This application relates to the field of optical communication, and in particular, to a light receiving module, device, and method.
Free space optical communication (FSOC) has been widely studied for advantages such as high security, strong anti-interference capability, and high bandwidth, and is an important part of the future wide area free space network.
Currently, a common technical method is to contract a space signal by using an optical beam contraction apparatus, couple the space signal into a single-mode or multi-mode optical fiber, and then enter a photoelectric detector to convert an optical signal into an electrical signal. As shown in
However, for the free space optical communication in the atmosphere, due to impact of turbulence in an atmospheric channel, a center position and a pointing angle of a light spot of the second optical signal offset to different degrees with time, and the light spot expands, reducing light receiving and detecting efficiency of the light receiving module, and causing a power jitter.
This application provides a light receiving module. An area for receiving a second optical signal can be increased by using a multi-core multi-mode waveguide, to reduce impact of offsets of a center position and a pointing angle of a light spot on light receiving and detecting efficiency, and to reduce a power jitter.
According to a first aspect of this application, a light receiving module is provided. The light receiving module includes a beam contraction module, a multi-core multi-mode waveguide, and a detector. The beam contraction module is configured to: receive a first optical signal, and contract a mode spot of the first optical signal, to obtain a second optical signal. The multi-core multi-mode waveguide includes a cladding layer and N waveguides. N is an integer greater than 1. The multi-core multi-mode waveguide is configured to: receive the second optical signal, and concentrate energy of the second optical signal in a plurality of waveguides of the N waveguides, to obtain a plurality of third optical signals. The detector is an array formed by N sub-detectors. The N sub-detectors are in one-to-one correspondence with the N waveguides. A plurality of sub-detectors of the N sub-detectors are in one-to-one correspondence with the plurality of third optical signals. The plurality of sub-detectors are configured to receive the plurality of third optical signals, to obtain a plurality of electrical signals based on the plurality of third optical signals.
In an optional manner of the first aspect, the multi-core multi-mode waveguide is a multi-core multi-mode optical fiber. The multi-core multi-mode optical fiber meets a multi-mode condition. The multi-mode condition is as follows:
a is a radius of a fiber core of the multi-core multi-mode optical fiber. λ is a wavelength of the second optical signal. ncore is a refractive index of the fiber core. nclad is a refractive index of the cladding layer. By using the multi-core multi-mode optical fiber, energy of an optical signal that is irradiated on the cladding layer can be better coupled to the fiber core. Therefore, in this application, coupling efficiency can be improved.
In an optional manner of the first aspect, the multi-core multi-mode optical fiber further meets the following condition:
In an optional manner of the first aspect, the N waveguides are of Gex1Sby1Sez1 materials. 0≤x1≤30. 0≤y1≤45. z1=100−x1−y1. The cladding layer is of a Gex2Sby2Sez2 material. 0≤x2≤30. 0≤y2≤40. z2=100−x2−y2. Ge is a germanium element. Sb is an antimony element. S is a sulfur element. Se is a selenium element.
In an optional manner of the first aspect, the N waveguides are of Asx3Sey3 materials. 35≤x3≤45. y3=100−x3. The cladding layer is a Gex4Asy4Sez4 material. 0≤x4≤45. 0≤y4≤45. z4=100−x4−y4. Ga is a gallium element. As is an arsenic element.
In an optional manner of the first aspect, a length of the multi-core multi-mode waveguide is between M×1520 micrometers and M×2005 micrometers, and M is an integer greater than 0.
In an optional manner of the first aspect, a cross section of the multi-core multi-mode waveguide is a circle. A diameter of the circle is between 100 micrometers and 300 micrometers.
In an optional manner of the first aspect, a distance between centers of any two waveguides of the N waveguides is greater than or equal to 15 micrometers.
In an optional manner of the first aspect, materials of the N waveguides and the cladding layer are silicon nitride materials.
In an optional manner of the first aspect, a ratio of a light spot area S1 of the second optical signal irradiating on the multi-core multi-mode waveguide to a cross-sectional area S2 of the multi-core multi-mode waveguide is less than 1.5. Due to impact of turbulence, a position of a light spot of the second optical signal may offset. Limiting the light spot area to less than 1.5 times the cross-sectional area of the multi-core multi-mode waveguide can reduce the impact of the turbulence and improve the coupling efficiency.
In an optional manner of the first aspect, the multi-core multi-mode waveguide is a multi-core multi-mode silicon nitride waveguide array.
According to a second aspect of this application, a light receiving device is provided. The light receiving device includes a signal processor and a light receiving module. The light receiving module is configured to receive a first optical signal, to obtain a plurality of electrical signals based on the first optical signal. The signal processor is configured to add the plurality of electrical signals, to obtain a target electrical signal.
According to a third aspect of this application, an optical communication system is provided. The optical communication system includes a light transmitting device and the light receiving device according to the second aspect. The light transmitting device is configured to transmit a first optical signal to the light receiving device. The light receiving device is configured to receive the first optical signal, to obtain a plurality of third optical signals based on the first optical signal. The light receiving device is further configured to convert the plurality of third optical signals into a plurality of electrical signals.
According to a fourth aspect of this application, a light receiving method is provided. The light receiving method includes the following steps: A light receiving device receives a first optical signal. The light receiving device contracts a mode spot of the first optical signal, to obtain a second optical signal. The light receiving device concentrates energy of the second optical signal in a plurality of regions, to obtain a plurality of third optical signals. The plurality of third optical signals are in one-to-one correspondence with the plurality of regions. The light receiving device converts the plurality of third optical signals into a plurality of electrical signals. By adding the plurality of electrical signals, a target electrical signal is obtained.
This application provides a light receiving module, device, and method. An area for receiving a second optical signal can be increased by using a multi-core multi-mode waveguide, to reduce impact of offsets of a center position and a pointing angle of a light spot on light receiving and detecting efficiency, and reduce a power jitter. It should be understood that “first”, “second”, “target”, and the like used in this application are merely for differentiation and description, but cannot be understood as an indication or implication of relative importance or an indication or implication of a sequence. In addition, for brevity and clarity, reference numbers and/or letters are repeated in a plurality of accompanying drawings of this application. Repetition is not indicative of a strictly limiting relationship between the various embodiments and/or configurations.
The light receiving module in this application is applied to the field of optical communication. In the field of optical communication, an FSOC technology may be used to implement air-to-air communication between a light transmitting device and a light receiving device. In an actual application, due to impact of turbulence, a center position of a light spot of an optical signal may offset, thereby reducing coupling efficiency.
Therefore, this application provides a light receiving module.
The beam contraction module 201 is also referred to as an optical receiving antenna. The beam contraction module 201 may be formed by a lens group or a reflector group. The beam contraction module 201 is configured to receive a first optical signal, and contract a mode spot of the first optical signal, to obtain a second optical signal. The second optical signal irradiates on an input end surface of the multi-core multi-mode waveguide 202. The multi-core multi-mode waveguide 202 includes a cladding layer 2022 and N waveguides 2021. N is an integer greater than 1. In
The multi-core multi-mode waveguide 202 may be a multi-core multi-mode optical fiber. The multi-core multi-mode optical fiber meets the following condition:
When the multi-core multi-mode waveguide 202 meets the foregoing multi-mode condition, each waveguide 2021 in the multi-core multi-mode waveguide 202 corresponds to one multi-mode optical fiber. a is a radius of the waveguide 2021. λ is a wavelength of the second optical signal. ncore is the refractive index of the waveguide 2021. nclad is the refractive index of the cladding layer 2022. The multi-core multi-mode waveguide 202 is configured to: receive the second optical signal, and concentrate energy of the second optical signal in a plurality of waveguides 2021 of the N waveguides 2021, to obtain a plurality of third optical signals. In
In this application, a plurality of detectors are used to receive the plurality of third optical signals, so that an area for receiving the second optical signal can be increased, to reduce impact of offsets of a center position and a pointing angle of a light spot on light receiving and detecting efficiency, and reduce a power jitter. To reduce impact of turbulence, in this embodiment of this application, a ratio of a light spot area S1 of the second optical signal irradiating on the multi-core multi-mode waveguide 202 to a cross-sectional area S2 of the multi-core multi-mode waveguide 202 may be limited to less than 1.5. The cross section of the multi-core multi-mode waveguide 202 is perpendicular to an X axis.
In this embodiment of this application, coupling efficiency of the multi-core multi-mode waveguide 202 is related to dimensions of the waveguide 2021 and the cladding layer 2022. When the cladding layer 2022 and the waveguide 2021 are cylindrical, a diameter of the cladding layer 2022 may be between 100 micrometers and 300 micrometers. A diameter of the waveguide 2021 may be between 0.05 micrometers and 99 micrometers. The diameter of the cladding layer 2022 includes 100 micrometers or 300 micrometers. The diameter of the waveguide 2021 includes 0.05 micrometers or 99 micrometers.
In this embodiment of this application, the coupling efficiency of the multi-core multi-mode waveguide 202 is related to the refractive indexes of the waveguide 2021 and the cladding layer 2022. The refractive indexes of the waveguide 2021 and the cladding layer 2022 may be between 2 and 3. A refractive index contrast ratio of the waveguide 2021 and the cladding layer 2022 may meet the following condition:
For example, a material of the waveguide 2021 is Gex1Sby1Sez1. x1 is between 0 and 30. y1 is between 0 and 45. z1=100−x1−y1. The refractive index of the waveguide 2021 varies with an element ratio. In this case, the refractive index of the waveguide 2021 is between 2.4 and 2.7. A material of the cladding layer 2022 is Gex2Sby2Sz2. x2 is between 0 and 30. y2 is between 0 and 45. z2=100−x2−y2. The refractive index of the cladding layer 2022 is between 2.1 and 2.2.
For another example, a material of the waveguide 2021 is Asx3Sey3. x3 is between 35 and 45. y3=100−x3. The refractive index of the waveguide 2021 is between 2.8 and 2.9. A material of the cladding layer 2022 is Gex4Asy4Sez4. x4 is between 0 and 45. y4 is between 0 and 45. z4=100−x4−y4. The refractive index of the cladding layer 2022 is between 2.5 and 2.6.
In this embodiment of this application, the second optical signal may oscillate between the cladding layer and the waveguide of the multi-core multi-mode waveguide 202. Therefore, the coupling efficiency of the multi-core multi-mode waveguide 202 is related to a length of the multi-core multi-mode waveguide 202. A length direction of the multi-core multi-mode waveguide 202 is an X-axis direction in
It should be understood that, the light receiving module in
In
In
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The foregoing describes the light receiving module provided in this application, and the following describes a light receiving device provided in this application.
The following describes an optical communication system provided in this application.
By using the optical communication system 500 provided in this application, coupling efficiency of the light receiving device 502 can be improved. The following uses a specific simulation example for description. In
The beam contraction module 201 is configured to contract a mode spot of an incident first optical signal to a dimension D (diameter). The multi-core multi-mode waveguide 202 includes N optical fibers and a cladding layer. To reduce a dimension of a waveguide and increase a numerical aperture of a single-root multi-mode fiber or a waveguide, a refractive index ncore of a fiber core is greater than a refractive index nclad of the cladding layer, where ncore−nclad>0.05. The N fiber cores may be arranged according to a specific rule to form a multi-mode multi-core optical fiber. For example, a material for manufacturing the fiber core and the cladding layer is a sulfur-based glass material. Refractive indexes ncore of the N fiber cores are all 2.6. The refractive index nclad of the cladding layer is 2.2. A diameter of the fiber core is greater than a distance between fiber cores.
After the beam contraction module 201 contracts a first optical signal, an area of a light spot of the first optical signal irradiating on the input end surface of the multi-core multi-mode waveguide 202 is basically the same as a cross-sectional area of the multi-core multi-mode waveguide 202. Alternatively, an area of a light spot of the first optical signal irradiating on the input end surface of the multi-core multi-mode waveguide 202 is slightly smaller than a cross-sectional area of the multi-core multi-mode waveguide 202. It should be understood that, the cross-sectional area of the multi-core multi-mode waveguide 202 only includes cross-sectional areas of the fiber core and the cladding layer. The cross-sectional area of the multi-core multi-mode waveguide 202 does not include a cross-sectional area of a coating layer or a sheath layer. Theoretically, all optical signals that are irradiated on the input end surface of the multi-core multi-mode waveguide 202 enter the fiber core after being transmitted for a distance, and oscillate between the fiber core and the cladding layer. Therefore, the coupling efficiency of the multi-core multi-mode waveguide 202 is related to a length of the multi-core multi-mode waveguide 202. By intercepting a proper length of the multi-core multi-mode waveguide 202, most energy of the optical signal may be contracted to the fiber core at an output end surface of the multi-core multi-mode waveguide 202. The plurality of detectors 203 are at a rear end of the multi-core multi-mode waveguide 202. The plurality of optical signals that are output from the output end surface of the multi-core multi-mode waveguide 202 directly enter the photoelectric detector. To enable to-be-received optical signals to be received by the detector as many as possible, a dimension of a photosensitive surface of the photoelectric detector is equal to a dimension of the fiber core, or a dimension of a photosensitive surface of the photoelectric detector is slightly larger than a dimension of the fiber core.
In an actual application, after passing through atmosphere, the light spot may appear phenomena such as diffusion and crack. For example, under interference of weak turbulence, a shape of a light spot of a Gaussian beam does not change obviously, and a center position of the light spot does not offset obviously. Under interference of medium turbulence, the light spot begins to split, and the center position of the light spot offsets obviously. Under interference of strong turbulence, the light spot is broken seriously.
The foregoing describes the optical communication system provided in this application, and the following describes a light receiving method provided in this application.
In step 1001, a light receiving device receives a first optical signal. For descriptions of the light receiving device, refer to the foregoing descriptions of the light receiving module, the light receiving device, or the optical communication system. The light receiving device may receive the first optical signal by using a beam contraction module.
In step 1002, the light receiving device contracts a mode spot of the first optical signal, to obtain a second optical signal. The light receiving device contracts the mode spot of the first optical signal by using the beam contraction module, to obtain the second optical signal. An area of a mode spot of the second optical signal irradiating on an input end surface of the multi-core multi-mode waveguide may be equal to a cross-sectional area of the multi-core multi-mode waveguide.
In step 1003, the light receiving device concentrates energy of the second optical signal in a plurality of regions, to obtain a plurality of third optical signals. The plurality of third optical signals are in one-to-one correspondence with the plurality of regions. By using the multi-core multi-mode waveguide, the light receiving device can concentrate the energy of the second optical signal in the plurality of regions. Each region corresponds to one third optical signal. Therefore, the light receiving device can obtain the plurality of third optical signals based on the second optical signal.
In step 1004, the light receiving device converts the plurality of third optical signals into a plurality of electrical signals. The light receiving device includes a plurality of detectors. The plurality of detectors are configured to receive the plurality of third optical signals, to obtain the plurality of electrical signals based on the plurality of third optical signals.
In step 1005, the light receiving device adds the plurality of third optical signals to obtain a target electrical signal.
The foregoing descriptions are merely specific implementations of this application, but are not intended to limit the protection scope of this application. Any variation or replacement readily figured out by a person skilled in the art within the technical scope disclosed in this application shall fall within the protection scope of this application.
Number | Date | Country | Kind |
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202210033151.1 | Jan 2022 | CN | national |
This application is a continuation of International Application No. PCT/CN2022/136463, filed on Dec. 5, 2022, which claims priority to Chinese Patent Application No. 202210033151.1, filed on Jan. 12, 2022. The disclosures of the aforementioned applications are hereby incorporated by reference in their entireties.
Number | Date | Country | |
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Parent | PCT/CN2022/136463 | Dec 2022 | WO |
Child | 18770283 | US |