Patent Application
20200033188
The present invention relates to a divergence angle measurement device, a divergence angle measurement method, a laser apparatus, and a laser system.
In recent years, a fiber laser apparatus attracts attention as a high-power laser apparatus used in the industrial field. This fiber laser apparatus is characterized in that its beam quality (BPP: Beam Parameter Product or M2) is superior and its light concentrating property is higher as compared with the high-power laser apparatus in the related art (for example, a carbon dioxide gas laser apparatus). Therefore, if the fiber laser apparatus is used instead of the carbon dioxide gas laser apparatus or the like in the related art, the processing time can be shortened, and energy saving can be achieved.
In such a fiber laser apparatus, for example, it is considered that the divergence angle of the launched laser light may increase due to deterioration over time or the like. When the divergence angle of the laser light increases, the beam quality is deteriorated, and the processing characteristics are changed. Therefore, in order to maintain the performance of the fiber laser apparatus, it is necessary to monitor the divergence angle of the laser light and to perform maintenance of the fiber laser apparatus according to the monitoring result.
Patent Documents 1, 2 disclose an example of related arts for measuring the divergence angle of a laser beam. Specifically, in Patent Document 1, in order to obtain the divergence angle θ, a part of the laser beams to be measured are branched by a beam splitter and focused by a measurement lens (focal length f), and the beam diameter d is measured by a charge coupled device (CCD) camera. Patent Document 1 discloses a technique for obtaining the divergence angle θ by the calculation expression θ=d/f. Further, Patent Document 2 discloses a technique for converting the radiant infrared energy into energy of a shorter wavelength at a predetermined distance from the end of the optical fiber, and recording the distribution of the energy of the shorter wavelength to calculate the numerical aperture of the optical fiber.
[Patent Document 1] Japanese Unexamined Patent Application, First Publication No. H10-47938
[Patent Document 2] Published Japanese Translation No. S64-500539 of the PCT International Publication
Meanwhile, under the present circumstances, fiber laser apparatuses having a low output of about several tens of watts [W], a medium output of several hundreds of watts [W], and a high output of several kilowatts [kW] are realized. In the future, research and development of fiber laser apparatuses having high output are considered to be conducted in the direction of increasing output power, and fiber laser apparatuses having output power of several tens to hundreds of kW may be realized in the future.
In the configuration of Patent Document 1, it is necessary to split a part of the laser beams to be measured by the beam splitter. Therefore, it is difficult to monitor the divergence angle of the laser light launched from the fiber laser apparatus with high output in the actual operating state. In addition, in the configuration of Patent Document 1, in addition to optical elements such as a beam splitter and a measurement lens, an image pickup element such as a CCD camera is required, so the measurement apparatus becomes large.
In the configuration of Patent Document 2, it is necessary to dispose an up-conversion screen at a predetermined distance from the end of the optical fiber to convert the wavelength of infrared light launched from the end of the optical fiber. Therefore, as in the configuration of Patent Document 1, it is difficult to monitor the divergence angle of the laser light launched from the fiber laser apparatus with high output in the actual operating state.
One or more embodiments of the present invention provide a divergence angle measurement device, a divergence angle measurement method, a laser apparatus, and a laser system, capable of measuring the divergence angle of laser light of high output with a simple configuration.
A divergence angle measurement device according to one or more embodiments of the present invention monitors a divergence angle of laser light propagated in an optical fiber having a core and a cladding and includes: a first photodetector that is configured to detect the laser light leaked from the cladding of the optical fiber; and a calculation unit (processor) that is configured to obtain the divergence angle of the laser light, according to a detection result of the first photodetector and power information indicating power of the laser light propagated in the optical fiber.
Further, in the divergence angle measurement device, the optical fiber may be provided with a cladding light removal portion where cladding light propagated through the cladding leaks and where the cladding light is removed, and the first photodetector may be disposed in the cladding light removal portion, and is configured to detect the cladding light removed by the cladding light removal portion.
Further, the divergence angle measurement device may further include a second photodetector that is disposed in a vicinity of the optical fiber, and is configured to detect Rayleigh scattered light of the laser light propagated in the optical fiber, and the calculation unit may be configured to obtain the divergence angle of the laser light using a detection result of the second photodetector as the power information.
Further, the divergence angle measurement device may further include a second photodetector that is disposed in a vicinity of the optical fiber, and is configured to detect Rayleigh scattered light of the laser light propagated in the optical fiber, and the second photodetector may be provided farther on a light input side of the optical fiber than the cladding light removal portion.
Alternatively, the divergence angle measurement device may further include a temperature detector that is configured to detect the temperature of the cladding light removal portion, and the calculation unit may be configured to obtain the divergence angle of the laser light using a detection result of the temperature detector as the power information.
Alternatively, in the divergence angle measurement device, the calculation unit may be configured to obtain the divergence angle of the laser light using a detection result of a current detector that is configured to detect a drive current supplied to a laser light source which launches the laser light propagated in the optical fiber, as the power information.
Further, the divergence angle measurement device may further include an output unit that is configured to output first information indicating the divergence angle of the laser light obtained by the calculation unit, or second information indicating whether or not the divergence angle of the laser light obtained by the calculation unit is within a predetermined range.
Further, a divergence angle measurement method according to one or more embodiments of the present invention is a divergence angle measurement method for monitoring a divergence angle of laser light propagated in an optical fiber having a core and a cladding. The method includes: a detection step of detecting the laser light leaked from the cladding of the optical fiber; and a calculation step of obtaining the divergence angle of the laser light, according to the detection result of the detection step and power information indicating power of the laser light propagated in the optical fiber.
Further, a laser apparatus according to one or more embodiments of the present invention includes: a laser light source; an optical fiber which has a core and a cladding, the optical fiber propagating laser light launched from the laser light source; and the divergence angle measurement device.
Further, the laser apparatus may further include an adjusting device that is configured to adjust the divergence angle of the laser light propagated in the optical fiber; and a control device (controller) that is configured to control the adjusting device according to a measurement result of the divergence angle measurement device.
Further, a laser system according to one or more embodiments of the present invention includes: a plurality of laser apparatuses; a combiner that is configured to combine light launched from the plurality of laser apparatuses; an launching optical fiber that is configured to guide the light combined by the combiner; and the divergence angle measurement device which is configured to monitor a divergence angle of laser light propagated in the launching optical fiber.
According to one or more embodiments of the present invention, laser light leaked from a cladding of an optical fiber having a core and the cladding is detected by a first photodetector, and the divergence angle of the laser light is obtained according to the detection result of the first photodetector and power information indicating power of the laser light propagated in the optical fiber. Therefore, it is possible to measure the divergence angle of the laser light of high output with a simple configuration.
Hereinafter, a divergence angle measurement device, a divergence angle measurement method, a laser apparatus, and a laser system according to embodiments of the present invention will be described in detail with reference to the drawings.
As shown in
The first end 12a of the delivery fiber 12 is connected to the laser light source 11 and receives the laser light L. The second end 12b of the delivery fiber 12 is connected to the connector 14. In one or more embodiments, along the light propagation direction, a side closer to the first end 12a is referred to as a light input side and a side closer to the second end 12b is referred to as a light launch side. The direction from the laser light source 11 toward the connector 14 is referred to as a launch direction D.
The laser light source 11 is, for example, a fiber laser provided with a plurality of pumping light sources, and it excites the rare earth ions added to the core of the optical amplification fiber by the pumping light launched from the pumping light source and launches the laser light L. The types and the number of pumping light sources provided in the laser light source 11 are appropriately selected according to the wavelength and power of the laser light L. The delivery fiber 12 is an optical fiber that functions as a transmission medium for transmitting the laser light L launched from the laser light source 11. The first end 12a of the delivery fiber 12 is connected to the laser light source 11. The second end 12b of the delivery fiber 12 is connected to the connector 14. The connector 14 functions as a launch end of the laser light L, and is connected to the second end 12b of the delivery fiber 12.
Here, the delivery fiber 12 used in the laser apparatus 1 will be described.
The core C and the inner cladding CL1 of the optical fiber F shown in
Here, the specifications of the optical fiber F constituting the delivery fiber 12 are, for example, as follows.
Core C: Composition: silica glass, diameter: 100 [μm], refractive index: 1.46
Inner cladding CL1: Composition: Fluorinated silica glass, outer diameter: 360 [m], refractive index: 1.44
Outer cladding CL2: Composition: silicone, outer diameter: 500 [μm], refractive index: 3.9
The cladding light removal portion 13 is provided in the middle of the delivery fiber 12 (between the first end 12a and the second end 12b). The cladding light removal portion 13 removes cladding light of the laser light L propagated in the launch direction D in the delivery fiber 12.
As shown in
The housing 20 is formed of, for example, a metal material such as aluminum subjected to black alumite treatment. However, the material of the housing 20 is not particularly limited. The housing 20 is formed with a groove 20M which is recessed downward from the top surface. The groove 20M includes an upper groove 20M1 and a lower groove 20M2. The lower groove 20M2 is disposed below the upper groove 20M1 in
In the coating removal area 21, at least a part of the coating CV in the circumferential direction of the optical fiber F is removed. In the coating removal area 21, the coating CV is removed along both the longitudinal direction and the circumferential direction of the optical fiber F. A portion where the coating CV is removed and the inner cladding CL1 of the optical fiber F is exposed to the opening side of the groove 20M is referred to an exposed portion 22. The exposed portion 22 is covered with a sealing material 23 (details will be described later). That is, the upper surface of the coating removal area 21 is covered with the sealing material 23.
In the longitudinal direction of the optical fiber F, as in the example shown in
The sealing material 23 is filled in the space (lower groove 20M2) around the optical fiber F inside the groove 20M. The sealing material 23 is formed of, for example, a silicone resin having light transmissive properties. Thereby, the position of the optical fiber F inside the groove 20M is fixed. The sealing material 23 is formed of a material having a refractive index equal to the refractive index of the inner cladding CL1 or a refractive index higher than the refractive index of the inner cladding CL1. That is, in the coating removal area 21, the inner cladding CL1 is in contact with the sealing material 23 having a refractive index equal to the refractive index of the inner cladding CL1 or a refractive index higher than the refractive index of the inner cladding CL1. Therefore, the light propagated in the inner cladding CL1 leaks from the inner cladding CL1 to the outside of the sealing material 23 through the sealing material 23.
As shown in
Further, the cladding light removal portion 13 is provided with the first photodetector 31 of the divergence angle measurement device 15. The first photodetector 31 is, for example, an infrared photodiode, and receives leaked light of the laser light L leaked from the cladding of the optical fiber F. As shown in
The lid 25 to which the first photodetector 31 is attached is provided to cover the upper side of the groove 20M of the housing 20, as shown in
However, the coating removal area 21 may not necessarily face the light receiving surface R of the first photodetector 31. Even in such a configuration, the cladding light leaked from the optical fiber F is reflected and scattered on the inner surface of the groove 20M, so the first photodetector 31 can receive the cladding light. Similarly, the light receiving surface R may not be located inside the groove 20M, but may be located inside, for example, a through hole formed in the lid 25.
The divergence angle measurement device 15 monitors the divergence angle of the laser light L propagated in the delivery fiber 12, and outputs information (first information I1) indicating the divergence angle of the laser light L or information (second information I2) indicating whether or not the divergence angle of the laser light L is within the range defined in advance. Here, the first information I1 described above may be information indicating the divergence angle itself of the laser light L, or may be a value obtained by converting the divergence angle of the laser light L into a numerical aperture (NA).
The “divergence angle of the laser light L” refers to an angle (degree θ) between the propagation direction of the laser light L and the central axis of the optical fiber. As the divergence angle of the laser light L propagated in the delivery fiber 12 increases, the divergence angle of the laser light L launched from the second end 12b of the delivery fiber 12 (or the connector 14) tends to increase. Therefore, the divergence angle of the laser light L launched from the second end 12b of the delivery fiber 12 (or the connector 14) can be obtained by obtaining the divergence angle of the laser light L propagated in the delivery fiber 12. Further, the above-described “value obtained by converting the divergence angle into a numerical aperture (NA)” is a value defined by sin θ.
As shown in
The second photodetector 32 is disposed in the vicinity of the delivery fiber 12 and detects Rayleigh scattered light of the laser light L propagated in the delivery fiber 12. Here, the Rayleigh scattered light has a power according to the power of the light propagated in the optical fiber F, regardless of the guiding direction of the laser light L in the delivery fiber 12. For example, a PIN photodiode can be used as the second photodetector 32 described above. In a case where a PIN photodiode is used as the second photodetector 32, the second photodetector 32 is disposed, for example, at a position spaced apart from the side surface of the optical fiber F (from the coating resin) by about a few [mm].
The second photodetector 32 is provided farther on the light input side (the side closer to the first end 12a) of the delivery fiber 12 than the cladding light removal portion 13. This is to minimize as much as possible the influence of the cladding light removed by the cladding light removal portion 13 on the detection result of the second photodetector 32. If the influence of the cladding light removed by the cladding light removal portion 13 is small, the second photodetector 32 may be provided farther on the light launch side (the side closer to the second end 12b) than the cladding light removal portion 13. That is, the second photodetector 32 can be disposed at any position as long as it can detect the Rayleigh scattered light of the laser light L propagated in the optical fiber F without being affected by the disturbance (for example, stray light or the like).
The calculation unit 33 monitors the divergence angle of the laser light L propagated in the delivery fiber 12, according to the detection result of the first photodetector 31 and the detection result of the second photodetector 32. Specifically, the calculation unit 33 obtains the power (power information IP) of the laser light L propagated in the optical fiber F, from the detection result of the second photodetector 32. Then, according to the power information IP and the detection value characteristic information IF, the divergence angle of the laser light L is obtained. Here, the detection value characteristic information IF is prepared for each power of the launched light which is launched from the laser apparatus 1, and is information in which the ratio of the detection results of the first and second photodetectors 31, 32 and the first information I1 are associated with each other. Further, the calculation unit 33 stores a threshold which is the maximum value of the divergence angle of the laser light L that can be tolerated by the laser apparatus 1, and determines whether the divergence angle of the laser light L exceeds the threshold.
Here, the measurement principle of the divergence angle of the laser light L in the calculation unit 33 will be described.
Referring to
NA1, NA2, and NA3 shown in the legend in
Further, regardless of the magnitude of the light output, it can be seen that both the detection result of the first photodetector 31 (cladding monitor output) and the detection result of the second photodetector 32 (Rayleigh monitor output) increase as the divergence angle of the laser light increases. Specifically, assuming that the light output is, for example, 800 [W] to facilitate understanding, the detection results of the first photodetector 31 (cladding monitor output) increase in the order of the divergence angles NA1, NA2, NA3 of the laser light, and the detection results of the second photodetector 32 (Rayleigh monitor output) also increase in the order of the divergence angles NA1, NA2, NA3 of the laser light. Here, as shown in
As described above, according to
Therefore, the divergence angle of the laser light L launched from the laser apparatus 1 is measured in advance, the power of the laser light L at that time is detected by the second photodetector 32, and the cladding light (the laser light L leaked from the cladding of the optical fiber F) is detected by the first photodetector 31. Then, detection value characteristic information IF which is information in which the ratio of the detection results of the first and second photodetectors 31, 32 and the first information I1 are associated with each other is prepared in advance for each power of the launched light which is launched from the laser apparatus 1. In this way, the power of the laser light L propagated in the optical fiber F is obtained from the detection result of the second photodetector 32, and the divergence angle of the laser light L is obtained according to this power and the detection value characteristic information IF. The calculation unit 33 obtains the divergence angle of the laser light L according to such a principle.
The monitor signal output unit 34 outputs the first information I1 or the second information I2 obtained by the calculation unit 33 to the outside. For example, the monitor signal output unit 34 includes a display device such as a liquid crystal display device, and displays the first information I1 or the second information I2 obtained by the calculation unit 33 on the display device. Alternatively, the monitor signal output unit 34 has an external output terminal, and outputs the first information I1 or the second information I2 obtained by the calculation unit 33 from the external output terminal to the outside.
Next, the operation of the laser apparatus 1 with the above configuration will be described. When the power of the laser apparatus 1 is turned on, the launch of the laser light L from the laser light source 11 is started. The laser light L launched from the laser light source 11 enters the optical fiber F constituting the delivery fiber 12 from the first end 12a. The laser light L incident on the optical fiber F propagates in the optical fiber F. Here, when the laser light L propagates in the optical fiber F in the launch direction D, Rayleigh scattered light corresponding to the power of the laser light L is generated. Therefore, in the second photodetector 32 of the divergence angle measurement device 15, Rayleigh scattered light corresponding to the power of the laser light L is detected.
Further, when the laser light L propagated in the optical fiber F in the launch direction D reaches the cladding light removal portion 13, the cladding light is removed. Here, the laser light L propagated through the core C of the optical fiber F passes through the cladding light removal portion 13. However, the laser light (cladding light) propagated through the inner cladding CL1 is removed by leaking from the coating removal area 21 (see
The laser light L having passed through the cladding light removal portion 13 is launched from the connector 14 connected to the second end 12b of the optical fiber F. Here, when a work or the like is disposed in front of the connector 14, the laser light launched from the connector 14 is applied to the processing surface of the work, whereby the processing of the work is performed.
The second photodetector 32 provided in the divergence angle measurement device 15 outputs a detection signal according to the light amount of the Rayleigh scattered light, and the first photodetector 31 outputs a detection signal according to the light amount of the cladding light. The detection signals output from the first and second photodetectors 31, 32 are input to the calculation unit 33. The calculation unit 33 performs a calculation for obtaining the divergence angle of the laser light L, according to the detection signal of the first photodetector 31 and the detection signal of the second photodetector 32 (calculation step).
Specifically, the calculation unit 33, first, performs a calculation of obtaining the power (power information IP) of the laser light L propagated in the optical fiber F, from the detection result of the second photodetector 32. Next, according to the power information IP and the detection value characteristic information IF, a calculation of obtaining the divergence angle of the laser light L is performed. The information indicating the obtained divergence angle of the laser light L (or NA conversion value) (first information I1) is output from the monitor signal output unit 34 to the outside. The first information I1 is displayed, for example, on a display device (not shown).
As described above, in one or more embodiments, the second photodetector 32 that detects the Rayleigh scattered light of the laser light L propagated in the delivery fiber 12 and the first photodetector 31 that detects cladding light which has been removed by the cladding light removal portion 13 are provided. Then, the calculation unit 33 is configured to obtain the divergence angle of the laser light L, according to the detection results of the first and second photodetectors 31, 32. Therefore, it is possible to measure the divergence angle of the laser light L of high output with a simple configuration.
As shown in
The temperature detector 41 is a detector that detects the temperature at a specific position of the cladding light removal portion 13 (for example, the temperature at a predetermined position of the housing 20 or the lid 25 shown in
As described above, in one or more embodiments, the temperature detector 41 that detects the temperature in the cladding light removal portion 13 and the first photodetector 31 that detects cladding light which has been removed by the cladding light removal portion 13 are provided. Further, the calculation unit 33 obtains the power (power information IP) of the laser light L propagated in the delivery fiber 12, according to the detection result of the temperature detector 41. Then, according to the obtained power information IP and the detection result of the first photodetector 31, the divergence angle of the laser light L is obtained using the detection value characteristic information IF. Therefore, it is possible to measure the divergence angle of the laser light L of high output with a simple configuration.
As shown in
The current detector CD detects a drive current (for example, a current for driving a pumping light source provided in the laser light source 11) supplied to the laser light source 11. The power of the laser light launched from the laser light source 11 is approximately proportional to the drive current of the laser light source 11. Therefore, the current value detected by the current detector CD is a value corresponding to the power of the laser light (the laser light L propagated in the delivery fiber 12) launched from the laser light source 11.
As described above, in one or more embodiments, the detection result of the current detector CD is input to the calculation unit 33, and the calculation unit 33 obtains the power (power information IP) of the laser light L propagated in the delivery fiber 12, according to the detection result of the current detector CD. Then, according to the obtained power information IP and the detection result of the first photodetector 31, the divergence angle of the laser light L is obtained using the detection value characteristic information IF. Therefore, it is possible to measure the divergence angle of the laser light L of high output with a simple configuration.
As shown in
The control device 60 controls the NA adjusting device 61 while referring to the measurement result of the divergence angle measurement device 15 such that the divergence angle of the laser light L does not exceed a preset threshold. Further, if necessary, the control device 60 performs control to lower the output of the laser light source 11 (or control to stop the laser light source 11), or performs to issue an alarm, according to the measurement result of the divergence angle measurement device 15.
The NA adjusting device 61 is configured to adjust the numerical aperture (NA) of the laser light L propagated in the delivery fiber 12.
When the plurality of tension members TM move away from one another along the arrow direction of
As described above, in one or more embodiments, the control device 60 and the NA adjusting device 61 are provided to enable adjustment of the divergence angle of the laser light L propagated in the delivery fiber 12 and the like. However, it is similar to one or more embodiments described above in that the second photodetector 32 that detects the Rayleigh scattered light of the laser light L propagated in the delivery fiber 12 and the first photodetector 31 that detects cladding light which has been removed by the cladding light removal portion 13 are provided. Therefore, since the calculation unit 33 obtains the divergence angle of the laser light L, according to the detection results of the first and second photodetectors 31, 32, it is possible to measure the divergence angle of the laser light L of high output with a simple configuration, as in one or more embodiments described above.
Similar to the laser light source 11 shown in
The combiner 72 optically couples a plurality of beams of laser light launched from the plurality of laser apparatuses 71. Specifically, in the inside of the combiner 72, the optical fibers FB extending from the laser apparatuses 71 are bundled, and integrated by melt elongated to form a single optical fiber. The integrated single optical fiber is fusion-spliced to the first end 12a of the optical fiber F which is the delivery fiber 12. Like the optical fiber F in one or more embodiments, an optical fiber for guiding the light combined by the combiner 72 (combining device) is referred to as a launching fiber.
The configuration of the light launch side rather than the combiner 72 in the laser system LS of one or more embodiments is the same as the configuration of the light launch side rather than the laser light source 11 in the laser apparatus 1 described above. Therefore, as in one or more embodiments, the calculation unit 33 obtains the divergence angle of the laser light L, according to the detection results of the second photodetector 32 that detects the Rayleigh scattered light of the laser light L propagated in the delivery fiber 12 (launching optical fiber) and the detection results of the first photodetector 31 that detects cladding light which has been removed by the cladding light removal portion 13.
Therefore, it is possible to measure the divergence angle of the laser light L of high output with a simple configuration.
Although one or more embodiments of the present invention have been described above, the present invention is not limited to the above-described embodiments, and can be freely changed within the scope of the present invention. For example, in the above embodiments, the divergence angle of the laser light L propagated in the optical fiber F is measured. However, for example, the divergence angle of the laser light L propagated in the optical fiber may be measured by each of the laser apparatuses 71 provided in the laser system LS of one or more embodiments described above. Thus, it is possible to specify one of the laser apparatus 71 in which the divergence angle of the laser light L has increased.
Further, in one or more embodiments, the example in which the divergence angle measurement device 15 is provided farther on the light launch side than the combiner 72 has been described. However, the divergence angle measurement device 15 may be provided farther on the light input side than the combiner 72, and the divergence angle of the laser light propagated in the optical fiber FB may be measured. Further, at least one of the first or second photodetectors 31, 32 provided in the divergence angle measurement device 15 may be provided farther on the light input side than the combiner 72, and the other may be provided farther on the light launch side than the combiner 72. For example, the first photodetector 31 may be provided farther on the light input side than the combiner 72, and the second photodetector 32 may be provided farther on the light launch side than the combiner 72.
Further, in one or more embodiments, the cladding light removal portion 13 has a structure provided with the coating removal area 21 in which the coating CV of the at least a part of the optical fiber F in the circumferential direction is removed. However, two optical fibers may be fused to each other, and a fusion-spliced point may be used as the cladding light removal portion 13. Further, in one or more embodiments described above, the second photodetector 32 is configured to detect Rayleigh scattered light of the laser light L propagated in the delivery fiber 12. However, the second photodetector 32 may be configured to detect laser light reflected by a slant type FBG formed in the core of the delivery fiber 12, for example.
Further, the divergence angle measurement devices 15, 40, 50 of the present invention are applicable to laser apparatuses other than the laser apparatuses 1 to 4 according to one or more embodiments described above. For example, the divergence angle measurement devices 15, 40, 50 may be applied to a fiber laser apparatus. Alternatively, they may be applied to a laser apparatus in which the oscillator is configured with those other than an optical fiber and the laser light launched from the oscillator is coupled on the optical fiber, such as a semiconductor laser (DDL: Direct Diode Laser) or a disk laser.
In addition, the specific description about the shape, dimension, arrangement, and material of each component of the laser apparatuses is not limited to the embodiments and can be suitably changed. For example, although the example in which the double cladding fiber is used as an optical fiber is shown in the above embodiments, a single cladding fiber may be used.
Although the disclosure has been described with respect to only a limited number of embodiments, those skilled in the art, having benefit of this disclosure, will appreciate that various other embodiments may be devised without departing from the scope of the present invention. Accordingly, the scope of the invention should be limited only by the attached claims.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2017-059779 | Mar 2017 | JP | national |
This is a U.S. National Stage application of International Application No. PCT/JP2018/009628 filed on Mar. 13, 2018, which claims priority to Japanese Patent Application No. 2017-059779 filed on Mar. 24, 2017. These references are incorporated herein by reference in their entirety.
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/JP2018/009628 | 3/13/2018 | WO | 00 |
