TW202032931A - Wavelength selective enable bidirectional access system - Google Patents

Abstract

A wavelength selective enables bidirectional optical wireless access system, includes an access node and multiple optical terminals, which can transmit/receive multiple wavelengths to/from the access node. The access node is composed of more than two transmitter modules, a static wavelength separation element and a spatial light modulator (SLM, a programmable phase grating element). Based on the design of SLM, serving as a dynamic phase grating element, which combines with a static diffraction grating element, wavelength and beam steering switching can be performed to achieve a bidirectional optical wireless communication between the access node and optical terminals.

Description

Division wave multiplexing two-way transmission access system

The invention relates to a division-wave multiplexing two-way transmission and access system, in particular to a system that can use a spatial light modulator as a programmable diffraction element to achieve the purpose of two-way transmission and access for wireless optical communication.

The origin of the development of wireless optical communication technology is to support the technologies and ideas proposed by some areas that have difficulties in installing optical fibers and enjoying optical fiber broadband networks, that is, without using wired media such as optical fibers and cables as communication media, so it is also called It is the Free Space Optical Communication (FSOC).

The propagation characteristics of light sources of different wavelength bands when transmitted in the transmission channel are not the same. Therefore, suitable light sources must be selected based on different applications and occasions. By the wavelength characteristics of the selected light sources, they can be simply divided into visible wireless optical communication systems, Two categories of invisible wireless optical communication systems;

The wireless optical communication technology is mainly used to overcome the difficulty of laying optical fibers at the user receiving end after optical signals are transmitted through a passive optical network (PON). However, in view of the various wireless optical communication systems currently proposed The architecture is all Point to Point (P2P) communication, and only one output port can be fixed at the receiving end, so the system flexibility is not high.

Therefore, in order to improve the traditional wireless optical communication system architecture that can only perform P2P communication, if the spatial light modulator (SLM) with programmable diffraction element can be used as the dynamic diffraction element, and Through the control of the spatial light modulator of the programmable diffractive element, the output beam width and position are reconfigured for the incident beam, so that the two-way wireless optical communication system can be accessed, and the traditional system architecture can be improved through the above system The shortcomings of insufficient flexibility, therefore, the present invention should be an optimal solution.

The demultiplexing two-way transmission and access system of the present invention includes: two or more optical terminals, wherein each optical terminal includes at least one optical detection receiver; at least one wireless optical communication node terminal includes at least two More than one light emitting module, which can respectively emit two or more beams with different wavelengths; a wavelength separation element, which can separate the beams of different wavelengths and transmit to optical terminals in different directions; and A spatial light modulator is arranged on the travel path of beams with different wavelengths emitted by the light emitting module at the wireless optical communication node end, and the spatial light modulator element is used to control different wavelengths through phase modulation After the beam is shifted, it is incident on the wavelength separation element at different angles. Since the beams of different wavelengths enter the wavelength separation element at different incident angles, the angle after exiting the optical terminal through the wavelength separation element can be changed to face different directions. Optical terminal.

More specifically, the optical terminal further includes a beam concentrator, so that the beam emitted by the wavelength separation element can first pass through the beam concentrator and then contact the optical detection receiver.

More specifically, the light emitting module is a graded index lens fiber.

More specifically, a beam expander is provided between the light emitting module and the spatial light modulator to expand and adjust the beam emitted by the light emitting module.

More specifically, a beam collimator is arranged between the light emitting module and the spatial light modulator to adjust the collimation of the beam emitted by the light emitting module.

More specifically, the spatial light modulator is a programmable diffractive element, and the programmable diffractive element can be a silicon-based liquid crystal element, a liquid crystal element, or a microelectromechanical system.

More specifically, the wavelength separation element is a reflective blazed grating or a reflective holographic grating.

More specifically, the wavelength separation element is a reflective holographic grating, and a half-wave plate can be arranged between the spatial light modulator and the wavelength separation element, wherein the half-wave plate is used for The control beam is emitted from the spatial light modulator and then enters the polarization direction of the wavelength separation element.

A demultiplexing bidirectional transmission and access system, which includes: two or more optical terminals, each of which includes at least one light emitting module, which can emit a beam of different wavelengths ; At least one wireless optical communication node end contains at least two or more optical receiving modules, which are used to receive more than two beams with different wavelengths; a spatial optical modulator, which can simulate multi-level phase modulation It can be changed to a blazed grating, so that the beam incident on the spatial light modulator can be transmitted at different angles to separate the light receiving modules facing different directions; and a wavelength separating element, which is arranged in the light emitting module of the optical terminal The beams of different wavelengths emitted by the group are on the traveling path, and the wavelength separation element can separate the beams of different wavelengths and transmit them toward the spatial light modulator.

More specifically, the light emitting module of the optical terminal further includes a graded index lens fiber.

More specifically, the optical terminal further has a beam expander, which is used to expand and adjust the beam emitted by the light emitting module of the optical terminal.

More specifically, the optical terminal machine further has a beam collimator, which is used for collimating and adjusting the beam emitted by the light emitting module of the optical terminal machine.

More specifically, the spatial light modulator is a programmable diffractive element, and the programmable diffractive element can be a silicon-based liquid crystal element, a liquid crystal element, or a microelectromechanical system.

More specifically, the wavelength separation element is a reflective blazed grating or a reflective holographic grating.

More specifically, the wavelength separation element is a reflective holographic grating, and a half-wave plate can be arranged between the spatial light modulator and the wavelength separation element, wherein the half-wave plate is used for The control beam is emitted from the spatial light modulator and then enters the polarization direction of the wavelength separation element.

More specifically, the light receiving module at the node end of the wireless optical communication further includes a graded index lens fiber.

More specifically, the optical receiving module of the wireless optical communication node end is a multi-mode optical fiber array.

More specifically, a beam concentrator is further included between the light receiving module of the wireless optical communication node and the spatial light modulator, so that the beam emitted by the spatial light modulator can pass through the beam first The focuser then contacts the light emitting module.

More specifically, the optical receiving module of the single wireless optical communication node can receive one, two, or more than two beams.

The other technical content, features and effects of the present invention will be clearly presented in the following detailed description of the preferred embodiment with reference to the drawings.

The implementation description of the download link direction of the present invention is as follows: Please refer to Figures 1A~1C, which are the overall architecture diagram of the first implementation of the download link of the demultiplexing two-way transmission and access system of the present invention, and the wireless optical The schematic diagram of the structure of the communication node terminal and the schematic diagram of the structure of the optical terminal of the first implementation. It can be seen from the figure that the demultiplexing two-way transmission and access system includes more than two optical terminals 2 and at least one wireless optical communication node. 1. Each of the optical terminals 2 includes a light detecting receiver 21 and a beam focuser 22, wherein the beam focuser 22 is used to enable the beam emitted by the wavelength separation element 15 to pass through the beam focuser 22 first Then contact the light detecting receiver 21.

The wireless optical communication node terminal 1 includes more than two light emitting modules 11, a beam expander 12 (Beam Expander), a beam collimator 13 (Collimated Lens Set), and a spatial light modulator 14 ( SLM) and a wavelength separation element 15, wherein the light emitting module 11 further includes a graded index lens fiber (GRIN Lens Fiber), so when the laser light emitted in the light emitting module 11 is coupled to the gradient After the refractive index lens fiber, the graded refractive index lens fiber can be used as the emission of laser light signals;

The beam expander 12 and the beam collimator 13 can control the size and parallel degree of the beams of different wavelengths emitted by the light emitting module 11, and then, when the beams are incident on the spatial light modulator element After 14, the spatial light modulator is a programmable diffractive element (SLM). Since the programmable diffractive element is a periodic structure composed of multiple pixels, the programmable diffractive element is used as In the case of diffractive elements, the diffraction angle of the diffracted light of each wavelength is limited by the basic periodic structure of the programmable diffraction element, so each wavelength has an independent maximum diffraction angle for the programmable diffraction element. However, to ensure that each wavelength can be switched to the same output position, the minimum deflection angle must be used as the maximum deflection angle limit for each wavelength;

The programmable diffraction element can be a liquid crystal on silicon (LCoS), a liquid crystal (LC), or a microelectromechanical system (MEMS).

Therefore, the spatial light modulator element 14 can control the displacement of the beams of different wavelengths through phase modulation and then enter the wavelength separation element 15 at different angles. Since the beams of different wavelengths enter the wavelength separation element at different angles of incidence, they pass through the The angle at which the wavelength separation element 15 exits the optical terminal 2 can be changed, so that beams of different wavelengths can be respectively transmitted toward the optical terminal in different directions.

In addition, the wavelength separation element 15 is a reflective blazed grating (Phase Only Reflective Blazed Grating) or a reflective holographic grating (Reflective Holographic Grating). As shown in Figure 2A, the wavelength separation element 15 is a reflective holographic grating. Blazed grating, so the beam first passes through the spatial light modulator 14 and with its phase modulation characteristics, the beam can be displaced and incident on the reflective blazed grating at various angles, because the beam is incident on the reflective blazed grating The incident angle is different, so the angle will also change after exiting through the reflective blazed grating to achieve the effect of beam steering (Beam Steering);

Wherein the first described embodiment download link as follows: mainly constituted by two diffractive elements, the parameter elements will be locked so that the diffraction wavelength range of the present embodiment may be used as the embodiment, the use of its structure and its beam wavelength The displacement angle is calculated as follows (reflective grating equation): 𝐷(sin𝜃 _𝑖 +sin𝜃 _𝑚 )=mλ (Formula 1) where D is the grating period, 𝜃 _𝑖 is the beam incident angle, and 𝜃 _𝑚 is the m-order diffracted light The angle with the grating normal, m is the diffraction order, and λ is the wavelength;

Based on the reflection-type grating equation and the geometric relationship diagram of the programmable diffraction element and Grating as shown in Figure 2B, and discussing its first-order diffracted light, the normal line between the beam and the programmable diffraction element can be obtained. The included angle is: 𝜃 _𝑚𝐿 =sin ⁻¹ (𝜆/𝐷 _𝐿 −sin(𝑥)) (Equation 2) where 𝐷 _𝐿 is the period of the grating pattern on the programmable diffraction element, and 𝑥 is the beam incident programmable winding The incident angle (here is also the angle between the placement of the programmable diffractive element and the vertical plane), 𝜆 is the wavelength;

From Figure 2B, we can see that the incident angle of Grating is: 𝜃 _𝑖𝐺 =𝑥+𝑦−sin ⁻¹ (𝜆/𝐷 _𝐿 −sin(𝑥2)) (Equation 3) where 𝜃 _𝑖𝐺 is the beam incident on the grating and the grating method The angle of the line, 𝑥 is the angle between the placement of the programmable diffraction element and the vertical plane, 𝑦 is the angle between the placement of the grating and the vertical plane, 𝐷 _𝐿 is the period of the grating pattern on the programmable diffraction element, and 𝜆 is the wavelength . And since the incident angles of this 𝜃 _𝑚𝐿 and the beam incident programmable diffracting element are on both sides of the normal of the programmable diffracting element, the incident angle of the grating must be added before 𝜃 _𝑚𝐿. One negative sign.

The angle between the beam and the normal of the grating after exiting the grating is: 𝜃 _𝑚𝐺 =sin ⁻¹ (𝜆/𝐷𝐺−sin(𝑥+𝑦−sin ⁻¹ (𝜆/𝐷𝐿−sin(𝑥)))) (Equation 4) Among them, 𝜃 _𝑚𝐺 is the angle between the beam _emitted from the grating and the grating normal, 𝐷 _𝐺 is the grating period, 𝑥 is the angle between the placement of the programmable diffraction element and the vertical plane, and 𝑦 is the angle between the _placement of the grating element and the vertical plane , 𝐷 _𝐿 is the period of the grating pattern on the programmable diffraction element, and 𝜆 is the wavelength.

The angular range of beams of different wavelengths that can be displaced in the download link direction is limited by the resolution of the programmable diffraction element, that is, 𝐷 _𝐿 has a minimum of 2 × 6.4 (μm) and a maximum of 1920 × 6.4 (μm). Substituting these two restrictions into Equation 4, the beam displacement angle of each wavelength of this architecture is the angle between the exit beam and the grating normal (10 deg.). The restrictions are as follows: (1) _1530nm → 𝜃 _𝑚𝐺 = 8.94°~ 13.98° → Displacement Angle ∆𝜃 _𝑚𝐺 = 5.04° (2) 1550nm → 𝜃 _𝑚𝐺 = 9.63°~14.76° → Displacement Angle ∆𝜃 _𝑚𝐺 = 5.13° (3) _1570nm → 𝜃 _{𝑚 15.} 𝜃 _𝑚𝐺 = 5.21° (4) _1590nm → 𝜃 _𝑚𝐺 = 11.03°~16.33° → displacement angle ∆𝜃 _𝑚𝐺 = 5.3°

Since the wavelength separation element 15 can also be a reflective holographic grating (Reflective Holographic Grating), since the spatial light modulator of the reflective holographic grating and the programmable diffractive element requires the polarization direction of the input light wave, the former is The latter is 45 degree linear polarization. As shown in Figures 3 and 4A, half of the wave plate 16 must be added to the two diffractive elements to control the beam to exit from the first diffractive element and then enter the second The polarization direction of the two diffractive elements, and by substituting the polarization direction of the input light and the polarization direction of the light to be output after passing through the half-wave plate into the Jones Matrix calculation, it can be known that the input half The polarization direction of the wave plate and the light output from the half wave plate can be deflected by 45 degrees, so the half wave plate must be set to an angle of 22.5 degrees with the horizontal axis.

The description of the second implementation of the download link is as follows : Since the second implementation of the download link is mainly composed of two diffractive elements, the parameters of the diffractive elements will limit the wavelength range that can be used in this embodiment. The wavelength used by the architecture and the angle of beam displacement are calculated as follows (reflective grating equation): 𝐷(sin𝜃 _𝑖 +sin𝜃 _𝑚 )=mλ (Equation 5) where D is the grating period and 𝜃 _𝑖 is the beam incident angle , 𝜃 _𝑚 is the angle between the m-order diffracted light and the grating normal, m is the diffraction order, and λ is the wavelength;

Based on the reflection-type grating equation and the geometric relationship between the programmable diffractive element and the grating as shown in Figure 4B, and discussing its first-order diffracted light, it can be concluded that the beam passes through the programmable diffractive element and the LCoS The normal angle is: 𝜃 _𝑚𝐿 =sin ⁻¹ (𝜆/𝐷 _𝐿 −sin(𝑥2)) (Equation 6) where 𝐷 _𝐿 is the period of the grating pattern on the programmable diffraction element, and 𝑥2 is the beam incidence programmable The incident angle when the diffraction element is changed (here is also the angle between the placement of the programmable diffraction element and the vertical plane), 𝜆 is the wavelength;

From Figure 4B, we can see that the incident angle of Grating is: 𝜃 _𝑖𝐺 = 𝑥2+𝑦2−sin ⁻¹ (𝜆/𝐷 _𝐿 −sin(𝑥2)) (Equation 7) where 𝜃 _𝑖𝐺 is the beam incident on the grating and the grating method The angle of the line, 𝑥2 is the angle between the placement of the programmable diffraction element and the vertical plane, 𝑦2 is the angle between the placement of the grating and the vertical plane, 𝐷 _𝐿 is the period of the grating pattern on the programmable diffraction element, and 𝜆 is the wavelength . And because the incident angles of this 𝜃 _𝑚𝐿 and the beam incident programmable diffracting element are on both sides of the normal of the programmable diffracting element, the incident angle of the grating must be added before 𝜃 _𝑚𝐿 by observing Figure 4B. One negative sign.

The angle between the beam and the normal of the grating after exiting the grating is: 𝜃 _𝑚𝐺 =sin ⁻¹ (𝜆/𝐷𝐺−sin(𝑥2+𝑦2−sin ⁻¹ (𝜆/𝐷𝐿−sin(𝑥2)))) (Equation 8) Among them, 𝜃 _𝑚𝐺 is the angle between the beam _emitted from the grating and the grating normal, 𝐷 _𝐺 is the grating period, 𝑥2 is the angle between the placement of the programmable diffraction element and the vertical plane, and 𝑦2 is the angle between the _placement of the grating element and the vertical plane , 𝐷 _𝐿 is the period of the grating pattern on the programmable diffraction element, and 𝜆 is the wavelength.

The angular range of beams of different wavelengths that can be displaced in the download link direction is limited by the resolution of the programmable diffraction element, that is, 𝐷 _𝐿 has a minimum of 2 × 6.4 (μm) and a maximum of 1920 × 6.4 (μm). Substituting these two restrictions into Equation 8, the angle at which the beam of each wavelength of this architecture can be displaced is the angle between the exit beam and the grating normal (52 deg.). The restrictions are as follows: (1) _1530nm → 𝜃 _𝑚𝐺 = 51.66°~ 56.98° → Displacement angle ∆𝜃 _𝑚𝐺 = 5.32° (2) 1550nm → 𝜃 _𝑚𝐺 = 51.74°~57.07° → Displacement angle ∆𝜃 _𝑚𝐺 = 5.33° (3) _1570nm → 𝜃. 𝜃 _𝑚𝐺 = 5.35° (4) _1590nm → 𝜃 _𝑚𝐺 = 51.91°~57.27° → displacement angle ∆𝜃 _𝑚𝐺 = 5.36°

The implementation of the upload link direction of the present invention is described as follows : As shown in Figures 5A to 5C, the demultiplexing two-way transmission and access system includes more than two optical terminals 2 and at least one wireless optical communication node terminal 1. Each optical terminal 2 includes a light emitting module 23 (the light emitting module 23 further includes a graded index lens fiber), a beam expander 24 and a beam collimator 25, and the light emitting module The group 23 can emit a beam with different wavelengths, and the beam expander 24 and the beam collimator 25 can control the beams of different wavelengths emitted by the light emitting module 23 to control the beam size and the degree of parallelism;

The wireless optical communication node terminal 1 includes two or more light receiving modules 17, a spatial light modulator 14, a wavelength separation element 15 and a beam concentrator 18, wherein the wavelength separation element 15 can transmit light The beams of different wavelengths emitted by the transmitting module 23 are separated and transmitted toward the spatial light modulator 14;

The spatial light modulator 14 can further simulate a multi-stage phase modulation blazed grating, so that the beam incident on the spatial light modulator can be separated at different angles and transmitted toward the light receiving modules 17 in different directions. , Because the spatial light modulator is a programmable diffractive element, and the programmable diffractive element is an element composed of a matrix of pixels, it simulates the use of a phase-type blazed grating as a conventional technology, related fields The technicians must know how to simulate, so there is no additional explanation here.

In addition, the wavelength separation element 15 is a reflective blazed grating (Phase Only Reflective Blazed Grating) or a reflective holographic grating (Reflective Holographic Grating). As shown in Figures 6A and 6B, the wavelength separation element 15 is a The reflective blazed grating, and the corresponding light receiving module 17 has a graded index lens fiber. In addition, the difference between Figure 6A and Figure 6B is that a one-dimensional receiving structure or a two-dimensional receiving structure is adopted at the receiving end. Figure 6A uses a one-dimensional receiving architecture (a single optical receiving module 17 can receive one beam), and Figure 6B uses a two-dimensional receiving architecture (a single optical receiving module 17 can receive more than one beam );

Therefore, in the first implementation of the upload link, when the beam is transmitted upstream, it is first split by a reflective phase-type blazed grating, and then separately incident on the spatial light modulator (spatial light modulator) of the programmable diffraction element 14) Above, and by controlling the spatial light modulator of the programmable diffractive element to simulate the multi-stage phase modulation blazed grating, the design and calculation of the blazed grating pattern makes the beams of different wavelengths pass through this node Then the effect of wavelength selection and switching can be achieved at the receiving end.

The first implementation of the upload link is explained as follows : In the first implementation of the system upload link, the period of the grating and the size of the programmable diffraction element will limit the wavelength of the light source used by the system and the channel spacing between the wavelengths. (Channel Spacing), so the following is to calculate the relationship between the grating and the channel spacing using different periods without changing the architecture. The first implementation of the upload link architecture diagram is shown in Figure 6C, where, 𝑦1 is the angle between the programmable diffraction element (LCoS in this embodiment) and the vertical plane, 𝑥1 is the angle between the grating element (grating) and the vertical plane, and 𝜃 _𝑚𝐺 is the normal line of the beam after it is _emitted from the grating The included angle, 𝜃 _𝑚𝐿 is the angle between the beam and the normal of the programmable diffractive element. Since this structure is the same as the previous one, other parts are omitted. This embodiment directly calculates the relationship between the grating and the channel spacing using different periods. According to the reflection type grating equation (Equation 5), the following formula can be obtained: 𝐷 _𝐺 (sin𝜃 _𝑖 +sin𝜃 ₁ )=λ ₁ (Equation 9) 𝐷 _𝐺 (sin𝜃 _𝑖 +sin𝜃 ₂ )=λ ₁ +Δλ (Equation 10 ) Where 𝐷 _𝐺 is the grating period, 𝜃 _𝑖 the incident angle of the grating, 𝜃 ₁ and 𝜃 ₂ are respectively λ ₁ and λ ₁ + Δλ first-order diffraction angle, λ ₁ is the wavelength, Δλ is the channel spacing, and then Subtracting Equation 10 from Equation 9 can get the following formula: 𝐷 _𝐺 (sin𝜃 ₂ −sin𝜃 ₁ )=Δλ (Equation 11) And in this architecture, it is assumed that the largest light spot (RMS Spot Radius) is distributed on the programmable diffraction element It is 371.648μm, (λ ₁ + ∆λ=1530nm). Therefore, when calculating the grating period and the channel spacing, it is necessary to consider the two adjacent wavelengths under the conditions of the channel spacing of ∆λ and the grating period of 𝐷 _𝐺 At least one spot distance must be separated on the programmable diffraction element, so 𝜃 ₂ − 𝜃 ₁ must meet the condition of "𝜃 ₂ − 𝜃 ₁ ≥ 0.45°".

Therefore, the maximum wavelength of the light spot on the programmable diffraction element (λ ₁ + ∆λ = 1530nm) is used as the limit. When λ ₁ + ∆λ = 1530nm, 𝜃 ₂ = 48.1035°, 𝜃 ₁ = 47.6533°, and grating The relationship between period and channel spacing is as follows: 𝐷 _𝐺 (sin48.1035° − sin47.6533°) = ∆λ (Formula 12)

The first implementation of the upload link uses a grating period density of 600/mm, that is, the converted grating period (𝐷 _𝐺 ) is 1.67μm, and the grating period (𝐷 _𝐺 ) is substituted into Equation 12 to get the channel Channel Spacing ∆λ is 8.801nm, and if you want to reduce the channel spacing supported by this architecture to 0.8nm, which is the DWDM channel spacing specification, you must replace the grating with a grating period (𝐷 _𝐺 ) of 0.1518μm. The period density of the back grating is 6587.615/mm, and from the above results, it can be known that the smaller the use period of the grating in this architecture, the smaller the channel spacing that can be used in this architecture.

In addition, the wavelength separation element 15 can also be a reflective holographic grating (Reflective Holographic Grating), and corresponding to the light receiving module 17 is a multimode fiber array (Fiber Ribbon), as shown in Figures 7, 8A and 8B As shown, half of the wave plate 16 must be added to the two diffractive elements to control the polarization direction when the beam exits from the first diffractive element and then enters the second diffractive element. Therefore, the beam passes through the upload link When transmitting back to the wireless optical communication node system, the different carrier wavelengths are separated into the programmable diffractive element through a reflective holographic grating with a fixed period, and executed by the spatial light modulator that controls the programmable diffractive element The function of the phase-type blazed grating is to control the beams of each wavelength to produce different diffraction angles, so that each wavelength can achieve the effect of wavelength selection and switching at the wireless optical communication node system. The optical receiving module of the wireless optical communication node end is a multi-mode optical fiber array.

Wherein the second link upload embodiment described as follows: a second embodiment of the carrier of the link on the system, since the size of the grating period of the diffractive element and a programmable limit of the channel between the source wavelength and the wavelength spacing used in the system (Channel Spacing), so the following is to calculate the relationship between grating and channel spacing using different periods without changing the architecture. The second implementation of the upload link architecture is shown in Figure 8C, where, 𝑦3 is the angle between the programmable diffraction element (LCoS in this example) and the vertical plane, 𝑥3 is the angle between the grating element (grating) and the vertical plane, 𝜃 _𝑚𝐺 is the normal line of the beam with the grating after being _emitted from the grating The included angle, 𝜃 _𝑚𝐿 is the angle between the beam and the normal of the programmable diffractive element. Since this structure is the same as the previous one, other parts are omitted. This embodiment directly calculates the relationship between the grating and the channel spacing using different periods. According to the reflection type grating equation (Equation 5), Equation 9 and Equation 10 can be obtained, and then Equation 10 is subtracted from Equation 9 to obtain the following Equation 11.

In this architecture, it is assumed that the largest spot (RMS Spot Radius) distributed on the programmable diffractive element is 458.019μm, (λ ₁ + ∆λ=1550nm). Therefore, when calculating the grating period and channel spacing, it must be considered _Under the condition of the channel spacing of ∆λ and the grating period of 𝐷 _𝐺 , the two adjacent wavelengths of the channel spacing must be separated by at least one spot distance on the programmable diffraction element, so 𝜃 ₂ − 𝜃 ₁ must meet "𝜃 ₂ − 𝜃 ₁ ≥ 0.3361°”.

Therefore, the maximum wavelength of the light spot on the programmable diffraction element (λ ₁ + ∆λ = 1550nm) is used as the limit. When λ ₁ + ∆λ = 1550nm, 𝜃 ₂ = 66.5143°, 𝜃 ₁ = 66.1782° and the grating period The relationship with the channel spacing is as follows: 𝐷 _𝐺 (sin66.5143° − sin66.1782°) = ∆λ (Formula 13)

The second implementation of the upload link uses a grating period density of 1100/mm, that is, the converted grating period (𝐷 _𝐺 ) is 0.909μm, and substituting the grating period (𝐷 _𝐺 ) into Equation 13 can get the channel Channel Spacing ∆λ is 2.14nm. If you want to reduce the channel spacing supported by this architecture to 0.8nm, which is the DWDM channel spacing specification, you must replace the grating with a grating period (𝐷 _𝐺 ) of 0.3399μm. The period density of the back grating is 2942.042/mm, and from the above results, it can be known that the smaller the use period of the grating in this architecture, the smaller the channel spacing that can be used in this architecture.

Compared with other conventional technologies, the advantages of the division-wave multiplexing bidirectional transmission and access system provided by the present invention are as follows: (1) The present invention can use a spatial light modulator with programmable diffractive elements as dynamic diffractive elements. And through the control of the spatial light modulator of the programmable diffractive element, the output beam width and position are reconfigured for the incident beam. This will achieve the purpose of the two-way wireless optical communication system node, and improve the traditional system architecture through the above system The disadvantage of insufficient flexibility. (2) The present invention can apply a spatial light modulator with programmable diffractive elements to a wireless optical communication system to form a wireless optical communication node. At the fiber optic network end, it can use its ability to reconfigure the incident beam to construct a A Wavelength Selective System with wavelength selection and switching capabilities. At the user end, it can use its phase modulation characteristics to expand/contract beams of different wavelengths and change their propagation direction.

The present invention has been disclosed above through the above-mentioned embodiments, but it is not intended to limit the present invention. Anyone familiar with this technical field with ordinary knowledge should understand the aforementioned technical features and embodiments of the present invention without departing from the scope of the present invention. Within the spirit and scope, some changes and modifications can be made. Therefore, the patent protection scope of the present invention shall be subject to the definition of the claims attached to this specification.

1: Wireless optical communication node end 11: Light emission module 12: Beam expander 13: Beam collimator 14: Spatial light modulator 15: Wavelength separation element 16: Half wave plate 17: Optical receiving module 18: beam focuser 2: Optical terminal 21: Light detection receiver 22: beam focuser 23: light emitting module 24: beam expander 25: Beam collimator

[Figure 1A] is a schematic diagram of the overall architecture of the first implementation of the download link of the DWDM bidirectional transmission access system of the present invention. [Figure 1B] is a schematic diagram of the architecture of the wireless optical communication node end of the first implementation of the download link of the split-wave multiplexing two-way transmission and access system of the present invention. [Figure 1C] is a schematic diagram of the optical terminal structure of the first implementation of the download link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 2A] is a schematic diagram of the actual operation architecture of the first implementation of the download link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 2B] is a schematic diagram of the download link architecture of the first implementation of the download link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 3] is a schematic diagram of the architecture of the wireless optical communication node end of the second implementation of the download link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 4A] is a schematic diagram of the actual operation architecture of the second implementation of the download link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 4B] is a schematic diagram of the download link architecture of the second implementation of the download link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 5A] is a schematic diagram of the overall architecture of the first implementation of the upload link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 5B] is a schematic diagram of the architecture of the wireless optical communication node end of the first implementation of the upload link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 5C] is a schematic diagram of the architecture of the optical terminal of the first implementation of the upload link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 6A] is a schematic diagram of the actual operation architecture of the first implementation of the upload link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 6B] is a schematic diagram of another actual operation architecture of the first implementation of the upload link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 6C] is a schematic diagram of the upload link architecture of the first implementation of the upload link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 7] is a schematic diagram of the architecture of the wireless optical communication node end of the second implementation of the upload link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 8A] is a schematic diagram of the actual operation architecture of the second implementation of the upload link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 8B] is a schematic diagram of another actual operational architecture of the second implementation of the upload link of the split-wave multiplexing bidirectional transmission and access system of the present invention. [Figure 8C] is a schematic diagram of the upload link architecture of the second implementation of the upload link of the split-wave multiplexing bidirectional transmission and access system of the present invention.

1: Wireless optical communication node end

11: Light emission module

12: Beam expander

13: Beam collimator

14: Spatial light modulator

15: Wavelength separation element

2: Optical terminal

Claims (19)

A sub-wavelength multiplexing two-way transmission and access system, which includes: two or more optical terminals, each of which includes at least one optical detection receiver; at least one wireless optical communication node terminal, which includes at least: two More than one light emitting module, which can respectively emit two or more beams with different wavelengths; A wavelength separation element, which can separate beams of different wavelengths for transmission to optical terminals in different directions; and A spatial light modulator is arranged on the travel path of beams with different wavelengths emitted by the light emitting module at the wireless optical communication node end, and the spatial light modulator element is used to control different wavelengths through phase modulation After the beam is shifted, it is incident on the wavelength separation element at different angles. Since the beams of different wavelengths enter the wavelength separation element at different incident angles, the angle after exiting the optical terminal through the wavelength separation element can be changed to face different directions. Optical terminal. The demultiplexing and multiplexing two-way transmission and access system according to claim 1, wherein the optical terminal further includes a beam concentrator, so that the beam emitted by the wavelength separation element can pass through the beam concentrator and then contact the light detection receiver. The demultiplexed bidirectional transmission and access system according to claim 1, wherein the light emitting module further includes a graded index lens fiber. The division-wave multiplexing two-way transmission and access system according to claim 1, wherein a beam expander is arranged between the light emitting module and the spatial light modulator for the beam emitted by the light emitting module Make expansion adjustments. The division-wave multiplexing two-way transmission and access system according to claim 1, wherein a beam collimator is arranged between the light emitting module and the spatial light modulator, which is used to transmit the light emitting module The beam is collimated. The division-wave multiplexing bidirectional transmission and access system according to claim 1, wherein the spatial light modulator is a programmable diffractive element, and the programmable diffractive element can be a silicon-based liquid crystal element, a liquid crystal Components or MEMS. The demultiplexing bidirectional transmission and access system according to claim 1, wherein the wavelength separation element is a reflective blazed grating or a reflective holographic grating. The division-wave multiplexing bidirectional transmission access system according to claim 7, wherein the wavelength separation element is a reflective holographic grating, and a half wave plate can be arranged between the spatial light modulator and the wavelength separation element, wherein The half-wave plate is used for controlling the polarization direction of the beam emitted from the spatial light modulator and then incident on the wavelength separation element. A demultiplexing two-way transmission and access system, which includes: two or more optical terminals, each of which includes at least one light emitting module, which can emit a beam of different wavelengths ; At least one wireless optical communication node terminal includes at least: Two or more optical receiving modules, which are used to receive two or more beams with different wavelengths; A spatial optical modulator, which can simulate multi-stage phases The blazed grating is modulated, so that the beams incident on the spatial light modulator can be transmitted at different angles to separate the light receiving modules facing different directions; and a wavelength separation element, which is arranged on the light emitting terminal of the optical terminal The module emits beams with different wavelengths on the travel path, and the wavelength separation element can separate the beams of different wavelengths and transmit them toward the spatial light modulator. The demultiplexed bidirectional transmission and access system according to claim 9, wherein the light emitting module of the optical terminal further includes a graded index lens fiber. The demultiplexing and multiplexing two-way transmission and access system according to claim 9, wherein the optical terminal further has a beam expander for expanding and adjusting the beam emitted by the optical transmitting module of the optical terminal. The division-wave multiplexing two-way transmission and access system according to claim 9, wherein the optical terminal further has a beam collimator for collimating the beam emitted by the optical transmitting module of the optical terminal . The demultiplexed bidirectional transmission and access system according to claim 9, wherein the spatial light modulator is a programmable diffractive element, and the programmable diffractive element can be a silicon-based liquid crystal element, a liquid crystal Components or MEMS. The DWDM bidirectional transmission and access system according to claim 9, wherein the wavelength separation element is a reflective blazed grating or a reflective holographic grating. The division-wave multiplexing bidirectional transmission and access system according to claim 14, wherein the wavelength separation element is a reflective holographic grating, and a half wave plate can be arranged between the spatial light modulator and the wavelength separation element, wherein The half-wave plate is used for controlling the polarization direction of the beam emitted from the spatial light modulator and then incident on the wavelength separation element. The demultiplexed bidirectional transmission access system according to claim 14, wherein the wavelength separation element is a reflective holographic grating, and the light receiving module at the end of the wireless optical communication node further includes a graded index lens fiber. The division-wave multiplexing bidirectional transmission and access system according to claim 14, wherein the wavelength separation element is a reflective holographic grating, and the light receiving module at the end of the wireless optical communication node is a multimode optical fiber array. The demultiplexing two-way transmission and access system according to claim 9, wherein a beam concentrator is further included between the light receiving module of the wireless optical communication node and the spatial light modulator, so that the spatial light The beam emitted by the modulator can first pass through the beam concentrator and then contact the light emitting module. The demultiplexing and multiplexing two-way transmission and access system according to claim 9, wherein the optical receiving module of a single wireless optical communication node can receive one, two or more than two beams.

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