Gain and signal level adjustments of cascaded optical amplifiers

An optical amplification device which includes first and second optical amplifiers, and a controller. The first optical amplifier receives a light and amplifies the received light. The second optical amplifier receives the light amplified by the first optical amplifier, and amplifies the received light. When a level of the light received by the first optical amplifier changes by Δ, the controller controls a level of the light received by the second optical amplifier to change by approximately −Δ. In various embodiments, the controller causes the sum of the gains of the first and second optical amplifiers to be constant. In other embodiments, the optical amplification device includes first and second optical amplifier and a gain adjustor. The gain adjustor detects a deviation in gain of the first optical amplifier from a target gain, and adjusts the gain of the second optical amplifier to compensate for the detected deviation.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to cascaded optical amplifiers and, more particularly, to gain and signal level adjustments of cascaded optical amplifiers.

2. Description of the Related Art

Optical communication systems using optical fiber transmission lines are being used to transmit relatively large amounts of information. For this purpose, low-loss (e.g., 0.2 dB/km) optical fibers have been manufactured and used as optical fiber transmission lines. In addition, optical amplifiers are used to compensate for losses in the optical fiber transmission line to thereby allow long-haul transmission.

A conventional optical amplifier includes an optical amplifying medium which is pumped with pump light to provide a gain band. The optical amplifying medium and pump light are chosen so that they provide a gain band which includes a wavelength of signal light. As a result, the signal light will be amplified as the signal light travels through the optical amplifying medium. For example, an erbium doped fiber amplifier (EDFA) includes an erbium doped fiber (EDF) as the optical amplifying medium. A pumping light source supplies pump light having a predetermined wavelength to the EDF. By setting the wavelength of the pump light within a 0.98 μm band or a 1.48 μm band, a gain band including a wavelength band of 1.55 μm can be obtained. Therefore, signal light in the 1.55 μm wavelength band will be amplified.

Another type of conventional optical amplifier has a semiconductor chip as the optical amplifying medium. In this case, pumping is performed by injecting an electric current into the semiconductor chip.

Further, wavelength division multiplexing (WDM) is a known technique for increasing transmission capacity through a single optical fiber. In a system adopting WDM, a plurality of optical carriers having different wavelengths are individually modulated with data. Thus, each modulated carrier represents a channel of the WDM system transmitting an optical signal. The optical signals (that is, the modulated carriers) are then wavelength division multiplexed by an optical multiplexer to obtain WDM signal light. The WDM signal light is then transmitted through an optical fiber transmission line. The WDM signal light is received through the transmission line, and then demultipexed into individual optical signals by an optical demultiplexer. Data can then be detected from these individual optical signals. Therefore, by applying WDM, the transmission capacity of a single optical fiber can be increased in accordance with the number of WDM channels multiplexed together and transmitted through the optical fiber.

When an optical amplifier is inserted along the transmission line in an optical communication system adopting WDM, a transmission distance is limited by the wavelength characteristic of gain which is represented by a gain tilt or gain deviation of the optical amplifier. For example, in an EDFA, it is known that a gain tilt is produced at wavelengths in the vicinity of 1.55 μm, and this gain tilt varies with total input power of signal light and pump light power to the EDFA.

There is an optical amplification device for optical amplification which can maintain the wavelength characteristic of gain constant and obtain a wide input dynamic range. The optical amplification device includes first and second optical amplifiers and a variable optical attenuator optically connected between the first and second optical amplifiers. Automatic gain control (AGC) is applied to each of the first and second optical amplifiers, thereby maintaining constant the wavelength characteristic of gain of each of the first and second optical amplifiers. Further, automatic output level control (ALC) is performed for the second optical amplifier by using the variable optical attenuator, thereby obtaining a wide input dynamic range. That is, the output level of the second optical amplifier is maintained constant irrespective of the input level of the first optical amplifier, so that the input dynamic range of this device is widened.

In such an optical amplification device, AGC is performed so that the gain of the first optical amplifier is maintained constant irrespective of the input level of the first optical amplifier. Accordingly, there arises a problem such that when the power of signal light to be supplied to the first optical amplifier is increased, the power of pump light must be increased by the corresponding amount to increase the output power of the first optical amplifier to provide the required gain. That is, a high-power pumping light source is required for the first optical amplifier to ensure a required input dynamic range.

SUMMARY OF THE INVENTION

Accordingly, it is an object of the present invention to provide an optical amplification device and method which does not require a high-power pumping light source.

It is an additional object of the present invention to provide an optical amplification device and method which can maintain the wavelength characteristic of gain constant and can obtain a wide input dynamic range, while requiring a relatively low power pump light.

The foregoing objects of the present invention are achieved by providing an apparatus comprising first and second optical amplifiers, and a controller. The first optical amplifier receives a light and amplifies the received light. The second optical amplifier receives the light amplified by the first optical amplifier, and amplifies the received light. The controller, when a level of the light received by the first optical amplifier changes by Δ, controls a level of the light received by the second optical amplifier to change by approximately −Δ.

Objects of the present invention are further achieved by providing an apparatus which includes first and second optical amplifiers, a variable attenuator and a controller. The first optical amplifier receives a light and amplifies the received light. The second optical amplifier receives the light amplified by the first optical amplifier, and amplifies the received light. The variable attenuator is optically connected between the first and second optical amplifiers. The controller controls attenuation of the variable attenuator so that, when a level of the light received by the first optical amplifier changes by Δ, a level of the light received by the second optical amplifier changes by approximately −Δ.

Objects of the present invention are further achieved by providing an optical communication system. In the optical communication system, optical transmitters transmit optical signals at different wavelengths. A multiplexer multiplexes the optical signals into a wavelength division multiplexed (WDM) signal light. The WDM signal light is transmitted through an optical fiber transmission line. An optical amplification device amplifies the WDM signal light as the WDM signal light is transmitted through the transmission line. The optical amplification device includes first and second optical amplifiers and a controller. The first optical amplifier receives the WDM signal light and amplifies the received WDM signal light. The second optical amplifier receives the WDM signal light amplified by the first optical amplifier, and amplifies the received WDM signal light. The controller, when a level of the WDM signal light received by the first optical amplifier changes by Δ, controls a level of the WDM signal light received by the second optical amplifier to change by approximately −Δ.

Objects of the present invention are further achieved by providing an apparatus which includes optical amplifiers optically connected together, each optical amplifier having a corresponding gain. A controller causes the sum of the gains of the optical amplifiers to be constant. There can be two or more optical amplifiers optically connected together in this manner.

In addition, objects of the present invention are achieved by providing an apparatus comprising first and second optical amplifiers connected together, and a controller causing the sum of the gains of the first and second optical amplifiers to be constant. The controller can include a variable attenuator optically connected between the first and second optical amplifiers, where the attenuation of the variable attenuator is controlled to cause the sum of the gains of the first and second optical amplifiers to be constant.

Further, objects of the present invention are achieved by providing an apparatus which includes first and second optical amplifiers, and a gain adjustor. The first optical amplifier amplifies a light with a gain of the first optical amplifier. The second optical amplifier receives the light amplified by the first optical amplifier, and amplifies the received light with a gain of the second optical amplifier. The gain adjustor detects a deviation in gain of the first optical amplifier from a target gain, and adjusts the gain of the second optical amplifier to compensate for the detected deviation.

Objects of the present invention are also achieved by providing an apparatus including a first optical amplifier which amplifies a light with a gain of the first optical amplifier. A first gain controller controls the gain of the first optical amplifier to be constant at a target gain. A second optical amplifier receives the light amplified by the first optical amplifier, and amplifies the received light with a gain of the second optical amplifier. A gain deviation detector detects a deviation in gain of the first optical amplifier from the target gain. A gain adjustor adjusts the gain of the second optical amplifier to compensate for the detected deviation in gain of the first optical amplifier. A level controller can control a level of the light amplified by the first optical amplifier before being amplified by the second optical amplifier to be at a target level, wherein the level controller adjusts the target level to compensate for a detected deviation in gain of the first optical amplifier by the gain deviation detector.

Moreover, objects of the present invention are achieved by providing an optical amplifying device which includes first and second optical amplifiers. The first optical amplifier amplifies a light with a gain of the first optical amplifier. A first gain controller controls the gain of the first optical amplifier to be constant at a target gain for the first optical amplifier. The second optical amplifier receives the light amplified by the first optical amplifier, and amplifies the received light with a gain of the second optical amplifier. A second gain controller controls the gain of the second optical amplifier to be constant at a target gain for the second optical amplifier. A gain deviation detector detects a deviation in gain of the first optical amplifier from the target gain of the first optical amplifier. A gain adjustor adjusts the target gain of the second optical amplifier to compensate for the detected deviation in gain of the first optical amplifier.

Objects of the present invention are also achieved by providing an apparatus including first and second optical amplifiers and a gain adjustor. The first optical amplifier amplifies a light with a gain of the first optical amplifier. The second optical amplifier receives the light amplified by the first optical amplifier, and amplifies the received light with a gain of the second optical amplifier. The gain adjustor detects a deviation in gain of one of the first and second optical amplifiers from a target gain, and adjusts the gain of the other of the first and second optical amplifiers to compensate for the detected deviation.

In addition, objects of the present invention are achieved by providing an apparatus which includes a first optical amplifier amplifying a light with a gain of the first optical amplifier. A first gain controller controls the gain of the first optical amplifier to be constant at a target gain for the first optical amplifier. A second optical amplifier receives the light amplified by the first optical amplifier, and amplifies the received light with a gain of the second optical amplifier. A second gain controller controls the gain of the second optical amplifier to be constant at a target gain for the second optical amplifier. A gain adjustor detects a deviation in gain of one of the first and second optical amplifiers from its target gain, and adjusts the gain of the other of the first and second optical amplifiers to compensate for the detected deviation.

Objects of the present invention are achieved by providing an apparatus which includes a plurality of optical amplifiers cascaded together so that a light is amplified by each optical amplifier as the light travels through the cascaded plurality of optical amplifiers, each optical amplifier amplifying the light with a corresponding gain. A gain adjustor detects a deviation in gain of one of the plurality of optical amplifiers from a target gain, and adjusts the gain of at least one of the other of the plurality of optical amplifiers to compensate for the detected deviation.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

FIG. 1is a diagram illustrating an optical fiber communication system, according to an embodiment of the present invention. Referring now toFIG. 1, the system includes a first terminal station102, a second terminal station104, an optical fiber transmission line106connecting terminal stations102and104, and a plurality of optical repeaters108arranged along optical fiber transmission line106. Each optical repeater108includes an optical amplifier110optically connected to optical fiber transmission line106. AlthoughFIG. 1shows two optical repeaters108, more than two optical repeaters can be used, depending on the system design parameters. Further, in some systems, a single optical repeater may be used.

First terminal station102includes a plurality of optical transmitters (TX)112(#1to #N) respectively outputting a plurality of optical signals having different wavelengths. An optical multiplexer (MUX)114wavelength division multiplexes the optical signals output from optical transmitters112(#1to #N) to obtain WDM signal light. An optical amplifier (postamplifier)116amplifies the WDM signal light obtained from optical multiplexer114to output an amplified WDM signal light to optical fiber transmission line106.

Second terminal station104includes an optical amplifier (preamplifier)118amplifying the WDM signal light from optical fiber transmission line106. An optical demultiplexer (DMUX)120demultiplexes the amplified WDM signal light output from optical amplifier118into a plurality of optical signals. A plurality of optical receivers (RX)122(#1to #N) respectively receive the optical signals from optical demultiplexer120.

With this configuration, loss of the WDM signal light can be compensated by at least one optical repeater108arranged along optical fiber transmission line106, thereby allowing long-haul transmission. Furthermore, a plurality of channels are transmitted by optical fiber transmission line106, thereby increasing a transmission capacity.

FIG. 2is a graph illustrating gain tilt occurring in an optical amplifier. More specifically,FIG. 2illustrates the spectra of output light when WDM signal light based on optical signals of four channels (wavelengths of 1548, 1551, 1554, and 1557 nm, respectively) having the same power (−35 dBm/ch) is input into an EDFA (erbium doped fiber amplifier). InFIG. 2, the vertical axis represents output power (dBm), and the horizontal axis represents wavelength (nm).

The spectrum shown by A corresponds to the case where the power of pump light is relatively high, causing a negative gain tilt in a band of about 1.54 to 1.56 μm. That is, the negative gain tilt is a gain tilt such that the gain decreases with an increase in wavelength, and the derivative of gain (G) with respect to wavelength (λ) is negative (dG/dλ<0).

The spectrum shown by C corresponds to the case where the power of pump light is relatively low, causing a positive gain tilt in a band of about 1.54 to 1.56 μm. That is, the positive gain tilt is a gain tilt such that the gain increases with an increase in wavelength, and the derivative of gain (G) with respect to wavelength (λ) is positive (dG/dλ>0).

The spectrum shown by B corresponds to the case where the power of pump light is optimum so that no gain tilt is induced or the gain tilt becomes flat in a band of about 1.54 to 1.56 μm, and the derivative of gain (G) with respect to wavelength (λ) is zero (dG/dλ=0).

Each spectrum has such a shape that four sharp spectra corresponding to the optical signals of the four channels are superimposed on a gentle spectrum of ASE (amplified spontaneous emission). It is known that the wavelength characteristic of gain for a small signal depends on an ASE spectrum.

In the case that a plurality of optical amplifiers are cascaded as shown inFIG. 1, a gain tilt occurring in each optical amplifier is accumulated over the optical fiber transmission line, causing a degradation in signal-to-noise ratio in a low-level channel or a degradation in waveform due to nonlinear effects or the like in a high-level channel, so that a transmission distance for obtaining a required receiving sensitivity is limited. Accordingly, in this kind of system, it is greatly effective in increasing a transmission distance to perform a control such that the gain tilt in each optical amplifier becomes flat. Further, the output level of each optical amplifier has an optimum range. Accordingly, by controlling the output level of each optical amplifier so that it always falls within the optimum range irrespective of the input level of each optical amplifier, the input dynamic range can be widened.

FIG. 3is a diagram of a conventional optical amplification device for use as each of optical amplifiers110,116and118inFIG. 1. Referring now toFIG. 3, a first-stage optical amplifier6′ and a second-stage optical amplifier8′ are cascaded between an input port2and an output port4, and a variable optical attenuator (ATT)10′ is optically connected between optical amplifiers6′ and8′. Optical amplifier6′ is provided with a feedback loop12for automatic gain control (AGC), and optical amplifier8′ is provided with a feedback loop14for AGC. Variable optical attenuator10′ is included in a feedback loop16for automatic level control (ALC) to maintain a constant output level of the optical amplification device.

InFIG. 3, AGC is performed in each of optical amplifiers6′ and8′, so that the wavelength characteristic of gain in each of optical amplifiers6′ and8′ can be maintained constant. Furthermore, since feedback loop16for ALC is provided independently of feedback loops12and14for AGC, a wide input dynamic range can be obtained.

However, with the optical amplification device inFIG. 3, there is a problem that an excessive pump light power may be required in the case that first-stage optical amplifier6′ includes an erbium doped fiber (EDF) and a pumping light source for supplying pump light to the EDF. This problem will now be more specifically described.

FIG. 4is a power diagram of the optical amplification device inFIG. 3. InFIG. 4, the vertical axis represents optical power (dBm), and the horizontal axis represents position on an optical path extending from input port2to output port4. Assuming that the input level of first-stage optical amplifier6′ increases by Δ, the output level of optical amplifier6′ also increases by Δ because the gain G1of the optical amplifier6′ is maintained constant irrespective of the input level by feedback loop12. The gain G2of second-stage optical amplifier8′ is also maintained constant by feedback loop14. Accordingly, the attenuation to be given by variable optical attenuator10′ is increased by the operation of feedback loop16for ALC so that the output level of second-stage optical amplifier8′ is maintained constant.

In general, high-power pump light is required to obtain a high output level of an EDFA. Accordingly, in the case of using an EDFA as first-stage optical amplifier6′, high-power pump light is required to accept a high input level. That is, with the optical amplification device inFIG. 3, high-power pump light may be required to obtain a wide input dynamic range.

FIG. 5is a diagram illustrating an optical amplification device, according to an embodiment of the present invention. Referring now toFIG. 5, a first-stage optical amplifier6and a second-stage optical amplifier8are cascaded between an input port2and an output port4, and a variable optical attenuator10is optically connected between optical amplifiers6and8. Variable optical attenuator10variably attenuates the transmitted light in accordance with a control signal CS supplied thereto. Signal light (such as WDM signal light) supplied to input port2and to be amplified is sequentially subjected to amplification by optical amplifier6, attenuation by variable optical attenuator10, and amplification by optical amplifier8, and is finally output from output port4. Optical amplifier6is additionally provided with a feedback loop18for ALC. Feedback loop18serves to control optical amplifier6so that the output level of optical amplifier6is maintained constant. Similarly, optical amplifier8is additionally provided with a feedback loop20for ALC. Feedback loop20serves to control optical amplifier8so that the output level of optical amplifier8is maintained constant.

In this embodiment, the input level of first-stage optical amplifier6is detected, and the control signal CS is generated from a control unit22so that, when the input level of optical amplifier6changes by Δ (dBm in unit), the input level of optical amplifier8changes by −Δ.

Therefore, inFIG. 5, control unit22and variable optical attenuator10together operate as a controller which, when a level of the light received by optical amplifier6changes by Δ, controls a level of the light received by optical amplifier8to change by approximately −Δ.

Optical amplifiers6and8each may include an optical amplifying medium and a pumping light source. The pumping light source provides pump light to the optical amplifying medium. Signal light (such as WDM signal light) is then amplified as it travels through the optical amplifying medium, as long as the optical amplifying medium and the pump light provide a gain band which includes a wavelength of the signal light. The term of “gain band” is defined as a band in which the optical amplifying medium can generate a gain.

In the case that a doped fiber doped with a dopant including a rare earth element is used as the optical amplifying medium, the doped fiber can be pumped by supplying pump light having a predetermined wavelength to the doped fiber. In this case, the gain generated in the optical amplifying medium or the output level of the optical amplifying medium depends on the power of the pump light, so that a pumping light source may be included in the feedback loop for ALC.

In the case that an EDF is used as the optical amplifying medium, a laser diode oscillating in a 0.98 μm band (0.96 to 1.0 μm) or in a 1.48 μm band (1.46 to 1.50 μm) may be used as the pumping light source to thereby obtain a gain band including a 1.55 μm band (1.50 to 1.60 μm).

In the case that a semiconductor chip obtained by reducing the reflectance of opposite end faces of a laser diode is used as the optical amplifying medium, the pumping can be performed by injecting a current into the semiconductor chip. In this case, the gain generated in the semiconductor chip or the optical output level of the semiconductor chip depends on the injected current, so that a drive circuit for the semiconductor chip may be included in the feedback loop for ALC.

FIG. 6is a graph illustrating power levels in the optical amplification device ofFIG. 5, according to an embodiment of the present invention. InFIG. 6, the vertical axis represents optical power (dBm), and the horizontal axis represents position on an optical path extending from input port2to output port4.

Referring now toFIGS. 5 and 6, assuming that the input level of first-stage optical amplifier6increases by Δ (dBm in unit), the gain generated in optical amplifier6decreases from G1(dB in unit) to G1′ (dB in unit) because the output level of optical amplifier6is maintained constant by the feedback loop18for ALC. The attenuation of variable optical attenuator10is controlled by control unit22, so that the input level of second-stage optical amplifier8changes by −Δ. When the input level of optical amplifier8thus decreases by Δ, the gain generated in optical amplifier8increases from G2(dB in unit) to G2′ (dB in unit) because the output level of optical amplifier8is maintained constant by feedback loop20for ALC.

Accordingly, the output level of second-stage optical amplifier8is constant irrespective of the input level of first-stage optical amplifier6. Further, the sum of the gain generated in optical amplifier6and the gain generated in optical amplifier8is constant irrespective of the input level of optical amplifier6. That is, the relation of G1+G2=G1′+G2′ is satisfied.

Therefore, as can be seen fromFIG. 6, the total gain of a plurality of cascaded optical amplifiers is maintained constant. AlthoughFIGS. 5 and 6show only two optical amplifiers, the present invention is not intended to be limited in this manner. Instead, the present invention is applicable to a configuration of more than two optical amplifiers cascaded together, so that the total gain of the cascaded optical amplifiers is maintained constant.

By maintaining constant the total sum of the gains generated in a plurality of cascaded optical amplifiers, the wavelength characteristic of gain can be maintained constant. This will now be described more specifically in the case of cascading a plurality of doped fibers each doped with a dopant including a rare earth element.

In general, the wavelength characteristic G(λ) of the gain of one doped fiber is expressed as follows:
G(λ)={tg*(λ)−(1−t)α(λ)}L
where g*(λ) (dB/m) is the emission spectrum, α (dB/m) is the absorption spectrum, t is the population inversion coefficient (inversion parameter) of the doped fiber in its longitudinal direction, and L (m) is the length of the doped fiber.

Accordingly, in the case of cascading a plurality of doped fibers having the same emission spectrum and the same absorption spectrum, the total gain Gtotal(λ) is given as follows:

(∑k⁢Lk)
of the cascaded doped fiber.

Accordingly, by maintaining constant the total sum of the gains generated in a plurality of cascaded optical amplifiers, the wavelength characteristic of gain of the amplifier chain can be maintained constant.

Particularly, inFIG. 5, feedback loops18and20for ALC and control unit22for variable optical attenuator10are used, so that the total sum of the gains generated in the optical path extending from input port2to output port4can be maintained constant. Accordingly, by using an optical amplification device of the embodiments of the present invention as each of optical amplifiers110,116, and118inFIG. 1, accumulation of gain tilts can be prevented to thereby allow an increase in transmission distance.

Further, since feedback loop20for ALC is provided for second-stage optical amplifier8, the output level of second-stage optical amplifier8can be maintained constant irrespective of the input level of first-stage optical amplifier6, thereby widening the input dynamic range.

Further, feedback loop18for ALC is provided also for first-stage optical amplifier6. Therefore, in the case that optical amplifier6includes a doped fiber and a pumping light source, an undesirable increase in pump light power can be prevented, thus avoiding the problem in the related art shown inFIG. 3.

In addition, to maximize the obtainable total gain in the configuration ofFIG. 5, the attenuation of variable optical attenuator10may be controlled to become a minimum when the input level of first-stage optical amplifier6is a lower limit.

FIG. 7is a diagram illustrating details of the optical amplification device inFIG. 5, according to an embodiment of the present invention. Referring now toFIG. 7, EDFs24and26are adopted as the optical amplifying medium of optical amplifiers6and8, respectively, to obtain a gain band including a 1.55 μm band where a lowest loss is obtained in a silica fiber. A first end24A of EDF24is optically connected through a WDM coupler28and an optical coupler30to input port2, and a second end24B of EDF24is optically connected through an optical coupler32to an input port of variable optical attenuator10. A first end26A of EDF26is optically connected to an output port of variable optical attenuator10, and a second end26B of EDF26is optically connected through a WDM coupler34and an optical coupler36to output port4.

To prevent formation of an optical resonator structure including each of EDFs24and26, one or more optical isolators may be provided in the optical path between input port2and output port4. With this arrangement, the operation stability of the device can be improved.

Optical couplers30and32are used to detect the input level and the output level of first-stage optical amplifier6, respectively, and optical coupler36is used to detect the output level of second-stage optical amplifier8. Accordingly, each of optical couplers30,32and36can be fabricated without especially considering the wavelength dependence of branching ratio.

WDM coupler28is used to supply pump light from a laser diode (LD)38into EDF24from its first end24A, and WDM coupler34is used to supply pump light from a laser diode40into EDF26from its second end26B. The wavelength of each pump light is different from the wavelength of signal light to be amplified. Accordingly, each of WDM couplers28and34is fabricated in consideration of the wavelength dependence of branching ratio. The oscillation wavelength of each of laser diodes38and40is set to fall within a 0.98 μm band or a 1.48 μm band, for example, to obtain a gain band including a 1.55 μm band.

A drive current (bias current) is supplied from a drive circuit42to laser diode38. Feedback loop18for ALC for optical amplifier6includes a photodetector (PD)44such as a photodiode and an ALC circuit46. Monitor light branched by optical coupler32is supplied through an optical bandpass filter48to photodetector44. Photodetector44outputs an electrical signal having a voltage level (or current level) corresponding to the power of the received monitor light. ALC circuit46receives the output signal from photodetector44and controls the drive current to be supplied from drive circuit42to laser diode38so that the level of the received signal becomes constant.

The pass band of optical bandpass filter48is set so as to include the wavelength of the signal light amplified in EDF24and not to include the wavelength of the residual pump light from laser diode38having not contributed to the optical amplification in EDF24. This setting allows ALC such that the output level of the signal light amplified in EDF24becomes constant.

Laser diode40as the pumping light source for second-stage optical amplifier8is supplied with a drive current (bias current) from a drive circuit49. Feedback loop20for ALC for second-stage optical amplifier8includes a photodetector50and an ALC circuit52.

Monitor light branched by optical coupler36is supplied through an optical bandpass filter54to photodetector50. Photodetector50outputs an electrical signal having a voltage level (or current level) corresponding to the power of the received monitor light. ALC circuit52controls the drive current to be supplied from drive circuit49to laser diode40so that the level of the output signal from photodetector50becomes constant. Thus, the ALC for second-stage optical amplifier8is achieved by feedback loop20as similarly to feedback loop18.

Control unit22for generating the control signal CS includes a photodetector56and a control circuit58. Monitor light branched by optical coupler30is supplied through an optical bandpass filter60to photodetector56. Photodetector56outputs an electrical signal having a voltage level (or current level) corresponding to the power of the received monitor light. Control circuit58detects a change in the input level of the signal light to be supplied into EDF24and to be amplified therein, according to the output signal from photodetector56, and generates the control signal CS so that an opposite amount is given to the input level of EDF26by variable optical attenuator10.

The pass band of each of optical bandpass filters54and60is set so as to include the wavelength of the signal light to be amplified. In particular, the pass band of optical bandpass filter54is preferably set so as not to include the wavelength of the pump light, thereby eliminating the influence of the pump light from laser diode38.

According to this embodiment of the present invention, the total gain generated in the optical path extending from input port2to output port4can be maintained constant to thereby maintain the wavelength characteristic of gain constant. Furthermore, the output level at output port4can be maintained constant irrespective of the input level at input port2, thereby widening the input dynamic range of the device.

Moreover, ALC is performed so that the output level of the signal light amplified in EDF24becomes constant, thereby preventing an undesirable increase in the power of the pump light to be output from laser diode38.

In this embodiment of the present invention, the signal light and the pump light propagate in the same direction in EDF24of first-stage optical amplifier6. In other words, first-stage optical amplifier6is a forward pumping type optical amplifier. On the other hand, the signal light and the pump light propagate in opposite directions in EDF26of second-stage optical amplifier8. In other words, second-stage optical amplifier8is a backward pumping type optical amplifier. As a modification, first-stage optical amplifier6may be configured as a backward pumping type optical amplifier, and second-stage optical amplifier8may be configured as a forward pumping type optical amplifier. Further, each of optical amplifiers6and8may be configured as a bidirectional pumping type optical amplifier obtained by combining forward pumping and backward pumping.

FIG. 8is a diagram illustrating an optical amplification device, according to an additional embodiment of the present invention. Referring now toFIG. 8, a control unit66connected to gain monitors62and64controls variable optical attenuator10. By contrast, in the embodiment shown inFIG. 5, control unit22controls variable optical attenuator10according to the input level of first-stage optical amplifier6.

InFIG. 8, gain monitor62detects a first gain generated in first-stage optical amplifier6, and gain monitor64detects a second gain generated in second-stage optical amplifier8. Control unit66generates a control signal CS so that the sum of the first and second gains detected by gain monitors62and64becomes constant, and the control signal CS is supplied to variable optical attenuator10. Control signal CS controls the variable attenuation of variable optical attenuator10to appropriately attenuate the light signal travelling from optical amplifier6to optical amplifier8.

Therefore, inFIG. 8, control unit66and variable optical attenuator10together operate as a controller which causes the sum of the gains of optical amplifiers6and8to be constant.

A power diagram as inFIG. 6can be obtained for the optical amplification device illustrated inFIG. 8. Accordingly, the wavelength characteristic of gain can be maintained constant, and a wide input dynamic range can be obtained. Further, the power of pump light can be suppressed.

With the optical amplification device ofFIG. 8, it is apparent that the power diagram satisfying the conditions of the present invention can be obtained even if any one of feedback loops18and20is omitted. Accordingly, any one of feedback loops18and20may be omitted. Further, both feedback loops18and20may be omitted. In the case that each of optical amplifiers6and8includes an EDF and a pumping light source for supplying pump light to the EDF under the condition where none of feedback loops18and20are used, it is desirable to add to at least one of optical amplifiers6and8an APC (automatic power control) loop for maintaining the power of the pump light constant or an ACC (automatic current control) loop for maintaining a drive current for the pumping light source constant. The addition of APC or ACC is particularly effective to first-stage optical amplifier6, so as to achieve many of the objects of the present invention.

FIG. 9is a diagram illustrating details of the optical amplification device inFIG. 8, according to an embodiment of the present invention. Referring now toFIG. 9, the input level and the output level of first-stage optical amplifier6are reflected by output electrical signals from photodetectors56and44, respectively. Accordingly, the gain generated in first-stage optical amplifier6can be calculated by a gain calculating circuit68according to the ratio or difference in level between the output electrical signals from photodetectors56and44.

To detect the input level of second-stage optical amplifier8, an optical coupler69, an optical bandpass filter70, and a photodetector72are provided as respectively corresponding to optical coupler30, optical bandpass filter60, and photodetector56for first-stage optical amplifier6. The gain generated in second-stage optical amplifier8can be calculated by a gain calculating circuit74according to the ratio or difference in level between output electrical signals from photodetectors72and50.

A control circuit76(corresponding to control unit66inFIG. 8) generates a control signal CS so that the sum of the gains obtained from gain calculating circuits68and74becomes constant and adjusts the attenuation of variable optical attenuator10according to the control signal CS.

The pass band of each of optical bandpass filters48,54,60and70is set so as to include the wavelength of the signal light to be amplified. For example, in the case that the signal light to be amplified is WDM signal light, the pass band of each filter may be set so as to include the wavelength of an optical signal in one channel or may be set so as to include the wavelengths of optical signals in plural channels. Alternatively, the pass band may be set so as to pass ASE in a certain band not including the wavelength of the signal light, because the power of ASE included in this band reflects the gain.

In any case, the pass band of each of optical bandpass filters48,54and70is desirably set so as not to include the wavelength of the pump light, so as to avoid the influence of the pump light.

FIG. 10is a diagram illustrating details of the optical amplification device inFIG. 8, according to an additional embodiment of the present invention. Referring now toFIG. 10, modified gain calculating circuits68′ and74′ are used to detect the gains of first-stage and second-stage optical amplifiers6and8according to the absorptance of the pump light in EDFs24and26, respectively.

Of the pump light supplied from laser diode38to EDF24, the residual pump light not absorbed by EDF24is branched from a main optical path (an optical path between input port2and output port4) by a WDM coupler78provided between optical coupler32and variable optical attenuator10. The residual pump light branched by WDM coupler78is supplied to a photodetector80. Photodetector80outputs an electrical signal having a voltage level (or current level) corresponding to the power of the residual pump light received.

The output signal from photodetector80reflects the power of the residual pump light. The power of the pump light supplied from laser diode38to EDF24reflects the drive current supplied from drive circuit42to laser diode38. Accordingly, the absorptance of the pump light in EDF24can be obtained according to the output signal from photodetector80and a signal from drive circuit42. Gain calculating circuit68′ calculates the gain generated in EDF24according to the absorptance of the pump light obtained. To detect the power of the residual pump light in EDF26, a WDM coupler82and a photodetector84are provided as respectively corresponding to WDM coupler78and photodetector80. WDM coupler82is optically connected between EDF26and variable optical attenuator10.

Gain calculating circuit74′ can detect the gain generated in EDF26according to an output signal from photodetector84and a signal from drive circuit49. Control circuit76generates a control signal CS so that the sum of the two gains calculated by gain calculating circuits68′ and74′ becomes constant, thereby maintaining constant the wavelength characteristic of total gain generated in the main optical path.

FIG. 11is a graph illustrating a change in the wavelength characteristic of gain generated in an EDF with a change in population inversion coefficient (inversion parameter). InFIG. 11, the vertical axis represents gain (dB) or local gain (dB/m), and the horizontal axis represents wavelength (nm). The wavelength characteristic of gain continuously changes from a characteristic shown by reference numeral86toward a characteristic shown by reference numeral88with an increase in population inversion coefficient from 0 toward 1. The characteristic86corresponding to the case where the population inversion coefficient is 0 provides a so-called absorption cross section, whereas the characteristic88corresponding to the case where the population inversion coefficient is 1 provides a so-called emission cross section. Accordingly, the gain at a certain wavelength decreases with an increase in absorptance of pump light in an EDF. Thus, the gain generated in an EDF and the absorptance of pump light in the EDF are in a 1:1 correspondence, so that the gain can be calculated according to the absorptance of pump light.

FIG. 12is a diagram illustrating details of the optical amplification device inFIG. 8, according to a further embodiment of the present invention. Referring now toFIG. 12, the gains generated in EDFs24and26are detected in accordance with the fact that the gain generated in an EDF is reflected by the power of spontaneous emission light (SE light) emitted sideward from the EDF. To detect the power of spontaneous emission light emitted sideward from EDF24over its entire length or at a part thereof, a photodetector90is provided in the vicinity of EDF24. Similarly, to detect the power of spontaneous emission light emitted sideward from EDF26over its entire length or at a part thereof, a photodetector92is provided in the vicinity of EDF26.

Gain calculating circuits68″ and74″ calculate the gains generated in EDFs24and26according to output signals from photodetectors90and92, respectively. Accordingly, control circuit76can generate a control signal CS according to output signals from gain calculating circuits68″ and74″ so that the sum of the gains generated in EDFs24and26becomes constant.

The attenuation of the variable optical attenuator10is determined according to the control signal CS, thereby maintaining constant the total sum of the gains generated in the optical path between input port2and output port4. Accordingly, the wavelength characteristic of gain of the device can be maintained constant, and a wide input dynamic range can be obtained. Further, the power of pump light can be suppressed.

InFIG. 12, photodetectors90and92are used to respectively receive the spontaneous emission light emitted sideward from EDFs24and26. Alternatively, EDFs24and26may be wound to form the same loop, and a single photodetector may be provided in the vicinity of the loop of EDFs24and26to detect an optical power corresponding to the sum of the powers of the simultaneous emission light emitted sideward from EDFs24and26. This optical power reflects the sum of the gains generated in EDFs24and26. Accordingly, control circuit76may generate a control signal CS according to an output signal from the single photodetector, thereby maintaining constant the total sum of the gains generated in the optical path between input port2and output port4. In this case, one of photodetectors90and92and one of gain calculating circuits68″ and74″ can be omitted, thereby simplifying the configuration of the device.

FIG. 13is a diagram illustrating an optical amplification device, according to a further embodiment of the present invention. More specifically,FIG. 13illustrates the configuration of a wideband EDFA. Referring now toFIG. 13, an EDF200and a pumping light source210represent a low-noise preamplifier stage. An automatic gain control (AGC) circuit220controls pumping light source210to provide automatic gain control. A variable attenuator (VAT)230is controlled by an automatic level control (ALC) circuit240to appropriately attenuate the output of the preamplifier stage. EDFs242and244are pumped by pumping light sources246and248, respectively, to provide a post amplifier stage with high output power. An automatic gain control (AGC) circuit250controls pumping light sources246and248to provide automatic gain control. Therefore, AGC is employed in both the preamplifier stage and the post amplifier stage.

Gain equalizers (GEQ)252and254are utilized to flatten the gain in the entire signal band for the pre-amplifier stage and the post-amplifier stage, respectively. A dispersion compensating fiber (DCF)256can be positioned along the transmission line.

A supervisory (SV) circuit extracts supervisory information from a supervisory channel at a supervisory wavelength λsv, and uses the extracted information to control ALC circuit240.

FIGS. 14(A) and 14(B)are diagrams illustrating different operational modes of the optical amplification device inFIG. 13, according to an embodiment of the present invention. Referring now toFIG. 14(A), with this operational mode, the preamplifier stage employs automatic power control (APC) provided by AGC circuit220. As shown inFIG. 14(A), the decreasing amount of the preamplifier stage gain ΔG is added to the gain of the postamplifier stage by controlling variable attenuator230to keep the total gain constant.

As shown inFIG. 14(B), with this operational mode, the preamplifier stage employs automatic level control (ALC). As shown inFIG. 14(B), the decreasing amount of the preamplifier stage gain ΔG is added to the gain of the postamplifier stage by controlling variable attenuator230to keep the total gain constant.

FIG. 15is a diagram illustrating an optical amplification device according to an additional embodiment of the present invention.

Various of the above embodiments of the present invention relate to two optical amplifiers cascaded together. However, the present invention is applicable to configurations where three or more optical amplifiers are cascaded together.

Moreover, according to the above embodiments of the present invention, an optical attenuator is positioned between optical amplifiers. However, the present invention is applicable to configurations where more than one optical attenuator is positioned between optical amplifiers, and to configurations with more than two optical amplifiers cascaded together, and optical attenuators positioned at various locations amongst the cascaded optical amplifiers.

According to the above embodiments of the present invention, it is possible to provide a method and device for optical amplification and a novel system including the device which can maintain the wavelength characteristic of gain constant, can obtain a wide input dynamic range, and can suppress the power of pump light.

According to the above embodiments of the present invention, a variable optical attenuator is positioned between first and second optical amplifiers. The first and second optical amplifiers can each be provided with an ALC feedback loop, for maintain output levels at a constant value. The input level of the first optical amplifier is detected, and the variable optical attenuator is controlled so that, when the input level of the first optical amplifier changes by Δ (dBm in unit), the input level of the second optical amplifier changes by approximately −Δ.

Therefore, as indicated above, according to various embodiments of the present invention, when the input level of a first optical amplifier changes by Δ, the input level of a second optical amplifier changes by approximately −Δ. For example, to change by approximately −Δ, the input level of the second optical amplifier should preferably change by −(Δ±Δ/20). However, a change of approximately −Δis not intended to be limited to this preferable range, and other ranges may be sufficient to provide sufficient operation.

According to the above embodiments of the present invention, a variable optical attenuator is positioned between first and second optical amplifiers. The variable optical attenuation provides a variable attenuation in accordance with a control signal supplied thereto. A first gain monitor detects the gain of the first optical amplifier and a second gain monitor detects the gain of the second optical amplifier. The variable optical attenuator is controlled so that the sum of the detected gains of the first and second optical amplifiers becomes constant.

Various optical amplification devices for use in WDM optical communication systems are described above. Japanese Patent Laid-open Nos. Hei. 8-248455 and Hei. 10-51057, filed by the Applicants, disclose additional optical amplification devices for use in WDM optical communication systems. In these optical amplification devices, WDM signal light obtained by multiplexing a plurality of optical signals having different wavelengths is subjected to batch amplification by two-stage amplifier sections each employing, for example, an erbium doped fiber (EDF). In the batch amplification, AGC is performed to control the gain in each of the front-stage and rear-stage amplifier sections to be constant. By this control, the wavelength dependence of gain (which will be hereinafter referred to as gain-wavelength characteristic) of each EDFA can be maintained constant even when input light power changes. By effectively compensating for the gain-wavelength characteristic of the optical amplifier, WDM signal light whose channels are equalized in level can be obtained. Further, there has been proposed another optical amplification device which can obtain stable amplifying characteristics in the case that the number of wavelengths (the number of channels) included in WDM signal light is changed.

In such optical amplification devices, a large-capacity pumping source must be used to realize constant gain control. In general, the power level of WDM signal light per wavelength (per channel) input to the optical amplification device is not a fixed value, but is varied. To control the gain to be constant against such variations in input light level, the power of pump light must be controlled substantially exponentially. Accordingly, it is necessary to provide a relatively large-capacity pumping source which can support such exponential control.

While the optical amplification device is required to have a required input dynamic range supporting variations in input light level, it is also required to output WDM signal light whose channels are equalized in level. For example, this requirement is met by a proposed method for controlling an optical attenuation so that the output light level per channel becomes constant by providing a variable optical attenuator between the front-stage and rear-stage amplifier sections of the optical amplification device.

In this case, the gain of the front-stage amplifier section is set so that the level of output light from the front-stage amplifier section becomes a constant value or more when the input light level is minimum., Accordingly, also when the input light level is high, the amplification with the above set gain is carried out and thereafter the amplified signal light is attenuated to a given level by the variable optical attenuator. Therefore, when the input light level is high, excess optical amplification is performed in the front-stage amplifier section to realize AGC. Providing a costly high-capacity pumping source to allow such excess optical amplification is a disadvantage from the viewpoint of cost reduction of the optical amplification device.

Further, in an optical amplification device (such as an optical amplifier) having a two-stage amplifying configuration, it is effective to set the gain of the front-stage amplifier section to a high value in reducing a noise figure (NF). However, realization of this setting also requires providing a large-capacity pumping source. That is, setting the gain to a high value in the case of a low input light level can be relatively easily realized also by using a normal-capacity pumping source. However, when the input light level is increased under AGC with the gain being set to a high value, the power of pump light by the normal-capacity pumping source becomes lacking to cause a possibility that the AGC does not effectively function. For this reason, the large-capacity pumping source is required.

Thus, such an optical amplification device applied to a WDM optical communication system has a problem that an excess power of pump light is required in the front-stage amplifier section, so as to ensure a required input dynamic range supporting variations in input light level, to equalize the levels of all channels of output light, and to improve noise characteristics.

FIG. 16is a diagram illustrating an optical amplification device applicable to a WDM optical transmission system.

Referring now toFIG. 16, the optical amplification device has a two-stage amplification configuration including a front-stage amplifier section501amplifying WDM signal light input to an input terminal Tin, a middle-stage ALC section503connected to an output end of front-stage amplifier section501, and a rear-stage amplifier section505amplifying WDM signal light passed through middle-stage ALC section503and outputting amplified WDM signal light from an output terminal Tout.

In front-stage amplifier section501, the WDM signal light input to the input terminal Tin is supplied through a beam splitter510, an optical isolator511, and a WDM coupler512to an erbium doped fiber (EDF)513. Pump light is emitted from a pumping source (LD)518and supplied through WDM coupler512to EDF513from its front end. Thus, EDF513is forward pumped by the pump light.

The drive condition of pumping source518is controlled according to a signal from an AGC circuit520. More specifically, a part of the WDM signal light to be supplied to EDF513and a part of the amplified WDM signal light output from EDF513are respectively extracted by beam splitters510and516and respectively converted into electrical signals by photodetectors (PD)517and519. These electrical signals from photodetectors517and519are input to AGC circuit520. In AGC circuit520, an actual gain is obtained according to the input signals from photodetectors517and519, and a signal for controlling the drive condition of pumping source518so that the actual gain becomes constant is generated.

Thus, the gain by EDF513is controlled to be constant, and the WDM signal light is input into EDF513and passed therethrough, thereby amplifying the WDM signal light. The WDM signal light amplified by EDF513is supplied through an optical isolator514to a gain equalizer (GEQ)515. Gain equalizer515is an optical filter for compensating for a gain-wavelength characteristic of EDF513. More specifically, in the case that EDF513has a gain-wavelength characteristic at a predetermined gain as shown inFIG. 17, an optical filter having a transmittance-wavelength characteristic as shown by a solid line inFIG. 18may be used as gain equalizer515. The WDM signal light passed through gain equalizer515is supplied through beam splitter516to middle-stage ALC section503.

In middle ALC section503, the WDM signal light from front-stage amplifier section501is supplied to a variable optical attenuator (VATT)530as a level adjusting device. An optical attenuation by variable optical attenuator530is controlled according to a signal from an ALC circuit534. More specifically, a part of the WDM signal light output from variable optical attenuator530is extracted by a beam splitter531and converted into an electrical signal by a photodetector533. This electrical signal is input to ALC circuit534. In ALC circuit534, a signal for controlling the optical attenuation by variable optical attenuator530so that the level of the WDM signal light per channel to be output from variable optical attenuator530becomes constant is generated according to a result of comparison between an ALC reference value (Valcref) supplied from a reference value generating circuit535and the signal supplied from photodetector533.

Although not shown, information on the number of wavelengths (the number of channels) of the WDM signal light is given to reference value generating circuit535from the outside thereof, and the ALC reference value is output so as to support a change in the number of channels.

The WDM signal light output from variable optical attenuator530is supplied through a beam splitter531to a dispersion compensating fiber (DCF)532. Dispersion compensating fiber532functions to compensate for a chromatic dispersion characteristic of an optical transmission line connected to the optical amplification device. However, in the case that no dispersion compensation is required, dispersion compensating fiber532may be omitted. The WDM signal light passed through dispersion compensating fiber532is supplied to rear-stage amplifier section505.

In rear-stage amplifier section505, the WDM signal light from middle-stage ALC section503is supplied through a beam splitter550, a gain equalizer551, an optical isolator552, and a WDM coupler553to an EDF554. Similar to gain equalizer515in front-stage amplifier section501, gain equalizer551is an optical filter for compensating for a gain-wavelength characteristic of EDF554at a predetermined gain. Pump light emitted from a pumping source557is supplied through WDM coupler553to EDF554from its front end, thereby forward pumping EDF554.

The drive condition of pumping source557is controlled according to a signal from an AGC circuit559. More specifically, a part of the WDM signal light to be input to EDF554and a part of the amplified WDM signal output from EDF554are respectively extracted by beam splitters550and555and respectively converted into electrical signals by photodetectors556and558. These electrical signals from photodetectors556and558are input to AGC circuit559. In AGC circuit559, an actual gain is obtained according to the input signals from photodetectors556and558, and a signal for controlling the drive condition of pumping source557so that the actual gain becomes constant is generated. Thus, the gain by EDF554is controlled to be constant, and the WDM signal light is input into EDF554and passed therethrough, thereby amplifying the WDM signal light. The WDM signal light amplified by EDF554is passed through beam splitter555and output from the output terminal Tout of this optical amplifier.

EDFs513and554, pumping sources518and557, and WDM couplers512and553in front-stage and rear-stage amplifier sections501and505function as an example of an optical amplifying device. Further, AGC circuits520and559, photodetectors517,519,556, and558, and beam splitters510,516,550, and555in front-stage and rear-stage amplifier sections501and505function as examples of a constant gain control devices. Further, gain equalizers515and551in front-stage and rear-stage amplifier sections501and505function as examples of gain-wavelength characteristic compensating devices. Further, ALC circuit534, beam splitter531, photodetector533, and reference value generating circuit535in middle-stage ALC section503function as examples of a constant level control device.

AGC is performed in each of front-stage amplifier section501and rear-stage amplifier section505according to detected levels of the WDM signal light on the upstream and downstream sides of the corresponding EDF. As a modification, AGC may be performed by detecting amplified spontaneous emission (ASE) generated in each EDF and determining the gain by each EDF according to a detected level of the ASE. Further, while forward pumping is performed in each of front-stage amplifier section501and rear-stage amplifier section505, backward pumping or bidirectional pumping may be performed in each amplifier section.

FIG. 19is a graph illustrating changes in power level of the WDM signal light per channel propagating in the optical amplification device ofFIG. 16. As shown inFIG. 19, although there is a change in input level per channel input to the optical amplifier, the level of the WDM signal light per channel is controlled to be constant in middle-stage ALC section503. Accordingly, the level of the WDM signal light per channel amplified under the constant gain control in rear-stage amplifier section505is also maintained constant.

To ensure a required input dynamic range and maintain AGC for front-stage amplifier section501, pumping source518must be able to supply pump light having a high power to EDF513. In the case that pumping source518cannot supply pump light having a power enough to maintain a set gain for high-level input light as shown by a broken line inFIG. 19, the gain by EDF13becomes low to result in a change in the gain-wavelength characteristic shown inFIG. 17. If the gain-wavelength characteristic of EDF513changes, the compensation by gain equalizer515does not effectively function, and as a result, the level of the WDM signal light per channel output from the optical amplifier cannot be maintained constant.

A change in the gain-wavelength characteristic of an EDF will now be described in brief.

FIG. 20is a graph illustrating an example of changes in the gain-wavelength characteristic of an EDF with changes in the gain of the EDF. In the example shown inFIG. 20, the gain-wavelength characteristic has a negative tilt such that the gain decreases with an increase in wavelength when the gain of the EDF is higher, whereas the gain-wavelength characteristic has a positive tilt such that the gain increases with an increase in wavelength when the gain of the EDF is lower. In this manner, it has been confirmed that the gain-wavelength characteristic of an EDF is such that the gain tilt changes from a positive tilt to a negative tilt with an increase in the gain of the EDF, i.e., an increase in pump energy. Further, it has been reported that the gain tilt also changes according to an input light level or an EDF length (e.g., Y. Nakabayashi et al., “Flattening of multi-wavelength batch amplification of optical fiber amplifier using fiber amplification factor control”, ShingakuGiho, OCS94-66; S. Yoshida et al., “Wavelength multiplexed signal common amplification characteristics of high-concentration A1codoped EDFA”, ShingakuGiho, OCS95-9; Y, Sugaya et al., “A study of configuration method for wavelength multiplexing Er-doped fiber optical amplifier”, ShingakuGiho).

InFIG. 16, pumping source518having a relatively large capacity is required to maintain the constant gain control of front-stage amplifier section501, causing an increase in cost of the optical amplifier.

Noise characteristics of the optical amplification device inFIG. 16will now be described. The noise figure (NF) of the optical amplifier as a whole can be calculated in accordance with the following Equation (1).
NF [dB]=LOSSf+10×log {10NFf/10+(10LOSSm/10+10NFr/10)/10Gf/10}  Equation (1):
where LOSSf is the loss on the upstream side of EDF513, NFf is the noise figure of EDF513, LOSSm is the loss on the downstream side of EDF513and on the upstream side of EDF554(the loss in the middle portion of the optical amplifier), NFr is the noise figure of EDF554, and Gf is the gain of EDF513. In the case that LOSSf=2 dB, NFf=4 dB, LOSSm=15 dB, NFr=6 dB, and Gf=15 dB, the noise figure of the optical amplifier as a whole is calculated to NF=7.61 dB from Equation (1).

As apparent from Equation (1), the losses LOSSf and LOSSm or the noise figures NFf and NFr must be decreased or the gain Gf must be increased to reduce the noise figure NF of the optical amplifier as a whole. However, decreasing the losses LOSSf and LOSSm or the noise figures NFf and NFr is limited because they depend on the characteristics of the respective devices. On the other hand, increasing the gain Gf can be realized by increasing the power of the pump light to be supplied to EDF513. In particular, when the level of signal light input to the optical amplifier becomes low, a small value of the noise figure NF of the optical amplifier must be ensured for the purpose of increasing an S/N ratio at a receiving end.

In the case that the level of input light is low, the noise figure NF can be relatively easily reduced by increasing the gain Gf of EDF513, because not so high pump light power is required. However, the gain Gf of EDF513must be controlled to be constant because the gain-wavelength characteristic of EDF513must be compensated by gain equalizer515. Accordingly, although the noise figure NF can be reduced by setting the gain Gf of EDF513to a high value in the case that the level of input light is low, there is a possibility that when the level of input light becomes high, the pump light power may lack to cause a problem that AGC is not effected and there occurs a difference in level of output light between channels.

Consequently, as far as the optical amplification device inFIG. 16is required to have a required input dynamic range, the power of pump light to be supplied to EDF513must be increased to increase the gain Gf for the purpose of reducing the noise figure NF.

In these circumstances, according to embodiments of the present invention as will be discussed in more detail below, an optical amplification device (such as an optical amplifier) for WDM has been achieved by improving the configuration inFIG. 16to thereby ensure a required input dynamic range and allow effective compensation for the gain-wavelength characteristic of the EDF and a reduction in the noise figure NF without restriction by AGC.

FIG. 21is a diagram illustrating an optical amplification device according to an embodiment of the present invention. InFIG. 21, substantially the same parts as those of the optical amplification device inFIG. 16are denoted by the same reference numerals.

The optical amplification device shown inFIG. 21has been improved over the configuration shown inFIG. 16by detecting a change in gain of front-stage amplifier section501, making the ALC reference value in middle-stage ALC section503changeable according to the detected change in gain, and making the set gain in rear-stage amplifier section505changeable according to the detected change in gain. These improvements can eliminate the need for use of a large-capacity pumping source as pumping source518in front-stage amplifier section501. More specifically, the configuration of the optical amplification device inFIG. 21is different from the configuration inFIG. 16in that front-stage amplifier section501further includes log transformers (LOG)521and522and subtracters (−)523and524, in that middle-stage ALC section503further includes a log transformer536and a subtracter537, and in that rear-stage amplifier section505further includes a log transformer560, an adder561, and an anti-log transformer562.

In this embodiment of the present invention, log transformers521and522and subtracter523function as an example of a gain measuring device, and subtracter524functions as an example of a gain deviation computing device. Further, subtracter537functions as an example of a reference level changing device, and log transformer560, adder561, and anti-log transformer562function as an example of a reference gain changing device.

Input terminals of log transformers521and522in front-stage amplifier section501are connected to output terminals of photodetectors517and519, respectively, so that log transformers521and522respectively receive electrical signals from photodetectors517and519and transform the voltage levels of the electrical signals into logarithmic values, which are in turn supplied to subtracter523. Subtracter523subtracts the level of the output signal from log transformer521from the level of the output signal from log transformer522to obtain a voltage value Vagc corresponding to the gain of EDF513, which is in turn supplied to subtracter524. Subtracter524subtracts the voltage value Vagc output from subtracter523from a predetermined gain reference value Vagcref to obtain a gain correction value Vadj, which is in turn supplied to middle-stage ALC section503and rear-stage amplifier section505.

An input terminal of log transformer536in middle-stage ALC section503is connected to an output terminal of photodetector533, so that log transformer536receives an electrical signal from photodetector533and transforms a voltage level of the electrical signal into a logarithmic value, which is in turn supplied to one of two input terminals of ALC circuit534. Subtracter537receives the gain correction value Vadj from subtracter524in front-stage amplifier section501and an ALC reference value Valcref from reference value generating circuit535, and subtracts the gain correction value Vadj from the ALC reference value Valcref to obtain a new ALC reference value Valcref', which is in turn supplied to the other input terminal of ALC circuit534. ALC circuit534controls the optical attenuation of variable optical attenuator530according to the new ALC reference value Valcref' so that the level of the WDM signal light per channel becomes constant.

An input terminal of log transformer560in rear-stage amplifier section505is connected to an output terminal of photodetector556, so that log transformer560receives an electrical signal from photodetector556and transforms a voltage level of the electrical signal into a logarithmic value, which is in turn supplied to adder561. Adder561adds the gain correction value Vadj from subtracter524in front-stage amplifier section501to the voltage value output from log transformer560to obtain a sum, which is in turn supplied to anti-log transformer562. Anti-log transformer562transforms the logarithmic voltage value output from adder561into an anti-logarithmic value, which is in turn supplied to one of two input terminals of AGC circuit559. AGC circuit559controls the gain of EDF554to be constant according to the signal from anti-log transformer562and the signal from photodetector558.

Therefore, inFIG. 21, log transformer521, log transformer522, subtracter523, subtracter524, log transformer560, adder561and anti-log transformer562together operate as a gain adjustor which detects a deviation in gain of front-stage amplifier section501from a target (or reference) gain, and adjusts the gain of rear-stage amplifier section505to compensate for the detected deviation. However, the use of such log transformers, subtracters and anti-log transformers represents only one embodiment of such a gain adjustor, and modifications and other designs for a gain adjustor can easily be implemented.

Moreover, inFIG. 21, log transformer521, log transformer522, subtracter523, subtracter524and subtracter537together operate as a level controller which controls a level of the light amplified by front-stage amplifier section501before being amplified by rear-stage amplifier section505to be at a target level. The level controller adjusts the target level to compensate for a detected deviation in gain of front-stage amplifier section501from a reference gain. However, the use of such log transformers and subtracters represents only one embodiment of such a level controller, and modifications and other designs for a level adjuster can easily be implemented.

The operation of the optical amplification device inFIG. 21will now be described in more detail.

FIG. 22is a graph illustrating changes in power level of the WDM signal light per channel propagating in the optical amplification device inFIG. 21, according to an embodiment of the present invention. InFIG. 22, the changes in power level in the case of a low level of input light as shown by a long and short dashed line are similar to those shown inFIG. 19. That is, the low-level WDM signal light input to front-stage amplifier section501is amplified with a sufficiently high gain Gf set in consideration of decreasing a noise figure, and at this time the gain-wavelength characteristic of EDF513is effectively compensated by gain equalizer515. In this case, the gain correction value Vadj output from subtracter524is zero because the AGC gain reference value Vagcref is predetermined according to the gain Gf. The WDM signal light supplied from front-stage amplifier section501to middle-stage ALC section503is attenuated to a given level according to the ALC reference value Valcref because the gain correction value Vadj is zero. Thereafter, the WDM signal light is supplied through dispersion compensating fiber532to rear-stage amplifier section505. The WDM signal light input to rear-stage amplifier section505is amplified with the predetermined gain Gr, and at this time the gain-wavelength characteristic of EDF554is effectively compensated by gain equalizer551. Thus, in the case that the level of input light is low, the noise figure of the optical amplifier as a whole can be reduced by setting the gain Gf of front-stage amplifier section501to a high value. Further, the gain-wavelength characteristics of EDFs513and554in front-stage and rear-stage amplifier sections501and505are effectively compensated by gain equalizers515and551, respectively, because the pump light power is relatively low and the constant gain control can be maintained irrespective of a slight change in input light level. Therefore, the WDM signal light whose channels are equalized in level can be output from the optical amplifier.

In the case that the level of input light is high as shown by a solid line inFIG. 22, pumping source518cannot supply pump light having a high power enough to maintain the gain Gf constant, and the WDM signal light is amplified with a gain Gf' lower than the gain Gf. When the gain is reduced, the gain-wavelength characteristic of EDF513changes so as to have a positive tilt as shown inFIG. 20, so that the compensation of EDF513by gain equalizer515cannot be effectively performed.

To cope with this problem, such a change in the gain in front-stage amplifier section501is transmitted to middle-stage ALC section503and rear-stage amplifier section505to change the ALC reference value in middle-stage ALC section503and the set gain in rear-stage amplifier section505, thereby compensating for the gain-wavelength characteristic of the optical amplifier as a whole. That is, the voltage value Vagc expressed as a logarithmic value of the gain Gf' in front-stage amplifier section501is output from subtracter523, and the voltage value Vagc is then subtracted from the AGC gain reference value Vagcref by subtracter524. The difference obtained by subtracter524is then supplied as the gain correction value Vadj to both middle-stage ALC section503and rear-stage amplifier section505.

In middle-stage ALC section503, the ALC reference value Valcref is changed according to the gain correction value Vadj from front-stage amplifier section501. For example, in the case that the gain in front-stage amplifier section501decreases by 1 dB, the gain correction value Vadj=1 is input to subtracter537, and the difference obtained by subtracting the gain correction value Vadj from the ALC reference value Valcref, i.e., the difference of (Valcref−1) dB is supplied as a new ALC reference value Valcref' from subtracter537to ALC circuit534. Then, the optical attenuation of variable optical attenuator530is controlled according to this new ALC reference value Valcref', so that the WDM signal light having a level lower by 1 dB than the level maintained under the constant gain control in front-stage amplifier section501is output from middle-stage ALC section503to rear-stage amplifier section505.

In rear-stage amplifier section505, the set gain in AGC is changed according to the gain correction value Vadj from front-stage amplifier section501. In the above example, the gain correction value Vadj=1 from front-stage amplifier section501is input to adder561, and added to the voltage value expressed as a logarithmic value supplied from log transformer560. That is, the voltage value obtained by increasing the level of the WDM signal light to be supplied to EDF554by 1 is supplied from adder561to anti-log transformer562. Then, the voltage value obtained as an anti-logarithmic value from anti-log transformer562is supplied to AGC circuit559, thereby amplifying the WDM signal light with a gain Gr′ higher by 1 dB than the gain Gr. When the gain is increased, the gain-wavelength characteristic of EDF554changes so as to have a negative tilt as shown inFIG. 20, so that the compensation of EDF554by gain equalizer551cannot be effectively performed. However, the uncompensated amount of the gain-wavelength characteristic in front-stage amplifier section501is canceled in rear-stage amplifier section505, thereby allowing effective compensation for the gain-wavelength characteristic of the optical amplifier as a whole.

At this time, an increase in pump light power required to increase the gain in rear-stage amplifier section505can be suppressed to a relatively small amount by operating EDF554in a saturated region. This is due to the fact that the relation of gain to input light level in an EDF generally has a negative tilt of about −0.8 in a saturated region as shown inFIG. 23(e.g., when the input light level decreases by 1 dB, the gain increases by about 0.8 dB). Accordingly, an increase in pump light power required to increase the set gain can be suppressed.

As described above, in the case that the input light level is high, the gain Gf in front-stage amplifier section501is changed to the lower gain Gf' without restriction by AGC, thereby eliminating the need for use of a large-capacity light source as pumping source518, and it is sufficient for pumping source518to supply pump light in its attainable range of output power to EDF513. Even when the gain-wavelength characteristic of EDF513cannot be effectively compensated by gain equalizer515because of a change in gain in front-stage amplifier section501, the gain-wavelength characteristics in front-stage and rear-stage amplifier sections501and505can be counterbalanced with each other by changing the ALC reference value in middle-stage ALC section503and the set gain in rear-stage amplifier section505, thereby obtaining WDM signal light whose channels are equalized in level. Further, by operating rear-stage amplifier section505in a saturated region, an increase in pump light power in rear-stage amplifier section505can be minimized in spite of a decrease in gain in front-stage amplifier section501. Regarding noise characteristics, there is little need for especially reducing a noise figure to ensure an S/N ratio at a receiving end, because the input light level is high. Accordingly, it can be said that it is almost unnecessary to maintain a high gain in front-stage amplifier section501and reduce a noise figure in comparison with the case that the input light level is low.

InFIG. 21, the gain-wavelength characteristic in front-stage amplifier section501and the gain-wavelength characteristic in rear-stage amplifier section505change with the same tendency in response to a change in the set gains. That is, the Er doped fiber amplifiers used in front-stage amplifier section501and rear-stage amplifier section505are similar in configuration to each other. However, the present invention is not limited to this configuration. For example, even in the case that the amounts of change in the gain-wavelength characteristics in the front-stage and rear-stage amplifier sections are different from each other in response to a change in the set gains, it is sufficient that the tendencies of change in the gain-wavelength characteristics in the front-stage and rear-stage amplifier sections are to be the same as each other, thereby exhibiting the effect of counterbalancing the gain-wavelength characteristics in the front-stage and rear-stage amplifier sections according to the above preferred embodiment. In this case, however, precise compensation for the gain-wavelength characteristic in the optical amplifier as a whole is not assured. Further, also in the case that the tendencies of change in the gain-wavelength characteristics in the front-stage and rear-stage amplifier sections are opposite to each other in response to a change in the set gains, a similar effect can be obtained by using a subtracter in place of the adder561in rear-stage amplifier section505, for example.

While erbium doped fibers513and554are used in front-stage and rear-stage amplifier sections501and505, the present invention is not limited to this configuration. For example, rare earth doped fibers containing any rare earth elements other than erbium may also be used in front-stage and rear-stage amplifier sections501and505. Further, while the optical amplifier inFIG. 21has a two-stage amplifying configuration, three or more-stage amplifying configuration may be adopted.

FIG. 24is a diagram illustrating an optical communication system according to embodiments of the present invention. Referring now toFIG. 24, optical transmitters (TX1. . . TXN)600transmit optical signals at different wavelengths (λ1. . . λN), respectively. A multiplexer (MUX)610multiplexes the optical signals into a WDM signal light, and provides the WDM signal light to an optical fiber transmission line620. An optical amplification device630amplifies the WDM signal light as the WDM signal light is travels through the transmission line620. A demultiplexer (DEMUX)640demultiplexes the WDM signal light so that the individual optical signals can be received by receivers (RX1. . . RXN)650. Optical amplification device630can have a configuration as described herein for any of the embodiments of the present invention. For example, optical amplification device630can have a configuration as disclosed, for example, in eitherFIGS. 5,7,8,9,10,12,13,15or21.

According to the above embodiments of the present invention, an optical amplification device (such as an optical amplifier) for WDM includes a gain deviation detecting device and a reference gain changing device. Accordingly, even in the case that the level of input light to the optical amplification device largely changes, the wavelength dependence of gain of each optical amplification stage can be reliably compensated without restriction by constant gain control. As a result, the optical amplification device can output WDM signal light whose channels are equalized in level. Further, there is no need for using a large-capacity pumping source to maintain the constant gain control, thereby attaining a cost reduction. Further, noise characteristics can be improved because the gain of the front-stage optical amplifying device can be set to a higher value. In addition, because a constant level control device and a reference level changing device are provided, it is possible to obtain WDM signal light whose optical signals in all the channels are amplified with a uniform gain and a constant level. Thus, it is possible to provide an optical amplifier for WDM having more stable amplification characteristics.

According to the above embodiments of the present invention, an optical amplification device (such as an optical amplifier) for wavelength division multiplexing includes a front-stage amplifier section501and a rear-stage amplifier section505each for amplifying WDM signal light having changing input level under constant gain control, and a middle-stage ALC section503for controlling the WDM signal light to a constant level. In front-stage amplifier section501, a gain correction value Vadj indicative of a gain deviation is detected by log transformers521and522and subtracters523and524. According to the gain correction value Vadj, an ALC reference value Valcref in middle-stage ALC section502and a reference gain in rear-stage amplifier section505are changed. Accordingly, a change in the gain-wavelength characteristic of front-stage amplifier section.501is canceled by the gain-wavelength characteristic of rear-stage amplifier section505, thereby effectively compensating for the gain-wavelength characteristic of the optical amplification device as a whole.

According to the above embodiments of the present invention, there is provided in an optical amplification device for WDM. A plurality of optical amplifying devices are cascaded together, each having a rare earth doped fiber for amplifying WDM signal light by receiving pump light. A plurality of constant gain control devices control the power of the pump light so that the gain of each optical amplifying device becomes a predetermined reference gain. A gain-wavelength characteristic compensating device compensates for the wavelength dependence of gain of each optical amplifying device at the reference gain. Moreover, a gain deviation detecting device detects a gain deviation between the gain of each optical amplifying device and the reference gain. A reference gain changing device changes the reference gain so that when the gain deviation of at least one of the plurality of optical amplifying devices is detected by the gain deviation detecting device, the reference gain of the other optical amplifying devices whose gain deviation is not detected is changed to cancel a change in the wavelength dependence of gain generated in the optical amplifying device whose gain deviation is detected.

With this configuration, the WDM signal light input to the optical amplification device is sequentially amplified by the plural cascaded optical amplifying devices. The pump light power in each optical amplifying device is controlled by the constant gain control device to thereby maintain the gain of each optical amplifying device constant in an attainable output range of the pump light. When the constant gain control for each optical amplifying device is maintained, the wavelength dependence of gain in each optical amplifying device is compensated by the gain-wavelength characteristic compensating device to thereby obtain WDM signal light whose channels are equalized in level. When the control by the constant gain control device in each optical amplifying device becomes out of the attainable output range of the pump light, the constant gain control for the optical amplifying device cannot be maintained to result in generation of a deviation between the gain of the optical amplifying device and its reference gain. As a result, the wavelength dependence of gain in the optical amplifying device changes to cause a problem that the compensation by the gain-wavelength characteristic compensating device does not effectively function. To cope with this problem, when this gain deviation is detected by the gain deviation detecting device, the reference gain of the other optical amplifying devices whose gain deviation is not detected is changed by the reference gain changing device according to the detected gain deviation. As a result, the change in the wavelength dependence of gain of the optical amplifying device whose constant gain control cannot be maintained is canceled by the wavelength dependence of gain of the other optical amplifying device whose reference gain has been changed, thereby obtaining WDM signal light whose channels are equalized in level.

Accordingly, even in the case that the level of input light to each optical amplifying device largely changes, the wavelength dependence of gain of each optical amplifying device can be reliably compensated without restriction by the constant gain control, thereby allowing output of WDM signal light having a flat gain-wavelength characteristic as the whole of the optical amplifier. Accordingly, the need for especially using a large-capacity pumping source can be eliminated to thereby reduce the costs of the optical amplifier for WDM. Further, the gain of the front-stage amplifying device can be set to a higher value, so that noise characteristics can also be improved.

Preferably, an optical amplification device according to embodiments of the present invention further comprises a level adjusting device, a constant level control device and a reference level changing device. The level adjusting device is provided on the front stage or rear stage of the plurality of optical amplifying devices or between the plurality of optical amplifying devices, for adjusting the level of the WDM signal light. The constant level control device controls an adjusting amount by the level adjusting device so that the power level of the WDM signal light per channel becomes a predetermined constant reference level. The reference level changing device changes the reference level so that when the gain deviation is detected by the gain deviation detecting device and the level adjusting device is provided on the rear stage of the optical amplifying device whose gain deviation is detected, the reference level is changed according to the gain deviation detected.

With this configuration, WDM signal light whose optical signals of all the channels are amplified with the same gain to a constant level can be obtained irrespective of whether or not the constant gain control is maintained for each optical amplifying device. Accordingly, it is possible to provide an optical amplifier for WDM which can be more stabilized in amplification characteristics.

Preferably, the gain deviation detecting device comprises a gain measuring device for measuring the gain of any one of the plurality of optical amplifying devices in which gain control by the constant gain control device cannot be maintained in a range of change in input light level, and gain deviation computing device for comparing the gain measured by the gain measuring device and the reference gain to obtain the gain deviation. The reference gain changing device is provided for any one of the plurality of optical amplifying devices in which the gain control by the constant gain control device can be maintained in the range of change in input light level.

According to the above embodiments of the present invention, the gain measuring device measures the gain according to the level of the WDM signal light input to the optical amplifying device and the level of the WDM signal light output from the optical amplifying device. As a modification, the gain measuring device may measure the gain according to the level of amplified spontaneous emission generated in the rare earth doped fiber of the optical amplifying device.

According to the above embodiments of the present invention, when the wavelength dependence of gain of the plurality of optical amplifying devices change with the same tendency in response to a change in gain, the reference gain of the other optical amplifying devices is increased with a decrease in gain in the optical amplifying device whose gain deviation is detected, whereas the reference gain of the other optical amplifying device is decreased with an increase in gain in the optical amplifying device whose gain deviation is detected.

Preferably, the gain deviation detecting device outputs a logarithmic value of the gain deviation, and the reference gain changing device changes the reference gain by using the logarithmic value of the gain deviation and the reference gain. More preferably, the reference level changing device changes the reference level by using the logarithmic value of the gain deviation and the reference level.

Therefore, according to the above embodiments of the present invention, an optical amplifier for use in a WDM optical communication system can ensure a required input dynamic range, can compensate for the gain-wavelength characteristic of each optical amplifying device within the optical amplifier without restriction by constant gain control, and can improve noise characteristics.

Various of the above embodiments of the present invention relate to an optical amplification device, such as an optical amplifier or an optical repeater, which has two optical amplifiers, or two optical amplification stages, cascaded together. However, the embodiments of the present invention are not intended to be limited to optical amplification devices having two stages. Instead, the present invention is applicable to apparatuses and methods in which more than two optical amplifiers, or optical amplification stages, are cascaded together. As an example, according to embodiments of the present invention as described above, an apparatus can include a plurality of optical amplifiers cascaded together so that a light is amplified by each optical amplifier as the light travels through the cascaded plurality of optical amplifiers. Each optical amplifier amplifies the light with a corresponding gain. A gain adjustor detects a deviation in gain of one of the plurality of optical amplifiers from a target gain, and adjusts the gain of at least one of the other of the plurality of optical amplifiers to compensate for the detected deviation. Here, the plurality of optical amplifiers cascaded together can include two or more optical amplifiers cascaded together.

Various wavelengths, frequencies and/or other numerical examples are provided herein to describe optical signals, pump lights, wavelength bands, etc. The present invention is not intended to be limited to these wavelengths, frequencies and/or other numerical examples.