KR100355153B1 - Optical amplifier for clamping and equalizing gain in optical communication system - Google Patents

Abstract

The present invention provides a gain fixed optical amplifier having a flat gain of an optical communication system. The present invention receives an optical signal and applies a compensation signal to obtain a gain such that the input signal has the same output for each channel. A gain fixing amplifier section for fixing; A second isolator for passing the signal light input from the gain fixed amplifier and blocking light coming in the opposite direction; A gain flatten filter which receives the signal of the second isolator and flatly changes the shape of the output gain spectrum; And a post amplifier configured to amplify the signal of the gain flattened filter having a fixed gain, so that the density reversal of the amplifier according to the change of the input signal is kept constant, thereby automatically fixing the gain and increasing the transmission capacity. Gain flattening to widen the band is performed.

Description

Optical amplifier for clamping and equalizing gain in optical communication system

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a gain flattened amplification gain fixed optical amplifier of an optical communication system, and in particular, to maintain a constant density reversal of an amplifier according to a change in an input signal, thereby automatically fixing a gain and increasing a transmission capacity. A wider gain fixed flat optical amplifier in an optical communication system has been made that widens gain flattening.

In general, an optical amplifier is used in an optical communication system to compensate for signal loss. The optical amplifier is an apparatus for amplifying an optical signal to compensate for the attenuation of the optical signal due to long distance optical communication.

Such optical amplifiers are expected to be widely used in future communication systems. Erbium Doped Fiber Amplifiers (EDFAs), in particular, are designed to prevent the attenuation of optical signals due to long-distance transmissions when large amounts of data are transmitted over long distances without regeneration through one strand of fiber. Used to amplify the optical signal.

In the wavelength division multiplexing (WDM) optical transmission system, since a large amount of data is carried on multiple carriers having different wavelengths, the total transmission capacity increases rapidly in proportion to the number of wavelengths.

In WDM networks, the number of channels changes due to network configuration changes, component failures, and frequent add / drop of channels. As a result, the change in the overall input signal intensity causes a transient phenomenon to occur in the optical output of the remaining channel, and the transmission error is instantaneously increased due to the variation in the gain. Therefore, in the WDM network, the gain change due to the change of the magnitude of the input signal should be minimized.

As a method of automatically adjusting the gain of the optical amplifier, it can be divided into a method of adjusting the pump light and a method of applying a compensation signal. A recent study on the method of applying the compensation signal shows a relatively low output using a flat gain band of up to 16 nm.

Recently, however, the movement to use more than 32 channels is active. In this case, the intensity of the signal light corresponding to one wavelength is almost the same, so that the intensity of the entire input signal is significantly increased, and accordingly, the total output must be increased in proportion to the number of wavelengths. In this case, conventional gain-fixed optical amplifiers cannot produce sufficient output. In addition, the flat gain band should be wide enough, and the flat gain should have very good flatness for long-distance transmission. In this case, a gain flat filter is necessary. Its development is very important because these problems must be solved simultaneously before they can be used in future WDM networks. The present invention solves these problems with a simple and reliable structure.

1 is a block diagram of a conventional gain fixed optical amplifier.

As shown therein, a first isolator 21 which passes only one direction to the input signal light; A first optical coupling part 11 coupling the output of the first isolator 21 and the filter 31; A pump 71 for causing density inversion in the amplification medium (EDF) 41 to occur; A second optical coupling part (12) for coupling the output of the first optical coupling part (11) and the pump (71); An amplifying medium 41 for amplifying the signal input from the second optical coupling part 12; A second isolator 22 which blocks the reflected light to the output of the amplifying medium 41 and passes the transmitted light; A third optical coupling part (13) for distributing the output of the second isolator (22); A third isolator 23 for isolating the signal distributed by the third optical coupling unit 13; A filter 31 for transmitting only a specific wavelength at the output of the third isolator 23 to the first optical coupling unit 11; It is composed of a fourth isolator 24 for receiving the signal distributed by the third optical coupling unit 13 to perform isolating to output the optical signal to which the compensation signal is applied.

Thus, the optical amplifier structure of FIG. 1 is a structure for applying a compensation signal.

An amplifying medium 41 for amplifying the signal input from the second optical coupler 12, a pump 71 for causing density inversion to the amplifying medium 41, and two optical couplers having an annular structure for applying a compensation signal. (11) (13) are used, and consist of the filter 31 which passes a specific wavelength.

The gain of such a conventional fixed gain optical amplifier is determined by the loss of two optical couplers 11 and 13 forming an annular structure. When the power of the pump 71 is increased to increase the output of the signal, only the laser signal used as the compensation signal is amplified and the output of the input signal does not change. In addition, the output is reduced due to the loss of the third optical coupler 13 at the output end.

As a result, the conventional gain-fixed optical amplifier shown in Fig. 1 cannot be applied to a WDM system because gain flattening is not considered.

FIG. 2 is a block diagram illustrating an optical amplifier including a gain flattening filter in FIG. 1.

As shown therein, a first isolator 21 for blocking the reflected light with respect to the input signal light and allowing the transmitted light to pass therethrough; A first optical coupling part 11 coupling the output of the first isolator 21 and the filter 31; A pump 71 for increasing the power of the input signal so that density inversion occurs in the amplifying medium 41; A second optical coupling part (12) for coupling the output of the first optical coupling part (11) and the pump (71); An amplifying medium 41 for amplifying the signal input from the second optical coupling part 12; A second isolator 22 which blocks the reflected light to the output of the amplifying medium 41 and passes the transmitted light; A third optical coupling part (13) for distributing the output of the second isolator (22); A third isolator (23) for isolating the signal distributed by the third optical coupler (13); A filter 31 for transmitting only a specific wavelength at the output of the third isolator 23 to the first optical coupling part 11; A gain flattening filter 51 for receiving a signal distributed by the third optical coupler 13 and performing gain flattening filtering; And a fourth isolator 24 for isolating the output of the gain flattening filter 51 to output the optical signal to which the compensation signal is applied.

The optical amplifier including the conventional gain flattening filter of FIG. 2 is an example in which a gain flattening filter and a gain fixing are simply applied to a gain flattening filter at an output terminal of the gain fixed type optical amplifier of FIG.

According to the configuration of FIG. 2, a flat gain band of about 30 nm is obtained from 1530 to 1560 nm.

However, even in the case of the optical amplifier including the gain flattening filter, a filter is used at the output stage, which causes a lot of loss in the output of the signal.

3 is a block diagram of a conventional gain flat optical amplifier.

As shown therein, the first isolator 21 passes the input signal light and blocks the light coming in the opposite direction; A first pump (71) for increasing the power of the input signal to cause density inversion in the first amplifying medium (41); A second optical coupling part 12 coupling the output of the first isolator 21 and the first pump 71; A first amplifying medium (41) for amplifying a signal input from the second optical coupler (12); A second isolator 22 for isolating the output of the first amplifying medium 41; A gain flattening filter 51 which receives the signal of the second isolator 22 and performs gain flattening filtering

Wow; A second pump 72 for increasing the power of the input signal to cause density inversion in the second amplifying medium 42; A third optical coupling part (13) for coupling the gain flattening filter (51) and the output of the second pump (71); A second amplifying medium 42 for amplifying a signal input from the third optical coupling unit 13; And a fourth isolator 24 for isolating the output of the second amplifying medium 42 to output a gain flattened signal.

Therefore, in this gain flattened optical amplifier, a gain flattening filter 51 is provided between the first amplifying stage and the second amplifying stage to obtain a flat gain of 30 nm or more and a large output.

FIG. 4 is a block diagram illustrating a gain fixed optical amplifier using the gain flattened optical amplifier of FIG. 3.

As shown therein, the first isolator 21 passes the input signal light and blocks the light coming in the opposite direction; A first optical coupling part 11 coupling the output of the first isolator 21 and the filter 31; A first pump (71) for increasing the power of the input signal to cause density inversion in the first amplifying medium (41); A second optical coupling part (12) for coupling the output of the first optical coupling part (11) and the first pump (71); A first amplifying medium (41) for amplifying a signal input from the second optical coupler (12); A second isolator (22) for isolating the output of the first amplifying medium (41); A gain flatten filter that receives the signal of the second isolator 22 and performs gain flattening filtering

51; A second pump 72 for increasing the power of the input signal to cause density inversion in the second amplifying medium 42; A third optical coupling part (13) for coupling the gain flattening filter (51) and the output of the second pump (71); A second amplifying medium 42 for amplifying a signal input from the third optical coupling unit 13; A fourth optical coupling part 14 for distributing an optical signal output from the second amplifying medium 42; A third isolator (23) for isolating the output of the fourth optical coupler (14); A filter 31 for transmitting only a specific wavelength at the output of the third isolator 23 to the first optical coupling part 11; And a fourth isolator 24 for isolating the output of the fourth optical coupler 14 to output a gain-fixed and flattened signal.

Therefore, since the gain fixed optical amplifier to which the gain flattened optical amplifier of FIG. 4 is applied has a two-stage configuration in the annular structure as in the case of FIG. 1, and the gain flattening filter 51 is used, a flat gain can be obtained.

However, the same problem as in FIG. 1 occurs. That is, the fourth optical coupling unit at the output terminal

(14), it is difficult to obtain a high output.

As described above, the conventional fixed gain optical amplifier, which simply combines the two techniques, has a problem in that the system does not obtain sufficient gain desired because the gain obtained by applying the compensation signal is limited. In addition, in order to flatten the gain, a filter is placed at the last stage of the amplifier, which reduces the gain and increases the output loss.

As a result of obtaining a gain band of 30 nm or more in the gain-fixed optical amplifier, no results have been published. Even in the case of extending the concept, there were problems in that good characteristics could not be obtained due to the various problems described above.

In addition, the number of channels is increasing to increase the transmission capacity. In the long-distance transmission system, the wide gain band of 30nm or more is already used, but the optical amplifier used in the WDM network system is still in the network due to the change of the input signal. The development of amplifiers to be used is sluggish.

Accordingly, the present invention has been proposed to solve the conventional problems as described above, and an object of the present invention is to maintain the constant density inversion of the amplifier according to the change of the input signal to automatically fix the gain and increase the transmission capacity. It is to provide a gain fixed flat optical amplifier of an optical communication system so that gain flattening to widen the signal band can be performed.

Another object of the present invention is to provide a wideband gain fixed optical amplifier having a fixed gain per channel in a WDM network, providing a flat gain band of 30 nm or more, and having the high power required by the WDM system.

1 is a block diagram of a conventional gain fixed optical amplifier,

FIG. 2 is a block diagram illustrating an optical amplifier including a gain flattening filter in FIG. 1.

3 is a block diagram of a conventional gain flat optical amplifier,

4 is a block diagram illustrating a gain-fixed optical amplifier using FIG. 3.

5 is a block diagram of a gain fixed flat optical amplifier of the optical communication system according to the present invention;

6 is a detailed configuration diagram of FIG.

FIG. 7 is a graph illustrating gain characteristics according to the strength of the input signal of FIG. 5;

FIG. 8 is a graph illustrating a uniform gain spectrum according to an input change when the gain of FIG. 5 is fixed.

Explanation of symbols on the main parts of the drawings

100: fixed gain amplifier 200: post amplifier

11, 12, 13: optical coupling portion 21, 22, 23, 24: isolator

31: filter 41, 42: amplification medium

51: gain flattening filter 61, 62: FBG

71, 72, 73: pump

Hereinafter, with reference to the accompanying drawings an embodiment according to the present invention, the technical spirit of the fixed fixed optical amplifier of the optical communication system as follows.

5 is a block diagram of a gain fixed flat optical amplifier of the optical communication system according to the present invention.

As shown in the figure, an optical amplifier of an optical communication system, comprising: a gain fixed amplifier unit 100 for fixing a gain by receiving an optical signal and applying a compensation signal so that the input signal has the same output for each channel; A second isolator (22) for passing the signal light input from the gain fixed amplifier unit (100) and blocking the light coming in the opposite direction; A gain flattening filter 51 which receives the signal of the second isolator 22 and smoothly changes the shape of the output gain spectrum; Post-amplification part for amplifying the signal of the gain flattening filter 51

And 200.

The gain fixed amplifier 100 is configured as a ring laser to apply a compensation signal to the laser resonance at both ends of the amplification medium.

In the above, the fixed gain amplifier 100 applies a compensation signal using the FBG.

In the above, the fixed gain amplifier 100 applies a compensation signal directly by using the additional LD.

The gain flattening filter 51 may include the gain fixed amplifier 100 and the post amplifier.

It considers the gain characteristic of 200, and comprises it.

In the above, the post amplifier 200 is configured to obtain a high output by using a forward pumping structure.

The post-amplification part 200 in the above, to obtain a high output by using a reverse pumping structure.

The post-amplification part 200 in the above, to obtain a high output using a bidirectional pumping structure.

6 is a detailed configuration example of FIG. 5.

As shown in the drawing, the fixed gain amplifier 100 increases the power of the input signal so that the density inversion in the first amplifying medium 41 is generated.

Wow; A first optical coupling part (11) for coupling the input signal with the output of the first pump (71); A first amplifying medium (EDF1) for amplifying the signal input from the first optical coupling unit 11

(41); It consists of a laser resonator that makes a compensation signal and fixes the gain.

The gain fixed amplifier may further include a first isolator 21 for passing the input signal light and blocking the light coming in the opposite direction.

The post amplifier 200 includes: second and third pumps 72 and 73 for increasing density of the input signal so that density inversion occurs in the second amplifier medium 42; The second optical coupling unit for coupling the output of the gain flattening filter 51 and the first pump 71

12; A second amplifying medium (EDF2) 42 for amplifying a signal input from the second optical coupling part 12; It comprises a third optical coupling portion 13 for coupling the output of the second amplifying medium 42 and the third pump (73).

In the present invention, the post amplifier 200 further includes a third isolator 23 for isolating the output of the third optical coupling unit 13 to output a gain-fixed and flattened signal.

The operation of the gain-fixed flat optical amplifier of the optical communication system according to the present invention configured as described above will be described in detail with reference to the accompanying drawings.

First of all, the number of channels is increasing to increase the transmission capacity, and the long-distance transmission system already uses a wide gain band of 30 nm or more. However, optical amplifiers used in WDM network systems have been underdeveloped due to changes in input signals.

FIG. 5 is a block diagram of a gain fixed flat optical amplifier of the optical communication system according to the present invention, and FIG. 6 is a detailed configuration example of FIG.

Thus, the present invention operates largely composed of a gain fixed amplifier 100 and a post amplifier 200.

The fixed gain amplifier 100 includes a first optical coupling unit 11 for coupling an input optical signal, a first amplifying medium 41 for amplifying and outputting a signal from the first optical coupling unit 11, and the amplification unit 100. The medium comprises a FBG (Fiber Bragg Grating) 61 (62) having a first pump (71) for causing density inversion in the medium, and constituting a laser resonator for providing a compensation signal for gain fixing.

The signal amplified by the gain fixed amplifier 100 passes through the second isolator 22 and the gain flattening filter 51 and is input to the post amplifier 200 which is the second amplification stage.

The post amplifier 200 includes a second optical coupling unit 22, an amplifying medium 42, and a pump 72, 73 so that the signal has a sufficient gain and then outputs the signal.

In the design of the intermediate gain flattening filter 51, the gain characteristics of the gain fixed amplifier 100, which is the first amplifier stage, and the post amplifier 200, which is the second amplifier stage, should be considered.

According to the present invention, a constant amplification gain can be obtained even with a change in the input signal according to a change in the number of channels in the WDM network system, and at the same time, a gain flattened optical amplifier can be realized.

Therefore, the gain fixing amplifier 100, which is the first amplifying stage, fixes the gain using a method of applying a compensation signal. In this case, the density reversal of the amplifier stage is kept constant due to the compensation signal. Accordingly, the gain for each channel is also fixed, and the overall output including the compensation signal is also fixed.

When the signal having the fixed total output and gain spectrum is transmitted to the post amplifier 200 which is the second amplifier stage, the intermediate gain flattening filter 51 outputs the output gain spectrum so that the gains of the first amplifier stage and the second amplifier stage are flattened. Change the shape of the flat. Thus, the post amplifier 200 as the second amplifier stage amplifies the passed signal to have the same value for each channel and also fixes the gain for each channel.

By using this structure, the gain flattening technique of FIG. 3 can be applied as it is, and the techniques of various gain fixed optical amplifiers as shown in FIG. 1 can be applied. Thus, a gain fixed optical amplifier having a wide gain band in each case can be applied. Will be able to produce.

In addition, as shown in FIG. 6, the signal input to the gain fixed amplifier 100 through the first optical coupling unit 11 is fixed by a resonator composed of two FBGs 61 and 62 having the same wavelength. . In this case, when the compensation signal is applied for gain fixing, the compensation signal may be directly configured by using a ring laser, using an FBG, or using an additional laser diode (LD). As a result, the density inversion becomes constant, passes through the second isolator 22, and passes through the gain flattening filter 51 and is input to the post-amplification part 200 which is the second amplification stage. The post amplifier 200 adopts a bidirectional pumping structure using two optical couplers 12 and 13 for high power. Such a structure may use a pumping structure in the forward or reverse direction or in both directions.

FIG. 7 is a graph illustrating gain characteristics according to the strength of the input signal of FIG. 5.

180mW pumping power and EDF 19m and 11m were used at the front and rear, respectively, and the return wavelength was 1560nm. The input signal uses 32 (64) channels, and the overall input signal strength is -2dBm, corresponding to -17 (-20) dBm per channel.

When gain-clamping is not performed, the gain of the small signal input signal is 34 dB, and the gain decreases as the input signal increases. This indicates that the overall gain changes as the input changes, and cannot be used in WDM systems with Add / Drop of channels.

In the case of gain-locking, we can see that the gain is fixed at 20dB for the input change of -22dBm to -2dBm.

Therefore, it can be seen that the input signal obtains a constant 20dB of gain from -2dBm to -20dBm at 18dB, that is, change from one channel to 64 channels.

Since EDFA has a high gain of 1530 nm, the gain must be flattened in order to use a wide band of 30 nm or more.

FIG. 8 is a graph illustrating a uniform gain spectrum according to an input change when the gain of FIG. 5 is fixed.

In the case of Figure 8, the input signal per channel is -20dBm, and -2dBm corresponding to 64 channels were input. The fixed gain amplifier 100 uses a 980nm pump 160mW, the post amplifier 200

1480nm pump 220mW was applied as a backward (Backward). FIG. 8 shows the characteristics of the gain and noise figure according to the wavelength at the change of the input signal from -2dBm corresponding to 64 channels to -20dBm corresponding to one channel in this case.

It can be seen that the gain of about 20nm in the gain region of about 30nm, the gain according to the intensity of the entire input signal is almost constant. The noise figure is less than 6dB overall. In addition, pumping the 1480nm pump in both directions improves the gain to 23dB, resulting in up to 21dBm of output.

Therefore, in FIG. 8, it can be seen that a flat gain spectrum is obtained at 33 nm or more from 1529 nm to 1562 nm.

As described above, the present invention provides a high output while performing gain flattening to widen the signal band to automatically fix the gain and increase the transmission capacity by maintaining the constant density inversion of the amplifier according to the change of the input signal.

Although the preferred embodiment of the present invention has been described above, the present invention may use various changes, modifications, and equivalents. It is clear that the present invention can be applied in the same manner by appropriately modifying the above embodiments. Accordingly, the above description does not limit the scope of the invention as defined by the limitations of the following claims.

As described above, the gain fixed flat optical amplifier of the optical communication system according to the present invention maintains a constant density reversal of the amplifier according to the change of the input signal, thereby automatically fixing the gain and increasing the transmission capacity. Widening has the effect of performing gain flattening.

In addition, the present invention enables a high output with a wide flat gain of more than 30 channels even in a WDM network system, and implements an optical amplifier having a structure having a constant gain in accordance with the change of the channel to be useful as a next-generation all-optical amplifier. do.

Claims (12)

In the optical amplifier of the optical communication system, A gain fixed amplifier which receives an optical signal and applies a compensation signal to fix the gain so that the input signal has the same output for each channel; A second isolator for passing the signal light input from the gain fixed amplifier and blocking light coming in the opposite direction; A gain flatten filter which receives the signal of the second isolator and flatly changes the shape of the output gain spectrum; And a post amplifier to amplify the signal of the gain flat filter. The method of claim 1, wherein the gain fixed amplifier, A gain-fixed flat optical amplifier in an optical communication system, comprising a ring laser applied to both ends of an amplifying medium to apply a compensation signal. The method of claim 1, wherein the gain fixed amplifier, A gain fixed flat optical amplifier in an optical communication system, comprising applying a compensation signal by constructing a laser resonator using an FBG. The method of claim 1, wherein the gain fixed amplifier, A gain fixed flat optical amplifier in an optical communication system, characterized in that a direct compensation signal is applied using an additional LD. The method of claim 1, wherein the gain fixed amplifier, A first pump for increasing the power of the input signal to cause density inversion in the first amplifying medium; A first optical coupling unit coupling the input signal with the output of the first pump; A first amplifier medium for amplifying a signal input from the first optical coupling unit; A gain fixed flat optical amplifier of an optical communication system comprising a laser resonator for generating a compensation signal and fixing a gain. 6. The gain fixed flat optical amplifier of claim 5, wherein the gain fixed amplifier further comprises a first isolator for passing the input signal light and blocking the light coming in the opposite direction. The method of claim 1, wherein the gain flattening filter, And a gain fixed flat optical amplifier of the optical communication system, characterized by using the gain characteristics of the fixed gain amplifier and the post amplifier. The post amplifier of claim 1, A gain fixed flat optical amplifier in an optical communication system, characterized by high forward power using a forward pumping structure. The post amplifier of claim 1, A gain fixed flat optical amplifier in an optical communication system, characterized in that a high power is obtained using a reverse pumping structure. The post amplifier of claim 1, A gain fixed flat optical amplifier in an optical communication system, characterized in that a high power is obtained using a bidirectional pumping structure. The post amplifier of claim 1, Second and third pumps for increasing the power of the input signal to cause density inversion in the second amplifying medium; A second optical coupling unit coupling the gain flattening filter and the output of the first pump; A second amplifying medium for amplifying a signal input from the second optical coupling unit; And a third optical coupling unit for coupling the second amplifying medium and the output of the third pump to the gain fixed flat optical amplifier of the optical communication system. The method of claim 11, wherein the post amplifier is, And a third isolator for isolating the output of the third optical coupling part (13) to output a gain fixed and flattened signal.