Optical monitor device and optical intensity wavelength measuring method

Abstract

The object of the present disclosure is to make it possible to monitor wavelengths of optical signals in an optical monitoring device for a plurality of optical fibers.　The present disclosure is an optical monitoring device that detects the intensity of light propagating through a plurality of optical fibers, the device being characterized by comprising: a light branching part that causes a portion of incident light from the plurality of optical fibers to branch in a first direction and the remaining portion to branch in a second direction at a fixed branching ratio, and emits the branched light; and a light-receiving part that receives the light emitted from the light branching part to the second direction, wherein the light-receiving part comprises a wavelength dependence part in which a greater number of light-receiving elements than the number of optical fibers are arrayed in two dimensions, and which causes the light to be received by the light-receiving unit at different positions on a light-receiving surface in accordance with the wavelengths of the emitted light, and the wavelengths of the emitted light are derived on the basis of the positions of the emitted light on the light-receiving surface.

Description

[Technical Field]

[0001] The present disclosure relates to an optical monitoring device, and more particularly to an optical monitoring device for detecting the intensity of light in an optical transmission device or the like and feeding back the detection result to other components. [Background technology]

[0002] In recent years, the increase in Internet traffic has created a strong demand for increased communication capacity in communication systems. To achieve this, optical fiber communication systems are used in access networks between communication centers and user homes, and in core networks connecting communication centers. In optical fiber communication, the detection of the optical power propagating through optical fibers is often used to control communication and verify the health of equipment. For example, in access networks, test light is propagated through optical fibers, and the optical power is measured to verify the loss and health of the optical fiber, as well as the fiber optics and connections. In addition, WDM (Wavelength Division Multiplexing) transmission used in core networks requires monitoring of optical power for feedback control.

[0003] For example, technology such as that described in Patent Document 1 is used for monitoring optical power in access networks. Patent Document 1 describes a technology that uses two parallel waveguides to split light at a fixed splitting ratio, which enables measurements of optical signal power and propagation loss in access networks.

[0004] For example, the technology described in Patent Document 2 is used for optical intensity monitoring in WMD transmission. Patent Document 2 describes a technology for simultaneously monitoring the intensity of optical signals from multiple optical fibers by combining optical fibers arranged one-dimensionally with a dielectric multilayer film.

[0005] However, conventional optical monitor devices with an arrangement configuration still have the following problems.

[0006] As optical communications become more widespread and the number of optical fibers in optical facilities / cables increases, firstly, in the case of optical monitoring devices that use an optical coupler for each optical fiber, the cost and size increase as the number of optical fibers increases.Even in the case of optical monitoring devices that arrange optical fibers and optical intensity sensors in a one-dimensional array, there is a limit to the array arrangement of optical fibers, and if the number of optical fibers increases, the cost and size increase accordingly.

[0007] As a spatial optical system for constructing such an optical monitoring device, for example, Patent Document 2 uses a dielectric multilayer film for optical branching. However, dielectric multilayer films generally have a high optical reflectivity, which causes a problem of large loss of signals passing through the optical monitoring device. In addition, dielectric multilayer films generally reflect only a specific wavelength band, which makes them unsuitable for monitoring communications that use a wide wavelength band, such as WDM transmission. [Prior art documents] [Patent documents]

[0008] [Patent Document 1] Patent No. 3450104 [Patent Document 2] Patent Publication No. 2004-219523 Summary of the Invention [Problem to be solved by the invention]

[0009] One possible technique to solve the above problem and enable monitoring of optical signals over a wide wavelength range is to use Fresnel reflection to extract light over a wide wavelength range and measure the intensity of the optical signals from multiple optical fibers at once. However, this method extracts all wavelengths in the same way, making it impossible to know the wavelength of the extracted optical signal.

[0010] An object of the present disclosure is to enable an optical monitoring device for multiple optical fibers to monitor the wavelengths of optical signals in a wide wavelength range. [Means for solving the problem]

[0011] In order to achieve the above object, the optical monitoring device of the present disclosure comprises: An optical monitor device for detecting the intensity of light propagating through a plurality of optical fibers, an optical branching unit that branches a part of incident light in a first direction and the rest in a second direction at a specific branching ratio and outputs the branched light; a light receiving unit that receives light emitted from the optical branching unit in the second direction, The light receiving unit The number of light receiving elements is greater than the number of the optical fibers, and the light receiving elements are two-dimensionally arranged. a wavelength-dependent unit that causes the light-receiving unit to receive the emitted light at different positions on a light-receiving surface depending on the wavelength of the emitted light; The wavelength of the emitted light is determined based on the position of the emitted light on the light receiving surface.

[0012] The disclosed method includes detecting the intensity of light propagating through a plurality of optical fibers using an optical monitoring device, the method comprising: a branching step in which an optical branching unit branches a part of the incident light from the plurality of optical fibers in a first direction and the rest in a second direction at a certain branching ratio; a light receiving step in which a light receiving unit receives light emitted in a second direction from the optical branching unit; Equipped with In the light receiving step, a wavelength dependent unit causing the light receiving unit to receive the emitted light at different positions on the light receiving surface according to the wavelength of the emitted light; The wavelength of the emitted light is determined based on the position of the emitted light on the light receiving surface.

[0013] In the optical monitoring device disclosed herein, which detects the intensity of light propagating through multiple optical fibers, the light emitted in the second direction passes through the wavelength-dependent portion and reaches the light-receiving portion at an emission angle that varies depending on the wavelength. Therefore, in the present disclosure, the light intensity detected by each light-receiving element in the light-receiving portion varies depending on the wavelength, and the arriving wavelength can be determined from this change. This allows the optical monitoring device disclosed herein to measure the wavelength and light intensity of multiple optical fibers.

[0014] The optical branching unit may include a single-layer film having a uniform thickness, an incident-side member provided on the incident side of the single-layer film and having a refractive index different from that of the single-layer film, and an output-side member provided on the output side of the single-layer film and having the same refractive index as that of the incident-side member. In this case, a first refractive index interface between the single-layer film and the incident-side member and a second refractive index interface between the single-layer film and the output-side member may be formed at specific angles with respect to the optical axis of the incident light, and the first direction may be a direction of transmission through the first refractive index interface and the second refractive index interface, and the second direction may be a direction of reflection at the first refractive index interface and the second refractive index interface.

[0015] The wavelength-dependent portion may be an optical prism that receives the light emitted in the second direction and emits the light in a different direction depending on the wavelength of the light. In this case, a light-receiving surface of the light-receiving portion may be substantially perpendicular to the light transmitted through the optical prism. The distance between the optical prism and the array-type light-receiving element may be sufficiently larger than the thickness of the single-layer film.

[0016] The optical monitoring device of the present disclosure comprises: a plurality of incident-side optical fibers arranged in a two-dimensional array so that light is incident on the optical branching portion; a plurality of output-side optical fibers arranged in a two-dimensional array so as to receive each of the output light beams from the optical branching unit in the first direction; an incident-side optical lens disposed between the optical branching unit and the incident-side optical fiber, and converting each light beam incident on the optical branching unit into a parallel beam; an output optical lens disposed between the optical branching unit and the output optical fiber, for coupling each output light from the optical branching unit to the output optical fiber; The device may also include:

[0017] The above disclosures can be combined as much as possible. [Effects of the Invention]

[0018] The present disclosure makes it possible to monitor the wavelengths of optical signals in a wide wavelength range in an optical monitoring device for multiple optical fibers. [Brief explanation of the drawings]

[0019] [Figure 1] 1 illustrates an example embodiment of an optical monitoring device of the present disclosure. [Figure 2] 1 shows an example of light propagating through a spatial optical system. [Figure 3A] 1 shows an example of an image of emitted light reaching a light receiving element. [Figure 3B] 1 shows an example of an image of emitted light reaching a light receiving element. [Figure 4] 1 shows an example of the arrangement of the optical fiber on the input side. [Figure 5A] 1 shows an example of an image of emitted light reaching a light receiving element. [Figure 5B] 1 shows an example of an image of emitted light reaching a light receiving element. [Figure 6] 1 shows an example of a method for measuring light intensity and wavelength according to the present disclosure. DETAILED DESCRIPTION OF THE INVENTION

[0020] Hereinafter, embodiments of the present disclosure will be described in detail with reference to the drawings. Note that the present disclosure is not limited to the embodiments shown below. These implementation examples are merely illustrative, and the present disclosure can be implemented in various forms with various modifications and improvements based on the knowledge of those skilled in the art. Note that components with the same reference numerals in this specification and drawings indicate the same components.

[0021] (First embodiment) The optical monitoring device of this embodiment has the configuration shown in FIG. The optical monitoring device of this embodiment is an optical monitoring device that detects the intensity of light propagating through a plurality of incident-side optical fibers 11, a spatial optical system (30) that splits a majority of each incident light (41) from an incident-side optical fiber (11) into a specific first direction and the remainder into another specific second direction at a fixed splitting ratio, and outputs each split light; a plurality of incident-side optical fibers 11 that propagate light and are arranged in a two-dimensional array so as to input light into the spatial optical system 30; an output-side optical fiber 12 for propagating a plurality of beams, the output-side optical fiber 12 being arranged to receive most of the output beam 42 output from the spatial optical system 11 in a first direction; an array-type light-receiving element 51 arranged to receive a portion of the emitted light 43 emitted in the second direction from the spatial optical system 30; an incident-side optical lens 21 disposed between the spatial optical system 30 and the incident-side optical fiber 11, for converting each incident light from the incident-side optical fiber 11 to the spatial optical system 30 into a parallel light; an output-side optical lens 22 that is disposed between the spatial optical system 30 and the output-side optical fiber 12 and efficiently couples each output light from the spatial optical system 30 to the output-side optical fiber 12 corresponding to the input-side optical fiber 11; It has.

[0022] In the present disclosure, the array type light receiving element 51 receives light emitted in the second direction, (i) the light intensity received by the array type light receiving element 51, (ii) the light intensity of the incident light from the plurality of incident-side optical fibers 11; (iii) the light intensity of the output light emitted to the plurality of output-side optical fibers 12; At least one of the above can be measured.

[0023] 1 shows an example in which the first direction is the x-axis direction and the second direction is the z-axis direction. In the present disclosure, the spatial optical system 30 functions as the "light branching unit" of the present disclosure, and the array-type light-receiving element 51 functions as the "light-receiving unit" of the present disclosure.

[0024] 2, the spatial optical system 30 includes a single-layer film 33 having a uniform refractive index and disposed between an incident-side member 30A and an output-side member 30B, both of which are made of a material having a uniform refractive index, and the single-layer film 33 is disposed at a specific angle (45 degrees in the figure) with respect to the optical axis of the incident light 41. As a result, a first refractive index interface 33A between the single-layer film 33 and the incident-side member 30A and a second refractive index interface 33B between the single-layer film 33 and the output-side member 30B are disposed at specific angles with respect to the optical axis of the incident light 41.

[0025] 1 and 2 show an example in which the specific angle is 45 degrees and the direction of the emitted light 43 is 90 degrees, but the direction of the emitted light 43 is not fixed at 90 degrees and can be changed as needed. Furthermore, the spatial optical system 30 is not limited to a spatial system, and any optical component having a branching surface capable of branching into two light beams with different directions can be used.

[0026] 1 and 2, the incident light from the incident-side optical fiber 11 is converted into parallel light by the incident-side optical lens 21, thereby preventing loss due to diffusion. Furthermore, most of the emitted light 42 is guided to the output-side optical lens 22 by the spatial optical system 30. The output-side optical lens 22 collects the light that has passed through the spatial optical system 30 and couples it to the output-side optical fiber 12. In this way, most of the emitted light from the incident-side optical fiber 11 can be guided to the output-side optical fiber 12 with little loss.

[0027] Meanwhile, a portion of the emitted light 43 branched by the spatial optical system 30 is refracted by an optical prism 52 arranged in a different direction from the majority of the emitted light 42, and transmitted light 44 from the optical prism 52 is guided to the array-type light-receiving element 51. The optical prism 52 functions as the "wavelength-dependent portion" of the present disclosure, and the refraction angle at the optical prism 52 changes depending on the wavelength. As a result, the amount of light incident on each element of the array-type light-receiving element 51 changes depending on both the light intensity and wavelength of the incident-side optical fiber 11, and the optical monitoring device of this embodiment can measure the intensity and wavelength of the light propagating from the incident-side optical fiber 11 to the output-side optical fiber 12 from this change.

[0028] 3A and 3B illustrate the arrangement of light receiving elements on the light receiving surface of the array-type light receiving element 51 and the images of the emitted light 43 arriving from each incident-side optical fiber 11. For example, as shown in FIG. 4, four incident-side optical fibers F1 to F4 are two-dimensionally arranged, two by two, at a constant pitch, and emit light of the same wavelength λ0. Also, assume that 25 light receiving elements M1 to M25 are two-dimensionally arranged at a constant pitch. In this disclosure, the pitch of the incident-side optical fibers F1 to F4 does not match the pitch of the light receiving elements M1 to M25, and no special alignment is performed. In this case, on the light receiving surface of the array-type light receiving element 51, four images Im1 to Im4 of the emitted light 43 are formed at positions corresponding to the arrangement of the incident-side optical fibers F1 to F4, as shown in FIG. 3A.

[0029] Here, if the light receiving surface of the array type light receiving element 51 is arranged so as to be approximately perpendicular to the transmitted light 44 emitted from the optical prism 52, when the wavelength λ1 of the incident light 41 from the incident-side optical fiber F1 changes, the refraction angle at the optical prism 52 changes, and the positions of the images Im1 to Im4 on the light receiving surface change. For example, suppose that the position of the image Im1 of the incident-side optical fiber F1 changes, as shown by the dotted line Im1' in FIG. 5B.

[0030] At this time, the image in Fig. 3A is equal to the sum of the images (reference images) from each of the incident-side optical fibers F1 to F4, as shown in Fig. 5A. Therefore, the image in Fig. 3B is equal to the result of adding the reference image of the incident-side optical fiber F1 to the images of the other incident-side optical fibers F2 to F4 after moving it by the amount of image position movement due to wavelength differences, as shown in Fig. 5B.

[0031] The output matrices (reference matrices) of the array-type photodetector 51 when light of wavelength λ0 with unit light intensity is individually emitted from each of the incident side optical fibers F1 to F4 are SF1 to SF4, and the output matrix X0 of the array-type photodetector 51 when each of the incident side optical fibers F1 to F4 emits light with light intensities PF1 to PF4 is expressed by the following equation 1.

number

[0032] At this time, the optical intensities PF1 to PF4 of the optical fibers are expressed as the general inverse matrix {SF1 SF2 SF3 SF4} + Using this, it can be calculated using the following equation 2.

number

[0033] By measuring the reference matrix in advance, the light intensity of each of the incident side optical fibers F1 to F4 when the wavelength of all the incident side optical fibers F1 to F4 is λ0 can be calculated from the output matrix X0 of the arrayed light receiving element 51.

[0034] Here, for example, if the wavelength of the incident optical fiber F1 is changed to λ1, the light intensity of the image Im1' at wavelength λ1 can be obtained in the same way as when the wavelength is λ0 by using a reference matrix SF1' obtained by shifting the matrix SF1 by the amount of shift of the image Im1 corresponding to λ1. If the distance Dp between the optical prism 52 and the array type light receiving element 51 is sufficiently larger than the thickness of the single layer film 33, the amount of shift of the image Im1 is determined by the change in the refraction angle due to the change in wavelength and the distance Dp. The change in the refraction angle is determined by the vertex angle θ of the prism and the refractive index n p Therefore, the refractive index of the prism n p , vertex angle θ, distance D between the optical prism 52 and the array type light receiving element 51 p By knowing this, the amount of image movement in response to changes in wavelength can be calculated.

[0035] Therefore, the light intensity wavelength measurement method of this embodiment is as follows: 1. A method for detecting the intensity of light propagating through a plurality of optical fibers using an optical monitoring device, comprising: a branching step in which the spatial optical system 30 branches a part of the incident light from the plurality of optical fibers 11 in a first direction and the rest in a second direction at a certain branching ratio; a light receiving step in which the array-type light receiving element 51 receives the light 43 emitted in the second direction from the spatial optical system 30; Equipped with In the light receiving step, The optical prism 52 causes the array type light receiving element 51 to receive the emitted light 43 at different positions on the light receiving surface according to the wavelength of the emitted light 43, The wavelength of the emitted light 43 is determined based on the position of the emitted light 43 on the light receiving surface.

[0036] Specifically, in the light receiving procedure, as shown in FIG. 6, the calculation processing unit 53 calculates the light intensity of each of the incident side optical fibers F1 to F4 using Equation 2 (S11), and then calculates the output matrix using Equation 1 while changing the wavelength of the reference matrix for each of the incident side optical fibers F1 to F4 using the calculated light intensity (S12 to S15), and determines the wavelength that is closest to the actual output matrix (S17), thereby determining the wavelength of each of the incident side optical fibers F1 to F4 (S18 to S21).

[0037] Specifically, the output matrix is ​​calculated as follows: The reference matrix SF1' of the optical fiber whose wavelength is to be measured is moved according to the wavelength (S12); A synthetic image is created using the reference image obtained by the reference matrix SF1' (S13). A difference value between the image received by the array type light receiving element 51 and the created composite image is calculated (S14). This calculation of the difference value is carried out for all communication wavelengths (S15). In step S17, the wavelength with the smallest difference value among the difference values ​​calculated in step S14 is output as the wavelength measurement result of the optical fiber under wavelength measurement.

[0038] The calculation processing unit 53 performs steps S12 to S17 for the incident side optical fibers F1 to F4 (S18), thereby obtaining the wavelengths of the incident side optical fibers F1 to F4. The calculation processing unit 53 calculates the wavelengths of the incident side optical fibers F1 to F4 obtained by the calculation processing unit 53 using the general inverse matrix {SF1 SF2 SF3 SF4} + The optical intensity of each of the incident side optical fibers F1 to F4 is calculated using the above formula (S20). As a result, the calculation processing unit 53 outputs the wavelength and optical intensity of each of the optical fibers F1 to F4 as the optical intensity measurement result.

[0039] As indicated by the dashed arrows in Fig. 6, after the calculation processing unit 53 has determined the wavelength of each of the incident-side optical fibers F1 to F4, it can calculate the light intensity again using Equation 2, thereby enabling a more accurate calculation of the light intensity. In this case, the second step simply involves "setting the reference matrix of each of the incident-side optical fibers F1 to F4 to a position corresponding to the previous wavelength measurement result, and then moving the reference matrix of the incident-side optical fiber F1 to F4 whose wavelength is to be measured according to the wavelength." Furthermore, by repeating this process several times, it is expected that the wavelength and light intensity can be calculated more accurately.

[0040] (Effects of the present disclosure) As described above, the optical monitoring device of the present disclosure is an optical monitoring device that detects the intensity of light propagating through multiple optical fibers, and splits incident light using a single-layer film 33 with a uniform thickness. Of the split incident light, output light 34 in the second direction passes through the optical prism 52 and reaches the array-type photodetector 51 at an output angle that varies depending on the wavelength. Therefore, the light intensity detected by each photodetector varies depending on the wavelength, and the wavelength that has arrived can be determined from this change. Therefore, the present disclosure makes it possible to simultaneously measure the optical intensity and wavelength of optical signals passing through multiple optical fibers.

[0041] The above is an example of an embodiment, but the present invention is not limited to this. For example, although an example has been shown in which the wavelength-dependent portion is the optical prism 52, the wavelength-dependent portion is not limited to a form that uses the wavelength dependency of the refraction angle, and any form that can cause the light emitted in the second direction to be incident on different positions on the light-receiving surface of the array-type light-receiving element 51 depending on its wavelength, such as a form that uses the wavelength dependency of the reflection angle, can be adopted.

[0042] Furthermore, although the present disclosure has shown an example in which the single-layer film 33 is an air layer, it may be glass or resin. Furthermore, the spatial optical system 30 is not limited to a cubic shape, and may be any shape, such as a rectangular parallelepiped. Furthermore, the array-type light-receiving element 51 may be disposed at any position where it can receive light branched by the spatial optical system 30.

[0043] The optical monitoring device of the present disclosure can also be used to monitor any light transmitted in an optical transmission system. For example, the optical monitoring device of the present disclosure can be installed in any device used in an optical transmission system, such as a transmitter, receiver, or repeater, and the measurement results from the array-type photodetector 51 can be used for feedback or feedforward to any component inside or outside the device. Furthermore, the optical monitoring device of the present disclosure can be inserted midway along a transmission line in an optical transmission system to measure the intensity and propagation loss of an optical signal in the transmission line.

[0044] The arithmetic processing unit 53 included in the optical monitoring device of the present disclosure can also be realized by a computer and a program, and the program can be recorded on a recording medium or provided via a network. The program of the present disclosure is a program for realizing a computer as the arithmetic processing unit 53 included in the optical monitoring device of the present disclosure, and is a program for causing a computer to execute each step included in the method performed by the optical monitoring device according to the present disclosure. [Industrial Applicability]

[0045] The present disclosure can be applied to the information and communications industry. [Explanation of symbols]

[0046] 11: Input optical fiber 12: Output optical fiber 21: Input optical lens 22: Output optical lens 30: Spatial optical system 30A:Incidence side member 30B: Output side member 33: Single layer membrane 51: Array type photodetector 52: Optical prism 53: Processing unit

Claims

1. An optical monitor device that detects the intensity of light propagating through a plurality of optical fibers arranged two-dimensionally, an optical branching unit that branches a part of the incident light from the plurality of optical fibers in a first direction and the rest in a second direction at a constant branching ratio and outputs the branched light; a light receiving unit that receives light emitted from the optical branching unit in the second direction; Equipped with The light receiving unit a plurality of light receiving elements are two-dimensionally arranged in a number greater than the number of optical fibers; a wavelength-dependent unit that causes the light receiving unit to receive light at different positions on a light receiving surface formed by the plurality of light receiving elements according to the wavelength of the emitted light; determining the wavelength of the emitted light by solving simultaneous equations of the light intensities of the plurality of light receiving elements using a reference matrix determined by wavelength; 1. An optical monitor device comprising:

2. the wavelength-dependent unit is an optical prism that receives the light emitted in the second direction and emits the light in a different direction depending on the wavelength of the emitted light, a light receiving surface of the light receiving unit is substantially perpendicular to the light transmitted through the optical prism; 10. The optical monitor device of claim 1.

3. The optical branching unit is a monolayer film having a uniform thickness; an incident-side member provided on an incident side of the single-layer film and having a refractive index different from that of the single-layer film; an exit-side member provided on the exit side of the single-layer film and having the same refractive index as the incident-side member; Equipped with a first refractive index interface between the single layer film and the incident-side member and a second refractive index interface between the single layer film and the output-side member are provided at specific angles with respect to an optical axis of the incident light, the first direction is a direction passing through the first refractive index interface and the second refractive index interface, the second direction is a direction of reflection at the first refractive index interface and the second refractive index interface; 2. The optical monitor device according to claim 1.

4. 4. The optical monitor device according to claim 3, wherein the distance between the wavelength dependent portion and the light receiving portion is greater than the thickness of the single layer film.

5. A method for detecting the intensity of light propagating through a plurality of optical fibers arranged two-dimensionally using an optical monitor device, comprising: a branching step in which an optical branching unit branches a part of the incident light from the plurality of optical fibers in a first direction and the rest in a second direction at a constant branching ratio; a light receiving step in which the light receiving unit receives the light emitted from the optical branching unit in the second direction using a plurality of light receiving elements that are two-dimensionally arranged in a number greater than the number of the plurality of optical fibers; Equipped with In the light receiving step, a wavelength dependent unit causing the light receiving unit to receive the emitted light at different positions on a light receiving surface formed by the plurality of light receiving elements according to the wavelength of the emitted light; determining the wavelength of the emitted light by solving simultaneous equations of the light intensities of the plurality of light receiving elements using a reference matrix determined by wavelength; A method characterized by:

Images