising the steps of:
s1, emitting incident light, and inputting the incident light to a preset collimating lens;
s2, converting the incident light into collimated light based on the collimating lens, and inputting the collimated light to a preset converging lens;
s3, converging the collimated light based on the converging lens, and inputting the converged collimated light to a PD chip in an inclined manner;
and one part of the collimated light after being converged is absorbed by the PD chip, and the other part of the collimated light is reflected on the surface of the PD chip to form a return loss optical path.
10. An optical device comprising the return loss increasing optical path structure according to any one of claims 1 to 8.
CN202210545447.1A 2022-05-19 2022-05-19 Optical path structure and method for increasing return loss and optical device Pending CN114859470A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202210545447.1A CN114859470A (en) 2022-05-19 2022-05-19 Optical path structure and method for increasing return loss and optical device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202210545447.1A CN114859470A (en) 2022-05-19 2022-05-19 Optical path structure and method for increasing return loss and optical device

Publications (1)

Publication Number Publication Date
CN114859470A true CN114859470A (en) 2022-08-05

Family

ID=82639642

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202210545447.1A Pending CN114859470A (en) 2022-05-19 2022-05-19 Optical path structure and method for increasing return loss and optical device

Country Status (1)

Country Link
CN (1) CN114859470A (en)

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN2716853Y (en) * 2003-12-24 2005-08-10 武汉光迅科技有限责任公司 Single-fiber two-way receiving and transmitting integrated module
CN101021602A (en) * 2006-02-16 2007-08-22 日本板硝子株式会社 Optical tap module
CN109239852A (en) * 2018-10-15 2019-01-18 深圳市亚派光电器件有限公司 Light receiving element
CN111650701A (en) * 2020-06-29 2020-09-11 成都新易盛通信技术股份有限公司 Structure for improving return loss and application
CN111796369A (en) * 2020-08-18 2020-10-20 上海光卓通信设备有限公司 Integrated ceramic ferrule and optical fiber socket
CN113391408A (en) * 2021-07-19 2021-09-14 鹰潭市科海光器件有限公司 SL-type integrated four-core optical fiber movable connector
CN214335303U (en) * 2020-10-27 2021-10-01 武汉联特科技股份有限公司 EML TOSA device packaged by coaxial TO-CAN technology

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN2716853Y (en) * 2003-12-24 2005-08-10 武汉光迅科技有限责任公司 Single-fiber two-way receiving and transmitting integrated module
CN101021602A (en) * 2006-02-16 2007-08-22 日本板硝子株式会社 Optical tap module
CN109239852A (en) * 2018-10-15 2019-01-18 深圳市亚派光电器件有限公司 Light receiving element
CN111650701A (en) * 2020-06-29 2020-09-11 成都新易盛通信技术股份有限公司 Structure for improving return loss and application
CN111796369A (en) * 2020-08-18 2020-10-20 上海光卓通信设备有限公司 Integrated ceramic ferrule and optical fiber socket
CN214335303U (en) * 2020-10-27 2021-10-01 武汉联特科技股份有限公司 EML TOSA device packaged by coaxial TO-CAN technology
CN113391408A (en) * 2021-07-19 2021-09-14 鹰潭市科海光器件有限公司 SL-type integrated four-core optical fiber movable connector

Similar Documents

Publication Publication Date Title
JP5714229B2 (en) Double lens single optical receiver assembly
US4904043A (en) Optical data link dual wavelength coupler
US7128477B2 (en) Optical transmitter and receiver module
WO2017118271A1 (en) Parallel transmission and reception optical module for dual-link transmission, and preparation method
WO2011056187A1 (en) Expanded beam interface device and method for fabricating same
US5892868A (en) Fiber optic coupler combiner and process using same
US6721511B1 (en) Optical communication equipment and optical communication network equipment
US20050074213A1 (en) Bi-directional transceiver module based on silicon optic
CN111650701A (en) Structure for improving return loss and application
KR101227182B1 (en) Optical module using lenz having coated concave plane
CN219302727U (en) High-speed optical module receiving end assembly
CN114859470A (en) Optical path structure and method for increasing return loss and optical device
US7010190B2 (en) Silicon optic based wavelength division multiplexing device
CN101887152B (en) Single-fiber bidirectional symmetrical optical transceiver optical element for 10G-EPON
CN210605095U (en) Optical module
US20080137519A1 (en) Multi-channel optical communication lens system and optical module using the same
CN211293365U (en) Optical receiving subassembly
JP2018182108A (en) Plano-convex lens, fiber array module and light receiving module
US6704478B2 (en) Wavelength separation optical device and multiple wavelength light transmission module
US20020006252A1 (en) Tap coupler
US6853767B1 (en) Methods for manufacturing optical coupling elements
CN215005964U (en) Wavelength division demultiplexer
KR101507376B1 (en) Expanded beam interconnects based on compound-lens
JP7028490B1 (en) Optical connection parts and optical parts
KR100701728B1 (en) Wavelength dependant optical device

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination