阅读说明：本技术 Lcos调节方法，光器件以及可重构光分插复用器 (LCOS adjusting method, optical device and reconfigurable optical add-drop multiplexer ) 是由 毛磊 宗良佳 常泽山 于 2020-05-21 设计创作，主要内容包括：本申请实施例公开了一种LCOS调节方法,应用于光通信领域。本申请的LCOS调节方法包括：调节第一区域上光栅的灰度分布的交界线,以使得第一光斑覆盖尽量少的光栅的灰度分布的交界线,第一区域为LCOS的K×H个区域中的一个区域,K为大于0的整数,H为大于1的整数,LCOS加载有光栅的灰度分布,第一区域为第一光信号形成第一光斑的区域,第一区域用于对第一光信号进行重定向。其中,光栅的交界线会产生串扰,通过调节第一区域的光栅的交界线,以使得第一光斑覆盖尽量少的光栅的交界线,因此可以减少串扰。(The embodiment of the application discloses an LCOS adjusting method, which is applied to the field of optical communication. The LCOS adjusting method comprises the following steps: adjusting a boundary line of gray distribution of the grating on the first area to enable the first light spot to cover the boundary line of the gray distribution of the grating as less as possible, wherein the first area is one area of K multiplied by H areas of the LCOS, K is an integer larger than 0, H is an integer larger than 1, the LCOS is loaded with the gray distribution of the grating, the first area is an area where the first light signal forms the first light spot, and the first area is used for redirecting the first light signal. The grating boundary lines of the first area are adjusted to enable the first light spots to cover the grating boundary lines as few as possible, so that the crosstalk can be reduced.)

1. A Liquid Crystal On Silicon (LCOS) tuning method, comprising:

adjusting a boundary line of gray distribution of a grating on a first area to enable a first light spot to cover the boundary line of the gray distribution of the grating as little as possible, wherein the first area is one area of K × H areas of the LCOS, K points to a port direction of the LCOS, K is an integer greater than 0, H points to a wavelength direction of the LCOS, H is an integer greater than 1, the LCOS is loaded with the gray distribution of the grating, the first area is an area where a first light signal forms the first light spot, and the first area is used for redirecting the first light signal.

2. The method of claim 1, wherein prior to said adjusting the boundary line of the gray scale distribution of the grating of the first region, the method further comprises:

obtaining a first intensity value of the first optical signal, the first intensity value being a power of the redirected first optical signal;

after the adjusting the boundary line of the gray scale distribution of the grating of the first region, the method further comprises:

obtaining a second intensity value of the first optical signal, the second intensity value being a power of the redirected first optical signal;

when the following conditions are met, the first light spot covers the boundary line of the gray level distribution of the grating as less as possible:

the second intensity value is greater than the first intensity value.

3. The method according to claim 1 or 2, wherein the adjusting the boundary line of the gray distribution of the grating of the first region comprises:

adjusting the boundary line of the gray scale distribution of the grating of the first area, so that the distance between the center line of the first light spot and the center line of the gray scale distribution of one period of the grating of the first area is less than A/4, wherein A is the full width at half maximum of the first light spot.

4. The method according to any one of claims 1 to 3, wherein the adjusting the boundary line of the gray scale distribution of the grating of the first region comprises:

translating a gray scale distribution of the grating of the first region along a port direction of the LCOS.

5. The method according to any one of claims 1 to 3, wherein the adjusting the boundary line of the gray scale distribution of the grating of the first region comprises:

adjusting a period of a gray distribution of the grating of the first region;

the method further comprises the following steps:

adjusting a maximum phase of a gray scale distribution of the grating of the first region such that a redirection angle of the first optical signal is unchanged.

6. The method according to any one of claims 1 to 5, wherein the adjusting the boundary line of the gray scale distribution of the grating of the first region comprises:

if the height of the first light spot is equal to the height of the gray scale distribution of one period grating of the first area, adjusting the boundary line of the gray scale distribution of the grating of the first area to enable the first light spot to be matched with one period grating of the first area;

if the height of the first light spot is smaller than the height of the gray scale distribution of one period grating of the first area, adjusting the boundary line of the gray scale distribution of the grating of the first area, so that the first light spot is in one period grating of the first area.

7. The method of any of claims 2 to 6, wherein after obtaining the second intensity value, the method further comprises:

adjusting a profile coefficient of the gray level distribution of the grating in the first region;

obtaining a third intensity value, the first intensity value being the power of the redirected first optical signal, the third intensity value being obtained after adjusting a profile coefficient of a gray scale distribution of the grating of the first region, the third intensity value being greater than the second intensity value.

8. The method according to any one of claims 1 to 7, further comprising:

adjusting a boundary line of gray scale distribution of a grating of a second area, so that a second light spot covers as little as possible of the boundary line of gray scale distribution of the grating of the second area, the second area is one area of K × H areas of the LCOS, the second area is an area where a second light signal forms the second light spot, the second area is used for redirecting the second light signal, and a center line of the second light spot is different from a center line of the first light spot.

9. The method according to any one of claims 1 to 8, further comprising:

adjusting a boundary line of gray scale distribution of a grating of a third area, so that a third light spot covers as little as possible of the boundary line of gray scale distribution of the grating of the third area, where the third area is one of K × H areas of the LCOS, the third area is an area where a third light signal forms the third light spot, the third area is used for redirecting the third light signal, and a center line of the third light spot is the same as a center line of the first light spot.

10. The method according to any one of claims 1 to 9, wherein the first spot is a flat-topped spot.

11. A light device, comprising:

a first input port, a first output port, a dispersive element and a liquid crystal on silicon LCOS;

the first input port is for incidence of a first incident optical signal to the dispersive element;

the dispersion element is configured to decompose the first incident light signal into a first light signal group of light signals with different wavelengths, and transmit the first light signal group to the LCOS, where the LCOS includes K × H regions, K is directed to a port direction of the LCOS, K is an integer greater than 0, H is directed to a wavelength direction of the LCOS, H is an integer greater than 1, and the LCOS is loaded with a gray scale distribution of a grating, where a first region of the K × H regions is a region where a first light signal forms a first light spot, the first light signal belongs to the first light signal group, and an intersection line of the gray scale distribution of the grating of the first region is configured so that the first light spot covers as few intersection lines of the gray scale distribution of the grating as possible;

the LCOS is used for redirecting the first optical signal and transmitting the redirected first optical signal to the first output port.

12. A light device according to claim 11, wherein the boundary line of the gray-scale distribution of the grating of the first region is arranged so that the first spot covers as little as possible of the boundary line of the gray-scale distribution of the grating when the following condition is satisfied:

a second intensity value is greater than a first intensity value, wherein the first intensity value is the power of the first optical signal passing through the first output port before the boundary line of the gray-scale distribution of the grating of the first region is configured, and the second intensity value is the power of the first optical signal passing through the first output port after the boundary line of the gray-scale distribution of the grating of the first region is configured.

13. A light device as claimed in claim 11 or 12, characterized in that the boundary line of the gray distribution of the grating of the first area is configured such that the distance of the centre line of the first light spot from the centre line of the gray distribution of one period of the grating of the first area is less than a/4, a being the full width at half maximum of the first light spot.

14. The optical device according to any one of claims 11 to 13, wherein the boundaries of the gray scale distribution of the grating in the first region are arranged such that the first light spot covers as little as possible of the gray scale distribution of the grating, which is obtained by shifting the gray scale distribution of the grating in the first region in the direction of the port of the LCOS.

15. A light device as claimed in any one of claims 11 to 13, characterized in that, with a constant redirection angle of the first light signal, the boundaries of the grey scale distribution of the grating of the first area are arranged such that the first spot covers as little as possible of the boundaries of the grey scale distribution of the grating;

the condition that the redirection angle of the first optical signal is not changed is obtained by adjusting the period and the maximum phase of the gray scale distribution of the grating in the first area.

16. The optical device according to any one of claims 11 to 15, wherein if the height of the first light spot is equal to the height of the gradation distribution of one period grating of the first region, in a case where the first light spot matches the gradation distribution of one period grating of the first region, an intersection line of the gradation distributions of the gratings of the first region is arranged so that the first light spot covers as little as possible of the intersection line of the gradation distributions of the gratings;

if the height of the first spot is smaller than the height of the gray-scale distribution of the one-period grating in the first region, when the first spot is within the gray-scale distribution of the one-period grating in the first region, the boundary line of the gray-scale distribution of the grating in the first region is arranged so that the first spot covers as little as possible of the boundary line of the gray-scale distribution of the grating.

17. The optical device according to any one of claims 12 to 16, wherein a profile coefficient of a gray scale distribution of the grating in the first region is configured such that a third intensity value is larger than the second intensity value, the second intensity value being a power of the optical signal at the first output port before the profile coefficient of the gray scale distribution of the grating in the first region is configured, and the third intensity value being a power of the optical signal at the first output port after the profile coefficient of the gray scale distribution of the grating in the first region is configured.

18. A light device as claimed in any one of claims 11 to 17, wherein the device further comprises a second input port;

the second input port is configured to input a second incident optical signal to the dispersive element;

the dispersion element is further configured to decompose the second incident optical signal into a second optical signal group of optical signals with different wavelengths, and transmit the second optical signal group to the LCOS, where a second area of the K × H areas is an area where a second optical signal forms a second optical spot, the second optical signal belongs to the second optical signal group, a center line of the second optical spot is different from a center line of the first optical spot, and an intersection line of gray scale distributions of gratings of the second area is configured such that the second optical spot covers as little as possible of an intersection line of gray scale distributions of gratings of the second area.

19. The optical device according to any one of claims 11 to 18, wherein a third region of the K × H regions is a region where a third optical signal forming a third light spot belongs to the first optical signal group, a center line of the third light spot is the same as a center line of the first light spot, and an intersection line of the gradation distributions of the gratings of the third region is arranged so that the third light spot covers as little as possible of the intersection line of the gradation distributions of the gratings of the third region.

20. A light device as claimed in any one of claims 11 to 19, characterized in that the first light spot is a flat-topped light spot.

21. A reconfigurable optical add/drop multiplexer, comprising:

a wave splitting module and a wave combining module;

the wavelength division module is used for downloading a first optical wavelength signal to a website;

the wave combination module is used for receiving a second optical wavelength signal uploaded by the site;

the optical device according to any one of claims 11 to 20, wherein the wavelength division module and/or the wavelength combination module is a wavelength selective switch.

22. A computer storage medium having stored therein instructions that, when executed on a computer, cause the computer to perform the method of any one of claims 1 to 10.

23. A computer program product, characterized in that the computer program product, when executed on a computer, causes the computer to perform the method according to any one of claims 1 to 10.

Technical Field

The present invention relates to the field of optical communications, and in particular, to a Liquid Crystal On Silicon (LCOS) adjusting method, an optical device, and a reconfigurable optical add-drop multiplexer.

Background

LCOS is a matrix liquid crystal device based on reflective mode, with very small dimensions. Such a matrix liquid crystal device is fabricated on a silicon chip using a Complementary Metal Oxide Semiconductor (CMOS) technology.

An optical device that utilizes a phase-modulated optical signal, such as a Wavelength Selective Switch (WSS) or a Dynamic Gain Flattening Filter (DGFF), typically includes an LCOS. The working principle of the LCOS is that different voltages are loaded on different pixel points (pixels) of the LCOS, and due to the birefringence effect of the liquid crystal, the different voltages correspond to different phase delay amounts, so that a structure similar to a grating can be formed. By applying a periodic voltage in the Y direction across the pixel of the LCOS, a grating can be formed as shown in fig. 1. As shown in fig. 1, fig. 1 includes a raster front view 101 and a raster left view 102. The periodic grating 103 is one period of the grating. The periodic grating 103 is in phase with the Y-axis. After the beam 104 perpendicular to the Y-axis hits the blazed grating, because of the phase of the blazed grating, the beam 104 will be reflected back at an angle different from the incident angle to form a reflected beam 105. It will also be appreciated that the beam 104 is deflected in the Y-axis direction.

In practice, the LCOS-formed grating will produce a reflected beam that is in a different direction than the reflected beam 105, resulting in cross-talk.

Disclosure of Invention

The application provides an LCOS adjusting method, an optical device and a reconfigurable optical add-drop multiplexer, which can reduce crosstalk.

A first aspect of the present application provides a LCOS adjusting method, including: the controller adjusts the boundary line of the gray-scale distribution of the grating of the first area so that the first light spot covers as little of the boundary line of the gray-scale distribution of the grating as possible. The boundary line of the gray level distribution of the grating refers to the boundary line of the gratings with different periods in the port direction, which is hereinafter referred to as the boundary line of the gratings for short. In the direction of the ports of the LCOS, there are 2 lines of boundary between one periodic grating and two adjacent periodic gratings. Adjusting the boundaries of the gratings means that in the first region, the boundaries of some or all of the gratings are shifted in the port direction. In LCOS, the grey distribution of the grating is loaded. In a specific implementation manner, different voltages can be loaded on different pixel points (pixels) of the LCOS, and due to the birefringence effect of the liquid crystal, the different voltages correspond to different phase delay amounts, so that a structure similar to a grating can be formed. The LCOS comprises K multiplied by H areas, wherein K points to the direction of the port of the LCOS, K is an integer larger than 0, H points to the direction of the wavelength of the LCOS, and H is an integer larger than 1. Wherein the first region is one of the K × H regions. After the first optical signal is incident on the first area of the LCOS, the first area is used to redirect, e.g., reflect or transmit, the first optical signal and form a first light spot at the first area. In the wavelength direction of LCOS, different regions may have different grating gray scale distributions. Since H is an integer greater than 1, there are a minimum of 2 regions in the wavelength direction of LCOS.

Wherein crosstalk is generated at the boundary of the gratings. In the first aspect of the present application, the controller adjusts the boundary line of the gratings in the first area, so that the first light spot covers as few as possible of the boundary line of the gratings, thereby reducing crosstalk.

In a first embodiment of the first aspect of the present application, before adjusting the boundary line of the grating of the first area, the controller obtains a first intensity value of the first optical signal, where the first intensity value is the power of the redirected first optical signal. After adjusting the boundary of the grating of the first area, the controller obtains a second intensity value of the first optical signal, wherein the second intensity value is the power of the redirected first optical signal. If the second intensity value is greater than the first intensity value, the first light spot covers as few of the boundary lines of the grating as possible. Wherein the first intensity value may be a target intensity value or a crosstalk intensity value. The target intensity value refers to the power of the first optical signal output from the target output port, and the crosstalk intensity value refers to the negative value of the power of the first optical signal output from the non-target output port. The target output port refers to a port where the first optical signal is expected to be output, and the non-target output port refers to a port where the first optical signal generates crosstalk. The power of the first optical signal output by the target output port is generally greater than the power of the first optical signal output by the non-target output port.

Whether the first light spot covers the boundary line of the grating as little as possible is judged, a positioning sensor needs to be arranged in the LCOS, the starting position and the end position of the first light spot in the port direction are obtained, and the number of the boundary line of the grating between the starting position and the end position needs to be calculated. Compared with the technical means, whether the first light spot covers the boundary line of the grating as less as possible is judged by the intensity value of the first light signal, so that the method is simpler and reduces the cost. Wherein the intensity value of the first optical signal may be measured by an intensity sensor, which is simpler to implement than a positioning sensor. Moreover, the intensity sensor is not required to be arranged on the LCOS, so that the measurement of one intensity sensor on a plurality of LCOSs can be realized, and the cost is reduced.

Based on the first aspect of the present application or the first implementation manner of the first aspect, in a second implementation manner of the first aspect of the present application, the controller adjusts the boundary line of the grating of the first area so that a distance between the center line of the first light spot and the center line of the gray scale distribution of the one-period grating of the first area is smaller than a/4, where a is a full width at half maximum of the first light spot. Wherein, the central line of the first light spot is the central line of the first light spot perpendicular to the port direction. The first optical signal is incident to the LCOS, and in the direction of the port, the energy of the first optical signal is symmetrically distributed along a straight line, which is the center line of the first optical spot. The central line of the first light spot is located in a periodic grating in the first area, the central line of the gray scale distribution of one periodic grating is the position of the periodic grating in the port direction, which is equal to (X + Y)/2, X is the position of the minimum phase of the periodic grating, and Y is the position of the maximum phase of the periodic grating. The cross-talk is generated by the grating boundary line, and the controller adjusts the grating boundary line of the first area to enable the distance between the center line of the first light spot and the center line of the gray scale distribution of the grating in one period to be smaller than A/4, so that the cross-talk can be reduced.

In a third implementation form of the first aspect of the present application, based on the first aspect of the present application or any one of the first to second implementation forms of the first aspect of the present application, the controller is configured to adjust the boundary lines of the gratings by shifting a gray scale distribution of the gratings of the first area in a direction of the LCOS port. The gray scale distribution of the shifted grating means that different phases of the periodic grating are shifted equally in the port direction without changing the period of the periodic grating. In the case of the method of shifting the gradation distribution of the grating, the boundary lines of all the gratings are shifted in the port direction in the first region. By shifting the grey scale distribution of the grating, the redirection angle of the first optical signal does not change, i.e. the target output port corresponding to the first area does not change. The redirection angle of the first optical signal refers to an angle of the first optical signal before redirection and the first optical signal after redirection. By shifting the gray scale distribution of the grating, the boundary line of the grating can be adjusted without changing the target output port, and the grating can be shifted by a coefficient in the program, so that the difficulty of adjusting the boundary line of the grating can be reduced.

Based on the first aspect of the present application or any one of the first to second implementation manners of the first aspect, in a fourth implementation manner of the first aspect of the present application, the controller may adjust a period of the gray scale distribution of the grating of the first area, and the controller may further adjust a maximum phase of the gray scale distribution of the grating of the first area, so that a redirection angle of the first optical signal is unchanged. For convenience of description, the period of the gray-scale distribution of the grating is referred to as the period of the grating, and the maximum phase of the gray-scale distribution of the grating is referred to as the maximum phase of the grating. The controller adjusts the boundary line of the gratings by adjusting the period and the maximum phase of the gratings in the first area, so that the redirection angle of the first optical signal can be kept unchanged, the target number can be further reduced under the condition that the first period is smaller than the second period, and the sensitivity of the first optical signal can be reduced under the condition that the first period is larger than the second period. Wherein, the target number is the number of the boundary lines of the grating covered by the first light spot. The first period is the period of the grating of the first area before the controller adjusts the period of the grating of the first area. The second period is the period of the grating of the first area after the controller adjusts the period of the grating of the first area. The grating with fewer periods is covered by the first light spot formed by the first optical signal, and the more sensitive the first optical signal is, the more easily the power of the first optical signal output from the target output port fluctuates up and down. In particular, in the case where the first period is smaller than the second period, the sensitivity of the first optical signal is increased. But by adjusting the boundary line of the grating, the power of the first optical signal output from the target output port can be kept at a better value.

Based on the first aspect of the present application or any one of the first to fourth embodiments of the first aspect, in a fifth embodiment of the first aspect of the present application, if the height of the first light spot is equal to the height of the gray scale distribution of the one-period grating of the first region, the boundary line of the gratings of the first region is adjusted so that the first light spot matches the one-period grating of the first region. Matching means that the first spot is as much as possible coincident with a periodic grating of the first area. And if the height of the first light spot is smaller than the height of the gray scale distribution of one period grating of the first area, adjusting the boundary line of the gratings of the first area to enable the first light spot to be in the one period grating of the first area.

In a sixth implementation manner of the first aspect of the present application, after the controller obtains the second intensity value, the controller adjusts a profile coefficient of a gray scale distribution of the grating in the first area to obtain a third intensity value. The first intensity value is the power of the redirected first optical signal, the third intensity value is obtained after adjusting the profile coefficient of the gray scale distribution of the grating in the first area, the third intensity value is larger than the second intensity value, and the profile coefficient of the gray scale distribution of the grating is called the profile coefficient of the grating for short. The third intensity value may also be a target intensity value or a crosstalk intensity value, and if the second intensity value is the target intensity value, the third intensity value is the target intensity value; if the second intensity value is a crosstalk intensity value, the third intensity value is a crosstalk intensity value. By changing the profile coefficient of the grating, crosstalk can be further reduced.

In a seventh implementation form of the first aspect of the present application, based on the first aspect of the present application or any one of the first to sixth implementation forms of the first aspect, the controller further adjusts the boundary lines of the gratings in the second area such that the second spots cover as few boundary lines of the gratings as possible. The second area is one of K × H areas of the LCOS, the second area is an area where the second light signal forms the second light spot, and the second area can redirect the second light signal. The central line of the second light spot is different from the central line of the first light spot, namely the first area and the second area belong to different areas in the port direction, K is an integer greater than 1, and the first optical signal and the second optical signal belong to different input optical signals of the input port. In the case where a plurality of input ports are provided, different input optical signals are spread in the wavelength direction at different positions in the port direction. Compared with the LCOS with a single input port (i.e., when K is equal to 1), the LCOS with multiple input ports (i.e., when K is greater than 1) does not have a height in the port direction that is multiplied by the number of input ports, and even has the possibility of keeping the height in the port direction unchanged. Therefore, in order to avoid the input optical signals of different input ports from interfering with each other, the height of the first optical signal in the port direction needs to be reduced, specifically, the height of the first optical spot in the port direction needs to be reduced. Reducing the height of the first spot in the direction of the port results in a grating covered by the first spot with fewer periods, i.e. the first optical signal is made more sensitive. In the case that the first optical signal is more sensitive, the power of the first optical signal output from the target output port is more likely to fluctuate up and down, and by adjusting the boundary line of the grating, the power of the first optical signal output from the target output port can be stabilized, that is, the sensitivity of the first optical signal is reduced. In particular, since the first light spot covers less of the boundary lines of the grating by adjusting the boundary lines of the grating, the power of the first optical signal output from the target output port can be kept at a better value.

In an eighth implementation form of the first aspect of the present application, based on the first aspect of the present application or any one of the first to seventh implementation forms of the first aspect of the present application, the controller further adjusts the boundary lines of the gratings in the third area such that the third spots cover as few boundary lines of the gratings as possible. The third area is one of K × H areas of the LCOS, the third area is an area where the third optical signal forms the third optical spot, and the third area can redirect the third optical signal. The central line of the third optical spot is the same as the central line of the first optical spot, that is, the first optical signal and the third optical signal belong to the same input optical signal of the input port, and the wavelength ranges of the first optical signal and the third optical signal are different. In the case of a plurality of regions in the wavelength direction, the first region and the third region can individually adjust the boundary line of the grating so that the adjustment of the first region or the third region does not affect each other.

In a ninth implementation form of the first aspect of the present application, based on the first aspect of the present application or any one of the first to eighth implementation forms of the first aspect, the first light spot is a flat-topped light spot. The energy distribution of the flat-top light spot in the direction of the port is relatively even, so that the flat-top light spot needs to pay attention to the number of the boundary lines of the grating covered by the whole light spot.

A second aspect of the present application provides a light device. The optical device includes a first input port, a first output port, a dispersive element, and an LCOS. The first input port is for incidence of a first incoming optical signal to the dispersive element. The dispersion element is configured to decompose the first incident optical signal into a first optical signal group of optical signals having different wavelengths, and transmit the first optical signal group to the LCOS, in which a gray scale distribution of the grating is loaded. In a specific implementation mode, different voltages can be loaded on different pixel points of the LCOS, and due to the birefringence effect of the liquid crystal, the different voltages correspond to different phase delay amounts, so that a structure similar to a grating can be formed. The LCOS comprises K multiplied by H areas, wherein K points to the direction of the port of the LCOS, K is an integer larger than 0, H points to the direction of the wavelength of the LCOS, and H is an integer larger than 1. The first region of the K × H regions is a region where the first optical signal forms the first light spot, and the first optical signal belongs to the first optical signal group. The boundary lines of the gratings of the first area are arranged such that the first spot covers as few boundary lines of the grey scale distribution of the gratings as possible. The LCOS is configured to redirect the first optical signal and transmit the redirected first optical signal to the first output port.

Wherein crosstalk is generated at the boundary of the gratings. The boundaries of the gratings of the first area in the LCOS are arranged such that the first spot covers as few of the boundaries of the gratings as possible, so that an optical device comprising the LCOS may reduce crosstalk.

In accordance with the second aspect of the present invention, in the first embodiment of the second aspect of the present invention, the boundary line of the grating of the first region is arranged so that the first spot covers as little of the boundary line of the grating as possible, when the following condition is satisfied: the second intensity value is greater than the first intensity value. The first intensity value is the power of the first optical signal passing through the first output port before the boundary line of the grating of the first area is configured. The second intensity value is the power of the first optical signal passing through the first output port after the boundary line of the grating of the first area is configured. The first intensity value may be a target intensity value or a crosstalk intensity value. When the first output port is the target output port, the first intensity value is the target intensity value. When the first output port is a non-target output port, the first intensity value is a crosstalk intensity value. The target output port refers to a port where the first optical signal is expected to be output, and the non-target output port refers to a port where the first optical signal generates crosstalk. The power of the first optical signal output by the target output port is generally greater than the power of the first optical signal output by the non-target output port.

In a second embodiment of the second aspect of the present application, in the second embodiment of the second aspect of the present application, the boundary line of the grating of the first region is configured such that a distance between a center line of the first spot and a center line of the gray scale distribution of one period grating of the first region is smaller than a/4, where a is a full width at half maximum of the first spot. Wherein the central line of the first light spot is the central line of the first light spot in the direction of the port. The first optical signal is incident to the LCOS, and in the direction of the port, the energy of the first optical signal is symmetrically distributed along a straight line, which is the center line of the first optical spot. The central line of the first light spot is located in a periodic grating in the first area, the central line of the gray scale distribution of one periodic grating is the position of the periodic grating in the port direction, which is equal to (X + Y)/2, X is the position of the minimum phase of the periodic grating, and Y is the position of the maximum phase of the periodic grating.

In accordance with the second aspect of the present application or any one of the first to second embodiments of the second aspect, in a third embodiment of the second aspect of the present application, the boundary line of the gratings of the first region is arranged such that the boundary line of the gray-scale distribution of the gratings of the first region is obtained by shifting the gray-scale distribution of the gratings of the first region in the port direction as little as possible covered by the first spot. The gray scale distribution of the shifted grating means that different phases of the periodic grating are shifted equally in the port direction without changing the period of the periodic grating. By shifting the grey scale distribution of the grating, the redirection angle of the first optical signal does not change, i.e. the target output port corresponding to the first area does not change.

In a fourth embodiment of the second aspect of the present invention, based on the second aspect of the present invention or any one of the first to second embodiments of the second aspect, the boundary lines of the gratings of the first area are arranged such that the first spot covers as few boundary lines of the gratings as possible, with the redirection angle of the first optical signal unchanged. The condition that the redirection angle of the first optical signal is not changed is obtained by adjusting the period and the maximum phase of the grating of the first area.

In accordance with the second aspect of the present application or any one of the first to fourth embodiments of the second aspect, in a fifth embodiment of the second aspect of the present application, if the height of the first flare is equal to the height of the tone distribution of the one-period grating in the first region, when the height of the first flare matches the tone distribution of the one-period grating in the first region, the boundary line of the gratings in the first region is arranged so that the first flare covers as little of the boundary line of the tone distribution of the gratings as possible. If the height of the first spot is smaller than the height of the gray-scale distribution of the one-period grating in the first region, the boundary line of the gratings in the first region is arranged so that the first spot covers as little as possible of the boundary line of the gray-scale distribution of the gratings when the first spot is within the gray-scale distribution of the one-period grating in the first region.

In a sixth implementation form of the second aspect of the present application, based on any one of the first to fifth implementation forms of the second aspect of the present application, the profile factor of the gray-scale distribution of the grating of the first area is configured such that the third intensity value is greater than the second intensity value. The second intensity value is the power of the optical signal at the first output port before the configuration coefficient of the gray scale distribution of the grating in the first area is configured. The third intensity value is the power of the optical signal at the first output port after the configuration coefficient of the gray scale distribution of the grating in the first area is configured. The shape coefficient of the gray level distribution of the grating is called the shape coefficient of the grating for short. The third intensity value may also be a target intensity value or a crosstalk intensity value, and if the second intensity value is the target intensity value, the third intensity value is the target intensity value; if the second intensity value is a crosstalk intensity value, the third intensity value is a crosstalk intensity value.

In a seventh implementation form of the second aspect of the present application, based on the second aspect of the present application or any one of the first to sixth implementation forms of the second aspect, the optical device further comprises a second input port. The second input port is for injecting a second incoming optical signal into the dispersive element. The dispersion element is also configured to decompose the second incident optical signal into a second set of optical signals having optical signals of different wavelengths and transmit the second set of optical signals to the LCOS, wherein a second area of the K × H areas is an area where the second optical signal forms a second light spot. The second optical signal belongs to a second optical signal group. The central line of the second light spot is different from that of the first light spot, namely the first area and the second area belong to different areas in the port direction, and K is an integer larger than 1. The boundaries of the gratings of the second area are arranged such that the second spot covers as little of the boundaries of the grey scale distribution of the gratings as possible. The LCOS is also used to redirect the second optical signal.

Based on the second aspect of the present application or any one of the first to seventh embodiments of the second aspect, in an eighth embodiment of the second aspect of the present application, a third area of the K × H areas is an area where the third optical signal forms a third optical spot, the third optical signal belongs to the first optical signal group, a center line of the third optical spot is the same as a center line of the first optical spot, and wavelength ranges of the first optical signal and the third optical signal are different. The boundary lines of the gratings of the third area are arranged such that the third spot covers as little of the boundary lines of the gray scale distribution of the gratings as possible. The LCOS is also used to redirect the third optical signal.

In a ninth implementation form of the second aspect of the present application, based on the second aspect of the present application or any one of the first to eighth implementation forms of the second aspect, the first light spot is a flat-topped light spot.

For a related description of the advantageous effects of the second aspect of the present application, reference may be made to the related description of the aforementioned first aspect.

A third aspect of the present application provides a reconfigurable optical add-drop multiplexer (ROADM).

The reconfigurable optical add/drop multiplexer includes: a wave splitting module and a wave combining module. The wavelength division module is used for downloading the first optical wavelength signal to the website. The wave combination module is used for receiving the second optical wavelength signal uploaded by the station. The wavelength division module and/or the wavelength combination module are/is the optical device according to any one of the embodiments of the second aspect or the second aspect, and the optical device is a wavelength selective switch.

A fourth aspect of the present application provides a computer storage medium, wherein instructions are stored in the computer storage medium, and when executed on a computer, the instructions cause the computer to perform the method according to the first aspect or any one of the implementation manners of the first aspect.

A fifth aspect of the present application provides a computer program product, which, when executed on a computer, causes the computer to perform the method according to the first aspect or any one of the embodiments of the first aspect.

Drawings

FIG. 1 is a schematic diagram of one configuration of the gray scale distribution of a grating formed by LCOS;

FIG. 2 is another schematic diagram of the gray scale distribution of a grating formed by LCOS;

FIG. 3 is a schematic diagram of a WSS configuration;

FIG. 4 is a schematic diagram of a structure of DGFF or WE;

FIG. 5 is a schematic structural diagram of a gray scale distribution of a grating in a first region before adjustment in an embodiment of the present application;

FIG. 6 is a schematic flow chart of an LCOS adjusting method according to an embodiment of the present application;

FIG. 7 is a schematic diagram of the relationship between different areas of LCOS and ports according to an embodiment of the present application;

FIG. 8 is a structural diagram of the adjusted gray scale distribution of the grating in the first region in the embodiment of the present application;

FIG. 9 is a schematic diagram of gray scale distribution of gratings under different translation amounts in the embodiment of the present application;

FIG. 10 is another schematic structural diagram of the adjusted gray scale distribution of the grating in the first region in the embodiment of the present application;

FIG. 11 is a schematic diagram of a gray scale distribution of a grating when a profile factor is adjusted in an embodiment of the present application;

FIG. 12 is a schematic diagram illustrating the division of different regions when K is 2 in the embodiment of the present application;

FIG. 13 is a schematic diagram of an energy distribution of a flat-topped spot in an embodiment of the present application;

fig. 14 is a schematic structural diagram of a reconfigurable optical add/drop multiplexer according to an embodiment of the present application.

Detailed Description

The embodiment of the application provides an LCOS (liquid crystal on silicon) adjusting method, an optical device and a reconfigurable optical add-drop multiplexer, which are applied to the field of optical communication and can reduce crosstalk.

LCOS includes many pixel, and different voltage can form different phase delay in applying on pixel, when loading the gradient voltage on a series of continuous pixel, can simulate the diffraction effect of physical grating, forms the grey scale distribution of grating. The grey distribution of the grating is also called the phase distribution. The gray distribution of the grating comprises the corresponding relation between the gradient voltage and the pixel points. Figuratively, the gray scale profile of the grating includes the period of the grating, the starting point of the period of the grating, and the maximum phase of the grating. The starting point of the period of the grating can be understood as the starting point of the pixel point to which the gradient voltage is applied. The boundary line of the grating may refer to the starting point of the grating period or the maximum phase of the grating. The boundary line of the grating is described in detail later. The maximum phase of the grating generally corresponds to the pixel point to which the maximum voltage or the minimum voltage is applied. The period of the grating refers to the period of the gradient voltage. For example, 100 pixels are included along the port direction, the applied voltage values are 0.1mV to 1mV from the 1 st pixel to the 10 th pixel, the applied voltage values are 0.1mV to 1mV from the 11 th pixel to the 20 th pixel, and so on until the 100 th pixel. The gray distribution of the grating includes the height from the 1 st pixel to the 10 th pixel (period of the grating), the position of the 10 th pixel or the position of the 11 th pixel (boundary line of the grating), and the equivalent phase of the pixel (maximum phase of the grating) when 1mV voltage is applied. The period of the grating and the maximum phase of the grating act together to determine the inclination angle of the grating. When an incident optical signal is incident on the LCOS loaded with a gradient voltage, the LCOS behaves as a tilted mirror, or lens, and the incident optical signal is reflected or transmitted accordingly. Regardless of whether the incident optical signal is reflected or transmitted, the angle of the incident optical signal is deflected, i.e., the LCOS redirects the incident optical signal. Dividing the LCOS into different areas, and if the same gradient voltage is applied to the different areas, considering that the inclination angles of the different areas are the same and the redirection angle of the incident light signal is the same; if different gradient voltages are applied to different regions, it can be considered that the inclination angles of the different regions are different and the redirection angles of the incident light signals are different.

When gradient voltage is loaded on the pixel points, phase difference can be formed between the pixel point applying the maximum voltage and the pixel point applying the minimum voltage. And because certain distance exists between the pixel points, crosstalk can be generated at the boundary line of the grating. Fig. 2 is a schematic diagram of a structure of a gray scale distribution of a grating formed by LCOS, as shown in fig. 2. Fig. 2 includes a raster front view and a raster left view. The first light spot 210, the third light spot 209 and the fourth light spot 211 are formed by the light signal incident on the LCOS. One-period grating 203 includes a first grating region 206 and a second grating region 207. The tilt angle of the first grating region 206 is formed according to the applied voltage gradient, and the tilt angle of the second grating region 207 is formed according to the maximum voltage and the minimum voltage applied. Since the phase of each pixel in the LCOS can be changed in a certain range according to the applied voltage, a boundary line of a jump between the maximum phase and the minimum phase, that is, a boundary line of the gray distribution of the grating (which may be referred to as a grating boundary line for short) inevitably occurs. In this application, the boundary line of the grating may refer to the second grating region 207. In a drawing method not embodying the second raster region 207, the boundary line of the raster can also be understood as the boundary line 106 in fig. 1. When the optical signal 204 is incident on the first grating region 206, the angle between the reflected optical signal 205 and the optical signal 204 is a first redirection angle. When the optical signal 204 is incident on the second grating region 207, the angle between the reflected optical signal and the optical signal 204 is a second redirection angle. The first redirection angle is different from the second redirection angle, and the reflected light signal generating the second redirection angle is crosstalk.

According to the LCOS adjusting method, the starting point position of the pixel point applying the gradient voltage is adjusted, so that the boundary line of the grating is moved, light spots formed by the optical signals cover the boundary line of the grating as little as possible, and therefore crosstalk is reduced. The LCOS adjusting method in the present application can adjust an optical device including LCOS, such as WSS, DGFF, WB, etc.

The WSS can switch optical signals with multiple wavelengths to different ports according to the wavelengths, and wavelength scheduling of the communication nodes is achieved. As shown in fig. 3, fig. 3 is a schematic structural diagram of the WSS. The WSS includes a plurality of ports 301 for input and output of incident optical signals. After an incident optical signal enters the WSS from the input port, the incident optical signal needs to be separated into two light beams with orthogonal polarization states by a crystal or polarization beam splitter 302 (PBS), and then the polarization state of one of the two light beams is rotated to align the polarization states of the two light beams with the working polarization state of the LCOS 306. If a polarization independent LCOS306 is used, then no crystal or polarizing beam splitter 302 is required. The polarization-converted incident light signal is incident on a periodic grating 305 through a lens 304, the periodic grating 305 is a dispersive element, and the periodic grating 305 is configured to decompose the incident light signal into optical signals with different wavelengths and transmit the optical signals to the LCOS 306. The grating formed in the LCOS306 is not the same as the periodic grating 305, the periodic grating 305 being a physical entity and the grating formed in the LCOS306 being an equivalent grating. Optical signals of different wavelengths are emitted from the periodic grating 305 at different angles, pass through the lens 304, and are incident on different areas of the LCOS 306. By adjusting the gray scale distribution of the gratings in different areas of the LCOS306, the corresponding wavelengths can be controlled to realize the angular deflection in the port direction 308 perpendicular to the wavelength direction 307, the optical signal after the angular deflection is incident on the fourier lens 303, the fourier lens 303 performs the position displacement on the optical signal, and the optical signal after the position displacement is coupled to a specific output port. Controlling the gray scale distribution of the grating in an area of the LCOS306 allows the light signals incident on the area to be output from different output ports.

DGFF may achieve attenuation of certain wavelengths. WB can achieve blocking for certain wavelengths. As shown in FIG. 4, FIG. 4 is a schematic structural diagram of DGFF or WE. An incident optical signal is input from a port 401 into DGFF or WE, collimated by a lens 402, and incident on a dispersive element 403, and the dispersive element 403 is used to decompose the incident optical signal into optical signals having different wavelengths. Optical signals with different wavelengths are emitted from the dispersive element 403 at different angles, pass through the lens 404 and are focused on different areas of the LCOS405 along the wavelength direction 406, the LCOS405 reflects the optical signals, and the reflected optical signals return to the port 401. Controlling the gray scale distribution of the gratings in different areas of the LCOS405 can change the deflection angle of the optical signal, so that the reflected path deviates from the incident path, the output optical signal will be attenuated, and the attenuation will be larger the deviation is. The adjustment of attenuation can be realized by controlling the gray scale distribution of the grating in different areas corresponding to different wavelengths, and a filter curve is generated, which is the principle of DGFF. If the gray distribution of the grating in the area corresponding to certain wavelengths is controlled, the attenuation of optical signals is extremely large, which is equivalent to blocking certain wavelengths; if the gray scale distribution of the grating in the area corresponding to certain wavelength is controlled, the attenuation of the optical signal is very small, and certain wavelength is not attenuated, which is equivalent to certain wavelength passing.

It should be noted that the above structural diagrams of WSS, DGFF or WE are just an example, and those skilled in the art can modify them according to the relevant knowledge. For example, the output port and input port of the WE are not one port, and there is no need for the lens 402 to collimate the incident optical signal, etc. In the case that the optical device includes an LCOS, the LCOS is adjusted by using the LCOS adjusting method disclosed in the present application, and the principle of the LCOS is the same, all of which shall fall into the protection scope of the present application. In order to illustrate the LCOS adjusting method provided by the present application, a WSS will be taken as an example, and the details thereof will be described below. The LCOS adjusting method in the present application relates to the gray distribution of the grating, and therefore, the first region 201 in fig. 2 will be taken as an example for explanation. As shown in fig. 5, fig. 5 is a schematic structural diagram of a gray scale distribution of a grating formed in the first region 201 before adjustment in the embodiment of the present application. Fig. 5 includes a front view and a left side view of the first region 201. For example, the features or contents identified by broken lines in the drawings related to the embodiments of the present application can be understood as optional operations or optional structures of the embodiments.

Referring to fig. 6, fig. 6 is a schematic flowchart illustrating an LCOS adjusting method according to an embodiment of the present invention.

In step 601, the controller obtains a first intensity value of the first optical signal.

The first intensity value is a power of the first optical signal reflected by the first region of the LCOS. In LCOS, the grey distribution of the grating is loaded. The LCOS comprises K multiplied by H areas, wherein K points to the direction of the port of the LCOS, K is an integer larger than 0, H points to the direction of the wavelength of the LCOS, and H is an integer larger than 1. In the examples of the present application, K is 1 and H is 3. Referring to fig. 2, the LCOS includes a first region 201, a third region 202, and a fourth region 208.

Referring to fig. 3, a first incident optical signal input from a port 301 passes through a dispersion element 305, the dispersion element 305 decomposes the first incident optical signal into a first optical signal group of optical signals with different wavelengths, and transmits the first optical signal group to an LCOS 306. The first optical signal group includes a first optical signal, a third optical signal and a fourth optical signal, and the wavelengths of the different optical signals are different. The first optical signal is incident on the first region 201, the third optical signal is incident on the third region 202, and the fourth optical signal is incident on the fourth region 208.

As can be seen from the foregoing description of the WSS, controlling the gray scale distribution of the grating in an area of the LCOS306 can realize that the optical signals incident on the area are output from different output ports. In the embodiment of the present application, the relationship between the area and the port in the LCOS will be exemplified. Referring to fig. 7, fig. 7 is a schematic diagram illustrating association between different regions and ports of an LCOS according to an embodiment of the present application. The target output port of the first region 201 is the first port 701, the target output port of the third region 202 is the third port 703, the target output port of the fourth region 208 is the fourth port 704, the fourth port 704 is also an input port in the embodiment of the present application, and the second port 702 is not associated with a region of the LCOS. The target output port for the first optical signal and the target output port for the third optical signal may be the same port, e.g., both first ports 701. In the embodiment of the present application, the first port 701 is associated with the first region, and the third port 703 is associated with the third region for illustration only.

The first intensity value may be a target intensity value or a crosstalk intensity value. The target intensity value refers to the power of the first optical signal output from the target output port, and the crosstalk intensity value refers to the negative value of the power of the first optical signal output from the non-target output port. The target output port refers to a port where the first optical signal is expected to be output, and the non-target output port refers to a port where the first optical signal generates crosstalk. The power of the first optical signal output by the target output port is generally greater than the power of the first optical signal output by the non-target output port. In the present embodiment, the first port 701 is a target output port of the first optical signal, and the second port 702 to the eighth port are non-target output ports of the first optical signal.

In step 602, the controller adjusts the boundary of the gratings of the first region.

The controller adjusts the starting point position of the pixel point applying the gradient voltage in the first area, so as to move the boundary line of the grating, namely, the boundary line of the grating in the first area is adjusted. The controller can adjust the boundary of the grating of the first area by means of translation, and can also adjust the boundary of the grating by adjusting the period and the maximum phase of the grating of the first area, both of which will be described in detail below.

Translation refers to shifting the gray scale distribution of the grating, since the period and maximum phase of the grating are not changed, but the boundary lines of the grating are shifted, thus producing a translation-like effect. As shown in fig. 8, fig. 8 is a schematic structural diagram of a gray scale distribution of a grating formed by the adjusted first region 201 in the embodiment of the present application. In fig. 8, the coordinates of the boundary lines of the gratings in the port direction are 14,34,54, respectively. In fig. 5 before the adjustment, the coordinates of the boundary lines of the gratings in the port direction are 0,20,40,60, respectively. Thus, it can be understood that the gray scale distribution of the grating in fig. 5 is shifted downward in its entirety by 6, or that the gray scale distribution of the grating in fig. 5 is shifted upward in its entirety by 14. In the case of the method of shifting the gradation distribution of the grating, the boundary lines of all the gratings are shifted in the port direction in the first region. By shifting the gray scale distribution of the grating, the redirection angle of the first optical signal is not changed, i.e. the target output port corresponding to the first area is not changed, and the target output port of the first optical signal is still the first port 701. Compared to before the adjustment, the first light spot 210 covers 4 periodic gratings and 3 boundary lines, after the adjustment, the first light spot 210 covers 3 periodic gratings and 2 boundary lines.

When the LCOS calculates the grating position, it can be based on the grating formula:

Y＝X+move；

wherein Y is the phase of the gray distribution of the grating, X is the coordinate of the port direction, and move is the translation amount of the gray distribution of the translation grating. When using a translation, the controller may adjust the boundary line of the gratings of the first area based on the above formula. As shown in fig. 9, fig. 9 is a schematic diagram of the gray distribution of the grating under different translation amounts in the embodiment of the present application. In the case where the periods are all 20, the amounts of translation in fig. 9 are 0,5,10,15, respectively.

In order to make the redirection angle of the first optical signal constant, i.e. the target output port of the first optical signal constant, the controller needs to adjust not only the period of the grating of the first area, but also the maximum phase of the grating of the first area. As shown in fig. 10, fig. 10 is another structural diagram of the gray scale distribution of the grating formed by the adjusted first region 201 in the embodiment of the present application. As shown in fig. 10, the period of the grating is 40 and the maximum phase of the grating is 2 pi. In fig. 5 before the adjustment, the period of the grating is 20 and the maximum phase of the grating is pi. The boundary line of the grating is adjusted by adjusting the period and the maximum phase of the grating in the first area, so that the redirection angle of the first optical signal can be kept unchanged, and the number of the boundary lines of the grating covered by the first light spot can be further reduced under the condition that the first period is smaller than the second period. The first period is the period of the grating of the first area before the controller adjusts the period of the grating of the first area. The second period is the period of the grating of the first area after the controller adjusts the period of the grating of the first area. Compared to before the adjustment, the first light spot 210 covers 4 periodic gratings and 3 boundary lines, after the adjustment, the first light spot 210 covers 3 periodic gratings and 2 boundary lines.

Optionally, the controller also translates the boundary lines of the gratings after increasing the period and maximum phase of the gratings. By increasing the period of the grating, the period of the grating covered by the first light spot 210 is reduced, and thus the sensitivity of the first light signal is increased. However, by shifting the boundary line of the grating, the power of the first optical signal output from the target output port can be kept at a better value. For example, before increasing the period of the grating, it is assumed that the first intensity value of the first optical signal fluctuates between 4-6, and after increasing the period of the grating, the first intensity value of the first optical signal fluctuates between 2-8. By shifting the boundary line of the grating, the first intensity value of the first optical signal may be allowed to fluctuate between 4-8. Therefore, it is meaningful to coordinate the use of shifting the boundaries of the grating and increasing the period of the grating.

Optionally, whether the mode of translation or the mode of adjusting the period and the maximum phase of the grating is adopted, after the boundary line of the grating is adjusted, the distance between the central line of the first light spot and the central line of the gray scale distribution of one period grating of the first area is smaller than A/4, and A is the half-height width of the first light spot. After the boundary line of the grating is adjusted, the central line of the first light spot falls in a certain periodic grating, the central line of the gray distribution of one periodic grating refers to the position of the periodic grating in the port direction, wherein the position is equal to (X + Y)/2, X is the position of the minimum phase of the periodic grating, and Y is the position of the maximum phase of the periodic grating. As shown in fig. 8, the center line 801 of the first spot has a coordinate of 46, and the center line 802 of the periodic grating has a coordinate of (34+ 54)/2.

Optionally, if the height of the first light spot is equal to the height of the gray scale distribution of the one-period grating of the first area, the boundary line of the gratings of the first area is adjusted so that the first light spot matches the one-period grating of the first area. Matching means that the first spot is as much as possible coincident with a periodic grating of the first area. And if the height of the first light spot is smaller than the height of the gray scale distribution of one period grating of the first area, adjusting the boundary line of the gratings of the first area to enable the first light spot to be in the one period grating of the first area.

In step 603, the controller obtains a second intensity value of the first optical signal, where the second intensity value is greater than the first intensity value.

After the controller adjusts the boundary line of the grating of the first area, the controller obtains a second intensity value of the first optical signal. The second intensity value is obtained in a manner similar to the first intensity value. If the first intensity value is obtained through the third port, the second intensity value should also be obtained through the third port. If the second intensity value is greater than the first intensity value, the first light spot covers as few of the boundary lines of the grating as possible. Whether the first light spot covers the boundary line of the grating as little as possible is judged, a positioning sensor needs to be arranged in the LCOS, the starting position and the end position of the first light spot in the port direction are obtained, and the number of the boundary line of the grating between the starting position and the end position needs to be calculated. Compared with the technical means, whether the first light spot covers the boundary line of the grating as less as possible is judged by the intensity value of the first light signal, so that the method is simpler and reduces the cost.

A corresponding target output port, e.g., a first port, is determined in the first region, and after determining a measurement port of an intensity value, e.g., a target output port, the first intensity value and the second intensity value are bound to the first port. In terms of time sequence, the first optical signal corresponding to the first intensity value and the first optical signal corresponding to the second intensity value are not one optical signal, but the target output ports of the two first optical signals are both the first ports, so that the two first optical signals are both referred to as the first optical signals. The first optical signal generates different light intensity levels at the first port to the eighth port. The different light intensity orders include the +1 order (target order) and the crosstalk order. The +1 level is the level with the strongest energy of all light intensity levels. The +1 order is output at the target output port. At the same time, the first optical signals of other orders will be output as crosstalk signals from other non-target output ports, thereby causing crosstalk between different output ports of the WSS.

Alternatively, if the first and second intensity values are crosstalk intensity values, the first and second intensity values are negative values of the energy of the strongest crosstalk order. For example, the power of the first optical signal at the target output port (the first port) is 60 db mw, and the power of the second optical signal from the second port to the eighth port is 20 db mw, 10 db mw, 2 db mw, 1 db mw, and 1 db mw, respectively. Where the first intensity value and the second intensity value are crosstalk intensity values, the first intensity value and the second intensity value are measured at the second port. By measuring the crosstalk of the first optical signal at the second port, the change of the first intensity value and the second intensity value, namely the change of the crosstalk, can be more obviously seen before and after the controller adjusts the boundary line of the grating.

Alternatively, if the first intensity value and the second intensity value are both energies of +1 order, the first intensity value and the second intensity value are the target intensity values. The controller also obtains a third intensity value and a fourth intensity value, the fourth intensity value being greater than the third intensity index. The fourth intensity value and the third intensity value are both negative values of the energy of the strongest crosstalk order, i.e., the first intensity value and the second intensity value are crosstalk intensity values. The controller not only needs to confirm that the second intensity value is greater than the first intensity value, but also needs to confirm that the fourth intensity value is greater than the third intensity value, and only when the power of the first optical signal output by the target output port is increased and the power of the first optical signal output by the non-target output port is decreased, the controller confirms that the first light spot covers less boundary lines of the gratings. Whether the result of adjusting the boundary line of the grating is beneficial or not is judged through the positive condition and the negative condition, and the reliability can be improved. If the first intensity value and the second intensity value are negative values of the energy of the strongest crosstalk order, the third intensity value and the fourth intensity value are target intensity values, which is opposite to the above-mentioned contents and is not described herein again.

In step 604, the controller adjusts the profile factor of the grating of the first region.

And after the controller acquires the second intensity value, the controller adjusts the appearance coefficient of the grating in the first area. When the LCOS calculates the grating position, it can be based on the grating formula:

Y＝a*(X+move)+b*(X+move)²+c*(X+move)³+…；

wherein Y is the phase of the gray distribution of the grating, and X is the coordinate of the port direction. b and c are the appearance coefficients of the grating, and move is the translation amount of the gray distribution of the translation grating. a is used to adjust the slope of the first order linearity of the grating. In order to keep the redirection angle of the first optical signal constant, the slope of the first order linearity is constant. The coefficient b is used for adjusting the second-order parabolic coefficient of the grating, and the coefficient c is used for adjusting the third-order curve coefficient. The combined action of the coefficients, such as move, a, b, c, and the like, can fully cover all the topography possibilities that may occur in the grating. As shown in fig. 11, fig. 11 is a schematic diagram of gray scale distribution of a grating when a profile coefficient is adjusted under the condition that a is not changed in the embodiment of the present application.

The gray-scale profile 1101 is the gray-scale profile of the grating when a is equal to 1, b is equal to 0, and c is equal to 0.

The gray profile 1102 is the gray profile of the grating when a equals 1, b equals 20, and c equals 0.

The gray profile 1103 is the gray profile of the grating when a equals 1, b equals-20, and c equals 0.

The gray profile 1104 is the gray profile of the grating when a equals 1, b equals 0, and c equals 20.

The gray profile 1105 is the gray profile of the grating when a equals 1, b equals 20, and c equals-20.

The gray profile 1106 is the gray profile of the grating when a equals 1, b equals 20, and c equals 20.

In step 605, the controller obtains a third intensity value of the first optical signal, where the third intensity value is greater than the second intensity value.

After the controller adjusts the appearance coefficient of the grating in the first area, the controller obtains a third intensity value of the first optical signal. The third intensity value is obtained in a manner similar to the second intensity value.

Optionally, the controller also adjusts the boundaries of the gratings of the second area such that the second spot covers as little of the boundaries of the gratings as possible. The second area is one of K × H areas of the LCOS, the second area is an area where the second light signal forms the second light spot, and the second area can redirect the second light signal. The central line of the second light spot is different from the central line of the first light spot, namely the first area and the second area belong to different areas in the port direction, K is an integer greater than 1, and the first optical signal and the second optical signal belong to different input optical signals of the input port. In the case where a plurality of input ports are provided, different input optical signals are spread in the wavelength direction at different positions in the port direction. Referring to fig. 12, fig. 12 is a schematic diagram illustrating the division of different regions when K is 2 in the embodiment of the present application. The centerline 1204 of the first spot 1203 and the centerline 1201 of the second spot 1202 are not the same centerline. It can be determined that the two spots fall on different areas as long as the spot centre lines are determined not to be the same, so that there may not be a need for clear boundaries for the division of the areas in the port direction. For example, in the λ 1 region in fig. 12, the dividing line for the region in the port direction falls on one period grating. The controller adjusts the boundary lines of the gratings of the second area in a similar manner as the controller adjusts the boundary lines of the gratings of the first area.

Compared with the LCOS with a single input port (i.e., when K is equal to 1), the LCOS with multiple input ports (i.e., when K is greater than 1) does not have a height in the port direction that is multiplied by the number of input ports, and even has the possibility of keeping the height in the port direction unchanged. Therefore, in order to avoid the input optical signals of different input ports from interfering with each other, the height of the first optical signal in the port direction needs to be reduced, specifically, the height of the first optical spot in the port direction needs to be reduced. As shown in fig. 12, the height of the first spot 1203 in the port direction is only half of the height of the first spot 210 in fig. 2. Reducing the height of the first spot in the direction of the port results in a grating covered by the first spot with fewer periods, i.e. the first optical signal is made more sensitive. In the case that the first optical signal is more sensitive, the power of the first optical signal output from the target output port is more likely to fluctuate up and down, and by adjusting the boundary line of the grating, the power of the first optical signal output from the target output port can be stabilized, that is, the sensitivity of the first optical signal is reduced. In particular, since the first light spot covers less of the boundary lines of the grating by adjusting the boundary lines of the grating, the power of the first optical signal output from the target output port can be kept at a better value.

Optionally, the controller also adjusts the boundary line of the grating of the third area such that the third spot covers as little of the boundary line of the grating as possible. The third area is one of K × H areas of the LCOS, the third area is an area where the third optical signal forms the third optical spot, and the third area can redirect the third optical signal. The central line of the third optical spot is the same as the central line of the first optical spot, that is, the first optical signal and the third optical signal belong to the same input optical signal of the input port, and the wavelength ranges of the first optical signal and the third optical signal are different. In the case of a plurality of regions in the wavelength direction, the first region and the third region can individually adjust the boundary line of the grating so that the adjustment of the first region or the third region does not affect each other. As shown in fig. 12, the center line 1204 of the third spot 1205 of the third region is the same as the center line 1204 of the first spot 1203.

Optionally, the first light spot is a flat-topped light spot. The energy distribution of the flat-top light spot in the direction of the port is relatively even, so that the flat-top light spot needs to pay attention to the number of the boundary lines of the grating covered by the whole light spot. As shown in fig. 13, fig. 13 is a schematic diagram of energy distribution of a flat-topped light spot 1301 in the embodiment of the present application.

The LCOS adjusting method in the embodiment of the present application is described above, and the optical device in the embodiment of the present application is described below. The optical device in the present application is an optical device including LCOS, such as WSS, DGFF, WB, or the like.

The optical device includes a first input port, a first output port, a dispersive element, and an LCOS. The first input port is for incidence of a first incoming optical signal to the dispersive element. The dispersion element is configured to decompose the first incident optical signal into a first optical signal group of optical signals having different wavelengths, and transmit the first optical signal group to the LCOS, in which a gray scale distribution of the grating is loaded. The LCOS includes K × H regions, K being an integer greater than 0 and H being an integer greater than 1. The first region of the K × H regions is a region where the first optical signal forms the first light spot, and the first optical signal belongs to the first optical signal group. The boundaries of the gratings of the first area are arranged such that the first spot covers as little of the boundaries of the gratings as possible. The LCOS is configured to redirect the first optical signal and transmit the redirected first optical signal to the first output port.

The relevant description in the light device can refer to the relevant description in the foregoing LCOS conditioning method. The first input port may refer to the fourth port 704 in fig. 7, and the first output port may refer to the first port 701 in fig. 7. The first input port and the first output port may be the same port, for example, the fourth port 704 serves as both the input port and the output port corresponding to the fourth area.

Optionally, the boundary line of the grating of the first area is arranged such that the first spot covers as little of the boundary line of the grating as possible when the following condition is fulfilled: the second intensity value is greater than the first intensity value.

Optionally, the boundary line of the grating of the first region is configured such that a distance between a center line of the first spot and a center line of the gray scale distribution of one period of the grating of the first region is less than a/4, a being a full width at half maximum of the first spot.

Optionally, the boundary line of the gratings of the first area is configured such that the first light spot covers as little as possible of the gray scale distribution of the gratings, and the boundary line is obtained by shifting the gray scale distribution of the gratings of the first area in the port direction. The gray scale distribution of the shifted grating means that different phases of the periodic grating are shifted equally in the port direction without changing the period of the periodic grating. By shifting the grey scale distribution of the grating, the redirection angle of the first optical signal does not change, i.e. the target output port corresponding to the first area does not change.

Optionally, in case the redirection angle of the first optical signal is constant, the boundary lines of the gratings of the first area are arranged such that the first spot covers as few boundary lines of the gratings as possible. The condition that the redirection angle of the first optical signal is not changed is obtained by adjusting the period and the maximum phase of the grating of the first area.

Alternatively, if the height of the first spot is equal to the height of the gray scale distribution of the one-period grating of the first region, the boundary line of the gratings of the first region is arranged so that the first spot covers as little as possible of the boundary line of the gray scale distribution of the gratings in the case where the height of the first spot matches the gray scale distribution of the one-period grating of the first region. If the height of the first spot is smaller than the height of the gray-scale distribution of the one-period grating in the first region, the boundary line of the gratings in the first region is arranged so that the first spot covers as little as possible of the boundary line of the gray-scale distribution of the gratings when the first spot is within the gray-scale distribution of the one-period grating in the first region.

Optionally, the profile coefficient of the grey scale distribution of the grating of the first area is configured such that the third intensity value is greater than the second intensity value. The second intensity value is the power of the optical signal at the first output port before the configuration coefficient of the gray scale distribution of the grating in the first area is configured. The third intensity value is the power of the optical signal at the first output port after the configuration coefficient of the gray scale distribution of the grating in the first area is configured. The shape coefficient of the gray level distribution of the grating is called the shape coefficient of the grating for short. The third intensity value may also be a target intensity value or a crosstalk intensity value, and if the second intensity value is the target intensity value, the third intensity value is the target intensity value; if the second intensity value is a crosstalk intensity value, the third intensity value is a crosstalk intensity value.

Optionally, the optical device further comprises a second input port. The second input port is for injecting a second incoming optical signal into the dispersive element. The dispersion element is also configured to decompose the second incident optical signal into a second set of optical signals having optical signals of different wavelengths and transmit the second set of optical signals to the LCOS, wherein a second area of the K × H areas is an area where the second optical signal forms a second light spot. The second optical signal belongs to a second optical signal group. The central line of the second light spot is different from that of the first light spot, namely the first area and the second area belong to different areas in the port direction, and K is an integer larger than 1. The boundaries of the gratings of the second area are arranged such that the second spot covers as little of the boundaries of the gratings as possible. The LCOS is also used to redirect the second optical signal.

Optionally, a third area of the K × H areas is an area where a third optical signal forms a third optical spot, the third optical signal belongs to the first optical signal group, a center line of the third optical spot is the same as a center line of the first optical spot, and wavelength ranges of the first optical signal and the third optical signal are different. The boundary lines of the gratings of the third area are arranged such that the third spot covers as little of the boundary lines of the gray scale distribution of the gratings as possible. The LCOS is also used to redirect the third optical signal.

Optionally, the first light spot is a flat-topped light spot.

The optical device in the embodiment of the present application is described above, and the reconfigurable optical add/drop multiplexer in the embodiment of the present application is described below.

Referring to fig. 14, fig. 14 is a schematic structural diagram of a reconfigurable optical add/drop multiplexer according to an embodiment of the present application.

The reconfigurable optical add-drop multiplexer of the present embodiment includes a wavelength division module 1401 and a wavelength combination module 1402; the ROADM of this embodiment may also include a drop module 1403, an add module 1404, a receiver 1406, and a transmitter 1406.

The wavelength division module 1401 is configured to download a first optical wavelength signal to a current station, where the first optical wavelength signal may refer to a first optical signal in the optical device.

The wave combining module 1402 is configured to receive a second optical wavelength signal uploaded by the current station, where the second optical wavelength signal is an optical signal with a wavelength different from that of the first optical signal.

The optical device of the wavelength division module and/or the wavelength combination module is a WSS.

In the several embodiments provided in the present application, it should be understood that the disclosed system, apparatus and method may be implemented in other manners. For example, the above-described apparatus embodiments are merely illustrative, and for example, the division of the units is only one logical division, and other divisions may be realized in practice, for example, a plurality of units or components may be combined or integrated into another system, or some features may be omitted, or not executed. In addition, the shown or discussed mutual coupling or direct coupling or communication connection may be an indirect coupling or communication connection through some interfaces, devices or units, and may be in an electrical, mechanical or other form.

The units described as separate parts may or may not be physically separate, and parts displayed as units may or may not be physical units, may be located in one place, or may be distributed on a plurality of network units. Some or all of the units can be selected according to actual needs to achieve the purpose of the solution of the embodiment.

In addition, functional units in the embodiments of the present application may be integrated into one processing unit, or each unit may exist alone physically, or two or more units are integrated into one unit. The integrated unit can be realized in a form of hardware, and can also be realized in a form of a software functional unit.

The integrated unit, if implemented in the form of a software functional unit and sold or used as a stand-alone product, may be stored in a computer readable storage medium. Based on such understanding, the technical solution of the present application may be substantially implemented or contributed to by the prior art, or all or part of the technical solution may be embodied in a software product, which is stored in a storage medium and includes instructions for causing a computer device (which may be a personal computer, a server, or a network device) to execute all or part of the steps of the method according to the embodiments of the present application. And the aforementioned storage medium includes: various media that can store program codes, such as a flash disk, a removable hard disk, a ROM, a RAM, a magnetic or optical disk, and the like.