JP5682677B2 - Optical amplifier and optical amplification method - Google Patents

Description

  The present invention relates to an optical amplifier and an optical amplification method. The optical amplification method can be used, for example, in an optical amplifier capable of optically amplifying signal light with excitation light.

With the development of multimedia networks, the demand for communication traffic has increased dramatically.
For this reason, for example, an optical transmission system in which wavelength multiplexed signal light (WDM (Wavelength Division Multiplexing) light) is optically amplified by an optical amplifier using EDF (Erbium Doped Fiber) as an amplification medium is transmitted in a multi-media society. It plays a major role in promoting the economics of communication systems in Japan.

Here, since the amplification efficiency of the EDF is large with respect to the input signal light in the C band band (1530 nm to 1570 nm), the C band band is generally used as the wavelength band of the WDM light.
Further, as the wavelength band of the excitation light of the EDF, a 0.98 μm band, which is excellent in noise figure [NF (Noise Figure)] and has been advanced in recent years, may be used.

As a technique relating to the optical amplifier, for example, a configuration in which a variable optical attenuator (VOA) is provided between a preceding optical amplifying unit (for example, EDF) and a subsequent optical amplifying unit (for example, EDF). It has been known.
For example, in Patent Document 1 below, the attenuation amount of the variable optical attenuator is controlled so that the output level of each of the front stage side gain control unit and the rear stage side gain control unit becomes a constant level, while the device input level or dispersion compensation is controlled. In order to distribute the attenuation amount so that the noise figure is optimal to the plurality of variable optical attenuators when the interstage loss amount varies due to the gain, the gain is applied to each of the second optical amplification unit and the fourth optical amplification unit. An optical amplifier is described in which a target value is set and the gain sum from the first optical amplification unit to the fourth optical amplification unit is controlled to be constant.

  Further, in Patent Document 2 below, signal light is amplified by an Al-added EDF supplied with pumping light output from a pumping laser light source, then attenuated by a variable optical attenuator, and further, pumping laser light source The P / Al co-doped EDF and the optical fiber amplifier that is amplified by the Al-doped EDF are described. By adding Al to the EDF, erbium can be evenly dispersed without crystallizing, and the strong emission band (1.55 μm band) in the C-band band can be expanded. Further, by adding P to the EDF, the amplification band in the L-band band can be expanded.

JP 2003-258346 A Japanese Patent Laid-Open No. 10-144984

In the optical amplifier described above, the total power of signal light (for example, WDM light) input to and output from each of the upstream and downstream EDFs is monitored, and the amplification gain in each EDF is controlled to be constant based on the monitoring results [AGC (Auto Gain Control)].
Further, by changing the attenuation amount of the VOA provided between the EDFs in accordance with the fluctuation of the input level of the signal light, the predetermined output level is maintained while maintaining the flatness of the output wavelength characteristic with respect to the fluctuation of the input level. The attenuation amount may be controlled so as to maintain the above.

However, since the AGC control loop exists for each EDF in the above-described optical amplifier configuration, the AGC control delay may appear to be doubled when the wavelength of the input signal light is increased or decreased.
Further, in the above-described optical amplifier configuration, an excitation light source [for example, a laser diode (LD)] is provided for each EDF, which increases the manufacturing cost of the optical amplifier.
Furthermore, the pumping light power required for the pumping light source tends to increase, and the manufacturing cost of the pumping light source may increase.

  As described above, the present invention has an object to reduce the manufacturing cost of an optical amplifier.

(1) As a first proposal, a first excitation light source that outputs excitation light having a first wavelength, and a second excitation light source that outputs excitation light having a second wavelength different from the first wavelength, , A combining unit that combines the output from the first pumping light source and the output from the second pumping light source to output wavelength-multiplexed pumping light, and the wavelength output by the combining unit The amplified input signal light is further amplified using the first rare earth-added medium that amplifies the input signal light using the multiplexed pump light and the residual pump light that is output from the first rare earth-added medium. As the input level of the second rare earth-added medium and the input signal light is higher , the wavelength multiplexing of the second wavelength has a smaller amount of excitation light absorbed in the first rare-earth added medium than the first wavelength. It has been Pas to perform control to increase the definitive power over ratios to the excitation light And over the ratio controller, it is possible to use an optical amplifier equipped with.

  (2) As a second proposal, a first excitation light source that outputs excitation light having a first wavelength and a second excitation that outputs excitation light having a second wavelength different from the first wavelength are used. A light source, a multiplexing unit that combines the output from the first excitation light source and the output from the second excitation light source to output wavelength-multiplexed excitation light, and is output by the multiplexing unit A first rare earth-added medium that amplifies input signal light using the wavelength-multiplexed pump light, and a residual pump light that is output from the first rare earth-added medium, and further amplifies the input signal light that has been amplified. An optical amplification method for an optical amplifier comprising a second rare earth-added medium to be amplified, wherein an input level of the input signal light is monitored, and the higher the monitored input level is, the higher the input wavelength is than the first wavelength. Before the first rare earth-added medium has a small amount of absorption of excitation light The wavelength-multiplexed power ratio at the excitation light of the excitation light of the second wavelength is increased, it is possible to use optical amplification method.

  The manufacturing cost of the optical amplifier can be reduced.

It is a figure which shows an example of a structure of the optical amplifier which concerns on one Embodiment. It is a figure which shows an example of the level diagram of input signal light. It is a figure which shows an example of excitation light absorption amount. It is a figure which shows an example of a structure of the optical amplifier which concerns on one Embodiment. It is a figure which shows an example of the wavelength dependence characteristic of the excitation light absorption amount in EDF. It is a figure which shows an example of the control method which concerns on one Embodiment. It is a figure which shows an example of the level diagram of input signal light. It is a figure which shows an example of excitation light absorption amount. It is a figure which shows an example of the inversion distribution in 1st EDF. It is a figure which shows an example of the inversion distribution in 2nd EDF. It is a figure which shows an example of a structure of the optical amplifier which concerns on a 1st modification. It is a figure which shows an example of the control method which concerns on a 1st modification.

Hereinafter, embodiments will be described with reference to the drawings. However, the embodiment described below is merely an example, and there is no intention to exclude various modifications and technical applications that are not clearly shown in the embodiment described below. That is, the present embodiment can be implemented with various modifications (combining the embodiments and modifications) without departing from the spirit of the present embodiment.
[1] One Embodiment (1.1) Configuration Example of Optical Amplifier 100 FIG. 1 is a diagram illustrating an example of a configuration of an optical amplifier 100 according to an embodiment.

The optical amplifier 100 shown in FIG. 1 exemplarily includes a branching unit 1, a multiplexing unit 2, a first EDF 3, a duplexer 4, a VOA 5, a multiplexer 6, and a second EDF 7. And a branching portion 8. Further, the optical amplifier 100 includes, for example, a gain target value calculation unit 9, a gain error detection unit 10, a power control unit 11, a wavelength fixed pumping LD 12, and a VOA control unit 13.
Here, the branching unit 1 power-branches the input signal light to the optical amplifier 100. For example, an optical branching unit such as an optical coupler (splitter) can be used for the branching unit 1. The input signal light branched in power by the branching unit 1 is distributed to the multiplexing unit 2, the gain target value calculation unit 9, the gain error detection unit 10, and the VOA control unit 13, respectively. The input signal light may be WDM light or single wavelength signal light. Further, the wavelength band of the input signal light can be, for example, a C band band in which the amplification efficiency of the first EDF 3 and the second EDF 7 is large.

The fixed wavelength excitation LD 12 generates and outputs excitation light having a preset fixed wavelength. The excitation light generated and output by the fixed wavelength excitation LD 12 is input to the multiplexing unit 2. Here, the wavelength band of the pumping light can be set to a 0.98 μm band having a large amplification contribution to the input signal light in the C band.
The multiplexing unit 2 combines the input signal light from the branching unit 1 and the excitation light from the fixed wavelength pumping LD 12 and outputs the combined signal light to the first EDF 3. For the multiplexing unit 2, for example, an optical multiplexing unit such as an optical coupler can be used.

  The first EDF 3 is a rare earth-added medium (for example, an optical fiber, a planar lightwave circuit (PLC), etc.) that optically amplifies the input signal light using the excitation light from the fixed wavelength excitation LD 12. For the first EDF 3, for example, a fiber doped with (doped) rare earth ions such as erbium (Er) or thulium (Tm) can be used. Further, the fiber length of the first EDF 3 is such that, for example, a part of the pumping light (residual pumping light) is absorbed in the second EDF 7 in the subsequent stage while absorbing a part of the pumping light generated by the wavelength fixed pumping LD 12. It is preferable that the length is sufficient for output.

  The demultiplexer 4 separates (demultiplexes) the input signal light optically amplified by the first EDF 3 and the excitation light (residual excitation light) output from the first EDF 3. For the duplexer 4, for example, a wavelength selection filter or the like can be used. The signal light demultiplexed by the demultiplexer 4 is output to the path of the VOA 5, while the residual excitation light demultiplexed by the demultiplexer 4 is output to the path that bypasses (avoids) the VOA 5. . Thereby, the signal light can be input to the VOA 5, while the residual excitation light can be input to the second EDF 7 while avoiding the VOA 5.

The VOA 5 attenuates the signal light from the duplexer 4 based on the control by the VOA control unit 13. The signal light attenuated by the VOA 5 is input to the multiplexer 6.
In other words, the VOA 5 is inserted between the first EDF 3 and the second EDF 7 and functions as an example of an optical attenuator that attenuates the input signal light amplified by the first EDF 3.
The duplexer 4 is inserted between the first EDF 3 and the VOA 5 and functions as an example of a duplexer that demultiplexes the residual excitation light and bypasses the VOA 5.

The multiplexer 6 combines the signal light from the VOA 5 and the residual pumping light that bypasses (avoids) the VOA 5 and outputs the combined light to the second EDF 7. For the multiplexer 6, for example, an optical multiplexing unit such as an optical coupler can be used.
That is, the multiplexer 6 is inserted between the VOA 5 and the second EDF 7, and combines the residual excitation light demultiplexed by the demultiplexer 4 and inputs it to the second EDF 7. It serves as an example.

  The second EDF 7 is a rare earth-added medium (for example, an optical fiber, a planar optical waveguide (PLC), etc.) that optically amplifies the signal light using the residual pump light from the multiplexer 6. As the first EDF 7, for example, a fiber doped with (doped) rare earth ions such as erbium (Er) and thulium (Tm) can be used for the second EDF 7. The medium length (for example, fiber length) of the second EDF 7 is longer than the medium length of the first EDF 3 and is long enough to absorb the residual excitation light from the first EDF 3 without leakage. Is preferred.

As illustrated in FIG. 1, the direction of the excitation light in the first EDF 3 and the second EDF 7 in the optical amplifier 100 can be forward excitation.
The branching unit 8 branches the power of the signal light (output signal light) output from the second EDF 7. For the branching unit 8, for example, an optical branching unit such as an optical coupler (splitter) can be used. The output signal light whose power has been branched by the branching unit 8 is output from the optical amplifier 100 while being distributed to the gain error detection unit 10.

  The gain target value calculation unit 9 detects the input level of the input signal light branched by the branching unit 1, and the amplification gain in the optical amplifier 100 based on the detection result and the output level required for the optical amplifier 100. The target value of is calculated. For detection of the input level, for example, various photodetectors such as a photodiode [PD (Photo Diode)] can be used. The gain target value calculated by the gain target value calculation unit 9 is input to the gain error detection unit 10.

  The gain error detector 10 calculates the current amplification gain from the input level of the input signal light branched by the branching unit 1 and the output level of the output signal light branched by the branching unit 8. Then, based on the current amplification gain and the gain target value calculated by the gain target value calculation unit 9, an error between the amplification gain of the optical amplifier 100 for obtaining the required output level and the current amplification gain. (Gain error) is detected. The gain error detected by the gain error detection unit 10 is input to the power control unit 11.

  The power control unit 11 controls the power of the pumping light generated by the wavelength fixed pumping LD 12 based on the gain error detected by the gain error detecting unit 10. For example, when the gain error is positive, the power control unit 11 determines that the current amplification gain is larger than the amplification gain for obtaining the required output level, and reduces the power of the pumping light. To control. On the other hand, when the gain error is negative, the power control unit 11 determines that the current amplification gain is smaller than the amplification gain for obtaining the required output level, for example, and determines the power of the pump light. Control to increase.

Further, the VOA control unit 13 detects a change in the input level of the input signal light branched by the branching unit 1 and controls an attenuation amount (loss) in the VOA 5 based on the detected change in the input level.
The optical amplifier 100 having the above configuration controls the pumping light power based on, for example, the input level of the input signal light, so that the output level of the optical amplifier 100 becomes a desired output level. Controls the amplification gain. On the other hand, the optical amplifier 100 controls the loss in the VOA 5 based on, for example, fluctuations in the input level of the input signal light. Thereby, the optical amplifier 100 can obtain a desired output level while maintaining the flatness of the output wavelength characteristic with respect to the fluctuation of the input level.

Further, the optical amplifier 100 bypasses the VOA 5 so that the pumping light (residual pumping light) leaked without being absorbed by the first EDF 3 is not attenuated by the VOA 5, and is input again to the second EDF 7. The number of wavelength-fixed excitation LDs (excitation light sources) 12 is suppressed to one. Thereby, the manufacturing cost of the optical amplifier 100 can be reduced.
Furthermore, the optical amplifier 100 can suppress the AGC control delay when the wavelength of the input signal light is increased or decreased by using one AGC control loop.

In order to obtain a flat output level regardless of the input level fluctuation of the input signal light, the optical amplifier 100 includes, for example, a gain equalizer [GEQ (Gain Equalizer) between the first EDF 3 and the second EDF 7. )].
(1.2) Problems of Optical Amplifier 100 By the way, one of the factors that determine the manufacturing cost of the optical amplifier 100 is the manufacturing cost of an excitation light source (for example, LD). The manufacturing cost of the excitation light source increases, for example, as the maximum excitation light power that can be generated by the excitation light source increases.

For this reason, in order to further reduce the manufacturing cost of the optical amplifier 100, for example, it is effective to reduce the maximum pumping light power required for the LD.
This maximum pumping light power is determined by the operating conditions of the optical amplifier provided with the LD. The operating conditions include, for example, the number of wavelengths of input signal light and the input level of input signal light. It is assumed that the input signal light has a level fluctuation from the input lower limit to the input upper limit, for example.

Here, the conditions of the input signal light that maximizes the required pumping light power of the LD will be described with reference to FIGS.
FIG. 2 is a diagram illustrating an example of a level diagram of input signal light power (dBm / ch) per wave, and FIG. 3 is a diagram illustrating an example of an absorption amount of pump light power (mW) in each EDF 3, 7. It is. 2 and 3, as an example, the wavelength of the excitation light is 981 nm, but the wavelength of the excitation light is not limited to this.

First, at the time of input to the optical amplifier 100 and input to the first EDF 3, there is no change in the level difference between the input upper limit and the input lower limit as shown in FIG.
Next, focusing on the output of the first EDF 3, the output level corresponding to the input upper limit is larger than the output level corresponding to the input lower limit, but the amplification gain of the first EDF 3 decreases conversely. Yes. This decrease in amplification gain is due to the amplification characteristic of the first EDF 3.

When attention is paid to the attenuation amount of VOA 5 (level difference between the output of the first EDF 3 and the input of the second EDF 7), the attenuation amount corresponding to the input upper limit is equal to the level difference between the input lower limit and the input upper limit. Large (input upper limit is more attenuated).
Further, focusing attention on the output of the second EDF 7 and the output of the optical amplifier 100, the output level corresponding to the input upper limit and the output level corresponding to the input lower limit are substantially the same level. At this time, the amplification gain of the second EDF 7 is larger in the amplification gain corresponding to the input upper limit than in the amplification gain corresponding to the input lower limit.

On the other hand, when focusing on the excitation light amount (hereinafter referred to as excitation light absorption amount) absorbed by the first EDF 3, as shown in FIG. 3, the excitation light corresponding to the input upper limit rather than the excitation light absorption amount corresponding to the input lower limit. Absorption is greater.
When attention is paid to the excitation light absorption amount in the second EDF 7, the excitation light absorption amount corresponding to the input upper limit is slightly larger than the excitation light absorption amount corresponding to the input lower limit. The difference in the amount of excitation light absorption is smaller than the difference in the amount of excitation light absorption in the first EDF 3.

Further, paying attention to the amount of excitation light leaking from the second EDF 7 (hereinafter referred to as excitation light leakage amount), there is almost no leakage of excitation light at the input upper limit and the input lower limit. This is because the fiber length of the second EDF 7 is set to such a length that leakage of excitation light is eliminated.
As described above, the required pumping light power of the LD is maximized when the input level of the input signal light is the input upper limit because the pumping light absorption amount in the first EDF 7 is dominant. Since the values shown in FIGS. 2 and 3 are values per wave of the input signal light, the required pumping light power of the LD increases as the wavelength multiplexing number of the input signal light increases.

Accordingly, when the number of wavelength divisions of the input signal light is the maximum number of wavelengths and the input level of the input signal light is the input upper limit, the required pump light power of the LD becomes maximum.
Therefore, when the input level of the input signal light is large, if the pumping light absorption amount in the first EDF 3 can be reduced, the maximum pumping light power required for the LD can be reduced. The manufacturing cost can be greatly reduced.

However, as described above, the greater the input level of the input signal light, the greater the amount of excitation light absorbed by the first EDF 3.
Furthermore, as the amount of pumping light absorbed by the first EDF 3 increases, the power of the residual pumping light that reaches the second EDF 7 decreases. For this reason, in order to ensure the residual pumping light power in the second EDF 7 in order to keep the output level of the optical amplifier 100 at a predetermined level, a larger pumping light power is required at the time of input to the first EDF 3. The Rukoto.

As a result, an LD capable of generating a larger pumping light power is mounted in preparation for a case where the wavelength multiplexing number of the input signal light is large or a case where the input level of the input signal light is large. Manufacturing costs may increase.
Thus, for example, the following configuration of the optical amplifier 200 can be considered.
(1.3) Configuration Example of Optical Amplifier 200 FIG. 4 is a diagram illustrating a configuration example of the optical amplifier 200 according to an embodiment.

  The optical amplifier 200 shown in FIG. 4 exemplarily includes a branching unit 1, a multiplexing unit 2, a first EDF 3, a duplexer 4, a VOA 5, a multiplexer 6, and a second EDF 7. And a branching portion 8. Further, the optical amplifier 200 illustratively includes a gain target value calculation unit 9, a gain error detection unit 10, a power control unit 11, a VOA control unit 13, a wavelength control unit 14, and a wavelength variable pump LD 15. I have it. The branching unit 1, the combining unit 2, the first EDF 3, the demultiplexer 4, the VOA 5, the multiplexer 6, the second EDF 7, the branching unit 8, the gain target value calculating unit 9, the gain error detecting unit 10, The power control unit 11 and the VOA control unit 13 have functions similar to those illustrated in FIG.

  Here, the tunable pumping LD 15 is a pumping light source that can output by changing the wavelength of pumping light. The wavelength tunable pumping LD 15 generates, for example, pumping light having a variable wavelength according to the control by the wavelength control unit 14 and outputs it to the multiplexing unit 2. For example, a wavelength tunable laser may be used as the wavelength tunable pumping LD 15, or an LD capable of outputting pumping light having a predetermined bandwidth and a fiber Bragg grating (FBG) capable of selecting a predetermined wavelength. A configuration combining the above and the like may be used.

That is, the first EDF 3 functions as an example of a first rare earth-added medium that amplifies input signal light using the pump light output from the wavelength variable pump LD 15.
The second EDF 7 functions as an example of a second rare earth-added medium that further uses the residual pump light output from the first EDF 3 to further amplify the amplified input signal light.

The wavelength control unit 14 detects the input level of the input signal light branched by the branching unit 1 and controls the wavelength of the pumping light output from the wavelength variable pumping LD 15 based on the detected input level.
For example, the wavelength control unit 14 controls the wavelength of the excitation light so that the higher the input level is, the wavelength of the excitation light is such that the amount of absorption of the excitation light in the first EDF 3 is small. For example, the wavelength control unit 14 may control the wavelength of the excitation light so that the amount of excitation light absorbed by the first EDF 3 decreases as the input level of the input signal light increases. On the other hand, for example, the wavelength control unit 14 may control the wavelength of the excitation light so that the amount of excitation light absorbed by the first EDF 3 increases as the input level of the input signal light decreases.

Here, FIG. 5 shows an example of the wavelength dependence characteristics of the amount of excitation light absorbed in the 0.98 μm band of the first EDF 3 (or the second EDF 7).
As illustrated in FIG. 5, for example, the excitation light absorption amount of the EDFs 3 and 7 is maximum with respect to the excitation light of 981 nm, while the excitation light absorption amount of the EDFs 3 and 7 is with respect to the excitation light of 977 nm. Is about half of the amount of excitation light absorbed with respect to 981 nm excitation light.

Therefore, as the input level of the input signal light is larger, the amount of excitation light absorbed by the first EDF 3 can be reduced by shifting the wavelength of the excitation light from 981 nm. As a result, the maximum pumping light power required for the LD (pumping light source) can be reduced.
Therefore, the wavelength control unit 14 of this example, for example, based on the relationship between the input level and the excitation wavelength shown in FIG. 6 obtained by the characteristics shown in FIG. Control the wavelength.

  As illustrated in FIG. 6, for example, when the input level is about −20.4 (dBm / ch), the wavelength control unit 14 determines the wavelength of the excitation light generated and output by the wavelength variable excitation LD 15. Control to about 981 nm. Then, the wavelength of the excitation light is shifted as the input level of the input signal light increases. When the input level becomes about −15.4 (dBm / ch), the wavelength control unit 14 controls the wavelength of the excitation light to about 977 nm, for example. On the other hand, when the input level of the input signal light decreases, the wavelength control unit 14 may perform control in the opposite direction to the wavelength control, for example.

As shown in FIG. 5, even if the wavelength of the excitation light is increased from the center wavelength 981 nm and changed to about 985 nm, the amount of excitation light absorption equivalent to that when the wavelength of the excitation light is controlled to about 977 nm. Can be realized.
Therefore, for example, the wavelength control unit 14 can reduce the amount of pumping light absorbed by the first EDF 3 by shifting in the direction in which the wavelength of the pumping light increases as the input level of the input signal light increases. it can.

  As described above, the optical amplifier 200 shifts the wavelength of the pumping light to a wavelength with a small amount of pumping light absorption by the EDFs 3 and 7 as the input level of the input signal light increases, so that the first EDF3 It is possible to significantly reduce the amount of excitation light absorbed by the laser. Accordingly, since the residual excitation light amount from the first EDF 3 can be increased, the residual excitation light amount input to the second EDF 7 can be increased.

  As the wavelength control is performed, the amount of pumping light absorbed by the second EDF 7 also decreases, so that the amount of pumping light leakage from the second EDF 7 tends to increase. However, the fiber length of the second EDF 7 is The length is set in advance such that the amount of excitation light leakage is sufficiently small. For this reason, the amount of excitation light leakage from the second EDF 7 is negligible. In view of this point, for example, it is preferable that the wavelength control unit 14 shift-controls the wavelength of the excitation light so that the amount of excitation light leakage from the second EDF 7 is sufficiently negligible.

  Moreover, since the output level of the signal light output from the first EDF 3 is reduced by the amount of absorption of the excitation light in the first EDF 3, the input level of the signal light to the second EDF 7 is also reduced. The pumping light power required by the second EDF 7 tends to increase, but this is only a slight increase. Although the amplification efficiency of the first EDF 3 is reduced by the amount of absorption of the excitation light in the first EDF 3, the residual excitation light quantity input to the second EDF 7 is increased. The amplification gain is improved.

  As described above, the optical amplifier 200 of the present example shifts the pumping light wavelength to a wavelength at which the pumping light absorption amount in the first EDF 3 decreases as the input level of the input signal light increases, so that the first EDF 3 The amount of excitation light absorption at can be reduced. As a result, the maximum pumping light power required for the wavelength variable pumping LD 15 can be greatly reduced, and the manufacturing cost of the optical amplifier 200 can be greatly reduced.

  Note that NF is one of the performance indexes of the optical amplifier 200. This NF has a property that a better value is required as the input level of the input signal light is smaller. In general, the NF of the EDF becomes a better value as the amount of excitation light absorbed by the EDF increases. Therefore, as the input level of the input signal light is smaller, the wavelength of the excitation light is desirably controlled to a wavelength (for example, 981 nm) that increases the amount of excitation light absorbed by the first EDF 3. Conversely, as the input level of the input signal light increases, a better value of NF is not required as compared with the case where the input level is small. Therefore, the wavelength of the excitation light is a wavelength at which the amount of absorption of the excitation light decreases (for example, 977 nm ) Can be controlled.

  As described above, the optical amplifier 200 reaches the second EDF 7 by controlling the pumping light wavelength so that the pumping light absorption amount in the first EDF 3 is reduced as the input level of the input signal light increases. The power of the residual pumping light can be increased. In addition, NF can be improved by controlling the pumping light wavelength so that the amount of pumping light absorption increases as the input level of the input signal light decreases.

That is, since the optical amplifier 200 can reduce the maximum pumping light power required for the pumping light source (LD) by changing the pumping light wavelength according to the input level of the input signal light, the cost required for the LD. It is possible to significantly reduce the manufacturing cost of the optical amplifier 200.
(1.4) Example of Effect Here, an example of the effect obtained by the optical amplifier 200 will be described.

For example, wavelength-division multiplexed signal light (wavelength interval: 100 GHz, number of wavelengths: 40 waves, input lower limit: -20.4 dBm / ch, input upper limit: -15.4 dBm / ch) in the C band is input to the optical amplifier 200. Consider a case where an output signal with an output level of 2.5 dBm / ch is obtained.
At this time, for example, when the input level is the input lower limit, the wavelength control unit 14 sets the wavelength of the pumping light to 981 nm at which the pumping light absorption amount at the EDFs 3 and 7 becomes maximum (2.0 dB / m). Control (see FIG. 5).

  On the other hand, for example, when the input level is the input upper limit, the wavelength control unit 14 sets the excitation light wavelength to the excitation light absorption amount when the excitation light absorption amount at the EDFs 3 and 7 is 981 nm. To a wavelength (for example, 977 nm) that is less (half). It should be noted that the pumping light absorption amount in the EDFs 3 and 7 should be smaller than the pumping light absorption amount when the pumping light wavelength is 981 nm, and the wavelength control unit 14 may, for example, pump light when the input level is the input upper limit. May be controlled to a wavelength different from 977 nm (for example, 985 nm).

  Furthermore, when the input level is between the input lower limit and the input upper limit, the wavelength control unit 14 may control the wavelength of the excitation light based on a predetermined relational expression. For example, as illustrated in FIG. 6, the relational expression is such that the input level is the input lower limit (−20.4 dBm / ch) and the excitation light wavelength is 981 nm, and the input level is the input upper limit (−15.4 dBm / ch). ch) and an expression represented by a straight line passing through a point where the excitation light wavelength is 977 nm can be employed. In this case, the relational expression is expressed by the following expression (1).

Excitation light wavelength (μm) = (0.977−0.981) / {(− 15.4) − (− 20.4)} × input level (dBm / ch) +0.96468 (−20.4 ≦ input) Level ≦ −15.4) (1)
The relational expression (1) is merely an example, and the present invention is not limited to this. For example, a relational expression that reduces the value of the excitation light wavelength stepwise as the input level increases may be adopted.

Further, the wavelength variable pump LD 15 can variably control the oscillation wavelength of the LD, for example, by providing the variable wavelength FBG at the output end of the LD and the wavelength control unit 14 controlling the variable wavelength FBG.
Further, in this example, for example, the fiber length of the first EDF 3 is set to 10 m so that the residual pump light leaks from the first EDF 3, while the amount of the residual pump light leaking from the second EDF 7 is reduced. Therefore, the fiber length of the second EDF 7 is set to 15 m.

  In the optical amplifier 200 having the above configuration, when 981 nm excitation light is incident, the NF of the optical amplifier 200 at the input lower limit is 4.78 dB. Further, when 977 nm excitation light is incident, the NF of the optical amplifier 200 at the lower input limit is 4.89 dB, and NF is deteriorated by about 0.11 dB as compared with the case where 981 nm excitation light is incident. This also indicates that the excitation light wavelength at the lower input limit is desirably 981 nm.

On the other hand, when 977 nm excitation light is incident, the NF of the optical amplifier 200 at the upper limit of input is 5.85 dB. In addition, when 981 nm excitation light is incident, the NF of the optical amplifier 200 at the input upper limit is 5.48 dB, which is about 0.29 dB higher than when 977 nm excitation light is incident.
However, the OSNR (Optical Signal Noise Ratio) indicating the transmission performance including the transmission path is proportional to the NF of the optical amplifier 200, but is improved in proportion to the input level. Since the OSNR at the input lower limit and the input upper limit generally need to be equal, it is sufficient that the NF at the input upper limit is 4.78 dB + 5 dB = 9.78 dB or less. Therefore, it can be seen that NF at the upper limit of input is sufficiently good as NF = 5.85 dB at the excitation light wavelength of 977 nm.

  Next, in the optical amplifier 200 having the above configuration, when the input level is the input lower limit, the pumping light wavelength is controlled to 977 nm, while when the input level is the input upper limit, the wavelength when the pumping light wavelength is controlled to 981 nm. The required pumping light power of the variable pumping LD 15 will be described. As described above, when the input level is the input upper limit, the required pumping light power of the wavelength tunable pumping LD 15 becomes maximum.

  FIG. 7 is a diagram showing an example of a level diagram of input signal light power (dBm / ch) per wave of each pumping light wavelength. FIG. 8 shows each EDF3 of pumping light power (mW) of each pumping light wavelength. 7 is a diagram illustrating an example of an absorption amount at 7. FIG. For reference, inversion distributions in the longitudinal direction of the first EDF 3 and the second EDF 7 at the upper limit of input when each excitation light is incident are shown in FIGS. 9 and 10, respectively.

First, as illustrated in FIG. 7, there is no difference in the input signal light level at each pumping light wavelength when input to the optical amplifier 200 of this example and when input to the first EDF 3.
Next, paying attention to the input / output of the first EDF 3, the output level corresponding to the 981 nm excitation light is higher than the output level corresponding to the 977 nm excitation light with respect to the input of the same level. This is because the excitation light absorption amount in the first EDF 3 is reduced by changing the excitation light wavelength from 981 nm to 977 nm (see FIG. 5), and the amplification efficiency of the first EDF 3 is lowered.

  Focusing on the input / output of the second EDF 7, the input level corresponding to the 981 nm excitation light is higher than the input level corresponding to the 977 nm excitation light, but the output level is the same level. This is because the excitation light wavelength is changed from 981 nm to 977 nm, the residual excitation light quantity from the first EDF 3 is increased, and the amplification efficiency of the second EDF 7 is increased.

On the other hand, paying attention to the excitation light absorption amount in the first EDF 3, as shown in FIG. 8, the excitation light absorption amount for the 977 nm excitation light is smaller than the excitation light absorption amount for the 981 nm excitation light.
Focusing on the absorption amount of the excitation light in the second EDF 7, as shown in FIG. 8, the absorption amount of the excitation light with respect to the excitation light of 977 nm is slightly larger than the absorption amount of excitation light with respect to the excitation light of 981 nm. This indicates that the amount of residual excitation light from the first EDF 3 increased as the excitation light wavelength was changed from 981 nm to 977 nm.

Further, focusing attention on the amount of excitation light leakage from the second EDF 7, as shown in FIG. 8, the amount of excitation light leakage for the 977 nm excitation light is slightly larger than the amount of excitation light leakage for the 981 nm excitation light. . This also indicates that the amount of residual excitation light from the first EDF 3 increased due to the change of the excitation light wavelength from 981 nm to 977 nm.
Here, paying attention to the sum of the pumping light absorption amount of the first EDF 3, the pumping light absorption amount of the second EDF and the pumping light leakage amount (that is, the required pumping light power of the wavelength variable pumping LD 15), the pumping light of 981 nm When using, the power is 600 mW, whereas when using 977 nm excitation light, the power decreases to 531 mW. This indicates that the maximum pumping light power of the wavelength variable pumping LD 15 mounted on the optical amplifier 200 can be reduced by 69 mW.

Thus, in this example, by controlling the pumping light wavelength as described above according to the input level to the optical amplifier 200, the maximum pumping light power of the wavelength tunable pumping LD15 can be reduced. Since the cost can be reduced, the manufacturing cost of the optical amplifier 200 can be greatly reduced.
[2] First Modification In the embodiment described above, the wavelength of the pumping light is controlled based on the input level of the input signal light. However, for example, pumping light having different wavelengths can be generated and output as in this example. The power ratio of each pumping light output from a plurality of pumping light sources may be controlled.

FIG. 11 is a diagram illustrating an example of the configuration of the optical amplifier 300 according to the first modification.
An optical amplifier 300 shown in FIG. 11 exemplarily includes a branching unit 1, a multiplexing unit 2, a first EDF 3, a duplexer 4, a VOA 5, a multiplexer 6, and a second EDF 7. And a branching portion 8. Further, the optical amplifier 300 exemplarily includes a target gain calculation unit 9, a gain error detection unit 10, a power control unit 11, a VOA control unit 13, a first fixed wavelength pumping LD 16, a second A fixed wavelength pumping LD 17, a pumping light multiplexing unit 18, and a power ratio control unit 19 are provided. The branching unit 1, the combining unit 2, the first EDF 3, the demultiplexer 4, the VOA 5, the multiplexer 6, the second EDF 7, the branching unit 8, the gain target value calculating unit 9, the gain error detecting unit 10, The power control unit 11 and the VOA control unit 13 have functions similar to those illustrated in FIG.

Here, the first fixed wavelength excitation LD (first excitation light source) 16 generates and outputs excitation light having a preset fixed wavelength (first wavelength).
The second wavelength-fixed pumping LD (second pumping light source) 17 has a wavelength (second wavelength) different from the wavelength of the pumping light (first wavelength) generated and output by the first wavelength-fixed pumping LD 16. Excitation light having a wavelength) is generated and output. In this example, for example, the first wavelength can be 981 nm and the second wavelength can be 977 nm.

The pumping light multiplexer 18 combines the output from the first fixed wavelength pumping LD 16 and the output from the second fixed wavelength pumping LD 17 and outputs the wavelength-multiplexed pumping light. The excitation light combined by the excitation light combining unit 18 is input to the first EDF 3 via the multiplexing unit 2 as wavelength multiplexed excitation light.
Based on the input level of the input signal light, the power ratio control unit 19 determines the ratio between the power of the first wavelength pump light and the power of the second wavelength pump light included in the wavelength multiplexed pump light. Control.

For example, the power ratio control unit 19 in this example increases the power ratio of the pump light having the second wavelength among the pump lights included in the wavelength multiplexing pump light as the input level of the input signal light increases. Also good.
Here, an example of a control method in the power ratio control unit 19 will be described with reference to FIG.
For example, as illustrated in FIG. 12, when the input level is the input lower limit (−20.4 dBm / ch), the power ratio control unit 19 includes only the first wavelength (for example, 981 nm) in the wavelength multiplexed pump light. The power ratio of each of the LDs 16 and 17 is controlled so as to be included. On the other hand, when the input level is the input upper limit (−15.4 dBm / ch), the power ratio control unit 19 sets each of the LDs 16 and 17 so that only the second wavelength (for example, 977 nm) is included in the wavelength multiplexed pump light. Control the power ratio.

Further, when the input level is between the input lower limit and the input upper limit, the power ratio control unit 19 increases the power of the pumping light of the second wavelength included in the wavelength multiplexing pumping light as the input level increases, for example. While increasing the power ratio, the power ratio of the LDs 16 and 17 is controlled so as to decrease the power ratio of the excitation light having the first wavelength.
Even if it does in this way, since the effect similar to embodiment mentioned above can be acquired and wavelength variable LD can be abbreviate | omitted, it becomes possible to further reduce the manufacturing cost of the optical amplifier 300. FIG.

[3] Others The configurations and processes of the optical amplifiers 100, 200, and 300 described above may be selected as necessary or may be combined as appropriate.
Further, the number (stage number) of the demultiplexer 4, VOA 5, multiplexer 6, second EDF 7 and VOA control unit 13 provided between the first EDF 3 and the branching unit 8 is shown in FIGS. The example shown in FIG.

Furthermore, the combination of the first wavelength and the second wavelength in the above embodiment and the modification is merely an example, and the second wavelength is the first EDF 3 or the second EDF 7 rather than the first wavelength. As long as the amount of absorption of excitation light is small, it is sufficient.
Further, the fiber length of the first EDF 3 can be set to such a length that the residual excitation light leaks to the second EDF 7 in the subsequent stage, for example, and the fiber length of the second EDF 7 is set to, for example, the first EDF 3 It is possible to make the length enough to absorb the residual excitation light from the light without leakage.

Further, in the first modified example, the example in which the power ratio of two different wavelengths is controlled has been described. However, the excitation light absorption by the first EDF 3 is controlled by controlling the power ratio of three or more different wavelengths. The amount may be reduced.
Moreover, in the said embodiment and modification, each structure (The gain target value calculation part 9, the power control part 11, the VOA control part 13, the wavelength control part 14, and the power ratio control part 19) respectively receives input signal light. Although the level is detected, the input level may be supplied to each component from the outside.

The following supplementary notes are further disclosed with respect to the above embodiments and modifications.
[4] Appendix (Appendix 1)
An excitation light source that can output by changing the wavelength of the excitation light; and
A first rare earth-added medium that amplifies input signal light using the excitation light output from the excitation light source;
A second rare earth-added medium that further amplifies the amplified input signal light using residual pumping light output from the first rare earth-added medium;
A wavelength control unit for controlling the wavelength of the excitation light output from the excitation light source based on the input level of the input signal light;
An optical amplifier characterized by that.

(Appendix 2)
The wavelength controller is
As the input level is larger, the wavelength of the excitation light is controlled to a wavelength where the absorption amount of the excitation light in the first rare earth-added medium is smaller.
The optical amplifier according to appendix 1, wherein

(Appendix 3)
The wavelength of the excitation light is 0.98 μm band,
The optical amplifier according to appendix 1 or 2, characterized by the above.
(Appendix 4)
The excitation light source is
Having a tunable fiber Bragg rating,
The optical amplifier according to any one of appendices 1 to 3, wherein:

(Appendix 5)
A first excitation light source that outputs excitation light of a first wavelength;
A second excitation light source that outputs excitation light having a second wavelength different from the first wavelength;
A multiplexing unit that combines the output from the first excitation light source and the output from the second excitation light source to output wavelength-division-excited excitation light;
A first rare earth-added medium that amplifies input signal light using the wavelength-multiplexed excitation light output from the multiplexing unit;
A second rare earth-added medium that further amplifies the amplified input signal light using residual pumping light output from the first rare earth-added medium;
A power ratio control unit that controls a ratio of the power of the pumping light of the first wavelength and the power of the pumping light of the second wavelength included in the pumping light based on the input level of the input signal light; , With
An optical amplifier characterized by that.

(Appendix 6)
The second wavelength is a wavelength at which the amount of excitation light absorbed in the first rare earth-added medium is smaller than the first wavelength.
The optical amplifier according to appendix 5, wherein:
(Appendix 7)
The power ratio controller is
The greater the input level of the input signal light, the greater the power ratio of the pump light of the second wavelength included in the wavelength multiplexed pump light;
The optical amplifier according to appendix 6, wherein:

(Appendix 8)
The first wavelength and the second wavelength are in a 0.98 μm band,
The optical amplifier according to any one of appendices 5 to 7, characterized in that:
(Appendix 9)
The medium length of the second rare earth-added medium is longer than the medium length of the first rare earth-added medium.
The optical amplifier according to any one of appendices 1 to 8, characterized in that:

(Appendix 10)
An optical attenuator inserted between the first rare earth-added medium and the second rare earth-added medium and attenuating the input signal light amplified by the first rare earth-added medium;
A demultiplexer inserted between the first rare earth-added medium and the optical attenuator, demultiplexing the residual pumping light and bypassing the optical attenuator;
A multiplexer that is inserted between the optical attenuator and the second rare earth-added medium and multiplexes the residual pump light demultiplexed by the demultiplexer and inputs the multiplexed light to the second rare earth-added medium. And
The optical amplifier according to any one of appendices 1 to 9, characterized in that:

(Appendix 11)
The input signal light is wavelength-multiplexed signal light.
The optical amplifier according to any one of appendices 1 to 10, characterized in that:
(Appendix 12)
The wavelength band of the input signal light is a C band band.
The optical amplifier according to any one of appendices 1 to 11, characterized in that:

(Appendix 13)
The direction of the excitation light in the first rare earth-added medium and the second rare earth-added medium is forward excitation.
13. The optical amplifier according to any one of appendices 1 to 12, characterized in that:
(Appendix 14)
Using a pumping light source that outputs pumping light, a first rare earth-added medium that amplifies input signal light using the pumping light output from the pumping light source, and residual pumping light of the first rare-earth-added medium An optical amplification method for an optical amplifier, comprising: a second rare earth-added medium that amplifies the input signal light,
Monitoring the input level of the input signal light;
As the monitored input level is larger, the wavelength of the excitation light is controlled to a wavelength with less absorption of the excitation light in the first rare earth-added medium.
An optical amplification method characterized by that.

(Appendix 15)
A first excitation light source that outputs excitation light of a first wavelength, a second excitation light source that outputs excitation light of a second wavelength different from the first wavelength, and a first excitation light source A multiplexing unit that combines the output and the output from the second pumping light source to output wavelength-multiplexed pumping light, and the wavelength-multiplexed pumping light that is output from the multiplexing unit is used for input. A first rare earth-added medium for amplifying signal light; and a second rare earth-added medium for further amplifying the amplified input signal light using residual pumping light output from the first rare earth-added medium. An optical amplification method for an optical amplifier comprising:
Monitoring the input level of the input signal light;
The higher the monitored input level, the lower the amount of pump light absorbed in the first rare earth-added medium than the first wavelength, and the power ratio in the wavelength multiplexed pump light of the second wavelength. To increase the
An optical amplification method characterized by that.

1,8 Branching part 2 Multiplexing part 3 1st EDF
4 splitter 5 VOA
6 multiplexer 7 second EDF
9 Gain Target Calculation Unit 10 Gain Error Detection Unit 11 Power Control Unit 12, 16, 17 Fixed Wavelength Pump LD
13 VOA controller 14 Wavelength controller 15 Wavelength variable excitation LD
18 Pumping light multiplexing unit 19 Power ratio control unit 100, 200, 300 Optical amplifier

Claims (2)

A first excitation light source that outputs excitation light of a first wavelength;
A second excitation light source that outputs excitation light having a second wavelength different from the first wavelength;
A multiplexing unit that combines the output from the first excitation light source and the output from the second excitation light source to output wavelength-division-excited excitation light;
A first rare earth-added medium that amplifies input signal light using the wavelength-multiplexed excitation light output from the multiplexing unit;
A second rare earth-added medium that further amplifies the amplified input signal light using residual pumping light output from the first rare earth-added medium;
The higher the input level of the input signal light, the first power over which definitive said wavelength-multiplexed excitation light absorption amount of the excitation light is small the second wavelength in the first rare earth doped medium than the wavelength a power ratio control section that performs control to increase the specific rate, provided with a,
Wherein the optical amplifier device. A first excitation light source that outputs excitation light of a first wavelength, a second excitation light source that outputs excitation light of a second wavelength different from the first wavelength, and a first excitation light source A multiplexing unit that combines the output and the output from the second pumping light source to output wavelength-multiplexed pumping light, and the wavelength-multiplexed pumping light that is output from the multiplexing unit is used for input. A first rare earth-added medium for amplifying signal light; and a second rare earth-added medium for further amplifying the amplified input signal light using residual pumping light output from the first rare earth-added medium. An optical amplification method for an optical amplifier comprising:
Monitoring the input level of the input signal light;
The higher the monitored input level, the lower the amount of pump light absorbed in the first rare earth-added medium than the first wavelength, and the power ratio in the wavelength multiplexed pump light of the second wavelength. To increase the
An optical amplification method characterized by that.

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