JP2002303805A - Variable dispersion compensator and optical transmission system - Google Patents

Abstract

(57) Abstract: Provided is a variable dispersion compensator which is excellent in dispersion compensation accuracy and controllability and whose optical circuit is downsized, and an optical transmission system including the same. SOLUTION: The signal light to be subjected to dispersion compensation is split by an optical multiplexer / demultiplexer 2, and each frequency component of the split signal light is reflected by a corresponding reflection mirror 30 included in a reflection mirror group 3. Thus, a predetermined phase shift is given to each of the frequency components. The reflected frequency components are multiplexed by the optical multiplexer / demultiplexer 2 to obtain dispersion-compensated signal light. Also,
Regarding the reflection mirror group 3 used for imparting a phase shift to each frequency component of the signal light, a plurality of reflection mirrors 30
Are movable mirrors whose reflection positions for reflecting frequency components are variable. This makes it possible to compensate for the dispersion generated in the signal light with high accuracy and good controllability.

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a tunable dispersion compensator for compensating dispersion generated in signal light by being propagated through an optical transmission line such as an optical fiber transmission line, and an optical transmission system including the same. .

[0002]

2. Description of the Related Art In an optical transmission system for propagating signal light through an optical fiber transmission line or the like, dispersion is accumulated in light components of each frequency (each wavelength) contained in the signal light due to dispersion of the optical fiber. On the other hand, in order to suppress waveform deterioration of signal light due to propagation in an optical transmission line, it is desired to reduce the amount of dispersion in an optical transmission system in a frequency band including the signal light frequency. In addition, wavelength division multiplexing (WDM: Wavelength Division Multip
Similarly, in a lexing transmission system, it is necessary to reduce the amount of dispersion in a frequency band including the signal light frequency (signal light wavelength) of each of the multi-wavelength signal lights.

As a device for compensating for the dispersion accumulated in each frequency component of signal light, there is a dispersion compensator provided on an optical transmission line. The dispersion compensator compensates for dispersion generated in the signal light by giving an appropriate phase shift to the signal light. As such a dispersion compensator, for example, reference 1
"IEICE Technical Report (IEICE Technical Report) Vol.10
0, No. 379, OCS2000-61 ”, Reference 2“ OpplusE Vol.2
2, No. 9, p. 1151 ”and Reference 3“ OFC2000, Shi.
rasaki et al., Variable dispersion compensator usi
ng the virtually imaged phased array (VIPA) for 40
-Gbit / s WDM transmission systems ".

[0004]

In recent years, with the development of optical transmission systems, it is possible to perform dispersion compensation with higher accuracy on a dispersion compensator installed on an optical transmission line.
There is a demand for a dispersion compensator having excellent controllability of dispersion compensation. On the other hand, the conventional dispersion compensator does not provide sufficient dispersion compensation accuracy and controllability.

[0005] For example, the dispersion compensator described in the above reference 1 is an arrayed waveguide type diffraction grating (AWG: Arrayed-Wa).
veguide Grating). And
The signal light is input from the first slab waveguide side of the AWG, and the frequency components output from the opposite second slab waveguide are phase-adjusted by a spatial phase filter to compensate for the dispersion of the signal light. ing. However, in such a configuration, since a spatial phase filter is used to adjust the phase of each frequency component of the signal light, the applied phase shift is fixed, and the dispersion compensation cannot be controlled.

[0006] The dispersion compensator described in Document 2 is:
Mach Zender type optical circuit (MZI: Mach Zender Interf
This is configured to perform dispersion compensation using a planar waveguide type optical circuit in which an optical path difference is variable by an erometer. However, in such a configuration, the structure of the optical circuit becomes complicated,
Its size is also large (for example, about 5 cm square). Also, the response of the phase adjustment is low (for example, 10 m
s).

In the dispersion compensator described in Document 3, the optical path length is changed using a device that propagates signal light in space. However, such a configuration has a large system and high accuracy. Is difficult to adjust the phase. Further, the insertion loss into the optical fiber transmission line is as large as, for example, 10 dB or more.

SUMMARY OF THE INVENTION The present invention has been made to solve the above problems, and has a variable dispersion compensator which is excellent in the accuracy and controllability of dispersion compensation and whose optical circuit is downsized. An object is to provide an optical transmission system.

[0009]

In order to achieve the above object, a dispersion compensator according to the present invention is a variable dispersion compensator for compensating for dispersion of a signal light by giving a phase shift to the signal light. , (1) a signal light to be subjected to dispersion compensation is input, and a light demultiplexing means for demultiplexing the signal light within a predetermined frequency band for each frequency component; Each of the frequency components is reflected to give a predetermined phase shift to each of the frequency components, and the reflection position for each of the frequency components is variably configured in the signal light propagation direction. Optical multiplexing means for multiplexing frequency components to obtain dispersion-compensated signal light.

In the tunable dispersion compensator described above, a predetermined difference is used for each frequency component of the signal light by utilizing an optical path length difference from the optical demultiplexing means to the optical multiplexing means via the reflection means. Give a phase shift. The phase shift given to each frequency component is made variable by using a reflection unit that makes the reflection position variable for each frequency component.

With such a configuration, it is possible to compensate for the dispersion generated in the signal light with high accuracy. Further, by controlling the reflection position of each frequency component at the reflection means, it is possible to control dispersion compensation by giving a phase shift. Further, since the dispersion compensation is controlled only by the reflection means, the structure of the optical circuit can be simplified, and the optical circuit can be downsized.

Here, it is preferable that the optical demultiplexing means and the optical multiplexing means comprise a single optical multiplexing / demultiplexing means. Thereby, the configuration of the tunable dispersion compensator can be simplified.

As a configuration of the reflection means, the reflection means is composed of a plurality of reflection mirrors divided corresponding to frequency components, and each of the plurality of reflection mirrors individually moves its reflection surface in the signal light propagation direction. The movable mirror can be configured to be movable.

As a driving method of the reflecting means in this configuration, a movable mirror as each of a plurality of reflecting mirrors is used.
The reflecting surfaces are individually moved using electrostatic force generated by applying a voltage between a first electrode provided on a movable mirror and a second electrode provided at a predetermined position with respect to the first electrode. It is preferable that it is constituted so that it can be performed.

Further, as another configuration of the reflection means, the reflection means comprises a single reflection mirror, and the single reflection mirror deforms the entire reflection surface to thereby provide a reflection surface corresponding to the frequency component. Each of the portions may be a movable mirror capable of moving in the signal light propagation direction.

As a driving method of the reflecting means in this configuration, a movable mirror as a single reflecting mirror is provided at a first electrode provided on the movable mirror and at a predetermined position with respect to the first electrode. It is preferable that the entire reflecting surface is deformable by using an electrostatic force generated by applying a voltage between the second electrode and the second electrode.

The reflecting means having these structures can be manufactured by using, for example, MEMS (Micro Electro Mechanical System) technology. As for the driving method, by controlling the driving of the movable mirror using the electrostatic force as described above, the control of the phase shift and the dispersion compensation by the phase shift can be sped up.

The arrangement of the reflection mirrors constituting the reflection means or the shape of the reflection surface is substantially parabolic with respect to the frequency component to be reflected. Thereby, when the second-order dispersion D ⁽²⁾ is dominant in the dispersion generated in the optical transmission line, the dispersion compensation for the signal light can be satisfactorily performed over the entire frequency band targeted for dispersion compensation. Can be realized.

The optical transmission system according to the present invention comprises:
(A) an optical transmission line for transmitting signal light having a frequency component within a predetermined frequency band; and (b) compensation for dispersion generated in signal light that is installed at a predetermined position on the optical transmission line and propagates through the optical transmission line. And the variable dispersion compensator described above.

As a result, an optical transmission system is realized in which dispersion generated in signal light propagating through an optical transmission line such as an optical fiber transmission line is compensated with high accuracy and good controllability, thereby preventing waveform deterioration of the signal light and the like. Is done.

The bit rate of the signal light is 10 Gbp.
s or more. Alternatively, the bit rate is 40 Gbps or more. At such a high bit rate, dispersion is particularly problematic in the optical transmission line, but in such a case,
By applying the variable dispersion compensator having the above configuration,
Sufficient dispersion compensation can be performed on the signal light.

[0022]

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Preferred embodiments of a tunable dispersion compensator and an optical transmission system according to the present invention will be described below in detail with reference to the drawings. In the description of the drawings, the same elements will be denoted by the same reference symbols, without redundant description.
Also, the dimensional ratios in the drawings do not always match those described.

First, a schematic configuration of the variable dispersion compensator will be described. FIG. 1 is a configuration diagram schematically showing an embodiment of the variable dispersion compensator according to the present invention. The tunable dispersion compensator 1 of the present embodiment compensates the dispersion of the signal light by giving a predetermined phase shift to the input signal light,
It comprises an optical multiplexer / demultiplexer 2 and a reflection mirror group 3. In the dispersion compensation function, the amount of phase shift given to each frequency component of the signal light for dispersion compensation is variable.

A signal light having a frequency component (wavelength component) within a predetermined frequency band (wavelength band) and subject to dispersion compensation is input from the input terminal 1a of the tunable dispersion compensator 1 and has a predetermined phase shift. Is output from the output terminal 1b as dispersion-compensated signal light. Input terminal 1a and output terminal 1
The optical transmission line 11 through which the signal light propagates is provided between the optical transmission line 11 and the optical transmission line b.

An optical circulator 12 is provided at a predetermined position on the optical transmission line 11. The optical circulator 12 is connected to an optical transmission line 13 for dispersion compensation. As a result, the signal light before dispersion compensation from the optical transmission line 11 on the input end 1a side passes through the optical circulator 12 and is output to the optical transmission line 13. Also, the optical transmission line 13
The signal light having undergone the dispersion compensation from the optical signal passes through the optical circulator 12 and is output to the optical transmission line 11 on the output end 1b side.

The end of the dispersion compensating optical transmission line 13 opposite to the optical circulator 12 is provided with the optical multiplexer / demultiplexer 2.
And the reflection mirror group 3 are installed in this order. The optical multiplexer / demultiplexer 2 and the reflection mirror group 3 give a phase shift to the signal light, and the dispersion thereof is compensated.

The optical multiplexer / demultiplexer 2 receives the signal light before dispersion compensation, and functions as an optical demultiplexing means for demultiplexing the signal light within a predetermined frequency band for each frequency component. This is a single optical multiplexing / demultiplexing unit having a function as an optical multiplexing unit that multiplexes the components and makes the signal light after dispersion compensation. The signal light to be subjected to dispersion compensation is split or multiplexed by the optical multiplexer / demultiplexer 2 at a frequency ν (wavelength λ) along a predetermined demultiplexing direction (the ν axis direction shown in FIG. 1). You.

The reflection mirror group 3 is a reflection unit that reflects each frequency component of the signal light demultiplexed by the optical multiplexer / demultiplexer 2 and gives a predetermined phase shift to each frequency component. The phase shift is performed again from the optical multiplexer / demultiplexer 2 (optical demultiplexer) via the reflecting mirror group 3 (reflector).
It is given to each frequency component of the signal light by using the optical path length and the optical path length difference until reaching the (optical multiplexing means). Also,
The reflection mirror group 3 is configured such that the reflection position for each frequency component is variable in the signal light propagation direction (the d-axis direction shown in FIG. 1).

The reflecting mirror group 3 serving as the reflecting means in the present embodiment is composed of a plurality of reflecting mirrors 30 divided for each frequency corresponding to each frequency component of the signal light split by the optical multiplexer / demultiplexer 2. Become. These reflection mirrors 30 are arranged substantially continuously with the ν-axis direction, which is the direction in which the signal light is demultiplexed and substantially perpendicular to the signal light propagation direction, arranged. A reflection mirror group 3 that reflects the frequency components of the signal light is configured.

Each of the reflecting mirrors 30 constituting the reflecting mirror group 3 has a constant reflecting surface shape, but can move individually and independently in the d-axis direction which is the signal light propagation direction. It is a possible movable mirror.

In the above configuration, the signal light to be subjected to dispersion compensation, which is input to the tunable dispersion compensator 1 from the input terminal 1 a, is optically coupled through the optical transmission line 11, the optical circulator 12, and the optical transmission line 13. The signal is input to the wave device 2 and is divided into each frequency component by the frequency ν. Each frequency component of the demultiplexed signal light is propagated toward the reflecting mirror group 3, and
The light is reflected at a predetermined reflection position by the corresponding reflection mirror 30 of the reflection mirror group 3. Each of the reflected frequency components is multiplexed again by the optical multiplexer / demultiplexer 2 to become a signal light after dispersion compensation, and is output from the output terminal 1 b via the optical transmission line 13, the optical circulator 12, and the optical transmission line 11. Output to the outside.

Here, each reflection mirror 3 of the reflection mirror group 3
The reflection position of the frequency component of the signal light at 0 is determined based on the amount of phase shift to be given to the frequency component. By driving and controlling each of the reflecting mirrors 30 which are movable mirrors and moving them in the signal light propagation direction so as to be at the set reflection positions, dispersion compensation for the signal light within the entire frequency band can be performed. Realize.

Next, an optical transmission system including the above-described variable dispersion compensator will be described. FIG. 2 is a configuration diagram schematically showing an embodiment of the optical transmission system according to the present invention.

The optical transmission system of this embodiment includes a transmitter (transmitting station) T for transmitting signal light and an optical fiber transmission line L which is an optical transmission line for transmitting the signal light transmitted from the transmitter T.
And a receiver (receiving station) R for receiving the signal light propagated through the optical fiber transmission line L.

At a predetermined position on the optical fiber transmission line L, a tunable dispersion compensator 1 having the configuration shown in FIG. 1 is installed. The variable dispersion compensator 1 is preferably provided at a position on the optical fiber transmission line L close to the receiver R, for example, at a position immediately before the receiver R. Accordingly, the dispersion accumulated in the signal light while propagating through the optical fiber transmission line L from the transmitter T to the receiver R is compensated for by the variable dispersion compensation before the signal light is received by the receiver R. The dispersion compensation is performed by the device 1.

In the tunable dispersion compensator and the optical transmission system according to the present embodiment, the optical multiplexer / demultiplexer 2 serving as an optical demultiplexer is used.
The phase shift is given to each frequency component of the signal light by utilizing the optical path length until the signal light demultiplexed by the above is multiplexed again by the optical multiplexer / demultiplexer 2 which is the optical multiplexing means. Then, for the reflection mirror group 3 which is a reflection means used for setting the optical path length and the phase shift for each frequency component, the reflection position of the frequency component by the plurality of reflection mirrors 30 constituting the reflection mirror group 3 is determined. The reflection mirror 30 is variable.

As a result, since the phase shift given to each frequency component is variable, any phase adjustment can be performed, and the dispersion generated in the signal light can be compensated with high accuracy. Further, since the reflection position of the frequency component by each of the reflection mirrors 30 constituting the reflection mirror group 3 can be individually controlled, the amount of phase shift given to the signal light can be controlled with good controllability and dispersion compensation can be performed. The conditions can be set or changed in detail.

Further, since the dispersion compensation is controlled only by the reflection means, the structure of the optical circuit can be simplified and the optical circuit can be downsized. In addition, such a reflection means is, for example, a MEMS (Micro Electro
It can be manufactured using Mechanical System) technology.

According to the optical transmission system to which the variable dispersion compensator having such a configuration is applied, the optical fiber transmission line L
Thus, an optical transmission system is realized in which dispersion generated in signal light propagating through an optical transmission path is compensated with high accuracy and good controllability, and waveform deterioration of the signal light is reliably prevented.

In the tunable dispersion compensator 1 shown in FIG. 1, the optical demultiplexing means for demultiplexing the signal light before dispersion compensation into frequency components, and the signal light after dispersion compensation by combining the frequency components. The optical multiplexing means is a single optical multiplexing / demultiplexing device 2. Thereby, the configuration of the tunable dispersion compensator 1 can be simplified, and the optical circuit can be further downsized. However, these optical demultiplexing means and optical multiplexing means may be separately configured.

FIG. 3 is a plan view showing a specific configuration example of the variable dispersion compensator according to the embodiment shown in FIG. In FIG. 3, the optical transmission line 11 and the optical circulator 12 are not shown, but only an optical circuit including an optical multiplexer / demultiplexer 2 and a reflection mirror group 3 for actually performing dispersion compensation on signal light is shown. ing.

In the tunable dispersion compensator 1 of this embodiment,
As an optical multiplexer / demultiplexer 2 for demultiplexing or multiplexing signal light to be subjected to dispersion compensation, an arrayed waveguide type diffraction grating (AWG) using a planar waveguide type optical circuit formed on a substrate 10 with a predetermined waveguide pattern. : Arrayed Waveguide Grating) 2a is used.

The AWG 2a has an input / output channel waveguide 21 whose end is an input / output port, and a first slab waveguide 22 connected to the input / output channel waveguide 21.
And an arrayed waveguide section 23 composed of a plurality of channel waveguides connected to the first slab waveguide 22 and having different optical path lengths from each other, and a second slab waveguide 24 connected to the arrayed waveguide section 23. It is configured.

Array waveguide section 2 of second slab waveguide 24
A channel waveguide group 25 including a plurality of (n) channel waveguides 26 _{1 to} 26 _n is further connected to the side opposite to 3. On the other side of the group of channel waveguides 25 opposite to the second slab waveguide 24, n channel waveguides 2
_{6 1, 26 2, ...,} n number of movable reflective mirror 30 ₁ corresponding respectively to 26 _n, 30 _2, ..., the reflection mirror group 3 consisting of 30 _n are provided. These reflecting mirrors 30 ₁ to
30 _n is the substrate on the channel waveguide group 25 of the groove 31 formed so as to cross 10, respectively so as to reflect the corresponding signal light component can which is propagated through the channel waveguides 26 ₁ ~ 26 _n Installation Have been.

More specifically, the groove 31 extends substantially perpendicular to the signal light propagation direction in the channel waveguides 26 _{1 to} 26 _n of the channel waveguide group 25 and along the direction in which the signal light is split. (See FIG. 1). Then, the reflection mirror 30 ₁ to 30 _n of the reflection mirror group 3, in the groove portion within 31, each facing the corresponding channel waveguide 26 ₁ ~ 26 _n position (facing the core part of the channel waveguide position) is set up.

In the above configuration, when the signal light is input from the input / output port of the AWG 2a to the input / output channel waveguide 21, the first slab waveguide 22, the array waveguide section 2
While the signal light is sequentially guided through the third and second slab waveguides 24, the signal light is demultiplexed for each frequency (for each wavelength). Each frequency component of the demultiplexed signal light is divided and input to each of the channel waveguides 26 _{1 to} 26 _n of the channel waveguide group 25.

The frequency components propagated through each of the channel waveguides 26 _{1 to} 26 _n are reflected by the corresponding movable reflecting mirrors 30 ₁ to 30 _n of the reflecting mirror group 3, and again reflected by the channel waveguides 26 _{1 to} 26 _n . Each is propagated in the opposite direction. Then, the second slab waveguide 24 and the array waveguide section 2
3, while being guided sequentially through the first slab waveguide 22, the respective frequency components are multiplexed and output from the input / output port as dispersion-compensated signal light via the input / output channel waveguide 21. Is done.

Here, as described above, the reflecting mirror group 3 as the reflecting means in this embodiment is constituted by a plurality of movable reflecting mirrors 30 whose reflecting surfaces can be individually moved. As a method of driving these movable reflection mirrors 30, an electrode (first electrode) provided on the movable mirror 30 and an electrode (second electrode) provided at a predetermined position with respect to the first electrode are provided. It is preferable to control the drive using an electrostatic force generated by applying a voltage. As a result, it is possible to easily and quickly control the position of reflection by the reflection mirror, the amount of phase shift set thereby, and the condition of dispersion compensation.

FIG. 4 is a configuration diagram showing an example of a movable reflection mirror used for the reflection mirror group in the variable dispersion compensator shown in FIG. The reflection mirror group 3 has a plurality of movable reflection mirrors 30 arranged in the groove 31 as described above. Guide rails 32 are provided between the adjacent movable reflection mirrors 30 to guide the moving direction of the movable reflection mirror 30.

Each movable reflection mirror 30 is supported by a mirror support 33 preferably made of an insulator. The mirror support portion 33 is movable about an end opposite to the reflection mirror 30 as a fulcrum, and an electrode 34 serving as a first electrode is formed on one side thereof. Also,
An electrode 35 serving as a second electrode is provided on the opposite side of the electrode 34 with the mirror support 33 interposed therebetween. This electrode 35
It is fixed to the substrate 10.

Electrode 34 provided on mirror support 33
A variable power supply for variably applying a voltage is connected between the power supply and the electrode 35 fixed to the substrate 10. When the applied voltage between the electrode 34 and the electrode 35 is changed, the generated electrostatic force or its change causes the mirror support 33 to bend, and the movable reflection mirror 30 works in conjunction with the bend to guide the guide rail 32. Move in the direction of movement guided by.

FIG. 5 is a configuration diagram showing another example of the movable reflection mirror. In the reflecting mirror group 3, the movable reflecting mirror 30, the guide rail 32, and the mirror support 33 arranged in the groove 31 are the same as those in the configuration example of FIG. The structure of the electrodes is different.

The mirror support 33 has comb-shaped electrodes 36 formed on both sides thereof. On the other hand, on both sides of the mirror support 33, the same comb-shaped electrode 37,
38 are provided. These electrodes 36, 3
By changing the voltage applied to each of the mirrors 7 and 38, the movable reflection mirror 30 moves. When the comb-shaped electrode is used as described above, the reflection mirror 30 can be efficiently and accurately driven.

FIG. 1 shows dispersion occurring in signal light in an optical transmission system and dispersion compensation by a variable dispersion compensator.
This will be further described with reference to FIG. In the following, the light intensity of the signal light to be subjected to dispersion compensation is represented by the value of the amplitude | E | of the electric field or its square value.

In the optical transmission system, the signal light propagated through the optical fiber transmission line L is, as shown in FIG.
In, the light intensity | E | is generated so as to have a predetermined signal waveform A, and is transmitted as an input signal light to the optical transmission system. This input signal light has a signal light frequency ν ₀ (signal light wavelength λ ₀ = c / ν ₀ ) as a center frequency,
It has a signal light component spread in a predetermined signal light frequency band (wavelength band).

When such signal light propagates through the optical fiber transmission line L, dispersion in the optical fiber transmission line L is accumulated in the signal light. Then, in the signal light after the propagation, as shown as a signal waveform B in FIG. 2, the signal waveform of the light intensity | E '|

The signal light having the waveform deterioration is targeted for dispersion compensation, and the variable dispersion compensator 1 disperses the signal light into each frequency component of the signal light so as to cancel the phase shift due to the dispersion accumulated in the optical fiber transmission line L. A phase shift for compensation is given to compensate for the dispersion. As a result, a signal light having a signal waveform C of light intensity | E ″ | is obtained in which the influence of dispersion due to propagation through the optical fiber transmission line L has been removed as much as possible.

More specifically, when the second-order dispersion (dispersion) D ⁽²⁾ and the third-order dispersion (dispersion slope) D ⁽³⁾ exist in the optical fiber transmission line L, the signal of the wavelength λ (= c / ν) The value of the total dispersion D for the light component is represented by the following equation, where D is the group delay time, and D (λ) = dτ / dλ = D ⁽²⁾ + D ⁽³⁾ (λ−λ ₀ ). Here, λ ₀ is the center wavelength of the signal light described above.

Assuming that the secondary dispersion D ⁽²⁾ is dominant in the total dispersion D, the group delay time τ for the signal light component of the wavelength λ is τ (λ) = D ⁽²⁾ (λ−λ ₀ ). At this time, a phase shift φ due to dispersion generated in each signal light component of the signal light propagated through the optical fiber transmission line L.
Sets the phase shift at the center frequency ν ₀ (center wavelength λ ₀ ) to 0.
Is as follows.

Φ = −πcD ⁽²⁾ ((ν−ν ₀ ) / ν ₀ ) ^{2 The} rate of change of the phase shift φ is: dφ / dν = − (2πcD ⁽²⁾ / ν ₀ ² ) × (ν −ν ₀ ). That is, in the signal light propagating through the optical fiber transmission line L, a phase shift that changes in a parabolic manner around the center frequency ν ₀ occurs due to the dispersion D ⁽²⁾ .

The signal light having such a phase shift undergoes dispersion compensation by the variable dispersion compensator 1 shown in FIGS. Here, as shown in FIG. 1, the total frequency band width of the entire reflecting mirror group 3 which is a frequency band for performing dispersion compensation is 2δν, and the frequency width of each of the plurality of reflecting mirrors 30 included in the reflecting mirror group 3 Let Δν be the dispersion compensation resolution.

Each of the reflecting mirrors 30 ₁ to 30 _n included in the reflecting mirror group 3 has a reflecting mirror 30 _i.
The center frequency of the frequency component of the signal light reflected by ν _i is denoted by ν _i , and the phase shift given to each frequency component of the signal light for dispersion compensation is denoted by ψ.

As for the reflection position of each frequency component by each of the reflection mirrors 30 ₁ to 30 _n , the phase shift given to the frequency component of the signal light by the reflection at the reflection mirror 30 _i is ψ = −φ (ν _i ). Thus, the phase shift φ in the optical fiber transmission line L is set to be canceled at the center frequency ν _i of the reflection mirror 30 _i .

After the reflection position for each of the reflection mirrors 30 is set, each movable reflection mirror 30 is moved to the set reflection position. As a result, a configuration capable of compensating for dispersion in the optical transmission system is realized. Movable reflective mirror 30 _i for providing phase shift ψ = −φ (ν _i )
The position d (see FIG. 1) can be obtained by the following expression d = cφ (ν _i ) / 4πnν _i, where n is the refractive index of the medium between the optical multiplexer / demultiplexer 2 and the reflecting mirror group 3.

Here, as in the above-described example, the reflection mirror group 3 serving as the reflection means is divided into a plurality of divided reflection mirrors 30.
, The amount of phase shift 与 え given to the frequency component of the signal light is constant within the range of each reflection mirror 30. Therefore, in order to effectively perform dispersion compensation on the signal light, the phase shift φ (ν) generated in the signal light does not significantly change within the frequency range Δν corresponding to one reflection mirror 30. In addition, it is preferable to set the frequency resolution Δν of dispersion compensation in the reflection mirror group 3. Specifically, the rate of change dφ / dν of the phase shift φ
In contrast, it is preferable that the frequency resolution Δν satisfies the following condition.

| Δν × (dφ / dν) | ≦ π Assuming that the secondary dispersion D ⁽²⁾ is dominant in the total dispersion D, the absolute value of the rate of change of the phase shift φ | (dφ / dν) |
The frequency ν = ν ₀ ± δν, i.e. away from the center frequency [nu ₀ only half the frequency .DELTA..nu full width 2Derutanyu, a maximum in the frequency components comprising the end of the frequency band, its maximum value, | dφ / dν | _max = | 2πcD ⁽²⁾ δν / ν ₀ ² | Therefore, the above-mentioned preferred conditions | Δν × (dφ / dν) | maximum value satisfy ≦ [pi compensable dispersion D ⁽²⁾ is, | D ⁽²⁾ | a _max = _{ν 0} ² / _2cΔνδν.

For example, for the signal light to be subjected to dispersion compensation, the center frequency is ν ₀ = 189.1 THz (the center wavelength is λ ₀ = 1585 nm), and the half width of the frequency band is δν.
= 50 GHz, and the frequency resolution, which is the frequency range per one reflecting mirror, is Δν = 5 GHz, the maximum dispersion that can be compensated is | D ⁽²⁾ | _max = 240 ps / nm. Further, under the same conditions, the half width of the frequency band is set to δν = 15 GHz.
Assuming that z and the frequency resolution are Δν = 3 GHz, the maximum dispersion that can be compensated is | D ⁽²⁾ | _max = 1300 ps / nm.

From the above expression, it can be seen that the value of the maximum dispersion | D ⁽²⁾ | _{max that} can be compensated increases by reducing the frequency resolution Δν. Regarding the frequency resolution Δν, the specific configuration of the tunable dispersion compensator, for example, the conditions for demultiplexing the signal light by the AWG 2a in the tunable dispersion compensator 1 shown in FIG. It is preferable to set a suitable value in consideration of the width of the mirror and the like.

Here, a specific configuration example of the tunable dispersion compensator 1 including the AWG 2a shown in FIG. 3 will be described. Channel waveguide group 25 connected to second slab waveguide 24
Adjacent channel waveguides between intervals [Delta] x of, if the wavelength spacing of the frequency components of adjacent channel waveguides are propagating signal light and [Delta] [lambda], the following equation _{Δx / Δλ = N c fΔL /} n s Δxλ 0 Holds. Here, N _c is the group refractive index of the waveguide, f is the length in the longitudinal direction of the slab waveguide, ΔL is the optical path length difference between the channel waveguides in the arrayed waveguide, and n _s is the effective refraction of the slab waveguide. Rate. Among these, the group refractive index _Nc and the effective refractive index _ns are each about 1.5.

On the other hand, the center wavelength of the signal light is λ ₀ =
1550 nm, the frequency band for performing dispersion compensation is 2δν = 1
00 GHz (corresponding to a wavelength band of 0.8 nm), this frequency band is divided into 10 and the frequency resolution is Δν = 10 GH
z. At this time, the wavelength resolution is Δλ = 0.08n
m. The distance between the channel waveguides is Δx = 2
0 μm.

By substituting these numerical values, fΔL = 7.75 × 10 ⁻⁶ m is obtained as a configuration condition to be satisfied by the AWG 2a of the tunable dispersion compensator 1. This condition is, for example, that the slab waveguide is f =
This can be satisfied by a configuration in which the length is 30 mm and the array waveguide portion is ΔL = 258 μm.

The frequency band 2δν of the dispersion compensation is preferably set so as to sufficiently include a frequency range in which the signal light component of the signal light to be subjected to the dispersion compensation is distributed.

Further, if the signal light to be subjected to dispersion compensation is a multi-wavelength signal light composed of a plurality of signal lights having different signal light wavelengths, a single signal light included in the multi-wavelength signal light is In the case of performing dispersion compensation by using, for example, the frequency interval between adjacent signal lights can be set to the full frequency width 2δν. If the total frequency width 2δν is larger than the frequency interval between signal lights (for example, an integral multiple), dispersion compensation can be performed on a plurality of signal lights included in the multi-wavelength signal light.

The bit rate (modulation rate) of the signal light
The bit rate is preferably 10 Gbps or more, or more preferably, 40 Gbps or more. At such a high bit rate, dispersion is particularly problematic in the optical transmission line, but even in such a case, by applying the tunable dispersion compensator having the above configuration, the signal light can be reduced. Dispersion compensation can be performed satisfactorily with sufficient accuracy. However, the variable dispersion compensator 1
It is needless to say that can be effectively applied to the signal light having the smaller bit rate.

It is preferable that the arrangement of the reflecting mirrors constituting the reflecting means or the shape of the reflecting surface is substantially parabolic with respect to the frequency component to be reflected. Thereby, when the second-order dispersion D ⁽²⁾ is dominant in the dispersion generated in the optical transmission line, the dispersion compensation for the signal light can be satisfactorily performed over the entire frequency band targeted for dispersion compensation. Can be realized.

In the optical transmission system and the tunable dispersion compensator having the above-described configurations, simulation is performed by applying specific conditions to the waveform deterioration of the signal light due to the dispersion in the optical transmission line and the dispersion compensation for the signal light. The effect was confirmed.

With respect to the signal light to be subjected to dispersion compensation,
The center frequency is ν ₀ = 189.1 THz (the center wavelength is λ ₀ = 1585 nm), and the light modulation method is NR.
Z and the modulation speed (bit rate) M were set to 10 Gbps or 40 Gbps. In addition, the waveform of the optical pulse of the signal light was a non-chirp super-Gaussian shape.
At this time, the duration of the 1-bit signal is set to 2t ₀ (= 1 /
M), the signal waveform of the signal light is given by E (t) = exp {−log 2/2 × (t / t ₀ ) ^2m }. Here, m is a parameter that determines the light pulse shape, and here, m = 2.

The signal light actually subjected to dispersion compensation was evaluated by transmitting a random code of 2 ⁹ = 512 bits and displaying the obtained signal waveform in an eye pattern.

First, an example of dispersion compensation when the bit rate is M = 10 Gbps will be described. This bit rate 10
In Gbps, the clock that is the period of the signal is 100p
s.

FIG. 6 is a graph showing an example of the signal light transmitted through the 10 Gbps optical transmission system.
(A) shows the signal waveform of the input signal light immediately after the transmitter (FIG. 2).
6 (b) shows the signal waveform of the output signal light before dispersion compensation (without dispersion compensation) (see signal waveform B in FIG. 2).

The input signal light having the signal waveform shown in FIG. 6A has a frequency component in a frequency range of about ± 15 GHz around the signal light frequency ν ₀ = 189.1 THz. On the other hand, the dispersion generated in the signal light by propagating through the optical transmission line is represented by D ⁽²⁾ = + 1200
Assuming that ps / nm and D ⁽³⁾ = 0 ps / nm ² , the output signal light after propagation has a signal waveform in which the waveform is deteriorated due to dispersion, as shown in FIG.

FIG. 7 is a graph showing an example of dispersion compensation for signal light transmitted through the 10 Gbps optical transmission system. FIG. 7 (a) shows the phase shift of the signal light, and FIG. 3 shows a signal waveform of an output signal light after dispersion compensation (with dispersion compensation) (see signal waveform C in FIG. 2).

Here, in FIG. 7A, the horizontal axis represents the relative frequency ν with respect to the center frequency ν ₀ = 189.1 THz.
−ν ₀ (GHz). The vertical axis represents the variance D
⁽²⁾ = phase shift change rate dφ / dν (rad / GHz) corresponding to +1200 ps / nm, and phase shift φ,
−ψ (rad).

For each frequency component of the input signal light shown in FIG. 6A, the dispersion D.sub. ⁽²⁾ in the optical transmission line causes the output signal light after propagation shown in FIG. , FIG.
A parabolic phase shift φ shown in FIG.
On the other hand, in the present embodiment, the half width of the frequency band is δν
= 15 GHz and frequency resolution Δν = 3 GHz to perform dispersion compensation.

At this time, in the tunable dispersion compensator 1, a phase shift 示 す shown by a graph ψ in FIG. 7A is given to each frequency component of the signal light. This frequency width Δν =
The graph of the stepwise phase shift ψ at 3 GHz corresponds to the arrangement of the plurality of reflection mirrors 30 in the reflection mirror group 3. That is, the horizontal axis direction of the phase shift ψ corresponds to the position of the reflection mirror 30 in the ν-axis direction. The vertical axis direction corresponds to the position of the reflection mirror 30 in the d-axis direction (see FIG. 1).

As shown in FIG. 7 (a), the reflection mirror group 3 has two phase shifts at the center frequency ν _i of the frequency component Δν reflected by each reflection mirror 30 _i. ψ = φ (ν _i ). With such a configuration, the phase shift φ generated in the signal light in the optical transmission line is canceled as much as possible by the phase shift 与 え given by the tunable dispersion compensator 1. And FIG.
As shown in (b), the signal waveform of the output signal light after dispersion compensation, the dispersion of the signal light is sufficiently compensated.

FIG. 8 is a graph showing another example of dispersion compensation for the signal light transmitted through the 10 Gbps optical transmission system. FIG. 8A shows the phase shift of the signal light, and FIG.
FIG. 8B shows the signal waveform of the output signal light after dispersion compensation. In the graph of FIG. 8A, the phase shift change rate dφ / dν and the phase shift φ are shown in FIG.
It is the same as that shown in FIG.

For each frequency component of the input signal light shown in FIG. 6A, the dispersion D ⁽²⁾ in the optical transmission line causes the output signal light after propagation shown in FIG. , FIG.
A parabolic phase shift φ shown in FIG.
On the other hand, in the present embodiment, the half width of the frequency band is δν
= 15 GHz and the frequency resolution was Δν = 1 GHz to perform dispersion compensation.

At this time, in the tunable dispersion compensator 1, a phase shift 示 す shown by a graph ψ in FIG. 8A is given to each frequency component of the signal light. This frequency width Δν =
The graph of the stepwise phase shift ψ at 1 GHz corresponds to the arrangement of the plurality of reflection mirrors 30 in the reflection mirror group 3.

As shown in FIG. 8A, the reflection mirror group 3 has two phase shifts at the center frequency ν _i with respect to the frequency component of the frequency width Δν reflected by each reflection mirror 30 _i. ψ = φ (ν _i ). With such a configuration, the phase shift φ generated in the signal light in the optical transmission line is canceled as much as possible by the phase shift 与 え given by the tunable dispersion compensator 1. And FIG.
As shown in (b), the signal waveform of the output signal light after dispersion compensation, the dispersion of the signal light is sufficiently compensated. In particular, in this embodiment, the frequency resolution Δν is set to 3 GHz in the example shown in FIG.
By setting the frequency to 1 GHz, which is smaller than that, the accuracy of dispersion compensation is improved.

Next, an example of dispersion compensation when the bit rate is M = 40 Gbps will be described. This bit rate 40
In Gbps, the clock that is the period of the signal is 25 ps.
It is.

FIG. 9 is a graph showing an example of the signal light transmitted through the 40 Gbps optical transmission system.
FIG. 9A shows the signal waveform of the input signal light immediately after the transmitter, and FIG. 9B shows the signal waveform of the output signal light before dispersion compensation.

The input signal light having the signal waveform shown in FIG. 9A has a frequency component in a frequency range of about ± 50 GHz around the signal light frequency ν ₀ = 189.1 THz. On the other hand, the dispersion generated in the signal light by propagating through the optical transmission line is represented by D ⁽²⁾ = + 200p
Assuming that s / nm and D ⁽³⁾ = 0 ps / nm ² , the output signal light after propagation has a signal waveform in which the waveform has deteriorated due to dispersion, as shown in FIG. 9B.

FIG. 10 is a graph showing an example of dispersion compensation for signal light transmitted through the 40 Gbps optical transmission system. FIG. 10 (a) shows the phase shift of the signal light, and FIG. 5 shows a signal waveform of output signal light after dispersion compensation.

Here, in FIG. 10A, the horizontal axis is
The relative frequency ν-ν ₀ (GHz) with respect to the center frequency ν ₀ = 189.1 THz is shown. The vertical axis represents the phase shift change rate dφ / dν (rad / GHz) corresponding to the dispersion D ⁽²⁾ = + 200 ps / nm, and the phase shift φ,
−ψ (rad).

For each frequency component of the input signal light shown in FIG. 9A, the dispersion D ⁽²⁾ in the optical transmission line causes the output signal light after propagation shown in FIG. , FIG.
A parabolic phase shift φ shown in FIG. On the other hand, in the present embodiment, dispersion compensation was performed by setting the half width of the frequency band to δν = 50 GHz and the frequency resolution to Δν = 2 GHz.

At this time, in the tunable dispersion compensator 1, a phase shift 示 す shown by a graph ψ in FIG. 10A is given to each frequency component of the signal light. This frequency width Δν
The graph of = stepwise phase shift at 2 GHz corresponds to the arrangement of the plurality of reflection mirrors 30 in the reflection mirror group 3.

As shown in FIG. 10 (a), the reflection mirror group 3 has two phase shifts at the center frequency ν _i for the frequency components of the frequency width Δν reflected by the respective reflection mirrors 30 _i. ψ = φ (ν _i ). With such a configuration, the phase shift φ generated in the signal light in the optical transmission line is canceled as much as possible by the phase shift 与 え given by the tunable dispersion compensator 1. And FIG.
The dispersion of the signal light is sufficiently compensated so that the signal waveform of the output signal light after dispersion compensation is shown in FIG.

The tunable dispersion compensator according to the present invention and the optical transmission system including the same are not limited to the above-described embodiments and examples, and various modifications are possible.

For example, in the above-described embodiment, as shown in FIGS. 1 and 3, the reflecting mirror group 3 including a plurality of movable reflecting mirrors 30 is used as the reflecting means. Can be used.

FIG. 11 is a diagram showing another example of a movable reflection mirror used as a reflection means in the variable dispersion compensator. FIG. 11A is a schematic diagram showing the shape and driving method, and FIG. FIG. 2B is a configuration diagram showing a specific example. The reflecting means 4 shown in FIG. 11 includes a single movable reflecting mirror 40.

This movable reflection mirror 40 is similar to that shown in FIG.
As shown in (1), by deforming the curved surface shape of the entire reflecting surface (for example, to a parabolic shape), each of the reflecting surface portions corresponding to each frequency component of the signal light is moved in the signal light propagation direction. It has become possible. This makes it possible to variably and accurately perform dispersion compensation, similarly to the reflection mirror group 3 including the plurality of divided movable reflection mirrors 30.

A specific configuration of the reflecting means 4 having such a single movable reflecting mirror 40 is, for example, shown in FIG.
There is a configuration example shown in FIG. In this reflection means 4, a metal layer 40 serving as a movable reflection mirror is formed on the polysilicon layer 41.
Are formed. The metal layer 40 also functions as a first electrode provided on the movable mirror.

On the opposite side of the polysilicon layer 41 from the metal layer 40, a metal layer 43 formed on the silicon layer 44 is arranged. This metal layer 43 is a second electrode provided at a predetermined position with respect to the first electrode. Further, the polysilicon layer 41 and the metal layer 43 are
Separated by two. This silicon oxide layer 42
Are provided for the ends of the polysilicon layer 41 and the metal layer 43.

A metal layer 40 serving as a first electrode and a metal layer 43 serving as a second electrode function as a movable reflection mirror.
Is connected to a variable power supply for variably applying a voltage. When the applied voltage between the metal layer 40 and the metal layer 43 is changed, the generated electrostatic force or the change causes the deflection of the metal layer 40 and the polysilicon layer 41 in the central portion where the silicon oxide layer 42 is not provided. Occurs, the curved surface shape of the reflecting surface is deformed, and each of the reflecting surface portions moves. The reflection means 4 having such a configuration is, for example, an AWG similar to the embodiment shown in FIG.
Is preferably installed along the output end of the second slab waveguide.

The optical multiplexer / demultiplexer for demultiplexing and multiplexing the signal light is not limited to AWG, but various types may be used. Alternatively, the optical multiplexer / demultiplexer may be provided separately. Is also good. Further, the demultiplexing of the signal light may be performed such that the signal light is divided into a plurality of frequency components, depending on the configuration of the reflection means, or may be continuously demultiplexed in a spectral manner by frequency. May be.

FIG. 12 is a block diagram schematically showing another embodiment of the variable dispersion compensator. In the present embodiment, the signal light from the optical fiber transmission line 13 for dispersion compensation is input to the diffraction grating 2b, which is an optical multiplexing / demultiplexing unit, is demultiplexed, and is reflected by the reflection unit 5 for each frequency component. Then, the reflected frequency components are multiplexed again by the diffraction grating 2 b to become dispersion-compensated signal light, which is input to the optical fiber transmission line 13.

FIG. 13 is a block diagram schematically showing another embodiment of the variable dispersion compensator. In the present embodiment, two diffraction gratings 2d, 2e
The silicon oxide (SiO ₂ ) plate 2c on which is formed is used. The signal light from the input optical fiber transmission line 14 is incident on the plate 2c from the upper surface side, then is input to the diffraction grating 2d, which is an optical demultiplexing unit, and is demultiplexed. Is reflected. The reflected frequency components are multiplexed by the diffraction grating 2e, which is an optical multiplexing means, to become dispersion-compensated signal light, pass through the upper surface of the plate 2c, and enter the output optical fiber transmission line 15. Is done.

In addition to the above configuration examples, various forms can be applied to the light demultiplexing means, the reflection means, the light multiplexing means, or a combination thereof.

[0110]

As described in detail above, the tunable dispersion compensator and the optical transmission system according to the present invention have the following effects. That is, using the optical path length difference from the optical demultiplexing means to the optical multiplexing means via the reflection means, a phase shift is given to each frequency component of the signal light, and the reflection position for each frequency component is changed. According to the variable dispersion compensator in which the phase shift is variable using the variable reflecting means, it is possible to compensate for the dispersion generated in the signal light with high accuracy and high controllability. Further, since the dispersion compensation is controlled only by the reflection means, the structure of the optical circuit can be simplified, and the optical circuit can be downsized.

[Brief description of the drawings]

FIG. 1 is a configuration diagram schematically illustrating an embodiment of a tunable dispersion compensator.

FIG. 2 is a configuration diagram schematically illustrating an embodiment of an optical transmission system.

FIG. 3 is a plan view showing a specific configuration example of the variable dispersion compensator according to the embodiment shown in FIG. 1;

FIG. 4 is a configuration diagram illustrating an example of a movable reflection mirror.

FIG. 5 is a configuration diagram showing another example of a movable reflection mirror.

FIG. 6 is a graph showing an example of (a) an input signal light and (b) an output signal light before dispersion compensation in an optical transmission system of 10 Gbps.

FIG. 7 is a graph illustrating an example of (a) a phase shift of a signal light and (b) an output signal light after dispersion compensation in a 10 Gbps optical transmission system.

FIG. 8 is a graph showing another example of (a) the phase shift of the signal light and (b) the output signal light after dispersion compensation in the 10 Gbps optical transmission system.

FIG. 9 is a graph showing an example of (a) an input signal light and (b) an output signal light before dispersion compensation in an optical transmission system of 40 Gbps.

FIG. 10 is a graph showing an example of (a) a phase shift of signal light and (b) an output signal light after dispersion compensation in a 40 Gbps optical transmission system.

FIG. 11 is a diagram showing another example of a movable reflection mirror.

FIG. 12 is a configuration diagram schematically showing another embodiment of the variable dispersion compensator.

FIG. 13 is a configuration diagram schematically showing another embodiment of the variable dispersion compensator.

[Explanation of symbols]

1 variable dispersion compensator, 1a input terminal, 1b output terminal, 1
0 ... substrate, 11 ... optical transmission line, 12 ... optical circulator,
13: optical transmission line, T: transmitter, R: receiver, L: optical fiber transmission line, 2: optical multiplexer / demultiplexer, 2a: arrayed waveguide type diffraction grating (AWG), 21: input / output channel waveguide , 2
2 ... first slab waveguide, 23 ... array waveguide section, 24 ...
2nd slab waveguide, 25 ... channel waveguide group, 26 ₁ to
26 _n ... channel waveguide, 3 ... reflection mirror group, 30, 3
0 ₁ to 30 _n movable mirror, 31 groove, 32 guide rail, 33 mirror support, 34 to 38 electrode, 4
0: metal layer (movable reflection mirror), 41: polysilicon layer, 42: silicon oxide layer, 43: metal layer, 44: silicon layer.

 ──────────────────────────────────────────────────続 き Continuing from the front page (72) Inventor Masayuki Nishimura 1 Tayacho, Sakae-ku, Yokohama-shi, Kanagawa Prefecture Sumitomo Electric Industries, Ltd. Yokohama Works (72) Inventor Tomomi Sano 1-Tagamachi, Sakae-ku, Yokohama, Kanagawa Prefecture Sumitomo Electric Inside the Yokohama Works of Ki Industries Co., Ltd. (72) Inventor: Toru Iwashima, 1st place, Tayacho, Sakae-ku, Yokohama-shi, Kanagawa Prefecture Sumitomo Electric Industries, Ltd. (72) Inventor: Tomohiko Kanie 1st place, Tayacho, Sakae-ku, Yokohama-shi, Kanagawa Prefecture F-term (reference) in Yokohama, Ltd. 2H041 AA23 AB14 AC06 AZ02 2H047 KA03 LA18 NA10 5K002 BA02 BA05 CA01

Claims (9)

[Claims] 1. A variable dispersion compensator for compensating for dispersion of a signal light by giving a phase shift to the signal light, wherein the signal light to be subjected to dispersion compensation is input, and the signal within a predetermined frequency band is input. Light demultiplexing means for demultiplexing light for each frequency component, and each of the frequency components demultiplexed by the light demultiplexing means is reflected to give a predetermined phase shift to each frequency component, and each of the frequency components is A reflection unit whose reflection position with respect to the signal light propagation direction is variably configured, and multiplexes the frequency components reflected by the reflection unit,
A variable dispersion compensator, comprising: an optical multiplexing unit that converts the signal light into a dispersion-compensated signal light. 2. The optical demultiplexing means and the optical multiplexing means,
2. A single optical multiplexing / demultiplexing means.
The variable dispersion compensator according to claim 1. 3. The reflection means comprises a plurality of reflection mirrors divided corresponding to the frequency component, and each of the plurality of reflection mirrors individually moves its reflection surface in the signal light propagation direction. The variable dispersion compensator according to claim 1, wherein the movable mirror is a movable mirror. 4. The movable mirror, which is each of the plurality of reflection mirrors, includes a first electrode provided on the movable mirror, and a second electrode provided at a predetermined position with respect to the first electrode. 4. The tunable dispersion compensator according to claim 3, wherein the reflecting surfaces can be individually moved by using an electrostatic force generated by applying a voltage therebetween. 5. The reflection means comprises a single reflection mirror, and the single reflection mirror deforms the entire reflection surface so that each of the reflection surface portions corresponding to the frequency components is converted to the signal component. 2. The variable dispersion compensator according to claim 1, wherein the variable dispersion compensator is a movable mirror that can move in a light propagation direction. 6. The movable mirror, which is the single reflecting mirror, is provided between a first electrode provided on the movable mirror and a second electrode provided at a predetermined position with respect to the first electrode. 6. The tunable dispersion compensator according to claim 5, wherein the entire reflection surface can be deformed by using an electrostatic force generated by applying a voltage to the variable dispersion compensator. 7. The tunable dispersion compensator according to claim 1, wherein the arrangement of the reflection mirrors constituting the reflection means or the shape of the reflection surface is substantially parabolic with respect to the frequency component to be reflected. . 8. An optical transmission line that propagates signal light having a frequency component within a predetermined frequency band, and a dispersion generated in the signal light that is installed at a predetermined position on the optical transmission line and propagates through the optical transmission line. Claim 1
An optical transmission system, comprising: the variable dispersion compensator according to any one of the preceding claims. 9. The signal light having a bit rate of 10 Gbp.
9. The optical transmission system according to claim 8, wherein the number is not less than s.