JP6014619B2 - Optical line switching device and optical line switching method - Google Patents

Description

  INDUSTRIAL APPLICABILITY The present invention is applied when switching a line in a troubled transfer work of an optical communication line, etc., and an optical communication line is fixed by fixing a probe for a detour path on the side of an existing optical fiber and combining an amplifier. The present invention relates to an optical line switching device and an optical line switching method.

  In an optical communication system using an optical line using an optical fiber cable, a line switching work is performed in which a working optical line is cut and connected to a new line. As an optical line switching technique that has already been proposed, an optical fiber cable switching connection system aimed at shortening the borrowing time and the switching work period (see, for example, Patent Document 1).

  However, there is a concern that the system proposed by the technique proposed above is unstable when receiving upstream light from an optical network unit (ONU (Optical Network Unit)) because it is a very weak signal.

JP 2012-252099 A

  An object of the present invention is to provide a more stable optical line switching device and optical line switching method that can obtain sufficient optical coupling efficiency between an existing optical fiber and a probe optical fiber.

  In order to achieve the above object, an optical line switching apparatus according to the present invention is an existing optical line that communicates optical signals between an optical line terminator (ONU) and a first optical subscriber line terminator (OLT). Is an optical line switching device for switching to a new optical line connecting a new second OLT, leaking an optical signal from the existing optical line, and all the optical signals of the existing optical line are radiated A first bend having a bend radius greater than a limit bend radius; and a second bend located on the first OLT side of the first bend and steeper than the first bend And one end of the first OLT or the second OLT connected to the detouring optical path that bypasses the existing optical path, and the other end is at a position where the maximum curvature of the first bent portion is reached. A first probe coupled to receive an upstream optical signal from the ONU; One end is connected to the detour line, and the other end is coupled to a position where the second bending portion has the maximum curvature, and the downstream optical signal from the first OLT or the second OLT is received by the second OLT. And a second probe capable of emitting light at the bent portion.

  According to this configuration, two bends are formed in the existing optical line, and the bending radius of the bent part on the ONU side of the two bends is set to be a limit at which all the optical signals of the existing optical line are radiated. The bending radius is larger than the bending radius, the bending portion located on the first or second OLT side is steep, the first probe is coupled to the position where the maximum curvature of the first bending portion is obtained, and the second bending portion By connecting the second probe to a position where the maximum curvature of the optical signal is obtained, an optical signal from the existing optical line to the probe is obtained at an optical signal input / output point between the existing optical line and the probe, which has been conventionally one place. By separating the output point and the optical signal input point from the probe to the existing optical line, sufficient optical coupling efficiency between the existing optical line and the probe, even when applied to a short break switch Is obtained. Further, by forming a gentle bend on the ONU side, a weak optical signal from the ONU can be coupled to the detour optical line with high efficiency, and a more stable optical line switching work can be performed. Furthermore, the upstream optical signal that has passed through the existing optical line is sufficiently blocked by the steep bent portion, and the influence of signal interference can be reduced.

One aspect of the optical line switching device according to the present invention includes the following aspects.
The first aspect includes a first amplifier that amplifies an upstream optical signal received by the first probe to a signal level necessary for transmitting the detour optical line, and the first OLT or the first OLT. A second amplifier that amplifies the downstream optical signal from the second OLT to a signal level necessary for the second probe to emit the second optical signal to the second bent portion, and the upstream optical signal and the downstream optical signal. And a WDM coupler for multiplexing or demultiplexing.

  According to the first aspect, the upstream optical signal output by the gentle bending portion is extracted by the first probe, and is immediately amplified to a signal level necessary for transmitting the detour optical line by the first amplifier. The Further, since the downstream optical signal input at the steep bent portion is sufficiently amplified by the second amplifier, the ONU can receive light even if the loss at the gentle bent portion is subtracted.

In order to increase the coupling efficiency between the first or second probe and the first or second bent portion of the existing optical line, the second aspect is as the first or second probe, Any one of a probe having a condensing property, a lens fiber, and a probe having a condensing lens on the coupling side with the existing optical line is used.
According to the 2nd aspect, the coupling efficiency of the 1st or 2nd probe and the 1st or 2nd bending part of the existing optical line can be raised.

  In a third aspect, the first or second amplifier is any one of an electric signal amplifier, an optical fiber amplifier, and a semiconductor amplifier that amplifies the signal level of the electric signal.

In a fourth aspect, when the core diameter of the light receiving end of the first probe is d1, the core diameter of the exit end of the second probe is d2, and the core diameter of the existing optical line is d0, The core diameter d1 of the light receiving end of the first probe is set to be equal to or larger than the core diameter d0 of the existing optical line, and the core diameter d2 of the emitting end of the second probe is set to be equal to or smaller than the core diameter d0 of the existing optical line. To do.
According to the 4th aspect, the condensing power of the whole optical line switching apparatus can be improved.

In a fifth aspect, the first probe is a probe having a core diameter larger than the core diameter d1.
According to the fifth aspect, the light receiving coupling efficiency can be further increased.

  In order to achieve the above object, an optical line switching method according to the present invention includes an existing optical line that communicates optical signals between an optical line terminator (ONU) and a first optical subscriber line terminator (OLT). Is an optical line switching method for switching to a new optical line that connects a new second OLT, in which an optical signal is leaked from the existing optical line to the existing optical line, Forming a first bend having a bend radius larger than a limit bend radius from which all optical signals are emitted, and being located on the first OLT side from the first bend, compared to the first bend; Then, a steep second bent portion is formed, and one end of the first probe capable of receiving the upstream optical signal from the ONU is coupled to the position where the maximum curvature of the first bent portion is obtained, and the first Connect the other end of one probe to the first OLT or the second OLT. The downstream optical signal from the first OLT or the second OLT is connected to a detour optical path that detours the existing optical line, and the first OLT or the second OLT is placed at a position where the maximum curvature of the second bent portion is reached. One end of the second probe capable of emitting light is coupled to the second bent portion, and the other end of the second probe is connected to the detour line.

  According to the present invention, a weak signal from the ONU is coupled to the detour optical line with high efficiency, thereby enabling more stable optical line switching work. Moreover, it becomes possible to improve the optical coupling efficiency of the short interruption switching system in an optical line.

The figure which shows the OLT switching procedure using the optical side entrance / exit technique as the 1st Embodiment of this invention. Similarly, the figure which shows the OLT switching procedure using the optical side entrance / exit technique. Similarly, the figure which shows the OLT switching procedure using the optical side entrance / exit technique. Similarly, the figure which shows the OLT switching procedure using the optical side entrance / exit technique. The figure which shows the detour optical path | route connected to the test port of old OLT as the 2nd Embodiment of this invention. The figure which shows the wavelength dependence of coupling efficiency as the 3rd Embodiment of this invention. The block lineblock diagram of the optical line switching device by the optical side input-output technology using gentle bending and steep bending as a 4th embodiment of the present invention. The figure for demonstrating the S-shaped optical side input / output part in the said 4th Embodiment. The figure for demonstrating the definition of a bending as the 5th Embodiment of this invention. The figure which shows the bending radius and bending angle dependence of the bending loss and the coupling loss in wavelength 1550nm in the said 5th Embodiment. The figure which shows the bending radius and bending angle dependence of the bending loss and the coupling loss in wavelength 1310nm in the said 5th Embodiment. The figure which shows the bending radius dependence of the fracture | rupture probability in the said 5th Embodiment. The figure which shows the structural example of the amplifier in the 7th Embodiment of this invention. The figure which shows the structural example of the amplifier in the 8th Embodiment of this invention. The figure which shows the structural example of the amplifier in the 9th Embodiment of this invention. The figure which shows an example of a structure of the probe for downstream light in the 11th Embodiment of this invention. The figure which shows the other example of a structure of the probe for downstream light in the said 11th Embodiment. The figure which shows an example of a structure of the probe for upstream light in the said 11th Embodiment. The figure which shows the other example of a structure of the probe for upstream light in the said 11th Embodiment.

  Prior to describing an embodiment according to the present invention, an optical fiber side input / output technique will be described.

  Optical fiber side input / output technology is a technology to bend an existing optical fiber and abut another optical fiber (probe optical fiber) from the side to the bent part to input / output an optical signal. Application to test light incident for core wire contrast, short break switching system related to path change of optical line, and the like are being studied. In this case, the existing optical fiber is sandwiched between a cylindrical rigid body (block 1) and a transparent rigid body (block 2) having a concave curved surface corresponding to the cylindrical shape of block 1, and is emitted from the working optical fiber to the concave curved surface of block 2. A side input / output device for receiving a received optical signal with a probe fiber disposed in the block 2 has been proposed.

  By the way, in recent years, a countermeasure for obtaining sufficient optical coupling efficiency between an existing optical fiber and a probe optical fiber is strongly desired in application to a short break switch.

Therefore, the present invention relates to an optical signal input / output point between the existing optical fiber and the probe optical fiber, which has conventionally been one place, an optical signal output point from the existing optical fiber to the probe optical fiber, By separating the optical signal input point to the optical signal input point, it is possible to obtain sufficient optical coupling efficiency between the existing optical fiber and the probe optical fiber even when applied to a short break switch. is there.
Based on the above optical fiber side input / output technology, embodiments of the present invention will be described below.

(First embodiment)
FIG. 1 to FIG. 4 show the procedure of optical subscriber line termination equipment (OLT (Optical Line Terminal)) switching using optical side input / output technology and new optical line installation work necessary for OLT switching. .

  First, before the construction, the construction worker confirms that the OLT (former OLT) 21 and the ONU 1 of the station 2 are connected by the test port 22 and the optical cable # 1 using the conventional technology (FIG. 1 (1)). ). Next, the OLT (new OLT) 31 of the station 3 to be switched, the detour optical line # 2, and the new optical line # 3 are prepared (FIG. 1 (2)). In addition, the builder connects both ends of the detour optical line # 2 to the optical line switching device 10 and the test port 32 of the new OLT 31 in the station 3, and installs the optical line switching device 10 at the switching point of the working optical line # 1. To do. Further, the construction engineer synchronizes the optical signals of the OLT (old OLT) 21 before the transfer and the OLT (new OLT) 31 to be transferred.

  Subsequently, the worker bends the optical fiber of the working optical line # 1 in the optical line switching device 10 (FIG. 2 (1)). Due to the bending of the optical fiber, the signal from the old OLT 21 is cut off because a loss occurs at the bent portion. At the same time, communication between the new OLT 31 and the ONU 1 is started by inputting / outputting an optical signal from the probe of the optical line switching device 10 to the optical fiber bending portion of the working optical line # 1. At this time, since the optical signal intensity at the bent portion is reduced, an amplifier corresponding to wavelengths 1.31, 1.49, 1.55 μm is installed in the optical line switching device 10 in advance, so that communication between the new OLT 31 and the ONU 1 is stabilized. Done.

  Next, after confirming communication from the new OLT 31, the construction worker stops the signal of the old OLT 21 (FIG. 2 (2)).

  The installer then connects the new optical line # 3 and the working optical line # 1 (FIG. 3 (1)). At this time, since the communication between the new OLT 31 and the ONU 1 is performed by the bypass optical line # 2, the communication service to the customer is continued, and the connection between the working optical line # 1 and the new optical line # 3 is normal. It can be implemented by construction.

  Next, the contractor removes the signal via the detour optical line # 3 by opening the optical fiber bend in the optical line switching device 10, and communication between the new OLT 31 and the ONU 1 is started by the new optical line # 3. , OLT 21, 31 is completely replaced (FIG. 3 (2)).

  Finally, the builder removes the optical line switching device 10, the detour optical line # 2, and the old OLT 21 to complete the construction (FIG. 4).

  As described above, it is understood that the service interruption time to the customer can be a momentary interruption that occurs when the optical fiber is bent and when the bending is released by performing the optical line switching work using the optical line switching device 10 by the worker.

(Second Embodiment)
The detour optical line # 2 shown in the first embodiment may be prepared by connecting to the test port 22 of the old OLT 21 as shown in FIG.

  In this case, the builder connects both ends of the bypass optical line # 2 to the optical line switching device 10 and the test port 22 of the old OLT 21 of the station 2, and the optical line switching device 10 is used as a switching point of the working optical line # 1. Install. Further, the construction engineer synchronizes the optical signals of the OLT (old OLT) 21 before the transfer and the OLT (new OLT) 31 to be transferred.

  Subsequently, the worker bends the optical fiber of the working optical line # 1 in the optical line switching device 10. Due to the bending of the optical fiber, the signal from the old OLT 21 is cut off because a loss occurs at the bent portion. At the same time, communication between the old OLT 21 and the ONU 1 is continued by inputting / outputting an optical signal from the probe of the detour optical line # 2 of the optical line switching device 10 to the optical fiber bending part of the working optical line # 1. At this time, since the optical signal intensity at the bent portion is reduced, an amplifier corresponding to wavelengths 1.31, 1.49, and 1.55 μm is installed in the optical line switching device 10 in advance, so that the old OLT 21 and the ONU 1 are routed via the detour optical line # 2. Communication with is performed stably.

  The installer then connects the new optical line # 3 and the working optical line # 1. At this time, since the communication between the old OLT 21 and the ONU 1 is performed by the bypass optical line # 2, the communication service to the customer is continued, and the connection between the working optical line # 1 and the new optical line # 3 is normal. It can be implemented by construction.

  Next, the contractor removes the signal via the detour optical line # 3 by opening the optical fiber bend in the optical line switching device 10, and communication between the new OLT 31 and the ONU 1 is started by the new optical line # 3. , OLT 21 and 31 are completely accommodated.

  Finally, the builder removes the optical line switching device 10, the detour optical line # 2, and the old OLT 21 to complete the construction.

(Third embodiment)
FIG. 6 shows the trend of wavelength dependence of communication light. In FIG. 6, the horizontal axis indicates the wavelength of communication light, and the vertical axis indicates the coupling efficiency.

  The amount of communication light leaked from the bent optical fiber depends on the wavelength of the communication light. Of the 1.31 μm, 1.49 μm, and 1.55 μm used in current communications, 1.31 μm on the short wavelength side has the least light leakage, and coupling efficiency is difficult to obtain. On the other hand, since 1.55 μm on the long wavelength side is likely to leak, the coupling efficiency is large.

  In view of the performance of the amplifier, if it is possible to amplify a wavelength of 1.31 μm, which is difficult to leak, to a desired intensity, switching work by bending the optical fiber at only one place can be performed. In the fourth embodiment, an apparatus and method for compensating for weak light intensity with a wavelength of 1.31 μm when the amplifier gain is insufficient will be described.

(Fourth embodiment)
FIG. 7 shows a configuration of the optical line switching device 10. The optical line switching device 10 includes a bending portion 11 that gently bends the optical fiber of the working optical line # 1, an upstream light probe 14 that receives light leaking from the gentle bending portion 11, and the received upstream light. An amplifying device 16, a bending portion 12 for sharply bending the optical fiber of the working optical line # 1, a downstream light probe 13 for entering downstream light at the steep bending portion 12, and amplifying the downstream light And a wavelength division multiplexing (WDM) coupler 17 for multiplexing or demultiplexing upstream light and downstream light. The working optical line # 1 is merely bent by the optical line switching device 10, and the bypass optical line # 2 is connected to the WDM coupler 17.

  For example, as shown in FIG. 8, the bending portion of the optical line switching apparatus 10 includes an S-shaped bending convex portion 41 and an optical glass material in which a downstream light probe 13 is embedded in an optical glass material and requires gentle bending and steep bending. S-shaped bending concave portion 42 that needs to bend gently and steeply is embedded, and the optical fiber is pushed and bent by the S-shaped bending convex portion 41 and the S-shaped bending concave portion 42. It is the bending part 40 comprised by a character-shaped optical side input / output part.

  The characteristics of the gentle bend 11 and the steep bend 12 in FIG. 7 will be described. For the gentle bending portion 11, the intensity of the upstream light leaking from the bending portion 11 satisfies the minimum light receiving sensitivity of the bending amplifier 16, and the downstream light incident from the new OLT 31 side has the minimum light receiving intensity of ONU1. It is a bent part that satisfies the sensitivity. Next, with respect to the steep bent portion 12, the bent portion 12 has such a steep degree that the optical fiber is not broken.

(Fifth embodiment)
(Details about two bends)
An example of specific numerical values for the two bent portions 11 and 12 of the fourth embodiment is shown in the fifth embodiment. As shown in FIG. 9, the bending portions 11 and 12 are defined by a bending radius R and a bending angle θ. Further, regarding the tightness of bending, the larger the R and θ, the smaller the bending strength, and the smaller R and θ, the larger the bending strength.

  FIG. 10 shows, for example, the bending radius and bending angle dependence of bending loss and coupling loss at a wavelength of 1550 nm. In FIG. 10, the horizontal axis represents the bending loss at a wavelength of 1550 nm, and the horizontal axis represents the coupling loss at a wavelength of 1550 nm.

  Similarly, FIG. 11 shows the bending radius and bending angle dependence of bending loss and coupling loss at a wavelength of 1310 nm. In FIG. 10, the horizontal axis represents bending loss at a wavelength of 1310 nm, and the horizontal axis represents coupling loss at a wavelength of 1310 nm.

  For example, in the downstream light (wavelength 1550 nm) from the OLTs 21 and 31, the light intensity amplified by the amplifiers 15 and 16 of the optical line switching device 10 is 20 dBm, and the coupling efficiency in the steep bend 12 of the optical line switching device 10 Is -20 dB, the splitter branching loss is 10 dB, and the minimum light receiving sensitivity of the ONU 1 is -12 dBm, the bending loss allowed in the gentle bending portion 11 is 2 dB. From FIG. 10, for example, (R, θ) is (3 mm). 150 °).

  Further, in the upstream light (wavelength 1310 nm) leaking from the ONU 1 leaking at the gentle bent portion 11, the upstream light intensity from the ONU 1 is −1 dBm, the minimum light receiving sensitivity of the amplifier 16 of the optical line switching device 10 is −33 dBm, and the splitter. When the branching loss is 10 dB, the coupling efficiency in the gentle bending portion 11 of the optical line switching device 10 must be −22 dB or more. Therefore, from FIG. 11, for example, (R, θ) may be (3 mm, 150 °).

  As described above, in the bending strength of the gentle bending portion 11, the upper limit is limited by the bending loss of downstream light, and the lower limit is limited by the coupling efficiency of upstream light.

FIG. 12 shows the dependence of the optical fiber breakage probability on the bending radius. In FIG. 12, the horizontal axis represents the bending radius of the optical fiber, and the vertical axis represents the breaking probability and coupling efficiency of the optical fiber. When the allowable breaking probability of the optical fiber bent by the optical line switching device 10 is 10 ⁻⁶ or more, for example, R may be 1.7 mm or more. Further, in the above optical characteristics, when the required coupling efficiency at the steep bending portion 12 of the optical line switching device 10 is −20 dB, and the downstream light blocking loss (corresponding to the bending loss) to the ONU 1 is −30 dB. From FIG. 10, for example, (R, θ) may be (2 mm, 90 °).

  As described above, in the bending stiffness of the steep bent portion 12, the upper limit is limited by the breaking probability of the optical fiber, and the lower limit is limited by the coupling efficiency and the cutoff loss.

(Sixth embodiment)
(About two bending positions)
The two bending positions in FIG. 7 will be described. As for the bending position, it is necessary to form a steep bent portion 12 and a gentle bent portion 11 on the basis of the old OLT 21 side. If the gentle bend 11 on the ONU ₁ side is R ₁ and the steep bend 12 on the OLT 21 side is R ₂ ,
R ₁ ≧ R ₂
It becomes.

Also, let R _lim be the bending radius at which all the optical signals of the working optical line # 1 are radiated
R ₁ > R _lim
It becomes.

  As described above, the light output section and the input section can be separated. Due to the gentle bending portion 11, the output upstream light is extracted by the upstream light probe 14 having high coupling efficiency, and the signal intensity in the detour optical line # 2 is immediately made sufficient by the amplifier 16. Further, the upstream light that has passed through the working optical line # 1 is sufficiently blocked by the steep bend 12 to reduce the influence of signal interference. Downstream light input at the steep bent portion 12 is sufficiently amplified immediately before, and can be received by the ONU 1 even if a loss at the gentle bent portion 11 is subtracted.

  If the position is reversed, the intensity of downstream light incident from the new OLT 31 side does not satisfy the minimum light receiving sensitivity of the ONU 1.

(Seventh embodiment)
(Configuration of amplifier)
FIG. 13 shows an example of the configuration of the upstream light amplifier 16. In FIG. 13, the probe 51 corresponds to the upstream light probe 14 in FIG. 7, and the amplifier 52 corresponds to the amplifier 16 in FIG. First, the leaked light coupled to the probe 51 is received by the PD 521 and converted into an electrical signal. Next, the amplification unit 522 amplifies the electric signal by a predetermined amplitude level. The output signal of the amplifying unit 522 is converted again into an optical signal by the LD 523 and transmitted to the OLT 31 side. Further, the configuration of the downstream light amplifier 15 may be the same as that of the upstream light amplifier 16, and it is sufficient that the light transmitted from the OLT 31 side is amplified.

(Eighth embodiment)
As the amplifier described in the seventh embodiment, for example, an optical fiber amplifier may be used as shown in FIG. In FIG. 14, a probe 61 corresponds to the upstream light probe 14 in FIG. 7, and an amplifier 62 corresponds to the amplifier 16 in FIG.

  First, the leaked light coupled to the probe 61 is received by the light receiving unit 621 and mixed with the light emitted from the light emitting element 622 by the optical multiplexer 623. The output light of the optical multiplexer 623 is amplified to output light of an output level necessary for transmission to the OLT 31 by the amplification unit 624 and transmitted to the OLT 31 side by the light sending unit 625.

  Further, the configuration of the downstream light amplifier 15 may be the same as that of the upstream light amplifier 16, and it is sufficient that the light transmitted from the OLT 31 side is amplified.

(Ninth embodiment)
As the amplifier described in the seventh embodiment, for example, a semiconductor amplifier may be used as shown in FIG. In FIG. 15, a probe 71 corresponds to the upstream light probe 14 in FIG. 7, and an amplifier 72 corresponds to the amplifier 16 in FIG.

  First, the leaked light coupled to the probe 71 is received by the semiconductor element 721 of the amplifier 72 and converted into an electrical signal. Next, the semiconductor element 721 amplifies the electric signal by a predetermined amplitude level, converts the amplified electric signal again into an optical signal, and transmits the optical signal to the OLT 31 side. Further, the configuration of the downstream light amplifier 15 may be the same as that of the upstream light amplifier 16, and it is sufficient that the light transmitted from the OLT 31 side is amplified.

(Tenth embodiment)
For example, in the case of the downstream light from the OLT 31, the amplifier described in the seventh embodiment demultiplexes wavelengths of 1490 nm and 1550 nm by the WDM coupler 17, and the seventh embodiment, the eighth embodiment, or the ninth embodiment, respectively. The amplifier described in the embodiment may be used. When a downstream optical signal having wavelengths of 1490 nm and 1550 nm is coupled from the downstream optical probe 13 to the steep bent portion 12, the optical signal is reduced at the time of coupling. Therefore, the optical signal is attenuated by increasing the intensity of the optical signal by the amplifier 15. You can make up for the minute.

(Eleventh embodiment)
(Characteristics of the probe)
The upstream light probe 14 from the ONU 1 will be described. As shown in FIG. 16, upstream light leaking radially is received by a large-diameter core fiber 81 and a signal is sent to an amplifier 82. As the large-diameter core fiber 81 used here, for example, a commercially available GI fiber or a fiber having a larger diameter is used. When the core diameter is d, for example, d is 50 μm, 62.5 μm, or 200 μm. The normally used upstream light probe 14 is a single mode fiber, and has a core diameter of 10 μm, for example. Further, the probe may use a condensing lens 91 as shown in FIG.

Next, the downstream light probe 13 will be described. As shown in FIG. 18, a GRIN lens fiber 1001 is used so that light can be coupled to the core of the optical fiber bent by narrowing the light. When the beam waist diameter 2ω ₀ of the GRIN lens fiber 1001 to be used is, for example, 17 μm or more and 35 μm or less, the coupling efficiency for receiving light by the ONU 1 can be obtained.

  Further, the GRIN lens fiber 1001 may use a condenser lens 2001 as shown in FIG. By doing so, the coupling efficiency between the GRIN lens fiber 1001 and the steep bent portion 12 can be increased.

(Operational effects of the first to eleventh embodiments)
According to each of the above embodiments, the two bent portions 11 and 12 are formed in the existing working optical line # 1, and the bending radius of the bent portion 11 on the ONU1 side among the two bent portions is set to the working optical line # 1. A bending radius larger than the limit bending radius from which all the optical signals of 1 are emitted, the bending portion 12 located on the old OLT 21 side is steep, and the upstream light probe 14 is coupled to a position where the bending portion 11 has the maximum curvature, The downstream light probe 13 is coupled to a position where the bending portion 12 has the maximum curvature.

  That is, with respect to the optical signal input / output point between the working optical line # 1 and the probe, which has conventionally been one place, the optical signal output point from the working optical line # 1 to the upstream optical probe 14 and the downstream optical probe 13 Even if it is applied to a short interruption switch by separating the optical signal input point to the working optical line # 1, the working optical line # 1, the downstream light probe 13, and the upstream light probe 14 are connected. Sufficient optical coupling efficiency can be obtained.

  In addition, by forming the gentle bent portion 11 on the ONU 1 side, a weak optical signal from the ONU 1 can be coupled to the bypass optical line # 2 with high efficiency, and a more stable optical line switching work can be performed. Furthermore, the upstream optical signal that has passed through the working optical line # 1 is sufficiently blocked by the steep bend portion 12, and the influence of signal interference can be reduced.

(Other embodiments)
In the first to tenth embodiments, the core diameter of the light receiving end of the upstream light probe 14 is d1, the core diameter of the outgoing end of the downstream light probe 13 is d2, and the core diameter of the working optical line # 1 is d0. In this case, the core diameter d1 of the light receiving end of the upstream light probe 14 is set to be equal to or larger than the core diameter d0 of the working optical line # 1, and the core diameter d2 of the emitting end of the downstream light probe 13 is set to that of the working optical line # 1. You may make it set it as core diameter d0 or less. Here, a single mode fiber is used for the upstream light probe 14.
By doing in this way, the condensing power of the whole optical line switching apparatus 10 can be improved.

  In short, the present invention is not limited to the above-described embodiment as it is, and can be embodied by modifying the constituent elements without departing from the scope of the invention in the implementation stage. Further, various inventions can be formed by appropriately combining a plurality of constituent elements disclosed in the embodiment. For example, some components may be deleted from all the components shown in the embodiment. Furthermore, you may combine suitably the component covering different embodiment.

  DESCRIPTION OF SYMBOLS 1 ... ONU, 2, 3 ... Station, 10 ... Optical-line switching apparatus, 11, 12 ... Bending part, 13 ... Downlink probe, 14 ... Uplink probe, 15, 16 ... Amplifier, 17 ... WDM coupler, 21, 31 ... OLT, 22, 32 ... test port, 40 ... bent part, 41 ... S-shaped bent convex part, 42 ... S-shaped bent concave part, 51 ... probe, 52 ... amplifier, 61 ... probe, 62 ... amplifier 71 ... probe 72 ... amplifier 81 ... large diameter core fiber 82 ... amplifier 91 ... condensing lens 521 ... PD 522 ... amplifier unit 523 ... LD 621 ... light receiving unit 622 ... light emitting element 623... Optical multiplexer, 625... Optical sending part, 721... Semiconductor element, 1001... GRIN lens fiber, 2001.

Claims (8)

The existing optical line that communicates optical signals between the optical line terminator (ONU) and the first optical subscriber line terminator (OLT) is switched to a new optical line that connects the new second OLT. An optical line switching device,
A first bent portion having a bending radius larger than a limit bending radius at which an optical signal is leaked from the existing optical line and all the optical signals of the existing optical line are emitted;
A second bend located on the first OLT side of the first bend and steeper than the first bend;
One end is connected to the detour optical line that connects the first OLT or the second OLT and bypasses the existing optical line, and the other end is coupled to a position where the maximum curvature of the first bent portion is obtained. A first probe capable of receiving an upstream optical signal from the ONU;
One end is connected to the detour line, the other end is coupled to a position where the second bending portion has the maximum curvature, and the downstream optical signal from the first OLT or the second OLT is transmitted to the second OLT. An optical line switching device comprising: a second probe capable of emitting light to the bent portion. A first amplifier that amplifies the upstream optical signal received by the first probe to a signal level necessary to transmit the detour optical line;
A second amplifier for amplifying a downstream optical signal from the first OLT or the second OLT to a signal level necessary for the second probe to emit the second bent portion to the second bent portion;
2. The optical line switching apparatus according to claim 1, further comprising a wavelength division multiplexing (WDM) coupler for multiplexing or demultiplexing the upstream optical signal and the downstream optical signal.   3. The optical line switching device according to claim 1, wherein the second bent portion is a steep bend in which a bending loss is optically larger than that of the first bent portion.   In order to increase the coupling efficiency between the first or second probe and the first or second bent portion of the existing optical line, the first or second probe has a light collecting property, 4. The optical line switching device according to claim 1, wherein any one of a lens fiber and a probe having a condensing lens on a coupling side with the existing optical line is used. 5.   The first or second amplifier is any one of an electric signal amplifier, an optical fiber amplifier, and a semiconductor amplifier that amplifies a signal level of an electric signal. The optical line switching device according to item.   When the core diameter of the light receiving end of the first probe is d1, the core diameter of the emitting end of the second probe is d2, and the core diameter of the existing optical line is d0, the light receiving of the first probe is received. The core diameter d1 at the end is made larger than the core diameter d0 of the existing optical line, and the core diameter d2 at the emission end of the second probe is made smaller than the core diameter d0 of the existing optical line. The optical line switching apparatus of any one of Claims 1 thru | or 5.   The optical line switching device according to claim 6, wherein the first probe is a probe having a core diameter larger than the core diameter d1. The existing optical line that communicates optical signals between the optical line terminator (ONU) and the first optical subscriber line terminator (OLT) is switched to a new optical line that connects the new second OLT. An optical line switching method,
Leaking an optical signal from the existing optical line to the existing optical line, and forming a first bending portion having a bending radius larger than a limit bending radius at which all the optical signals of the existing optical line are radiated;
A second bend that is located closer to the first OLT than the first bend and is sharper than the first bend;
One end of the first probe capable of receiving the upstream optical signal from the ONU is coupled to the position where the maximum curvature of the first bending portion is obtained,
The other end of the first probe is connected to a detour optical path that bypasses the existing optical path connecting the first OLT or the second OLT,
One end of a second probe capable of emitting a downstream optical signal from the first OLT or the second OLT to the second bent portion is coupled to the position where the maximum curvature of the second bent portion is obtained. ,
An optical line switching method, wherein the other end of the second probe is connected to the detour line.

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