JP2016111198A - Optical amplifier - Google Patents

Abstract

PROBLEM TO BE SOLVED: To achieve reduction of propagation mode dependent gain in multimode L band optical amplification.SOLUTION: An optical amplifier includes an optical fiber 14 for amplification capable of propagating in a plurality of propagation modes, more than the propagation modes of signal light, an excitation light source 11 generating excitation light having a wavelength capable of exciting the signal light in the optical fiber 14 for amplification, a mode converter 12 for converting the excitation light from the excitation light source 11 into at least any propagation mode included in the plurality of propagation modes, and a signal excitation optical multiplexer 13 for multiplexing the excitation light after converting the propagation mode in the mode converter 12 with the signal light.SELECTED DRAWING: Figure 8

Description

  The present invention relates to a technique related to an optical amplifier in mode multiplex transmission.

  In recent years, Internet traffic has continued to increase due to the diversification of services, and the transmission capacity has increased dramatically due to the increase in the number of wavelength multiplexing by the increase in the transmission speed and the wavelength division multiplexing (WDM) technology. . Further, in recent years, further expansion of transmission capacity is expected by digital coherent technology which has been actively studied. In digital coherent transmission systems, frequency utilization efficiency has been improved by using multilevel phase modulation signals, but higher signal-to-noise ratios are required. However, in a transmission system using a conventional single mode fiber (SMF), the transmission capacity is expected to saturate at 100 Tbit / sec due to input power limitation due to nonlinear effects in addition to the theoretical limit. Therefore, further increase in capacity has become difficult.

  In order to further increase the transmission capacity in the future, a medium that realizes innovative transmission capacity expansion is required. Therefore, mode multiplex transmission using a multimode fiber (MMF) that can be expected to improve the signal-to-noise ratio and the space utilization efficiency by using a plurality of propagation modes in an optical fiber as a channel is attracting attention. . Up to now, high-order modes propagating in the fiber have been a cause of signal degradation, but active use is being studied in the development of digital signal processing and multiplexing / demultiplexing techniques.

In addition, studies have been made to increase the distance of mode multiplex transmission, and reports have been made on the amplification of the LP01 mode of the basic mode using the Er ^{3 +} -doped optical amplifier and the LP02 mode of the fourth higher-order LP mode. Yes.

  In order to maintain the transmission quality of all modes in order to increase the distance of mode multiplex transmission, it is necessary to reduce the propagation mode dependent gain (MDG) in the optical amplifier. However, since light propagating in an EDF (Erbium Doped Fiber) has a different electric field distribution for each mode, a different gain is generally obtained.

  The gain of each mode is determined by the overlap between the excitation element number distribution determined by the electric field distribution of the excitation light incident on the amplification optical fiber and the rare earth element addition distribution and the electric field distribution of the signal light. At present, the rare earth element added region of the optical fiber for amplification mainly includes a step index type structure in which a rare earth element is added to the entire core and a center dope type structure in which a rare earth element is added only at the center of the core. However, in an amplification optical fiber for multimode transmission that needs to take into account higher-order mode gain, a structure in which a rare earth doping distribution is heavily doped at the edge of the fiber core has been proposed.

  In the current report, the configuration of optical amplifiers using spatial optical elements is the mainstream, and pumping is performed using a method (for example, Non-Patent Document 1) or a phase filter that excites the axis when the pumping light is incident on the amplification optical fiber. There has been proposed a method of adjusting gain for each propagation mode by converting light into an arbitrary mode and entering the optical fiber for amplification (for example, Non-Patent Document 2).

  In recent years, studies on L-band optical amplification technology for expanding the transmission band of mode multiplexing transmission have begun. Conventional single mode transmission has been realized by using a longer one than the EDF used in the C band. In general, in L-band optical amplification using a long EDF, an L-band signal is absorbed once in a part of the amplification process and then used using spontaneous emission of C-band (ASE: Amplified Spontaneous Emission). Light is amplified.

  FIG. 1 shows a measurement system for measuring the mode ratio of ASE generated in a multimode optical amplifier. The excitation light source 111 uses 1550 nm light, and the excitation light mode is LP01 or LP11 mode. A long period grating (LPG) is used for the excitation light mode converter 112. The generated ASE is separated by the mode demultiplexer 113. An OSA (Optical Spectrum Analyzer) 117 obtains the LP11 mode as the sum of two degenerate modes.

  FIG. 2 shows the wavelength dependence of the ASE mode ratio difference LP11-LP01 under these conditions. It can be seen that the generated ASE is less dependent on the mode of the excitation light as it shifts to the longer wavelength side. As a result, it is expected that the reduction of the propagation mode dependent gain by the conversion of the excitation mode that has been reported in the C band so far becomes more difficult as the wavelength becomes longer.

Y. Yung et al. “First demonstration of multimode amplifier for spatial division multiplexed transmission systems” ECOC2011 paper Th. 13. K. 4 Y. Jung et al. “Few-mode EDFA Supporting 5 Spatial Models with Reconfigurable Differential Modal Gain Control” ECOC2011 paper We. 4). A. 2.

  An object of the present invention is to realize a reduction in propagation mode dependent gain in multimode L-band optical amplification.

Specifically, the optical amplifier according to the present invention is:
An optical fiber for amplification capable of propagating a plurality of propagation modes equal to or higher than the propagation mode of signal light;
An excitation light source that generates excitation light having a wavelength capable of exciting the signal light in the amplification optical fiber;
A mode converter that converts excitation light from the excitation light source into at least one of the propagation modes included in the plurality of propagation modes;
A signal light pumping light multiplexer that combines the pumping light after the propagation mode is converted by the mode converter with the signal light;
Is provided.

  The optical amplifier according to the present invention may further include a gain equalizer for equalizing gains of the plurality of propagation modes, and the loss spectrum of the gain equalizer may be different for each propagation mode.

  In the optical amplifier according to the present invention, the amplification optical fiber is an erbium-doped fiber, the wavelength of the signal light is from 1565 nm to 1625 nm, and the wavelength of the excitation light is from 1530 nm to 1565 nm. Good.

  The optical amplifier according to the present invention includes a plurality of the signal light pumping light multiplexers, and one of the signal light pumping light multiplexers combines the pumping light with the signal light before the amplification optical fiber. The light is incident on the amplification optical fiber, and the other signal light pumping light multiplexer combines the pumping light with the signal light at a subsequent stage of the amplification optical fiber, and the pumping light is combined with the amplification optical fiber. You may make it enter into.

  In the optical amplifier according to the present invention, the highest order mode in which the amplification optical fiber can propagate may be higher than the highest order mode of the signal light.

  In the optical amplifier according to the present invention, the spontaneous emission light generated by the amplification optical fiber may include a propagation mode higher than the highest order mode of the signal light.

  In the optical amplifier according to the present invention, the amplification optical fiber includes an inner ring portion having a relative refractive index difference of 0 and a distance a1 from the core center, and a relative refractive index difference of Δ1 and from the core center. An erbium-doped fiber including an outer ring portion at a distance a2. In this case, the LP01 mode and the LP11 mode are propagated and 0.4 ≦ Δ1 ≦ 1 and Δ1 ≧ (−240 × (a1 / a2) +41.04) are satisfied, or the LP01 mode, the LP11 mode, and the LP21 mode are satisfied. Propagate and satisfy 0.4 ≦ Δ1 ≦ 1 and Δ1 ≧ (−678.0 × (a1 / a2) +31.47), or propagate LP01 mode, LP11 mode, LP21 mode and LP31 mode and 0 4 ≦ Δ1 ≦ 1, Δ1 ≧ (−56.2 × (a1 / a2) +135.32) and Δ1 ≧ (−20.66 × (a1 / a2) -14.55) are satisfied.

  The above inventions can be combined as much as possible.

  According to the present invention, the propagation mode dependent gain in the multimode L-band optical amplifier is reduced, thereby contributing to further widening of the mode multiplexing transmission.

An example of the measurement system of the mode ratio contained in ASE is shown. An example of the measurement result example of the mode ratio included in ASE is shown. 1 shows an example of a configuration of an L-band optical amplifier according to an embodiment of the present invention. A measurement example of the excitation wavelength dependence of gain at a wavelength of 1580 nm will be shown. A measurement example of the excitation wavelength dependence of gain at a wavelength of 1600 nm is shown. An example of a configuration of an L-band optical amplifier when bidirectional pumping is performed is shown. The measurement example of the wavelength dependence of MDG at the time of bidirectional | two-way excitation is shown. An example of a structure of the optical amplifier which has a mode gain equalizer is shown. An example of the configuration in which the mode gain equalizer is installed in the middle stage of the EDF is shown. An example of the relationship between the mode ratio of ASE in two modes and the magnitude of overlap between the signal light LP01 mode and the LP11 mode is shown. An example of the relationship between the mode ratio of ASE in three modes and the magnitude of overlap between the signal light LP01 mode and the LP11 mode is shown. An example of the structure of EDF is shown. An example of MDG in case excitation light is LP01 mode is shown. An example of MDG in case excitation light is LP11 mode is shown. An example of MDG in case excitation light is LP01 mode is shown. An example of MDG in case excitation light is LP21 mode is shown. An example of MDG in case excitation light is LP01 mode is shown. An example of MDG in case excitation light is LP31 mode is shown.

  Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings. In addition, this invention is not limited to embodiment shown below. These embodiments are merely examples, and the present invention can be implemented in various modifications and improvements based on the knowledge of those skilled in the art. In the present specification and drawings, the same reference numerals denote the same components.

  In the present invention, the MDG in the L-band optical amplifier is reduced by entering the light whose mode is converted with the wavelength close to the L-band signal light (for example, the C band) as excitation light into the amplification optical fiber. Alternatively, the gain medium of the optical amplifier is divided into two, and a gain equalizer for equalizing the gain of each mode is used in the middle or subsequent stage. Alternatively, MDG is reduced by using an amplification optical fiber that propagates in a higher-order mode than the signal light that propagates in the amplification optical fiber. Alternatively, MDG in the L band is reduced by designing an amplification optical fiber that does not depend on the mode of pumping light. The configuration and design method of an optical amplifier for realizing MDG reduction in multimode L-band optical amplification are shown below.

  FIG. 3 is a schematic diagram of the first embodiment of the optical amplifier according to the embodiment of the present invention. This optical amplifier includes a pumping light source 11, a mode converter 12, a signal light pumping light multiplexer 13, an amplification optical fiber 14, and an isolator 15. The signal light pumping optical multiplexer 13, the amplification optical fiber 14, and the isolator 15 are sequentially connected to a common multimode fiber.

  The excitation light source 11 generates excitation light. The mode converter 12 converts the mode of excitation light. The signal light pumping light multiplexer 13 combines the signal light and the pumping light. The amplification optical fiber 14 is, for example, an EDF, and amplifies signal light. The isolator 15 prevents the signal light from returning to the signal light excitation light multiplexer 13.

The signal light pumping light multiplexer 13 multiplexes the signal light having the N mode (N is an arbitrary two or more positive number) mode that has been propagated through the multimode fiber and the pumping light. The signal light excitation light multiplexer 13 is preferably a wavelength selective multiplexer. The mode converter 12 mode-converts the excitation light as necessary. The combined signal light and pumping light enter the amplification optical fiber 14. The incident signal light causes stimulated emission of Er ³⁺ in an inverted distribution state by excitation light to the medium, and is emitted after optical amplification. Further, an isolator 15 is inserted as necessary to prevent oscillation in the amplifier.

Since it becomes more difficult to reduce the propagation mode dependent gain by converting the excitation mode as the wavelength becomes longer, in this embodiment, a wavelength that does not pass through ASE is selected as the wavelength of the excitation light. For example, it is assumed that the wavelength of the signal light is a wavelength that causes stimulated emission between the ⁴ I _13/2 and ⁴ I _15/2 levels of erbium. In this case, when the amplifying optical fiber 14 is an erbium-doped fiber, it is preferable that light that has been mode-converted with a wavelength close to the L-band signal light (for example, the C band) as excitation light is incident on the amplifying optical fiber 14. For example, the wavelength of the signal light is set to 1565 nm to 1625 nm, and the wavelength of the excitation light is set to 1530 nm to 1565 nm.

  FIG. 4 shows a measurement example of the excitation wavelength dependence of the LP01 mode and the LP11 mode in the signal light 1580 nm and FIG. 5 in the signal light 1600 nm. The amplification optical fiber 14 used in this measurement has a structure that propagates the 2LP mode in the C and L bands. The input intensity of the signal light is −25 dBm, and the wavelengths of the excitation light are 1480, 1530, 1540, and 1550 nm. It is assumed that the measurement is performed under conditions where the gain of the LP01 mode of the signal light 1580 nm is 20 dB. 4 and 5, it can be confirmed that the MD11 in the LP11 mode and the LP01 mode is decreased from 4 dB to 2 dB at 1580 nm which is the short wavelength side of the L band. Therefore, by setting the wavelength of the signal light to 1565 nm to 1625 nm and the wavelength of the pumping light to 1530 nm to 1565 nm, the propagation mode dependent gain in the multimode L-band optical amplifier can be reduced.

  FIG. 6 is a schematic diagram of a second form of the optical amplifier according to the embodiment of the present invention. The second form of the optical amplifier further includes a pumping light source 11-2, a mode converter 12-2, and a signal light pumping light multiplexer 13-2 in addition to the first form of the optical amplifier shown in FIG. The signal light pumping optical multiplexer 13-1, the amplification optical fiber 14, the signal light pumping optical multiplexer 13-2, and the isolator 15 are sequentially connected to a common multimode fiber. The signal light pumping light combiner 13-1 combines the pumping light with the signal light before the amplification optical fiber 14, and the signal light pumping light combiner 13-2 converts the pumping light into the signal light after the amplification optical fiber 14. Combine.

  A measurement example is shown for reducing MDG by using a bidirectional excitation system in front and rear of the amplification optical fiber 14 as shown in FIG. In the system of FIG. 6, excitation light incident from the front and rear is converted into the LP11 mode by the mode converters 12-1 and 12-2 and then incident on the amplification optical fiber 14.

  In FIG. 7, an example of the wavelength dependence measurement result of MDG at the time of forward excitation and bidirectional | two-way excitation is shown. When the wavelength of the signal light is 1590 nm or less, the value of bidirectional excitation is lower than that of forward excitation. Thus, it confirmed that it had the effect of MDG reduction of the L band short wavelength side by bidirectional | two-way excitation of front and back. Therefore, by using the bidirectional pumping system of the amplification optical fiber 14, the propagation mode dependent gain in the multimode L-band optical amplifier can be reduced.

  Although FIG. 6 shows an example in which the individual mode converters 12-1 and 12-2 convert the excitation light into the common LP11 mode, the present invention is not limited to this. For example, the mode converters 12-1 and 12-2 may convert the excitation light into different modes. Moreover, the excitation light sources 11-1 and 11-2 may generate excitation light having a common wavelength or may generate different wavelengths.

により決まる。 The reduction of MDG using a mode gain equalizer will be described. As a gain equalizer in the single mode, there is a configuration using a long period grating (LPG) or a PLC type Mach-Zender. Among them, an equalizer using LPG has been conventionally applied to the LP01 mode, but a multimode optical amplifier is required to be applied to a higher order mode. The LPG is made with a period in which the mode propagating in the fiber is coupled to the cladding mode.

It depends on.

β _ml is a propagation constant of a mode propagating in the fiber, β _cl ⁿ is a propagation constant of an nth-order cladding mode, and Λ is an LPG pitch. Since β _ml -β _cl ⁿ generally takes a different value for each mode, a different loss spectrum is generated for each mode by producing a different LPG for each mode. If there is a mode in which the β _ml -β _cl ⁿ regions overlap, it can be avoided by connecting non-overlapping optical fibers and making an LPG.

  FIG. 8 is a schematic diagram of a third embodiment of the optical amplifier according to the embodiment of the present invention. The third form of the optical amplifier includes mode gain equalizers 16A to 16C instead of the first form isolator 15 of the optical amplifier shown in FIG. When the modes propagating in the multimode fiber are mode A, mode B, and mode C, the mode gain equalizers 16A to 16C make the gains of mode A, mode B, and mode C equal. When LPG is used for the mode gain equalizers 16A to 16C, it has a different period for each propagation mode. Thus, by further providing a gain equalizer for equalizing the gains of a plurality of propagation modes, the propagation mode dependent gain in the multimode L-band optical amplifier can be reduced.

  FIG. 9 is a schematic diagram of a fourth embodiment of the optical amplifier according to the embodiment of the present invention. In the fourth embodiment of the optical amplifier, amplification optical fibers 14-1 and 14-2 are connected to a multimode fiber. In the case of such a configuration, the mode gain equalizer 16 may be disposed at the interruption of the amplification optical fibers 14-1 and 14-2, or the mode gain equalizer is provided at the subsequent stage of the amplification optical fiber 14-2. 16 may be arranged. The equalizer group to be installed for each mode is preferably installed at an arbitrary position such as an interruption or a subsequent stage of the amplification optical fiber 14 in accordance with characteristics required for the optical amplifier.

  Although the reduction effect of MDG by bringing the wavelength of the signal light and the wavelength of the excitation light closer could be confirmed, it was limited to the short wavelength side of the L band. The cause is considered that the information on the mode of the excitation light incident as the LP11 mode is converted to the LP01 mode via the ASE on the long wavelength side, and the LP11 mode in the ASE is attenuated. It is done. Therefore, the problem is solved by using an amplification optical fiber capable of propagating ASE in a higher order mode than the signal light. In this study, an example is shown in which the amplification optical fiber is an EDF that can propagate from the LP01 mode to the LP21 mode.

ここで、Ｓ（ｘ，ｙ）は信号光、Ｐ（ｘ，ｙ）は励起光強度分布を表している。 In a multimode EDF, the gain of each mode can be determined by the magnitude of the overlap integral of the electric field strengths of the signal light and the excitation light. The magnitude of the overlap between the signal light and the excitation light can be expressed as in Equation (2).

Here, S (x, y) represents signal light, and P (x, y) represents the excitation light intensity distribution.

  The effect of adjusting the MDG by using an EDF in which not only the LP01 and LP11 modes but also the LP21 mode is used as the C-band ASE will be examined. FIGS. 10 and 11 show the relationship between the ASE mode ratio and the magnitude of the overlap integral between the signal light LP01 and LP11 modes. As for the modes included in the ASE, FIG. 10 shows an example of two modes (LP01, LP11 mode), and FIG. 11 shows an example of three modes (LP01, LP11, LP21 mode). 10 uses the LP11 mode intensity ratio with respect to the total excitation light intensity as a variable, and FIG. 11 uses the LP21 mode intensity ratio with respect to the total excitation light intensity (LP01 and LP11 have equal intensity) as a variable. By including the LP21 mode in the ASE, the magnitude of the overlap integral between the signal light LP11 mode and the LP01 mode can be adjusted more flexibly, and the adjustment of the MDG can be expected even in the L band. MDG can be reduced by using higher order modes of the signal light propagating in this way. In the EDF, since the wavelength region in which stimulated emission occurs is longer than about 1450 nm, it is desirable that the desired higher-order mode cutoff wavelength is also 1450 nm or less.

  Next, an example of MDG adjustment by changing the structural parameters of the amplification optical fiber will be described. In the amplification of the L band, as shown so far, it has been shown that it becomes difficult to maintain the mode information because the absorbed excitation light passes through the ASE. Therefore, the reduction of MDG in the L band is realized by using an EDF in which the mode of the excitation light hardly affects the MDG.

  FIG. 12 shows the structure of the EDF. It has an inner ring portion having a relative refractive index difference of 0 and a distance a1 from the core center and an outer ring portion having a relative refractive index difference Δ1 and a distance of a2 from the core center. A region that is less dependent on the mode of the excitation light is obtained using this structure. In this example, a2 was set to 12 μm, a1 was changed from 0.5 to 10 μm, and Δ1 was changed from 0.4 to 1%. Regarding the propagation modes of signal light and pumping light, the LP01, LP11, LP21, and LP31 modes will be discussed.

  The region where the MGD becomes small is obtained as follows. For example, when the EDF propagates through the signal light LP01, LP11, and LP21 modes, the intensity distribution between the LP01 mode that is the fundamental mode and the LP21 mode that is the highest order mode is different, so the difference in gain obtained in the EDF is also large. Become. That is, in the signal light LP01 mode, the highest gain is obtained in the pumping light LP01 mode, and the smallest gain is obtained in the pumping light LP21 mode. The signal light LP21 mode has the smallest gain in the pumping light LP01 mode and the largest gain in the pumping light LP21 mode. As described above, when the mode of the pumping light is the fundamental mode or the highest mode of propagation, the EDF is designed so that the MDG between the highest order and the basic mode of the signal light is reduced.

ここでＰ_ｓ，ｉはｉモード目の信号光および自然放出光の強度、ｚはＥＤＦにおける位置、νは光の波長である。位置ｚは光の伝搬方向における位置を示す。ｉモード目の信号光利得係数γ_ｅ，ｉ（ｚ，ν）と吸収係数γ_ａ，ｉ（ｚ，ν）は、各モードの規格化電界分布ψ_Ｓ，ｉ（ν，ｒ，θ）、信号光に対する放出断面積σ_ｅｓ，ｉ ^Ｓ及び励起光に対する放出断面積吸収断面積σ_ａｓ，ｉ ^Ｓを用いてそれぞれ以下のように表せる。 After describing the basic theory of amplification used for calculating the gain, MDG results under each excitation condition are shown by simulation.
The rate equation when Er ³⁺ is considered as a three-level system is solved, and the propagation equation of EDF can be expressed as Equation 3 below.

Here, P _{s, i} is the intensity of the i-mode signal light and spontaneous emission light, z is the position in the EDF, and ν is the wavelength of the light. The position z indicates a position in the light propagation direction. The i-mode signal light gain coefficient γ _{e, i} (z, ν) and the absorption coefficient γ _{a, i} (z, ν) are the normalized electric field distribution ψ _{S, i} (ν, r, θ) of each mode, Using the emission cross-sectional area σ _{es, i} ^S for the signal light and the emission cross-section absorption cross-section σ _{as, i} ^S for the excitation light, they can be expressed as follows.

N ₂ (r, θ, z) and N ₁ (r, θ, z) are the Er ³⁺ excitation level and the base when one point of the fiber cross section at the position z is expressed by the radius r and the deflection angle θ, respectively. It represents the ion density of the level. By solving the propagation equation of Formula (1) in each propagation mode, the gain of the signal light due to the difference in the mode of the excitation light can be found.

  The excitation light source of the Er-doped fiber (EDF) is generally used in the 980 nm band and 1480 nm band, but in the L band, since it is amplified through the C band ASE generated in the EDF, 1550 nm. The signal light wavelength is 1600 nm and the input power is −10 dBm.

  In conventional single mode L-band optical amplifiers, since the band gain deviation is 1 dB or less, the region where 1 dB or less is also used in MGD is used as an index. Further, in the optical amplifier according to the present embodiment, it is possible to satisfy MDG 1 dB or less in the wavelength range 1565 to 1600 nm by adjusting the EDF length and the excitation light intensity.

  FIGS. 13 and 14 show MDG calculation examples when the propagation modes of the EDF used as the amplification optical fiber 14 are LP01 and LP11 modes. FIG. 13 shows the result of setting the excitation light to the LP01 mode, and FIG. 14 shows the result of setting the excitation light to the LP11 mode. The MDG values are indicated by contour lines on a1 / a2 and Δ1. From this result, in the LP01 and LP11 modes, MDG satisfies 1 or less in the region of 0.4 ≦ Δ1 ≦ 1 and in the range of Δ1 ≧ −240 × (a1 / a2) +41.04.

  15 and 16 show MDG calculation examples when the propagation modes of the EDF used as the amplification optical fiber 14 are the LP01 and LP21 modes. FIG. 15 shows the result of setting the excitation light to the LP01 mode, and FIG. 16 shows the result of setting the excitation light to the LP21 mode. From this result, in the LP01 and LP21 modes, the MDG satisfies 1 or less in the range of 0.4 ≦ Δ1 ≦ 1 and Δ1 ≧ −678.0x (a1 / a2) +31.47.

  17 and 18 show examples of MDG calculation when the propagation mode of the EDF used as the amplification optical fiber 14 is set to the LP01 and LP31 modes. FIG. 17 shows the result of setting the excitation light to the LP01 mode, and FIG. 15 shows the result of setting the excitation light to the LP31 mode. As a result, in the LP01 and LP31 modes, the region of 0.4 ≦ Δ1 ≦ 1, Δ1 ≧ −56.2x (a1 / a2) +135.32 and Δ1 ≧ −20.66x (a1 / a2) −14 MDG satisfies 1 or less in the range of .55.

  The present invention is an optical amplifier that realizes gain adjustment for each propagation mode and lengthening of transmission distance in transmission using a plurality of modes.

11-1, 11-2, 111: excitation light sources 12-1, 12-2, 112: mode converters 13-1, 13-2: signal light excitation light multiplexers 14, 114: amplification optical fiber 15: isolator 16A , 16B, 16C: mode gain equalizer 113: mode demultiplexer 117: OSA

Claims (7)

An optical fiber for amplification capable of propagating a plurality of propagation modes equal to or higher than the propagation mode of signal light;
An excitation light source that generates excitation light having a wavelength capable of exciting the signal light in the amplification optical fiber;
A mode converter that converts excitation light from the excitation light source into at least one of the propagation modes included in the plurality of propagation modes;
A signal light pumping light multiplexer that combines the pumping light after the propagation mode is converted by the mode converter with the signal light;
An optical amplifier. A gain equalizer for equalizing gains of the plurality of propagation modes;
The loss spectrum of the gain equalizer is different for each propagation mode,
The optical amplifier according to claim 1. The amplification optical fiber is an erbium-doped fiber,
The wavelength of the signal light is 1565 nm or more and 1625 nm or less,
The wavelength of the excitation light is 1530 nm or more and 1565 nm or less.
The optical amplifier according to claim 1 or 2. A plurality of the signal light excitation light multiplexer,
One of the signal light pumping optical multiplexers combines the pumping light with the signal light at the previous stage of the amplification optical fiber, and makes the pumping light enter the amplification optical fiber,
The other signal light pumping optical multiplexer combines the pumping light with the signal light after the amplification optical fiber, and makes the excitation light enter the amplification optical fiber.
The optical amplifier according to claim 1. The highest order mode that the amplification optical fiber can propagate is higher than the highest order mode of the signal light,
The optical amplifier according to claim 1. The spontaneous emission light generated by the amplification optical fiber includes a propagation mode higher than the highest order mode of the signal light,
The optical amplifier according to claim 1. The amplification optical fiber is:
An inner ring portion having a relative refractive index difference of 0 and a distance a1 from the core center;
An outer ring portion having a relative refractive index difference of Δ1 and a distance a2 from the core center;
An erbium-doped fiber comprising:
Propagating through LP01 mode and LP11 mode and satisfying 0.4 ≦ Δ1 ≦ 1 and Δ1 ≧ (−240 × (a1 / a2) +41.04), or
Propagating through LP01 mode, LP11 mode and LP21 mode and satisfying 0.4 ≦ Δ1 ≦ 1 and Δ1 ≧ (−678.0 × (a1 / a2) +31.47), or
Propagate LP01 mode, LP11 mode, LP21 mode and LP31 mode and 0.4 ≦ Δ1 ≦ 1, Δ1 ≧ (−56.2 × (a1 / a2) +135.32) and Δ1 ≧ (−20.66 × ( a1 / a2) -14.55) is satisfied,
The optical amplifier according to claim 1.

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