Patent Document

FIELD OF INVENTION 
       [0001]    The present invention relates generally to dispersion compensation in optical fiber transmission systems. In particular, this invention relates to polarization mode dispersion (PMD) compensation in optical fiber transmission systems. 
       BACKGROUND 
       [0002]    Modern wavelength division multiplexing (WDM) techniques permit the simultaneous transmission of multiple high bandwidth channels on respective wavelengths in an optical medium in communication networks. Polarization-mode dispersion (PMD) has become one of the limiting factors for such high bandwidth transmission systems. 
         [0003]    A single-mode optical fiber carrying an optical signal of arbitrary polarization can be considered as a linear superposition of two orthogonally polarized HE 11  modes. Ideally, in a single mode fiber, the two optical modes are degenerate in terms of their propagation properties owing to the cylindrical symmetry of the fiber. 
         [0004]    Real optical fibers, however, have some unintentional loss of circular symmetry. The randomly varying birefringence of a fiber may be a result of the fiber manufacturing process, stresses on the fiber from cabling or environment effects such as temperature and vibration. Whether this asymmetry occurs during manufacturing or is due to external forces, the loss of circular symmetry gives rise to two distinct polarization modes, with distinct phase and group velocities. 
         [0005]    In the time domain, the differential group velocity is expressed as a propagation time difference known as the differential group delay (DGD), when an optical signal is propagated in the two orthogonally polarized HE 11  modes. 
         [0006]    PMD can be represented, to the first order, by differential group delay between two orthogonal principal states of polarization (PSP) with a fast axis and a slow axis, respectively. Since the birefringence of a fiber varies randomly along a fiber link, differential group delay is a random variable that has a Maxwellian probability density function, i.e. the maximum instantaneous differential group delay can be several times above the average differential group delay. The mean differential group delay grows as the square root of the length of the system. 
         [0007]    When an optical signal propagates down a fiber, the two component principal states of polarization of the light signal travel along the fast and slow axes of the fiber. Differential group delay may therefore result in bit-spreading of the optical signals. For signal propagating at 2.5 Gb/s or below, the impact of PMD for most fiber plant that has been deployed is minimal. As the data rate increases beyond 2.5 Gb/s towards 10 and 40 Gb/s, the signal pulse width narrows and the effect of PMD is the spreading of the original pulse in time, resulting in an overflow into a time slot of the transmitted signal which has been allotted to another bit, resulting in high BER and limiting total transmission distance. 
         [0008]    All states of polarization (SOP) of an optical signal can be represented on a Poincaré sphere at the same time by assigning each state of polarization its own specific point on the Poincaré sphere. Points on the equator represent states of linear polarization, the poles represent right-hand and left-hand circular polarization, and other points on the sphere represent elliptical polarization. 
         [0009]    One effective way of managing PMD is to reduce transmission distance by regeneration. However, this is a very costly option, in particular in WDM systems where channel capacity is high. 
         [0010]    Another approach is to negate the effect of PMD before the optical signal is decoded by the optical receiver through the use of PMD compensators. The PMD compensators accomplish this task by delaying one state of polarization with respect to the other by the amount of differential group delay. 
         [0011]    Various designs and configurations for PMD compensators have been proposed in the art. 
         [0012]    U.S. Pat. No. 5,793,511 describes an optical receiver, which receives and evaluates an optical signal with PMD. The optical receiver has a splitting facility splitting the optical signal into two electrical signal components. The electrical signal components are processed in an equalizing circuit. A control facility controls the splitting facility with the aid of a quality signal produced by the equalizing circuit. 
         [0013]    U.S. Pat. No. 6,674,936 teaches a system and a method using a wavelength-locked loop servo-control circuit and methodology that detects a PMD characteristic of the optical signal and enables real time adjustment of the center wavelength of the optical signal at the transmitter to minimize PMD in the optical fiber link. 
         [0014]    The disadvantages of using electronic devices to apply PMD corrections are complex and potentially costly, and signal processing technologies are often required. 
         [0015]    U.S. Pat. No. 6,661,937 describes an apparatus for changing the polarization state of an optical signal. The apparatus includes sequentially connected phase shifters, each of the phase shifters is adapted to exert a force on an optical fiber disposed in the respective shifter. Each of the phase shifters includes a registration key which selectively orients an axis of the optical fiber disposed in the registration key at a predetermined azimuth. 
         [0016]    Applying mechanical stress may result in breakage and coating delamination of the fiber and cause long term reliability issues. 
         [0017]    Therefore, all optical PMD compensation, in which the optical signal traffic remains in the optical domain, is the preferred choice for high bandwidth optical communications. 
         [0018]    A typical PMD compensator (PMDC) employing adaptive optics in an optical fiber system is shown in  FIG. 1 . A fiber optic system  100  includes a transmitter  102 , the optical transmission span  104 , and a receiver  106 . The PMD compensator includes the polarization controller  108  and PMD compensating element  110 . To correct the polarization state of optical signals emerging from the optical transmission span  104 , the polarization controller  108  typically transforms the state of polarization of the optical signals into prescribed or preferred polarization states of the PMD compensating element  110 . The PMD compensating element  110  may comprise a single-mode fiber which have polarization mode attenuating or maintaining properties with intentionally asymmetric cores. In fiber with attenuating properties, a first polarization mode is transmitted normally, whereas the orthogonal polarization mode is subject to attenuation, effectively stripping that mode and leaving the first mode for signal transmission. In polarization-maintaining fiber, input signal is split into two orthogonal modes along a core with an asymmetry which defines and maintains different refractive indices for each polarization. The two polarization modes travel at different speeds due to the relative refractive indices. 
         [0019]    The principal state of polarization of the incoming optical signals is rotated to align with the polarization controller  108 . Adjustments are then applied in the PMD compensating element  110  to the optical signal to remove the differential group delay between the component polarizations of the signal. The degree of polarization is monitored  112  by a polarimeter  114 . Control electronics  116  provides a feedback signal  118  to the polarization controller  108  to provide the optimized principal state of polarization. 
         [0020]    Therefore, prior art PMD compensator as described in  FIG. 1  generally rotates the incoming signal to align its principal state of polarization with the compensator element. This may require complex precision control algorithm and apparatus. In addition, the direction of the PMD in the incoming signal may not be easily determined. Furthermore, the monitored polarization compensation may be a result of both the alignment of the PMD axis of the incoming signal and the effect of the compensating element. 
         [0021]    Therefore, there is a need for a simple technique for implementing PMD compensation. 
       SUMMARY OF THE INVENTION 
       [0022]    In accordance with one aspect of the present invention there is provided an apparatus for compensating polarization mode dispersion in an optical communication system comprising: an input for receiving an optical input signal having two orthogonal principal states of polarization, and a differential group delay between the two orthogonal principal states of polarization resulting in polarization mode dispersion; the input operable to connect to an optical fiber having a fast axis and a slow axis, the fast axis being orthogonal to the slow axis; a compensating element connected to the input for compensating the polarization mode dispersion; a splitting device connected to the compensating element for tapping a fraction of the optical input signal; a monitoring element having birefringence properties for receiving the fraction; the monitoring element separating the fraction into two split signals with orthogonal principal states of polarization according to the birefringence properties of the monitoring element; detecting devices for registering the split signals; and a processor connected to the detecting devices for determining an optimised coefficient, the optimised coefficient being indicative of an angle between a fast axis of the monitoring element and the fast axis of the optical fiber. 
         [0023]    Preferably, the compensating element is adjusted according to the angle between a fast axis of the monitoring element and the fast axis of the optical fiber, for providing desired polarization mode dispersion. 
         [0024]    Preferably, the compensating element is a liquid crystal. 
         [0025]    Preferably, the monitoring element is a liquid crystal. 
         [0026]    Preferably, the detecting devices are photodetectors, the photodetectors register voltages V PD1  and V PD2  based on: 
         [0000]        V   PD1   =[S   in  cos(α)cos(β)+ S   in  cos(α)cos(β)] 2  
 
         [0000]        V   PD2   =[−S   in  cos(α)sin(β)+ S   in  sin(α)cos(β)] 2  
       wherein S in  is the fraction of the optical input signal; α is an angle between the principal state of polarization of the optical input signal and the fast axis of the optical fiber; and β is an angle between the fast axis of the monitoring element and the fast axis of the optical fiber.       
 
         [0028]    Preferably, the coefficient is: 
         [0000]        Coeff (α,β, PMD )=∫ V   PD1   V   PD2   dt  
 
         [0029]    Preferably, the processor is a digital signal processor. 
         [0030]    In accordance with another aspect of the present invention there is provided a method for compensating polarization mode dispersion in an optical communication system comprising the steps of: receiving an optical input signal having polarization mode dispersion (PMD); passing the optical signal through a compensating element; tapping a fraction of the optical input signal at a splitting element; separating the tapped fraction into two split signals having orthogonal principal states of polarizations (PSP) using a monitoring element having a fast axis; determining the split signals; adjusting the fast axis of the monitoring element for determining an optimized coefficient for the split signals; and setting the compensating element based on the optimized coefficient, to compensate PMD in the optical input signal. 
         [0031]    Preferably, the step of adjusting the fast axis of the monitoring element further comprises the steps of determining an angle between the fast axis of the monitoring element and a fast axis of an optical fiber carrying the optical input signal. 
         [0032]    Preferably, the compensating element is a liquid crystal. 
         [0033]    Preferably, the monitoring element is a liquid crystal. 
         [0034]    Preferably, the split signals are determined by: 
         [0000]        V   PD1   =[S   in  cos(α)cos(β)+ S   in  cos(α)cos(β)] 2  
 
         [0000]        V   PD2   =[−S   in  cos(α)sin(β)+ S   in  sin(α)cos(β)] 2  
       wherein V PD1  and V PD2  are voltages registered at photodetectors; S in  is the fraction of the optical input signal; α is an angle between the PSP of the optical input signal and a fast axis of an optical fiber; and β is an angle between the fast axis of the monitoring element and the fast axis of the optical fiber.       
 
         [0036]    Preferably, the coefficient is: 
         [0000]        Coeff (α,β, PMD )=∫ V   PD1   V   PD2   dt  
 
         [0037]    Unless otherwise defined, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the art. All publications, patent applications, patents, and other references mentioned herein are incorporated by reference in their entirety. In case of conflict, the present specification, including definitions, will control. In addition, the apparatus, methods, and examples are illustrative only and not intended to be limiting. 
     
    
     
       BRIEF DESCRIPTION OF THE FIGURES 
         [0038]    The invention and the illustrated embodiments may be better understood, and the numerous objects, advantages, and features of the present invention and illustrated embodiments will become apparent to those skilled in the art by reference to the accompanying drawings. In the drawings, like reference numerals refer to like parts throughout the various views of the non-limiting and non-exhaustive embodiments of the present invention, and wherein: 
           [0039]      FIG. 1  is a block diagram of a prior art polarization mode dispersion compensator; 
           [0040]      FIG. 2  is a block diagram of an exemplary embodiment of an apparatus operable to provide dynamic polarization mode dispersion according to the teaching of the present invention; 
           [0041]      FIG. 3  shows a projection of a Poincaré sphere for describing the determination of the fast axis of the input optical fiber; 
           [0042]      FIGS. 4  (A) and (B) are graphs showing the relationship between power and the angle between the fast axis of the incoming fiber and the fast axis of the monitoring element; 
           [0043]      FIG. 5  (A) depicts the coefficient in relation to the adjustment of the angle between the fast axis of the incoming fiber and the fast axis of the monitoring element; 
           [0044]      FIG. 5  (B) depicts the coefficient as a function of differential group delay; and 
           [0045]      FIG. 6  is a flowchart showing one example of a method for dynamic polarization mode dispersion compensation. 
       
    
    
     DETAILED DESCRIPTION 
       [0046]    Reference will now be made in detail to some specific embodiments of the invention including the best modes contemplated by the inventors for carrying out the invention. Examples of these specific embodiments are illustrated in the accompanying drawings. While the invention is described in conjunction with these specific embodiments, it will be understood that it is not intended to limit the invention to the described embodiments. On the contrary, it is intended to cover alternatives, modifications, and equivalents as may be included within the spirit and scope of the invention as defined by the appended claims. In the following description, numerous specific details are set forth in order to provide a thorough understanding of the present invention. The present invention may be practiced without some or all of these specific details. In other instances, well known process operations have not been described in detail in order not to unnecessarily obscure the present invention. 
         [0047]    In accordance with one aspect of the present invention, the monitoring and/or compensating elements of the PMD compensator are rotated to align with the state of polarization of the incoming signal. The monitoring components tracks the fast and slow axes of the fiber based on the polarization of the incoming signal. In a preferred embodiment, the inherent birefringence properties of liquid crystal are used for monitoring and/or compensating PMD. In another preferred embodiment, optical power is correlated to align the fast and slow axes of the compensating element and the state of polarization of the optical signal. 
         [0048]    Liquid crystal may be used as a polarization controller. Liquid crystals exhibit birefringence, which is a function of the orientation of the liquid crystal molecules that derive their anisotropic physical properties from the orientation of their constituent molecules. The orientation can be controlled by the intensity of an applied electric field. 
         [0049]    Reorientation of the liquid crystal molecules under the influence of the applied electric field introduces elastic strains in the material. These strains stem from constraints imposed on the molecular orientation at the boundaries confining the liquid crystal. These surface constraints, or surface anchoring, are such that molecules close to the surface are not free to reorient, and remain substantially along some preferred direction. 
         [0050]    When an electric field is applied to a liquid crystal element, the directors of the liquid crystal molecules are reoriented in response to the applied field. 
         [0051]      FIG. 2  provides an exemplary embodiment of the PMD compensator  200  in accordance with the present invention. The PMD compensator  200  receives an optical signal  202  with differential group delay  204 . The PMD compensator  200  includes a monitoring element  206 , which is used to locate the principal state of polarization of the optical signal. The monitoring element  204  may be a liquid crystal. The PMD compensator  200  further comprises a compensating element  208 , which is capable to align its fast axis with the fast axis of the fiber and applies the necessary delay to compensate the DGD from the fiber, resulting in an optical signal with reduced PMD  210 . The compensating element  208  may also be a liquid crystal. 
         [0052]    In operation, the compensating element  208  receives an incoming optical signal  202 . A small percentage, for example, 5% of the signal is tapped off to the monitoring element  206  at a splitting element  212 . The tapped signal  214 , S IN , is then separated into two split signals with orthogonal principal states of polarization, S F    216  and S S    218 , according to the birefringence properties of the monitoring element  206 , for example, the birefringence properties of a liquid crystal. 
         [0053]    Detecting devices, such as photodetectors PD 1    220  and PD 2    224  register voltages, V PD1    226  and V PD2    228 , corresponding to the amount of light detected. The registered voltages are sent to a processor  230 , for example, a digital signal processor (DSP). 
         [0054]    The processor  230  then applies a control signal  232  to the monitoring element  206 , in an exemplary embodiment a voltage to align a monitoring liquid crystal, such that a correlation coefficient is optimized. A corresponding control signal  234  can then be applied to the compensating element  208  such that the appropriate delay is applied to the optical signals  202  to compensate for the PMD. An example of the control signal  234  is a voltage applied to a compensating liquid crystal to provide an appropriate birefringence for compensating the PMD in the received optical signal. 
         [0055]      FIG. 3  shows a presentation of PMD as viewed from the direction  236  illustrated in  FIG. 2 . In this view, vector  302  represents the fast axis of the input fiber, vector  303  represents the slow axis of the input fiber, vector  304  represents the principal state of polarization of the incoming optical signal  202 . The vectors  302  and  304  form an angle α  306 , i.e. an angle between the principal state of polarization of the incoming optical signal and the fast axis of the input fiber. The vector  308  represents the fast axis of the monitoring element  206 . The vectors  302  and  308  form an angle β  310 , i.e., an angle between the fast axis of the monitoring element  206  and the fast axis of the input fiber. 
         [0056]    The fast axis of the input fiber, represented by the vector  302 , is actually unknown at the beginning of the process. By manipulating the monitoring element  206  and observing the changes of the voltages V PD1    226  and V PD2    228  on photodetectors PD 1    220  and PD 2    224 , the angles α  306  and β  310  can be calculated based on the voltages V PD1    226  and V PD2    228 : 
         [0000]        V   PD1   =[S   in  cos(α)cos(β)+ S   in  cos(α)cos(β)] 2  
 
         [0000]        V   PD2   =[−S   in  cos(α)sin(β)+ S   in  sin(α)cos(β)] 2  
 
         [0057]    Referring to  FIG. 4 , the x-axis represents time and the y-axis is the voltage registered at the photodetectors  220 ,  224  illustrated in  FIG. 2 . The curves  402 ,  406  are the voltages registered at the photodetector  220  and the curves  404 ,  408  are the voltages registered at the photodetector  224 .  FIG. 4  (A) illustrates detected voltages of an optical signal with a differential group delay of 10 ps. The fast axis of the input fiber aligns with the fast axis of the monitoring element (β=0°) and forms a 45° angle with the principal state of polarization of the optical signal (α=45°). This alignment results in comparable voltages being detected at photodetectors  220  and  224 . 
         [0058]      FIG. 4  (B) illustrates detected voltages of an optical signal with a differential group delay of 10 ps. The fast axis of the input fiber forms an angle of 20° with the fast axis of the monitoring element (β=20°) and forms a 45° angle with the principal state of polarization of the optical signal (α=45°). This alignment results in a higher voltage being detected at photodetector PD 2    224 . 
         [0059]    Accordingly, a coefficient can be calculated as: 
         [0000]        Coeff (α,β, PMD )=∫ V   PD1   V   PD2   dt  
 
         [0060]    Referring to  FIG. 5  (A), where the x-axis is the angle (β) between the fast axis of the input fiber and the fast axis of the monitoring element  206 , the fast axis of the monitoring element  206  is best aligned with the fast axis of the input fiber when the coefficient reaches a peak  502 . Therefore, the position of the fast axis in the input fiber is determined based on the values of the coefficient. 
         [0061]      FIG. 5  (B) shows the coefficient as a function of the differential group delay of the compensating element. As the ratio of coefficient to V PD1    226  and V PD2    228  is varied, so is the differential group delay. 
         [0062]    In a preferred embodiment, the fast axis of the compensating element  208  is controlled based on the determined position of the fast axis of the input fiber. Therefore, instead of using a polarization controller to adjust the state of polarization of the incoming optical signal as in the prior art PMD compensators, the present invention adjusts the fast axis of the compensating element, for example, the fast axis of a birefringent liquid crystal, based on the fast axis of a monitoring element, for example, the fast axis of a second birefringent liquid crystal. 
         [0063]      FIG. 6  illustrates a flowchart showing one example of a method in accordance with one embodiment of the present invention. Also referring to  FIG. 2 , an optical input signal  202  is received at the PMD compensator  200  at step  602 . The optical signal passes through a compensating element  208  at step  604 . A fraction  214  of the optical input signal is tapped at a splitting element at step  606 . The tapped fraction is separated into two split signals with orthogonal principal states of polarization (PSP)  216 ,  218  using a monitoring element  206 . The fast axis of the monitoring element  216  is adjusted to determine an optimized coefficient for the two PSPs at step  610 . The compensating element  208  is then set to compensate the PMD in the optical input signal based on the optimized coefficient at step  612 . 
         [0064]    Although various aspects of the present invention have been described in several embodiments, a myriad of changes, variations, alterations, transformations, and modifications may be suggested to one skilled in the art, and it is intended that the present invention encompass such changes, variations, alterations, transformations, and modifications as fall within the spirit and scope of the appended claims.

Technology Category: h