This application is based upon and claims the benefit of priority of the prior Japanese Patent Application No. 2010-088469, filed on Apr. 7, 2010, the entire contents of which are incorporated herein by reference.
The embodiments discussed herein are related to; a polarization fluctuation compensation device for compensating for deterioration of reception characteristic due to fluctuations in the polarization state of transmitted light in optical communication, and an optical communication system.
In wavelength division multiplexing (WDM) optical communication system, polarization scrambling may be applied to an optical signal in order to suppress the occurrence of polarization dependent gain (or polarization dependent loss) held by an optical repeater, and polarization hole burning (PHB), or to alleviate quality deterioration of a signal waveform due to nonlinearity of an optical fiber (for example, refer to Japanese Laid-Open Patent Publication No. 9-149006).
Moreover, in WDM optical communication system, an optical signal of a modulation format different from an existing channel may be added as a new channel at the time of upgrading the system. In this case, if wavelengths of optical signals of different modulation system are arranged adjacent to each other, performance of the system may be deteriorated resulting from a difference in the cross-phase modulation effect due to the difference of the modulation formats. In order to avoid this, a technique has been proposed where wavelength bands in which each optical signal is arranged, are grouped for each modulation format, and a guard band is provided between respective wavelength bands (for example, refer to Japanese Laid-Open Patent Publication No. 2006-50640).
To realize a large capacity of the optical communication system, research and development of a digital coherent receiver has been currently in progress. In the digital coherent receiver, polarization information included in received light needs to be restructured, following polarization fluctuations in the optical signal, which may occur at a certain rate due to an environmental change, for example, in an optical transmission path. This restructuring of polarization information of the received light is performed by subjecting a photoelectrically converted reception signal to digital signal processing by using a finite impulse response (FIR) filter or the like. In restructuring of polarization information by means of digital signal processing, the arithmetic processing thereof is under a high load, and hence there is a limitation on high speed processing. Therefore, a configuration in which the above-described polarization scrambling is basically not applied to an optical signal received by the digital coherent receiver has been studied.
When the existing optical communication system applied with polarization scrambling is to be upgraded by using the digital coherent receiver, a polarization scrambled optical signal and a non-polarization scrambled optical signal are simultaneously transmitted inside the optical fiber. At this time, the polarization state, phase, and amplitude of the non-polarization scrambled optical signal may fluctuate timewise due to the cross-phase modulation effect and Raman amplification effect resulting from the nonlinearity of the optical fiber. If the polarization state of the optical signal received by the digital coherent receiver fluctuates at a speed faster than a normally assumed speed due to an influence of polarization scrambling applied to other optical signals, digital signal processing for restructuring the polarization information cannot follow the fast fluctuation of the polarization state. Therefore, there is a problem in that quality deterioration of the signal waveform occurs at the time of restructuring the polarization information of the received light.
The above problem is not limited to the case in which the optical signal is received by using the digital coherent receiver, but is common to various types of reception systems using the polarization information of the optical signal. Moreover, the polarization state of the transmitted light may fluctuate faster than the normally assumed speed resulting from an interaction between respective optical signals, due to some sort of phenomenon other than polarization scrambling. Therefore, in reception processing of the optical signal using the polarization information, it is an important issue to reduce the influence of polarization fluctuations faster than the normally assumed speed, on the reception processing.
Accordingly, the invention provides a polarization fluctuation compensation device that compensates for the quality deterioration of a signal waveform occurring in reception processing of WDM light including a plurality of optical signals having different wavelengths. One aspect of the polarization fluctuation compensation device includes: an information collection circuit adapted to collect information related to the speed of polarization fluctuations in optical signals having respective wavelengths; a parameter calculator circuit adapted to obtain a target value of a control parameter corresponding to each wavelength, based on information collected by the information collection circuit, so that a control parameter in the reception processing related to polarization information of the optical signals having respective wavelengths takes a different value according to the speed of polarization fluctuations in the optical signals having respective wavelengths; and a parameter setting circuit adapted to set the target value obtained by the parameter calculator circuit, as a control parameter in the reception processing corresponding to the respective wavelengths.
The object and advantages of the invention will be realized and attained by means of the elements and combinations particularly pointed out in the claims.
It is to be understood that both the foregoing general description and the following detailed description are exemplary and explanatory and are not restrictive of the invention, as claimed.
Hereunder is a detailed description of embodiments of the present invention, with reference to the accompanying drawings.
In
The optical transmission device 1 generates optical signals having wavelengths λ1 to λM different from each other in M (M is an integer equal to or larger than 1) optical transmitters (TX) 11-1 to 11-M, multiplexes the respective optical signals by a multiplexer 12, and scrambles the polarization state of the optical signals having respective wavelengths λ1 to λM by providing output light of the multiplexer 12 to a polarization scrambler 13. Moreover, the optical transmission device 1 generates optical signals having wavelengths λM+1 to λM+N different from each other in N (N is an integer equal to or larger than 1) optical transmitters (TX) 14-1 to 14-N, and multiplexes the respective optical signals by a multiplexer 15. Then the optical transmission device 1 multiplexes output light from the polarization scrambler 13 and output light from the multiplexer 15 by a multiplexer 16 to generate WDM light having (M+N) waves, amplifies the WDM light to a required level by a post-amplifier 17, and outputs the WDM light to the optical transmission line 2.
The above configuration of the optical transmission device 1 corresponds to a configuration in which the optical transmitters 14-1 to 14-N and the multiplexers 15 and 16 are added to the existing configuration including the optical transmitters (TX) 11-1 to 11-M, the multiplexer 12, the polarization scrambler 13, and the post-amplifier 17, by for example upgrading the optical communication system.
A splitter 51 of the polarization fluctuation compensation device 5 is arranged on the optical transmission line 2 positioned near the output terminal of the optical transmission device 1, and a part of the WDM light output from the optical transmission device 1 to the optical transmission line 2 is extracted by the splitter 51 as monitoring light. The WDM light having passed through the splitter 51 is amplified by the optical repeater 3 arranged at a required interval on the optical transmission line 2, and repeatedly transmitted to the optical reception device 4.
The WDM light repeatedly transmitted on the optical transmission line 2 is input to the optical reception device 4, and the optical reception device 4 amplifies the WDM light to a required level by a pre-amplifier 41 and demultiplexes the WDM light to optical signals having respective wavelengths λ1 to λM+N by a demultiplexer 42. Then the optical reception device 4 receives the (polarization scrambled) optical signals output from the demultiplexer 42 and having respective wavelengths λ1 to λM by optical receivers (RX) 43-1 to 43-M corresponding to the respective wavelengths, and receives the (non-polarization scrambled) optical signals having respective wavelengths λM+1 to λM+N by respective optical receivers (RX) 44-1 to 44-N corresponding to the respective wavelengths. The respective optical receivers 43-1 to 43-M on the polarization scrambled side have a general configuration corresponding to a reception system that basically does not use the polarization information of the optical signal. On the other hand, the respective optical receivers 44-1 to 44-N on the non-polarization scrambled side correspond to a reception system that uses the polarization information of the optical signal.
The above configuration of the optical reception device 4 corresponds to a configuration for when the optical receivers 44-1 to 44-N are added by using an unused port of the demultiplexer 42, to the existing configuration including the pre-amplifier 41, the demultiplexer 42, and the optical receivers 43-1 to 43-M, by the aforementioned upgrading of the optical communication system. Specific configuration examples of the respective optical receivers 44-1 to 44-N will be described later.
The polarization fluctuation compensation device 5 provides monitoring light extracted by the splitter 51 to a polarization scrambling detector 52, and the polarization scrambling detector 52 detects whether the optical signals having respective wavelengths λ1 to λM+N included in the monitoring light have been polarization scrambled. Information related to the presence of polarization scrambling corresponding to the respective wavelengths λ1 to λM+N detected by the polarization scrambling detector 52 is collected by an information collection section 53. The information collection section 53 may be circuit. Then in the polarization fluctuation compensation device 5, a parameter calculator 54 obtains a target value of a control parameter to be applied to the processing related to the polarization information of received light performed by the respective optical receivers 44-1 to 44-N corresponding to a reception method using the polarization information of the optical signal, by using the information from the information collection section 53, and transmits the result thereof to a parameter setting section 55. The parameter calculator 54 and the parameter setting section 55 may be circuits. The parameter setting section 55 sets the target value obtained by the parameter calculator 54 as a control parameter p in the reception processing by the corresponding optical receivers 44-1 to 44-N inside the optical reception device 4. As a result, the reception processing for compensating for polarization fluctuations occurring in the respective wavelengths λM+1 to λM+N due to the influence of polarization scrambling with respect to the optical signals having respective wavelengths λ1 to λM is performed by the respective optical receivers 44-1 to 44-N. A specific configuration example of the polarization scrambling detector 52 and details of the processing in the parameter calculator 54 will be described later.
Here a specific configuration example of the respective optical receivers 44-1 to 44-N on the non-polarization scrambled side is described below.
Local oscillation light to be output from a local oscillation light source (LOL) 402 is respectively input to the respective optical hybrid circuits 403X and 403Y via a polarization beam splitter (PBS) 401B. The local oscillation light is continuous light having substantially the same frequency as the frequency of the input light. The optical hybrid circuit 403X mixes the X polarization component of input light and the local oscillation light, thereby generating optical signals of an in-phase (I) component and a quadrature-phase (Q) component with optical phases thereof being different by 90 degrees from each other. Moreover the optical hybrid circuit 403Y also mixes the Y polarization component of the input light and the local oscillation light, thereby generating optical signals of the I-component and the Q-component, with optical phases thereof being different by 90 degrees from each other.
The respective optical signals of the I-component and the Q-component respectively output from the respective optical hybrid circuits 403X and 403Y are converted to digital electric signals by respectively corresponding optical receivers (O/E) 404XI, 404XQ 404YI, and 404YQ, and AD converters (ADC) 405XI, 405XQ, 405YI, and 405YQ. As a result, I-component data and Q-component data corresponding to the X polarization of the input light, and I-component data and Q-component data corresponding to the Y polarization of the input light can be acquired, and respective data are output to a waveform equalization section 406. One set of I-component data and Q-component data corresponds to one complex number, and the I-component data expresses a value of a real part of a certain complex number, and the Q-component data expresses a value of an imaginary part of the complex number. An optical electric field (optical amplitude and optical phase) corresponding to one polarization component of the input light is expressed by one set of I-component data and Q-component data.
The waveform equalization section 406 performs arithmetic processing for compensating for dispersion or the like of the optical transmission path 2, with respect to output data from the AD converters 405XI, 405XQ 405YI, and 405YQ thereby performing waveform equalization of the optical signal. The respective data processed by the waveform equalization section 406 is output to a polarization information restructuring section 407. The polarization information restructuring section 407 performs arithmetic processing for restructuring information corresponding to the X polarization and the Y polarization with respect to respective output data from the waveform equalization section 406, according to the polarization fluctuations in the optical signal input to the digital coherent receiver.
The algorithm calculation circuit 407E calculates the filter coefficient w according to a well-known adaptive equalization algorithm by using the control parameter p provided from the polarization fluctuation compensation device 5. Specific examples of the adaptive equalization algorithm include a least mean square (LMS) algorithm expressed by equation (1) below, a constant modulus algorithm (CMA) expressed by equation (2) below, and the like.
where, in equations (1) and (2), w denotes a filter coefficient, r denotes a reception signal, yn denotes a filter output signal, sn denotes a training signal, γ denotes a constant, and μ denotes a step size. In these adaptive equalization algorithms, the control parameter p from the polarization fluctuation compensation device 5 is provided as the step size μ.
The adder 4073 adds up the multiplication results acquired by the respective multipliers 4072. A signal indicating the addition result of the adder 4073 is output from an output port OUT of the FIR filter. Moreover output signals from the two FIR filters 407A and 407B in the polarization information restructuring section 407 (
Returning to
Output light from the polarization controller 411 is separated into two different polarization components by the PBS 412. One polarization component (for example, the X polarization component) is output to an optical receiver (O/E) 413X, and the other polarization component (for example, the Y polarization component) is output to an optical receiver (O/E) 413Y. At this time, a part of the respective output lights from the PBS 412 is branched and provided to a controller 415. The controller 415 monitors the power of the respective branched lights, and feed-back controls the polarization controller 411 according to the monitoring results thereof. Here the control parameter p from the polarization fluctuation compensation device 5 is provided to the controller 415 as a loop gain in the feed-back control of the polarization controller 411 by the controller 415.
The respective optical receivers 413X and 413Y convert the respective output lights from the PBS 412 to electric signals, and output the electric signals to respective signal processing sections 414X and 414Y. The respective signal processing sections 414X and 414Y perform processing such as signal identification or error correction with respect to the output signals from the respective optical receivers 413X and 413Y, to thereby generate and output received data.
Next is a description of a specific configuration example of the polarization scrambling detector 52 illustrated in
In the configuration example (B) illustrated in the second stage in
The configuration example (C) illustrated in the third stage in
One set of polarizers 513A1 and 513B1 corresponding to wavelength λ1 respectively have an optical axis with the direction thereof being different from each other, and cut out a specific polarization component along the direction of the optical axis from the respective optical signals branched by the splitter 5121 into two, and output the polarization components to the PDs 514A1 and 514B1. The respective PD 514A1 and 514B1 convert the light cut out by the respective polarizers 513A1 and 513B1 to electric signals and output the electric signals to the fluctuation detection circuit 5151. The fluctuation detection circuit 5151 detects the speed (frequency) of the polarization fluctuations in the optical signal of wavelength λ1, based on the output signals from the respective PDs 514A1 and 514B1 to determine whether polarization scrambling has been performed, and transmits the determination result thereof to the information collection section 53. Polarizers 513A2, 513B2 to 513AM+N, and 513BM+N, PDs 514A2, 514B2 to 514AM+N, and 514BM+N, and fluctuation detection circuits 5152 to 515M+N corresponding to other wavelength λ2 to λM+N have the same configuration as those of the polarizers 513A1 and 513B1, the PDs 514A1 and 514B1, and the fluctuation detection circuit 5151 corresponding to the wavelength λ1.
In the configuration example (D) illustrated in the fourth stage in
In the configuration examples (C) and (D), for an optical signal of one wavelength, different polarization components are cut out by using a set of polarizers 513A and 513B. However, only a specific polarization component can be cut out by a single polarizer to determine the presence of polarization scrambling based on a change in the power. In this case, the detection accuracy for the presence of polarization scrambling decreases compared to the case of using one set of polarizers, however, further downsizing and cost reduction can be realized.
Next is a description of an operation of the optical communication system of the first embodiment.
In the optical communication system of the above configuration, an optical signal having wavelengths λ1 to λM polarization scrambled by the polarization scrambler 13 inside the optical transmission device 1, and an optical signal having wavelengths λM+1 to λM+N non-polarization scrambled, pass through the same optical transmission path 2 from the optical transmission device 1 and are repeatedly transmitted to the optical reception device 4, while being amplified by the optical repeater 3. At the time of repeated transmission of the WDM light, temporal fluctuations occur in the polarization state, phase, and amplitude of the non-polarization scrambled optical signals having wavelengths λM+1 to λM+N, due to the cross-phase modulation (XPM) effect and Raman amplification effect by the polarization scrambled optical signals having wavelengths λ1 to λM.
Here the influence of the XPM effect by the polarization scrambled optical signals is specifically explained. When it is assumed that a polarization scrambling frequency in the polarization scrambler 13 is f, and a polarization rotation frequency of the polarization scrambled optical signal is ω=2πf, an electric field Ep of the optical signal is expressed by the following equation (3).
where Epx denotes the electric field of the X polarization component, and Epy denotes the electric field of the Y polarization component. Moreover E0 denotes the electric field of the (linearly-polarized) optical signal before polarization scrambling, and t denotes time.
The amount of phase shift due to XPM applied to optical signals of other wavelengths by the polarization scrambled optical signal is expressed by the following equation (4) (for example, refer to G. P. Agrawal, Nonlinear Fiber Optics, 4th ed., Academic Press, San Diego, 2007, Chapter 6.2). Loss in the optical transmission path 2 and walk-off due to wavelength dispersion is ignored.
where ΦXPM
It is seen from the relation in equation (4) that the phase of the X polarization component and the phase of the Y polarization component in the optical signals of other wavelengths fluctuate at frequency 2f due to the influence of XPM by the polarization scrambled optical signal. That is, the polarization scrambled optical signal and the non-polarization scrambled optical signal are transmitted together on the optical transmission path 2, thereby adding a polarization fluctuation with frequency 2f to the polarization scrambled optical signal.
The polarization fluctuation with frequency 2f occurring in the non-polarization scrambled optical signal due to the influence of the above polarization scrambled optical signal is faster than the polarization fluctuations occurring due to an environmental change in the optical transmission path, and signal processing performed by the optical receiver that receives the optical signal cannot follow the fast polarization fluctuation. The level of polarization fluctuations occurring in the non-polarization scrambled optical signal due to the influence of polarization scrambling is related to the relative arrangement between the wavelength of the polarization scrambled optical signal and the wavelength of the non-polarization scrambled optical signal.
Therefore in the first embodiment, the polarization fluctuation compensation device 5 detects whether polarization scrambling has been performed with respect to the optical signals having respective wavelengths λ1 to λM+N transmitted from the optical transmission device 1 to the optical transmission path 2, and optimizes the control parameter p in the signal processing in the optical receivers 44-1 to 44-N corresponding to the non-polarization scrambled optical signal, taking the relation of relative wavelength arrangement into consideration based on the detection result thereof, thereby compensating for polarization fluctuations due to the influence of polarization scrambling.
When the optical communication system is activated, in step 110 in
In step 120, information related to whether the optical signals having respective wavelengths λ1 to λM+N detected by the polarization scrambling detector 52 have been polarization scrambled is collected by the information collection section 53.
In step 130, using the information of the information collection section 53, the parameter calculator 54 obtains a target value of the control parameter p provided to the optical receivers 44-1 to 44-N corresponding to the non-polarization scrambled wavelengths λM+1 to λM+N. Here, for example as illustrated in
The relation set in the table in
In the combination #2 of the non-polarization scrambled optical signals of wavelengths λ1 and λ2 and the polarization scrambled optical signals of wavelengths λ3 to λ8, comparatively fast polarization fluctuations occur in the optical signals of wavelengths λ1 and λ2 due to receiving a strong influence of polarization scrambling with respect to the optical signals of wavelength λ3 to λ5, as in the case of the combination #1. Therefore, α1 is respectively set as a target value of the control parameter p corresponding to wavelengths λ1 and λ2.
Furthermore in the combination #3 of the non-polarization scrambled optical signals of wavelengths λ1 to λ3 and the polarization scrambled optical signals of wavelengths λ4 to λ8, comparatively fast polarization fluctuations occur in the optical signals of wavelengths λ2 and λ3 due to receiving a strong influence of polarization scrambling with respect to the optical signals of wavelengths λ4 to λ6, and the influence of polarization scrambling also reaches the optical signal of wavelength λ1, and polarization fluctuations also occur in the optical signal of wavelength λ1, although slower than that of wavelengths λ2 and λ3. Therefore, in the setting p(#3) of the control parameter p corresponding to the combination #3, α1 is set as a target value of the control parameter p corresponding to wavelengths λ2 and λ3, and α2 smaller than α1 is set as a target value of the control parameter p corresponding to wavelength λ1.
Moreover, in the combination #4 of the non-polarization scrambled optical signals of wavelengths λ1 to λ4 and the polarization scrambled optical signals of wavelengths λ5 to λ8, comparatively fast polarization fluctuations occur in the optical signals of wavelengths λ3 and λ4 due to receiving a strong influence of polarization scrambling with respect to the optical signals of wavelengths λ5 to λ7, and the influence of polarization scrambling also reaches the optical signal of wavelength λ2, and polarization fluctuations also occur in the optical signal of wavelength λ2, although slower than that of wavelengths λ3 and λ4. Furthermore the influence of polarization scrambling also reaches the optical signal of wavelength λ1, though slightly, and a polarization fluctuation slower than that of wavelength λ2 occurs in the optical signal of wavelength λ1. Therefore, in the setting p(#4) of the control parameter p corresponding to the combination #4, α1 is set as a target value of the control parameter p corresponding to wavelengths λ3 and λ4, α2 smaller than α1 is set as a target value of the control parameter p corresponding to wavelength λ2, and α3 smaller than α2 is set as a target value of the control parameter p corresponding to wavelength λ1.
When the target value of the control parameter p corresponding to the presence of polarization scrambling is obtained by the parameter calculator 54 in this manner, control proceeds to step 140 in
In the explanation of the operation of the polarization fluctuation compensation device 5, the presence of polarization scrambling of the optical signals having respective wavelengths it is expressed by using a binary of “1” and “0” (in the upper stage in
Moreover, when the target value of the control parameter p corresponding to the combination of the polarization scrambled optical signal and the non-polarization scrambled optical signal is determined by using the tables illustrated in
Specifically, as in steps 110 and 120 illustrated in
where λSCR [k] denotes an index indicating whether a wavelength channel k has been polarization scrambled, with “0” indicating “non-polarization scrambled”, and “1” indicating “polarization scrambled”. Moreover, i denotes a wavelength channel for which a target value of the control parameter p is to be calculated. Ntotal denotes the number of wavelength multiplexing of the WDM light transmitted on the optical transmission path 2. N1 is a first determination parameter to be used for determining the control parameter p, and indicates a wavelength range in which a search is made of whether there is a polarization scrambled optical signal. For example, in the case of N1=3, a search is made of whether there is a polarization scrambled optical signal in a range of the wavelength channel i±3 based on the wavelength channel i to be calculated.
For the determination processing in step 131, combinations #5 to #7 of the polarization scrambled optical signals and the non-polarization scrambled optical signals having the respective wavelengths as illustrated for example in
In step 132, the following relation in equation (6) is determined.
where N2 is a second determination parameter to be used for determining the control parameter p, and a value smaller than the first determination parameter N1 is set (N1>N2).
For the determination processing in step 132, subsequent steps after step 131 in combinations #5 to #7 in
In the above manner, by determining the target value of the control parameter p corresponding to the respective wavelengths by the calculation processing according to the flowchart in
The number of conditional equations, and the value and number of determination parameters in the arithmetic processing according to the flowchart in
Next is a description of a second embodiment of an optical communication system.
In the above first embodiment, an example is described where, in the case when a non-polarization scrambled optical signal is transmitted together with a polarization scrambled optical signal by upgrading the optical communication system, fast polarization fluctuations occurring in the non-polarization scrambled optical signal due to the influence of polarization scrambling are compensated for. However, the source occurrence of the fast polarization fluctuations is not limited to polarization scrambling, and the polarization state of transmission light may fluctuate faster than the normally assumed speed due to some factors other than polarization scrambling. Here one example of an optical communication system that can accommodate such a situation is described in the second embodiment.
A polarization fluctuation compensation device 5 applied to the optical communication system extracts a part of the WDM light input to the optical reception device 4 as monitor light by a splitter 51, and provides the monitor light to a polarization fluctuation detector 56. The polarization fluctuation detector 56 detects the speed of polarization fluctuations in optical signals having respective wavelengths λ1 to λN included in the monitor light extracted by the splitter 51. The respective configuration examples (A) to (D) illustrated in
In the optical communication system, the polarization fluctuation detector 56 detects the speed of polarization fluctuations occurring in the optical signals having respective wavelengths λ1 to λN transmitted on the optical transmission path 2 and input to the optical reception device 4, and the information collection section 53 collects the information. Then a parameter calculator 54 determines a target value of the control parameter p corresponding to the information obtained by the information collection section 53, by referring to a table in which the speed of polarization fluctuations is expressed by multiple values as illustrated, for example, in
According to the optical communication system of the second embodiment, the influence of fast polarization fluctuations can be reliably compensated for by the polarization fluctuation compensation device 5, even if the polarization state of the optical signals having respective wavelengths λ1 to λN transmitted on the optical transmission path 2 fluctuates faster than the normally assumed speed due to some factors, thereby enabling to perform the reception processing of the optical signals using the polarization information, with high accuracy.
Next is a description of a third embodiment of an optical communication system.
In the first embodiment, a part of the WDM light transmitted from the optical transmission device 1 to the optical transmission path 2 is extracted by a splitter 51 to detect whether optical signals having respective wavelengths have been polarization scrambled by the polarization scrambling detector 52. However, when the optical transmission device 1 or the like has a function of outputting information related to the presence of polarization scrambling corresponding to respective wavelengths, the information related to the presence of polarization scrambling can be collected instead of directly monitoring optical signals having respective wavelengths, to determine the speed of polarization fluctuations in the non-polarization scrambled optical signal based on the information, thereby enabling to obtain a target value of the control parameter p for the optical receiver corresponding to each wavelength. The third embodiment corresponds to a configuration example in this case.
In the optical communication system in
Accordingly, a parameter calculator 54 determines a target value of the control parameter p corresponding to the information from the information collection section 53 by referring to the table as illustrated in
In the third embodiment, an example in which the presence of polarization scrambling is determined by using the flag information output from the respective optical transmitters 11-1 to 11-M and 14-1 to 14-N is described. However, information available for determining the presence of polarization scrambling is not limited to the example described above. For example, when reception processing is performed with respect to a non-polarization scrambled optical signal by the digital coherent receiver as illustrated in
Moreover, for example, for a meshed network as illustrated in
Next is a description of a fourth embodiment of an optical communication system. In the fourth embodiment, an application example for improving compensation accuracy of polarization fluctuations in the first to third embodiments is described.
In
In the subsequent step 240, the signal quality monitor 57 monitors the information related to the quality of the reception signal output from the signal processing sections in the respective optical receivers 44-1 to 44-N. In step 250, the parameter setting section 55 determines whether the signal quality of the respective wavelengths monitored by the signal quality monitor 57 satisfies a preset reference value. When the signal quality satisfies the reference value, the value of the current control parameter value is maintained. On the other hand, when the signal quality does not satisfy the reference value, control proceeds to step 260.
In step 260, the parameter setting section 55 changes the value of the control parameter set in the optical receiver so as to improve the signal quality monitored by the signal quality monitor 57, and control returns to step 240. As the change of the control parameter, when the target value of the control parameter obtained in step 220 is αj, for example, the control parameter is sequentially changed to αj+1, αj−1, αj+2, αj−2, and so on, to search for a value at which the signal quality satisfies the reference value near the target value αj. Moreover, for example, when the number of candidate values of the control parameter is limited, such a value at which the signal quality satisfies the reference value for all the candidate values can be searched.
According to the optical communication system of the fourth embodiment, because setting of the control parameter is feedback controlled according to the actual reception signal quality in the respective optical receivers 44-1 to 44-N, in addition to setting the control parameter with respect to the respective optical receivers 44-1 to 44-N in a feed forward manner according to the target value obtained by the parameter calculator 54 of the polarization fluctuation compensation device 5′, compensation of the polarization fluctuations can be more reliably performed.
All examples and conditional language recited herein are intended for pedagogical purposes to aid the reader in understanding the invention and the concepts contributed by the inventor to furthering the art, and are to be construed as being without limitation to such specifically recited examples and conditions, nor does the organization of such examples in the specification relate to a showing of the superiority and inferiority of the invention. Although the embodiments of the present invention have been described in detail, it should be understood that the various changes, substitutions, and alterations could be made hereto without departing from the spirit and scope of the invention.
Number | Date | Country | Kind |
---|---|---|---|
2010-088469 | Apr 2010 | JP | national |
Number | Name | Date | Kind |
---|---|---|---|
4903342 | Yamazaki | Feb 1990 | A |
5031236 | Hodgkinson et al. | Jul 1991 | A |
5111322 | Bergano et al. | May 1992 | A |
5191457 | Yamazaki | Mar 1993 | A |
5416628 | Betti et al. | May 1995 | A |
5424861 | Koning | Jun 1995 | A |
5432632 | Watanabe | Jul 1995 | A |
5841557 | Otsuka et al. | Nov 1998 | A |
5896211 | Watanabe | Apr 1999 | A |
5930414 | Fishman et al. | Jul 1999 | A |
6385357 | Jopson et al. | May 2002 | B1 |
6459830 | Pua et al. | Oct 2002 | B1 |
6522796 | Ziari et al. | Feb 2003 | B1 |
6538786 | Naito | Mar 2003 | B1 |
6577413 | Saunders | Jun 2003 | B1 |
6604871 | Cao | Aug 2003 | B2 |
6647176 | Pua et al. | Nov 2003 | B1 |
6738181 | Nakamoto et al. | May 2004 | B1 |
6847743 | Yamaguchi | Jan 2005 | B2 |
6891674 | Damask | May 2005 | B2 |
6999688 | Hui et al. | Feb 2006 | B1 |
7050658 | Chung et al. | May 2006 | B2 |
7054553 | Chung et al. | May 2006 | B2 |
7106970 | Fujiwara et al. | Sep 2006 | B2 |
7206517 | Yu et al. | Apr 2007 | B1 |
7391977 | Yao | Jun 2008 | B2 |
7583895 | Nakamura et al. | Sep 2009 | B2 |
7680412 | Anderson et al. | Mar 2010 | B2 |
7702241 | Veith | Apr 2010 | B2 |
7715717 | Weiershausen et al. | May 2010 | B2 |
7873286 | Frankel | Jan 2011 | B2 |
7933522 | Rasmussen et al. | Apr 2011 | B2 |
7995918 | Raddatz et al. | Aug 2011 | B2 |
8000610 | Yao | Aug 2011 | B2 |
8032022 | Zhou et al. | Oct 2011 | B2 |
8195046 | Xia et al. | Jun 2012 | B2 |
8229302 | Von Der Weid | Jul 2012 | B2 |
8280246 | Pincemin et al. | Oct 2012 | B2 |
8483573 | Kotake et al. | Jul 2013 | B2 |
20010055133 | Yamaguchi et al. | Dec 2001 | A1 |
20030223759 | Corbel et al. | Dec 2003 | A1 |
20060013592 | Isomura et al. | Jan 2006 | A1 |
20060029398 | Liu et al. | Feb 2006 | A1 |
20070248361 | Nakamura et al. | Oct 2007 | A1 |
20080101799 | Raddatz et al. | May 2008 | A1 |
20080107425 | Rasmussen et al. | May 2008 | A1 |
20080112706 | Kim et al. | May 2008 | A1 |
20080205886 | Anderson et al. | Aug 2008 | A1 |
20090047030 | Hoshida | Feb 2009 | A1 |
20090162059 | Nakamoto | Jun 2009 | A1 |
20090214201 | Oda et al. | Aug 2009 | A1 |
20110142440 | Xia et al. | Jun 2011 | A1 |
20110182589 | Kotake et al. | Jul 2011 | A1 |
20110249971 | Oda et al. | Oct 2011 | A1 |
20120237206 | Izumi | Sep 2012 | A1 |
Number | Date | Country |
---|---|---|
2159622 | Mar 2010 | EP |
5-136761 | Jun 1993 | JP |
5-327576 | Dec 1993 | JP |
9-149006 | Jun 1997 | JP |
2002-344426 | Nov 2002 | JP |
2006-50640 | Feb 2006 | JP |
2009-198364 | Sep 2009 | JP |
2011-155579 | Aug 2011 | JP |
Entry |
---|
Patent Abstracts of Japanese Patent Application No. 5-327576, Published Dec. 10, 1993. |
Patent Abstracts of Japanese Patent Application No. 2002-344426, Published Nov. 29, 2002. |
S. Hinz et al., “Interference detection enabling 2×20Gbit/s RZ polarisation division multiplex transmission”, Electronics Letters, vol. 37, No. 8, Apr. 12, 2001, pp. 511-512. |
Mikio Yagi, et al., “Field Trial of 214-KM-Long 160-GBIT/S Polarization-Division Multiplexed RZ-DQPSK Transmission System Using Automatic Polarization Control”, IEICE, Mar. 18-21, 2008, pp. S-98-S-99. |
Ito et al., “Comparison of 100Gb/s transmission performances between RZ-DQPSK and polarization multiplexed NRZ/RZ-DPSK with automatic polarization de-multiplexer”, OFC/NFOEC 2008, JThA46 (3 pages). |
Peter Noutsios, “In-Service Measurements of Polarization Fluctuations on Field-installed OC-192 DWDM Systems,” Signals, Systems and Electronics, 2007, Issue '07, International Symposium on IEEE, Jul. 1, 2007, pp. 323-326. |
European Patent Office Communication dated Aug. 4, 2011 in Appln. No. 11160179.5. |
Japanese Office Action mailed Dec. 17, 2013 in corresponding Japanese Patent Application No. 2010-088469. |
Espacenet English Abstract of Japanese Publication No. 2011-155579, Published Aug. 11, 2011. |
Number | Date | Country | |
---|---|---|---|
20110249971 A1 | Oct 2011 | US |