BACKGROUND OF THE INVENTION Optical communication systems use optical fiber as a communication medium and light as an information carrier. For instance, an optical signal may be a beam of light modulated to represent binary-coded information. When light is used to transmit information, the information may be extracted from the beam of light through the use of a photodetector in a receiver. A photodetector is an electronic component that detects the presence of light radiation through conversion of light energy to electrical energy. A common photodetector is called a photodiode which consists of a semiconductor having a property called photoconductivity, in which the electrical conductance varies depending on the intensity of radiation striking the semiconductor material comprising the photodiode. Essentially, a photodiode is the same as an ordinary diode, except that the package has some transparency that allows light energy to effect junctions between the semiconductor materials inside.

To make efficient use of a single optical fiber, many unique data signals may be transmitted over the same fiber so long as each data signal modulates an optical signal with a wavelength different from the other optical signals on the same fiber. When the wavelengths of the different optical signals are only marginally different from one another, the transmission scheme may be called Dense Wavelength Division Multiplexing (DWDM). In a network using DWDM, two elements connected by a single physical link (optical fiber) may communicate using a number of signal channels, where each signal channel is an optical signal with a distinct wavelength.

One detrimental factor to be considered in optical communication is attenuation.

Essentially, signal power is attenuated over the length of a fiber such that the power of a signal at the receiving end of a transmission link is less than the power of the signal at the sending end of the transmission link. To overcome attenuation, a long optical transmission link may be made up of several shorter spans. At a repeater at the beginning of each span

after the first, the optical signal is received and subsequently regenerated at a power level that will allow accurate reception at the end of the span. Unfortunately, these repeaters require that the optical signal be converted to an electrical signal and this conversion has several inherent drawbacks.

Fortunately, equipment that amplifies the optical signal without converting it to an electrical signal has been developed, one example of which is the Erbium Doped Fiber Amplifier (EDFA). The idea behind an EDFA is that if a fiber is doped (enhanced) with Erbium, and a signal from an external light source (for instance, a laser) is used to excite the Erbium, the power of an optical signal passing through the fiber will be increased.

Rather than amplify an optical signal in an amplifier, distributed amplification is possible wherein part of the transmission fiber acts as an amplifier. One such distributed amplification scheme is called"Raman amplification"wherein high-power laser light is sent (or pumped) on the same transmission fiber as the data signal. Raman amplification is named after the scientist who discovered a phenomenon in the scattering of light, called the Raman Effect, in 1928. Raman amplification takes advantage of stimulated Raman scattering, which occurs in a silica fiber when a laser beam, often produced at what is called a"pump"laser, propagates through it. Stimulated Raman scattering is an inelastic scattering process in which an incident pump photon loses its energy to create another photon of reduced energy at a lower frequency. That is, pump energy of a given wavelength amplifies, or provides gain to, a signal at a longer wavelength. To date, distributed Raman amplification is an open loop process where the pump powers, but not the gain, may be controlled.

Where, as described above Raman amplification can be used to benefit an optical signal, Raman amplification may also prove to be detrimental to an optical signal, especially when the source of the Raman amplification is a nearby signal channel. The effect of this inter-channel gain due to stimulated Raman scattering (SRS) is known, but may be difficult to determine for a given optical communication system.

Various measures of quality exist for measuring the operation of optical systems. The term"Q"may used to describe the"quality"of a particular optical transmission system in terms of the eye opening when a digital signal is transmitted over the particular optical transmission system. Additionally, the term"OSNR"may be used to describe an optical signal-to-noise ratio present in a given optical system.

For a particular span, the qualities of the transmitter, the medium and the receiver may be summarized in a single number, called a"link budget". The link budget represents the amount of allowable attenuation of a signal over the span, say 30 dB. If an ancillary component is included in a span, for instance for service channel transmission, additional attenuation may be introduced. If a component reduces signal power by one dB, the link budget would then be 29 dB. The one dB reduction in link budget is called a"link budget penalty".

With knowledge of the traffic signal at the input and output of a distributed Raman amplifier, the gain of the amplifier is relatively straightforward to determine. However, often the traffic signal is not available to the operator of such an amplifier. Clearly, it would be desirable to have closed loop control of the Raman amplification process in the transmission fiber in the absence of access to the input signal.

SUMMARY OF THE INVENTION A pump laser signal in a distributed Raman amplifier, which includes a length of transmission fiber and a pump laser, is modulated with a small amount of amplitude modulation. This amplitude modulation transfers to the traffic wavelengths and is detected at a Raman amplifier control system. The Raman amplifier control system, given knowledge of the received modulation and the applied modulation, may determine the gain of the distributed Raman amplifier. The Raman amplifier control system may then control the power supplied to the pump laser to result in a specific gain, thus providing closed loop gain control. Control of the gain of the distributed Raman amplifier results in more accurate control of the signal at the output of the distributed Raman amplifier. Advantageously, more accurate control of the output signal level leads to improved optical link budgets, which translates into better control of Q or OSNR.

In other aspects of the invention, an increase in determined gain may allow a determination of any increase in reflection caused by optical components at the far end of the length of transmission fiber. Further, the amplitude modulation may allow a receiver to identify a particular pump laser signal. This may assist in a determination of a power loss over the length of the optical transmission fiber.

Additionally, a distinct amplitude dither may be placed on each of the traffic wavelengths at the transmitting end of an optical communication system. At the receiving end, or a monitoring point between transmitter and receiver, a given traffic wavelength may be examined for the presence of amplitude dither associated with other traffic wavelengths.

In accordance with an aspect of the present invention there is provided a method for facilitating determination of a characteristic of an optical signal on an optical fiber, including amplitude modulating a pump laser signal of a distributed Raman amplifier.

In accordance with another aspect of the present invention there is provided a method for facilitating determination of a characteristic of an optical signal on an optical fiber. The method includes identifying a particular pump laser signal of a distributed Raman amplifier from amplitude modulation of the particular pump laser signal, measuring a power of the particular pump laser signal, receiving an indication of transmitted power in the particular pump laser signal and determining a power loss from the indication of transmitted power and a power determined from the measuring the power of the particular pump laser signal.

In accordance with a further aspect of the present invention there is provided a method of monitoring gain in a distributed Raman amplifier, where the distributed Raman amplifier includes a length of transmission fiber and a pump laser. The method includes receiving an indication of amplitude modulation applied to a pump laser signal of the distributed Raman amplifier, receiving an indication of amplitude modulation output from the distributed Raman amplifier and determining a gain from the indication of amplitude modulation applied and the indication of amplitude modulation output. In another aspect of the invention a gain monitoring system and a pump power controller are provided for performing this method. In a further aspect of the present invention, there is provided a software medium that permits a general purpose computer to carry out this method.

In accordance with a still further aspect of the present invention there is provided a method of controlling gain in a distributed Raman amplifier, the distributed Raman amplifier includes a length of transmission fiber and a pump laser, the method includes generating a pump laser controlling current, amplitude modulating the pump laser controlling current to create a modulated pump laser controlling current and outputting the modulated pump laser controlling current to the pump laser of the distributed Raman amplifier. In another aspect of the invention a gain controller for a distributed Raman amplifier is provided for performing

this method. In a further aspect of the present invention, there is provided a software medium that permits a general purpose computer to carry out this method.

In accordance with another aspect of the present invention there is provided a method of determining a characteristic of a given optical signal on an optical fiber, where the optical fiber is used to transmit at least one other optical signal. The method includes, at a transmitter, placing an amplitude modulation on an other optical signal and, at a monitor, examining the given optical signal for presence of the amplitude modulation.

In accordance with still another aspect of the present invention there is provided a method of determining a characteristic of a given optical signal on an optical fiber, where the optical fiber is used to transmit at least one other optical signal on which has been placed a distinctive dither signal. The method includes generating a received electrical signal from the given optical signal, filtering the received electrical signal to extract at least one distinctive dither signal and determining a characteristic of the given optical signal from an amplitude of the at least one distinctive dither signal. In another aspect of the present invention, a receiver is provided for performing this method. In a further aspect of the present invention, there is provided a software medium that permits a general purpose computer to carry out steps of this method.

In accordance with an even further aspect of the present invention there is provided a method for facilitating determination of a characteristic of a given optical signal on an optical fiber, where the optical fiber is used to transmit at least one other optical signal. The method includes amplitude modulating the at least one other optical signal with a distinctive signal, where, at a receiver, the distinctive signal may be associated with the other optical signal when detected on the given optical signal.

In accordance with still another aspect of the present invention there is provided an optical communication system including a transmitter for amplitude modulating at least one other optical signal with a distinctive input dither signal per other optical signal. The optical communication system also includes a receiver that includes a photo diode for generating a received electrical signal from a given optical signal, a filter for filtering the received electrical signal to extract at least one distinctive output dither signal and a processor for determining a characteristic of the given optical signal from an amplitude of the at least one distinctive output dither signal.

Other aspects and features of the present invention will become apparent to those of ordinary skill in the art upon review of the following description of specific embodiments of the invention in conjunction with the accompanying figures.

BRIEF DESCRIPTION OF THE DRAWINGS In the figures which illustrate example embodiments of this invention: FIG. 1 schematically illustrates a typical distributed Raman amplification system; FIG. 2 schematically illustrates a distributed Raman amplification system according to an embodiment of the present invention; FIG. 3 illustrates, in a flow diagram, the steps of a method of controlling a distributed Raman amplifier ; FIG. 4 schematically illustrates a distributed Raman amplification system for multiple wavelengths according to an embodiment of the present invention; FIG. 5 schematically illustrates components of the Raman amplifier control system of FIG. 4 according to an embodiment of the present invention; FIG. 6 graphically illustrates Raman gain tilt ; FIG. 7 schematically illustrates components of a DWDM system; and FIG. 8 schematically illustrates components of a receiving node in the DWDM system of FIG. 7.

DETAILED DESCRIPTION Illustrated in FIG. 1 is a typical distributed Raman amplifier 100 and a Raman amplifier control system 101. The Raman amplifier 100, which includes a pump laser 102 and a stub 118, acts on a length of optical transmission fiber 116. The Raman amplifier control system 101 includes a pump power supply 104 under control of a pump power controller 106. The length of optical transmission fiber 116 may also be called a span and may be terminated at each end by an EDFA (not shown).

Turning to FIG. 2, the Raman amplifier 100 remains as known, however a modified Raman amplifier control system 201 is introduced. The Raman amplifier control system 201 includes: a modulation source 208 for generating a modulation signal ; the pump power supply 104; an adder 210 for summing the output of the pump power supply 104 and the output of the modulation source 208; a photodiode 212 for receiving an output optical signal from a tap coupler 218 of the optical transmission fiber 116; a de-modulator 214 for sensing the modulation on the output signal received by the photodiode 212; and a pump power controller 206 for receiving an indication of the modulation on the signal received from the optical transmission fiber 116 as well as an indication of the modulation added to the output of the pump power supply 104 from the modulation source 208. Output of the pump power controller 206, which includes a processor 230 and a memory 232, is used to control the pump power supply 104. The processor 230 may be loaded with Raman amplifier control software for executing methods exemplary of this invention from software medium 234 which could be a disk, a tape, a chip or a random access memory containing a file downloaded from a remote source.

Control of a distributed Raman amplifier 400, which includes four pump lasers 402A, 402B, 402C, 402D, is illustrated in FIG. 4. Each of the pump lasers 402A, 402B, 402C, 402D may have a corresponding stub 418A, 418B, 418C, 418D through which to supply a transmission fiber 416 with energy. Alternatively, the output of the pump lasers 402A, 402B, 402C, 402D may be combined by a single combiner (not shown) before being introduced to the transmission fiber 416. The control is provided by the Raman amplifier control system 401, which receives an indication of the signal on the transmission fiber 416 via a tap coupler 420.

Components of the Raman amplifier control system 401 are illustrated in FIG. 5.

Control is provided by a pump power controller 506 that receives input from a set of de- modulators 514A, 514B, 514C, 514D including a de-modulator corresponding to each pump laser under control. Each of the de-modulators 514A, 514B, 514C, 514D receives the same electrical signal from a photo diode 512, which receives an optical signal from the stub 420.

A modulation unit 530A includes a pump power supply 504A, a modulation source 508A and an adder 510A to combine the output of the pump power supply 504A and the modulation source 508A. The pump power supply 504A is under control of the pump power controller 506 while the modulation source 508A reports a modulation level to the pump power

controller 506. Each of a set of remaining modulation units 530B, 530C, 530D correspond to the remaining three pump lasers 402B, 402C, 402D and have a parallel structure to that of the modulation unit 530A corresponding to the pump laser 402A (FIG. 4).

In a typical distributed Raman amplification system, as illustrated in FIG. 1, the pump laser 102 provides laser light into the optical transmission fiber 116 of a fiber optic system.

Typical pump laser wavelengths are 1425-1500 nm. The energy from the pump frequency is transferred to traffic wavelengths (typically between 1530-1603 nm) via the Raman effect.

This provides a gain, to the traffic wavelength, that is distributed along the fiber. The power of the laser light provided into the optical transmission fiber 116 may be set by controlling current supplied to the pump laser 102. This controlling current is received by the pump laser 102 from the pump power supply 104 under control of a pump power controller 106. This is an open loop process with control provided by the Raman amplifier control system 101 for the pump power but not for the gain of the distributed Raman amplifier 100.

In overview, determination of characteristics of an optical signal on the optical transmission fiber 116 are facilitated by amplitude modulating a signal at the output of the pump laser 102 of the distributed Raman amplifier 100. This amplitude modulation allows the pump power controller 206 to determine the gain introduced by the distributed Raman amplifier 100. Given knowledge of this gain, the pump power controller 206 may provide closed loop control of the gain. The amplitude modulated signal also allows the Raman amplifier control system 201 to recognize changes in reflectivity of an end of the optical transmission fiber 116, and thus act as a reflectometer. Further, the amplitude modulation allows identification of a particular pump laser signal that, given knowledge of the transmitted power, allows a receiver to determine a power loss over the length of the optical transmission fiber 116.

In operation, the supply of power to the pump laser 102 is modulated with a small amount of amplitude modulation such that the pump laser signal is amplitude modulated.

Preferably, the amplitude modulation is provided at a low frequency, say 10-1000 Hz. The frequency should be chosen to be low enough for efficient energy transfer. Notably, an EDFA at the end of a span on which a Raman amplifier is operating may block the amplitude modulation, allowing for reuse of the amplitude modulation frequency in the next span. This pump laser signal amplitude modulation transfers to the traffic wavelengths and is detected at

the Raman amplifier control system 201 using the photodiode 212. The processor 230 in the pump power controller 206 receives an indication of the received modulation. The processor 230, given knowledge of the signal level of the modulation that was applied (from modulation source 208), may determine the gain provided by the distributed Raman amplifier 100. The pump power controller 206 then controls the power supplied to the pump laser 102 by the pump power supply 104 to give a specific gain, thus providing closed loop control.

The steps performed by the pump power controller 206 while controlling the distributed Raman amplifier 100 are outlined in FIG. 3. Initially, the pump power supply 104 is provided with a nominal value of pump power by the pump power controller 206 (step 302). The modulation source 208, as well as providing an applied modulation signal to the adder 210, provides an indication of the applied modulation signal to the pump power controller 206 (step 304). The photodiode 212 receives the optical signal at the output of the Raman amplifier 100 and converts it to an electrical signal. The de-modulator 214 extracts a received modulation signal from this electrical signal and provides an indication of the received modulation signal to the pump power controller 206 (step 306). Having received indications of both the applied modulation and the received modulation, the pump power controller 206 may then proceed to determine the gain for the distributed Raman amplifier 100 (step 308). Based on the gain determined in step 308 and a predetermined desired gain, the pump power controller 206 may adjust the value of pump power provided to the pump power supply 104.

As it is likely, especially when in use in WDM transmission systems, that the transmission fiber will carry multiple wavelengths (signal channels), control may be provided for amplification of each of the multiple wavelengths. As illustrated in FIG. 4, the distributed Raman amplifier 400 includes four pump lasers 402A, 402B, 402C, 402D, each under the control of the Raman amplifier control system 401. Turning to FIG. 5, to distinguish the modulation provided by the modulation source 508A in the modulation unit 530A, from the modulation provided by modulation sources in the other modulation units 530B, 530C, 530D, the modulation may be a combination of two or three frequencies. For instance, a scheme similar to that used to generate Dual Tone Multi-Frequency (DTMF) signals for conventional tone dialing telephones may be used to amplitude modulate the power provided by pump power supply 504A. This modulation scheme allows the de-modulator 514A to recognize the

modulation provided by the modulation source 508A. Alternatively, the modulation may be coded to identify the modulation source 508A.

As will be apparent to a person skilled in the art, the de-modulators 514A, 514B, 514C, 514D may be implemented using signal processing techniques. In alternate modulation schemes the de-modulators 514A, 514B, 514C, 514D may be implemented to include tunable filters, each used to select a distinct wavelength, or may even be implemented to include a combination of a dispersive element and a detector array. The latter implementation may provide an indication of the mean power of the signal received from the optical transmission fiber 116 in addition to an indication of the power of the modulation at each wavelength.

Under conventional control, say if a control system similar to the Raman amplifier control system 101 (FIG. 1) is used to control each of the four pump lasers, the Raman Effect may transfer disparate amounts of energy to traffic signals at different wavelengths, even with identical pump laser powers. The result of this disparity in energy transfer can lead to Raman induced gain tilt. Such a gain tilt is illustrated by a graphical representation 600 of gain vs. wavelength in FIG. 6, where traffic wavelengths are represented by c and XD. However, under control of Raman amplifier control system 401, the gain due to each pump laser 402A, 402B, 402C, 402D, can be identified and measured. Thus, the amount of gain tilt can also be measured, assessed and, if necessary, corrected through control of the gain applied to one or more of the traffic wavelengths.

We can define the amount of modulation on a given pump laser as rp, which represents a ratio of root mean square (RMS) fluctuation of optical power on the pump laser due to the modulation to the square of the mean optical pump power This is analogous to relative intensity noise (RIN). We can show that for a Raman amplifier, the amount of modulation on the signal on the optical transmission fiber (rS) is given by:

where is the root mean square (RMS) fluctuation, due to the modulation, of optical power of the signal on the optical transmission fiber, (P5) is the mean optical power of the signal on the optical transmission fiber, GR is the amount of Raman gain provided by a pump laser with amplitude modulation at frequencyf, V, is the group velocity at the signal wavelength, ap is the attenuation of the fiber at the pump laser wavelength (in neper/km), L is length of the fiber, T is the transit time of the fiber and Leff is the effective length of the fiber: 1-ex<BR> Leff= a (4)<BR> ap If the fiber is long (this will be the case for most long-haul transmission systems), then equation 3 may be approximated as: It can be seen from equation 5 that the transfer function of the modulation from the pump laser signal to the signal will be a low pass filter. For typical fiber characteristics, the low frequency roll-off is at about 1 kHz. The frequency of the amplitude modulation may therefore be selected from a range extending from about 10 Hz to about 1000 Hz.

Therefore, by knowing the modulation depth of the amplitude modulation placed on a particular pump laser wavelength (giving rp), and by measuring the modulation depth of the modulation transferred to a given signal channel (giving rS), the amount of linear gain (GR) provided by that pump laser can be found by: By measuring the modulation depth (rS) for each signal channel, the relative amount of gain given by each pump laser to each signal channel can be determined.

The gain (GRi) given to a signal at wavelength B5 by the ith pump laser, where there are a total of Npump lasers, with modulation at individual frequencyf, is given by: The total Raman gain experienced by the signal is the sum of the gains from each pump laser: The total gain for each signal channel is useful in order to optimize the relative pump powers so as to create an optimum gain spectrum. It is also useful to know the gain contribution that each pump laser makes towards the total gain shape so that the control routine can be appropriately optimized.

Additionally, the Raman amplifier control system 201 may be able monitor aspects of the optical transmission fiber 116 other than gain. For instance, an increase in the amount of the amplitude modulation received by de-modulator 214, without a corresponding increase in the modulation supplied by modulation source 208, may signify an increase in reflection caused by optical components at the far end of the optical transmission fiber 116. Thus, the Raman amplifier control system 201 may be seen as acting as a reflectometer. Alternately, given an approximation for the amount of reflection received under normal conditions, the power supplied to the pump laser 102 may be shut off if the amount of reflection surpasses a threshold. Such a high amount of reflection may be an indication of a dirty connector, a fiber break or mismatch.

It may be that the generation of a particular pump laser signal, including addition of coded amplitude modulation to the current supplied by a pump power supply for a pump laser, is performed at one end of a fiber span and the receipt of the particular pump laser signal occurs at the other end of the fiber span. The coded amplitude modulation allows the receiving end to identify the particular pump laser signal. The receiving end can then determine the power in this signal. An optical service channel could be used to indicate to the receiving end the amount of power supplied to the pump laser. Given the amount of power

supplied to the pump laser and the amount of received power, an amount of power loss associated with the fiber may be determined.

As will be appreciated, the method of amplitude modulating the pump laser signal at the output of the pump laser 102 of the distributed Raman amplifier 100 need not be limited to controlling current supplied to the pump laser 102. For instance, the pump laser signal may be amplitude modulated, after being generated by the pump laser 102, by a lens with controllable transmittance.

Stimulated Raman scattering (SRS), which above may be used to enhance the performance of an optical communication system, may also lead to some detrimental effects.

Specifically, SRS may lead to crosstalk between signal channel sent from transmitter to receiver. Just as amplitude modulation is used above to facilitate the determination of the SRS-induced enhancement, amplitude modulation may be used to facilitate the determination of the SRS-induced detriment. To distinguish from the amplitude modulation used above in conjunction with Raman amplification, the amplitude modulation used below is termed "dither".

Where distinct wavelengths are selected or discriminated, as described above using tunable filters or filter arrays, an inter-channel gain between the signal channels may also be measured. In particular, it is an inter-channel gain due to stimulated Raman scattering (SRS), which is also known as inter-channel SRS crosstalk, that may be measured. To achieve this inter-channel SRS gain measurement, a distinct amplitude dither may be placed on each of the signal channels at the transmitting end of an optical communication system. The magnitude of a dither placed on a given signal channel is related to the launch power of the given signal channel by a preset modulation depth. At the receiving end of the optical communication system such as that illustrated in FIG. 5, a given signal channel (wavelength) may be optically discriminated by one of the de-modulator 514. Once this signal channel is optically discriminated, the contribution of each of the distinct dithers placed on the other signal channels can be measured.

The amplitude of dither associated with signal channel A that is measured on signal channel B (after optical discrimination) may be proportional to the amount of SRS gain signal channel B experienced from signal channel A."Gain", as used herein, may be enhance a signal (i. e., gain > 1), as is typical, or deplete a signal (i. e., 0 < gain < 1), in which case it may

be called"depletion". Similarly, all the amounts of inter-channel SRS gain experienced by each signal channel from each other signal channel can be measured.

Note that the detection point can be at any optical circuit pack in an optical system, where"circuit pack"may be defined to include optical filters, transmitters, receivers, photonic switches, optical amplifiers, etc. Advantageously, a measurement of the inter- channel SRS gains in an optical system may provide an indication of the health of the optical system. Additionally, a system for measuring the inter-channel SRS gains may serve as a monitoring system for a control system that may be arranged to reduce inter-channel SRS gain. Excessive inter-channel SRS gains between signal channels may lead to an optical noise penalty on signal channels with depleted optical power.

Note also that the magnitude of the dither associated with signal channel A that is measured on signal channel B is proportional to an amount of inter-channel SRS-induced data crosstalk from signal channel A on signal channel B. Excessive inter-channel SRS- induced data crosstalk can impact the performance of an optical system. The degree of this proportionality may be determined given the frequency of the dither, a dispersion map of the fiber and a knowledge of the wavelengths of the signal channels. For a particular signal channel, detection, at the receiver, of the magnitude of the dither associated with the particular signal channel combined with knowledge of the preset modulation depth of the dither, can lead to a determination, at the receiver, of the launch power of the signal channel.

Consequently, a total inter-channel SRS-induced data crosstalk on signal channel A may be determined by adding the magnitude of each of the dithers from the other signal channels (with knowledge of the preset modulation depth) detected on signal channel A after optical discrimination.

In FIG. 7, a DWDM system 700 includes a transmitting node 702, an optical fiber 716 and a crosstalk monitor 706. The transmitting node 702 includes N channel transmitters 710A, 710B,..., 710N (generally referred to as a channel transmitter 710) that each provide a wavelength channel to a multiplexer/demultiplexer (MUX/DEMUX) 708. The transmitting node 702 also includes a reporting channel receiver 704. The MUX/DEMUX 708 multiplexes the channels received from the channel transmitters 710 and sends the multiplexed signal to a receiving node (not shown) over the fiber 716. Additionally, the MUX/DEMUX 708 receives

a reporting channel and passes the reporting channel signal to the reporting channel receiver 704.

At the transmitting end of the DWDM system 700, transmission parameters may be given to each channel by each channel transmitter 710 as controlled by a system control unit 712. Such parameters may include launch power, signal channel wavelength and an amplitude and frequency of a distinctive dither. As such, each channel transmitter 710 may include a laser source and an attenuator/amplifier (not shown) to adjust the transmission parameters for the respective signal channel. Further, measurements of inter-channel SRS gains may be received at the system control unit 712 from the reporting channel receiver 704.

The system control unit 712 may be loaded with transmitter control software for executing methods exemplary of this invention from a software medium 714 which could be a disk, a tape, a chip or a random access memory containing a file downloaded from a remote source.

At the crosstalk monitor 706, a receiving stub 720 is used to receive the signal channels present on the fiber 716. A reporting stub 722 is used to place a reporting channel on the fiber 716 for reporting to the transmitting node 702.

Components of the crosstalk monitor 706 may be examined in detail in FIG. 8. A photo diode 812 receives an optical signal from the receiving stub 720. Each of a set of de- modulators 814A, 814B,..., 814N, including de-modulator corresponding to each signal channel, receives the same electrical signal from the photo diode 812. After de-modulating, and perhaps filtering, the electrical signal, a signal channel is passed to a SRS gain determining unit 806. The SRS gain determining unit 806 may determine the amount of dither from the other signal channels on each signal channel and report this information to a reporting channel transmitter 804. A reporting channel may be placed on the reporting stub 722 by the reporting channel transmitter 804.

The SRS gain determining unit 806 may include a set of filters (not shown) for filtering a signal channel to discern the presence of one or more dithers and a processor (not shown) to associate a dither of a particular frequency with a particular one of the other signal channels. The SRS gain determining unit 806 may be loaded with SRS gain determining software for executing methods exemplary of this invention from a software medium 824 which could be a disk, a tape, a chip or a random access memory containing a file downloaded from a remote source.

Note that the actions (amplitude modulation of pump laser, discrimination of signal channels, monitoring of gain) of the Raman amplifier control system 201 (FIG. 2) are typically performed at a point between the transmitting node 702 (FIG. 7) and a receiving node (not shown). Although the actions (discrimination of signal channels, measurement of dither, reporting crosstalk) of the crosstalk monitor 706 may be performed, as shown, at a point between the transmitting node 702 and a receiving node, it is more natural that the actions of the crosstalk monitor are performed at a receiving node. The signals are typically optically discriminated at the receiver as part of the receiver function such that the determination and reporting of crosstalk may be an additional feature of a receiver.

As will be apparent to a person skilled in the art, the combination of the reporting channel transmitter 804 and the reporting channel receiver 704 and the so-called reporting channel of the fiber 716 is generally representative of communication between network elements. Network management systems that allow communication between various network elements are well known and implemented in a number of ways.

Other modifications will be apparent to those skilled in the art and, therefore, the invention is defined in the claims.