Abstract:
The present invention provides a method and apparatus for obtaining a measure of the chromatic dispersion of a fibre bragg grating, the method comprising: disposing the grating in a reflection arm of an interferometer; inputting probe laser light into the interferometer; stepping the wavelength of the light across the reflection bandwidth of the grating, while at each step modulating the wavelength by a wavelength modulation less than the size of the respective step, and thereby producing a resulting phase modulation; and demodulating the phase modulation and determining therefrom a measure of the chromatic dispersion.

Description:
FIELD OF THE INVENTION 
     The present invention relates to a method and apparatus for estimating chromatic dispersion in fibre Bragg gratings. 
     BACKGROUND OF THE INVENTION 
     The technology of intra-core fibre Bragg gratings has spawned many new devices that have found applications in the telecommunication and optical sensing industries. These gratings are used to perform filter functions in the optical domain that are simply not possible (or cost-effective) in the electronic domain. Fibre Bragg gratings are playing an important role in the optical communication technology of wave division multiplexing. In one particular example, the application of chirped fibre Bragg gratings to chromatic dispersion compensation has become an important consideration in optical links as the data rates increase to meet market demands. Further, chromatic dispersion compensators based on fibre gratings are now commercially available. Accordingly, the fabrication and characterisation of fibre Bragg gratings has become of significant importance in the optical telecommunication market. 
     Fibre Bragg gratings have very similar characteristics to classical free space diffraction gratings where, for a nominal angle of incidence, the reflectivity is primarily a function of the incident wavelength. Fibre Bragg gratings can thus be considered a subset of the free-space diffraction gratings. The distinction, however, is that the angle of incidence in fibre gratings is fixed to being perpendicular to the grating length (assuming the grating cross-section is perpendicular to the fibre waveguide). The Bragg condition is satisfied when the partial reflectors that make up the grating contribute a reflected component of the incident electric field in phase with all the other partial reflectors in the grating. Accordingly, the Bragg wavelength is expressed as:
 
λ B =2{overscore (n)}Λ,  (1)
 
where
         λ B  is the Bragg wavelength (m),   {overscore (n)} is the average refractive index, and   Λ is the pitch of the grating (m).       

     As the wavelength is de-tuned away from the Bragg condition, the phase synchronicity between the ensemble of reflections rapidly deteriorates and the constructive interference ceases. In other words, the resonance condition rapidly ceases with increasing distance either side of the Bragg wavelength. A typical grating spectral response yields an extremely narrow band of wavelengths where the resonant reflection exists, so they represent a nearly ideal band-pass or notch filter in the optical domain. 
     An existing Michelson interferometer relevant to the present invention is shown schematically in FIG.  1 . The interferometer has two arms of different lengths, of path imbalance ΔL. In this Michelson interferometer, laser light is input along fibre  10  and transmitted to a beam splitter in the form of coupler  12 , where the light is split along arms  14  and  16  of length, respectively, L and L+ΔL. Light is reflected by respective mirrors  18  and  20 , and transmitted back to coupler  12 . The light—in fact as interference fringes—is then observed by means of a photodiode  24  located at the exit of output fibre  22 . 
     In uniform fibre Bragg gratings the spacing between successive partial reflectors is fixed throughout the grating. However, it is possible to fabricate fibre Bragg gratings in which the spacing is not fixed. This is the case in, for example, with linearly chirped fibre Bragg gratings, in which the spacing between successive partial reflectors changes at a constant rate over the length of the grating. Chirped and other non-uniformly spaced gratings have a number of interesting properties and advantages. For example, the linear chromatic dispersion of single mode optical fibre has become one of the limiting factors in exploiting the intrinsically large bandwidth that optical fibre communications offer. Chromatic dispersion is a result of both material and waveguide dispersion, which are in turn a function of the wavelength dependence of the effective refractive index and the profile of the core&#39;s refractive index respectively. The effect of chromatic dispersion may be illustrated with a transmitted optical pulse containing a finite band of wavelengths. As this pulse propagates through the optical fibre, the chromatic dispersion effectively advances the longer wavelength constituents and retards the shorter wavelengths. This induces the edges of the pulse to dilate in time which, in the context of a communication bit stream, may interfere with the adjacent bit cell. A typical figure for the dispersion in communication grade fibre is approximately −16 ps.nm −1 .km −1 . 
     Chirped fibre Bragg gratings can be designed to exhibit high degrees of linear chromatic dispersion. With a linear chirp in the pitch across a grating, the apparent reflection point varies linearly with wavelength. Thus, for a pulse that has been dilated through chromatic dispersion in optical fibre, it is possible to recompress the pulse by reflecting it off a correctly orientated Chirped fibre Bragg grating. It is possible to achieve 1000 ps.nm −1  of chromatic dispersion in a grating of a length 10 cm. Thus, it is possible to compensate optical fibre dispersion that occurred over many hundreds of kilometres using a very short low loss device. 
     As a consequence of the non-uniform spacing, the Bragg condition varies as a function of the spatial position within the grating. Also, whereas in a uniform grating the effective reflection point from within the grating is approximately constant with small detunings, small wavelength detunings in chirped gratings induce a movement in the Bragg resonance, the result of which is a change in the apparent reflection point from within the grating. Consequently, such gratings have found a number of important applications, so it has become important to be able to characterize accurately the properties, such as chromatic dispersion, of such gratings. 
     SUMMARY OF THE INVENTION 
     According to the present invention, therefore, there is provided a method of obtaining a measure of the chromatic dispersion of a fibre bragg grating, including:
         disposing said grating in a reflection arm of an interferometer;   inputting probe laser light into said interferometer;   stepping the wavelength of said light across the reflection bandwidth of said grating, while at each step modulating said wavelength by a wavelength modulation less than the size of said respective step, and thereby producing a resulting phase modulation; and   demodulating said phase modulation and determining therefrom a measure of said chromatic dispersion.       

     Thus, with the use of successive, slightly different wavelengths, the movement in the Bragg condition can be observed as a change in the time of flight of the reflected light. This provides a measure of or, if desired, values for the actual chromatic dispersion. In other words, the stepping of the tunable laser in centre wavelength, with—at each step—the output from the tunable laser is slightly frequency modulated, leads to an interference pattern at the photo-detector having a time dependence that is related to the rate of the slight frequency modulation applied to the laser. The phase amplitude of the demodulated interference pattern has information regarding the time of flight experienced by the probe laser light. 
     It should also be noted that references to “laser light” are intended to refer to laser output of any wavelength (whether visible, infra-red, ultraviolet, etc) that is suitable for use in the method or apparatus of the present invention. 
     Preferably said laser light is in the form of a continuous beam. 
     Preferably said measure of said chromatic dispersion comprises a time delay as a function of probe wavelength. 
     Preferably said wavelength modulation is much less than said size of said respective step. 
     Preferably said method includes normalising the response of said interferometer by means of a Mach Zehnder interferometer. 
     Preferably said demodulating is by means of a passive homodyne demodulation technique. 
     The present invention also provides an apparatus for obtaining a measure of the chromatic dispersion of a fibre bragg grating, including:
         an interference means optically connectable to said fibre bragg grating to form an interferometer;   tunable laser source means for providing wavelength tunable laser light so that the wavelength of said tunable laser source can be stepped across the reflection bandwidth of said grating;   modulation means for modulating said wavelength of said light by an amount less than said steps;   a photo-detector for detecting light from said interferometer and producing a signal indicative thereof;   demodulation means for demodulating said signal; and   computation means for determining a measure of said chromatic dispersion from said demodulated signal.       

     Preferably said laser light is in the form of a continuous beam. 
     Preferably said measure of said chromatic dispersion comprises a time delay as a function of probe wavelength. 
     Preferably said apparatus includes stepping means for stepping said tunable laser source across the reflection bandwidth of said grating. 
     Preferably said wavelength modulation is much less than said size of said respective step. 
     Preferably said apparatus includes a Mach Zehnder interferometer for normalising the response of said interferometer. 
     Preferably said demodulation means employs a passive homodyne demodulation technique. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       In order that the present invention may be more clearly ascertained, preferred embodiments will now be described, by way of example, with reference to the accompanying drawings, in which: 
         FIG. 1  is a schematic view of a prior art Michelson interferometer with a path imbalance of ΔL; 
         FIG. 2  is a schematic view of a simplified dispersion measurement apparatus according to one embodiment of the present; 
         FIG. 3  is a schematic view of a dispersion measurement apparatus according to a further embodiment of the present invention; and 
         FIG. 4  is a schematic view of a dispersion measurement apparatus according to a still further embodiment of the present invention. 
     
    
    
     DETAILED DESCRIPTION 
     The optical phase delay through a length of optical fibre can be written as:
 
φ−knL  (2)
 
where
         φ the optical phase delay (rad),   k the optical wave number in vacuum (rad.m −1 )   n the refractive index, and   L the length of fibre (m).       

     Thus there are several physical parameters that determine the phase delay in a length of optical fibre. In the present context, the relevant variable is wavelength, which is implicit in k, the wave number. 
     To obtain an expression describing the phase sensitivity to wavelength change, Eq (2) is differentiated with respect to wavelength to give: 
                 ∂   ϕ       ∂   λ       =     -       2   ⁢           ⁢   π   ⁢           ⁢   nL       λ   2                 (   3   )             
 
where
         φ the optical phase delay (rad),   λ the optical wavelength (m),   n the refractive index, and   L the length of fibre (m).       

     Eq (3) describes the relationship between phase delay and wavelength for a given length of fibre. Using the prior art Michelson interferometer depicted in  FIG. 1 , it is straightforward to observe that the relative phase change as a result of wavelength change can be written in the same form as Eq (3), but with ΔL in place of L: 
                 ∂   ϕ       ∂   λ       =     -         2   ⁢           ⁢   π   ⁢           ⁢   n   ⁢           ⁢   Δ   ⁢           ⁢   L       λ   2       .               (   4   )             
 
     The intensity at the output of the two beam Michelson interferometer shown in  FIG. 1  is a function of the optical phase relationship between the arms  14  and  16  of the interferometer according to
 
 I ( t )= A+V.E   1   .E   2  Cos(φ( t )+θ)  (5)
 
where
         I(t) is the intensity of the light at the face of the photodiode (W),   φ(t) is the optical phase difference between the arms  14  and  16  of the interferometer (rad),   θ is the phase bias of the interferometer arms (rad),   A is a constant term proportional to the input optical power,   V is a factor describing both the polarisation and coherence relationships between the two arms  14  and  16  of the interferometer,   E 1  is the electric field amplitude in the first arm  14  of the interferometer (N.C −1 ), and   E 2  is the electric field amplitude in the second arm  16  of the interferometer (N.C −1 ).       

     From the terms in Eqs (4) and (5), the relationship between the interferometer&#39;s path imbalance and the intensity output,
 
ΔL∝|φ(t)|∝I(t)  (6)
 
where
         ΔL is the interferometer path imbalance (m),   |φ(t)| is the demodulated peak to peak phase amplitude (rad), and   I(t) is the interferometer output intensity (W).       

     Thus for a known wavelength modulation, αλ, it is possible to demodulate the intensity change to obtain the amplitude of the phase excursion using Eq (5). The path imbalance of the interferometer can then be deduced using Eq (4). 
     A dispersion measurement apparatus according to one embodiment of the present invention is shown schematically in FIG.  2 . This apparatus includes an interferometer that is similar to the prior art interferometer shown in  FIG. 1 , but with one of the mirrors of the prior art device replaced with a chirped fibre Bragg grating. Thus, the interferometer of the apparatus shown in  FIG. 2  includes input fibre  30 , coupler  32 , first reflection arm  34  (of length L), second reflection arm  36  (of length L+ΔL, where ΔL depends on the wavelength dependent location of the reflection point within arm  36 ), mirror  38 , chirped fibre Bragg grating  40  and output fibre  42 . A probe laser beam (of wavelength λ p +Δλ m  sin(ωt)) entering input fibre  30  and transmitted thereby to coupler  32 , is directed along arms  34  and  36 , and reflected from mirror  38  and chirped fibre Bragg grating  40  respectively. It should be recalled that the reflection point from within a chirped grating varies depending on the probe wavelength; consequently, the path imbalance of the hybrid interferometer of  FIG. 2  will yield information about the position of the reflection point from within the grating  40 . 
     Since the chromatic dispersion of the chirped fibre Bragg grating  40  is the group delay measured as a function of wavelength, and the group delay is essentially the time of flight of power through the fibre, it is possible to define
 
 G (λ p )= k.ΔL (λ p ),  (7)
 
where
         G(λ p ) is the Group Delay at probe wavelength λ p  (ps),   ΔL(λ p ) is the path imbalance at probe wavelength λ p  (m), and   k is a constant accounting for the conversion of the path length to a time of flight, and the offset path imbalance of the interferometer.       

     It is therefore possible to characterise the Group Delay characteristics of a grating  40  with the apparatus depicted in  FIG. 2  by stepping the probe wavelength across the reflection band width of the grating  40 , while at each step modulating the probe wavelength by Δλ m . It should be noted that Δλ m &lt;&lt; (step size of λ p ). Demodulating the resulting phase modulation yields a time delay as a function of probe wavelength, that is, the chromatic dispersion characteristic of the grating  40 . 
     A dispersion measurement apparatus according to a further embodiment of the present invention, again including an interferometer, is shown schematically in FIG.  3 . The interferometer is essentially a Michelson configuration. The apparatus includes a tunable laser source  50 , an input fibre  52  and a 3×3 coupler  54 . The beam (the wavelength profile of which is depicted schematically at  51 ) from laser source  50  is directed along input fibre  52  to coupler  54 , which splits them three ways along reflection arms  56 ,  58  and  60 . However, the interferometer is essentially a two-beam interferometer since one of the second reflection arm  58  is terminated by means of mandrel  64 , so does not contribute a reflection to the output of the interferometer. Light directed along first reflection or reference arm  56  is reflected by mirror  62 , while that directed along third reflection arm  60  is reflected by chirped fibre Bragg grating  66 . 
     The 3×3 coupler  54  is used due to the particular demodulation technique employed, that is, passive homodyne. This technique requires that the phase relationship between the two outputs be other than π radians (as is the case with 2×2 terminated interferometers). This requirement is satisfied with the 3×3 coupler, which has a characteristic coupler angle of approximately 2π/3 radians. 
     The tunable laser source  50  provides both the discrete wavelength steps and the small amplitude wavelength modulation of the beam. A polarisation controller  68  is included in the reference arm  56  of the measurement interferometer to optimise the visibility of the interference pattern and improve the resolution of the measurement. Preferably extra isolation is provided on the output of the tunable laser source  50  so that the wavelength modulation is not perturbed by feedback. It is also preferable that the reflectivity of the mirror  62  match the peak reflectivity of the grating  66 , but this is not critical. 
     Light beams returned by the mirror  62  and grating  66  interfere within coupler  54 , and then detected at the exits of output fibres  70  and  72  by means of photodiodes  74  and  76  respectively. In use, the wavelength of the probe beam  51  is stepped across the reflection bandwidth of grating  66 , while at each step the wavelength is modulated—as discussed above—by an amount much less than the step size. The resulting phase modulation is measured by means of photodiodes  74  and  76 , and the time delay as a function of probe wavelength is calculated. This time delay is essentially the chromatic dispersion of grating  66 . 
     A dispersion measurement apparatus according to another embodiment of the present invention is shown schematically in FIG.  4 . The apparatus includes a tunable laser source  80  and a Michelson interferometer  82 , as well as a Mach Zehnder interferometer  84  to normalise the response of the Michelson interferometer  82  to undesirable variations in wavelength modulation from the tunable laser source  80 . This apparatus also has a degree of desensitisation to acoustically induced phase noise and thermal drift, owing to the close proximity of the two interferometers. 
     To further reduce the effect of external thermal and acoustic noise sources both interferometers  82  and  84  are enclosed in a thermally isolated anechoic chamber (not shown). 
     The probe beam from tunable laser source  80  are directed along input fibre  86   a  to first 2×2 coupler  88 . The other input arm  86   b  of 2×2 coupler  88  is terminated by means of mandrel  90   a.    
     First 2×2 coupler  88  splits the beam along arms  92  and  94  to the Michelson interferometer  82  and the Mach Zehnder interferometer  84  respectively. 
     The Michelson interferometer  82  is essentially identical to that shown in  FIG. 3 , including input arm  92  and first 3×3 coupler  96 . The latter directs the laser beam along reflection arms  98   a,b,c  to, respectively, mirror  100   a , mandrel terminator  100   b  and chirped fibre Bragg grating  100   c . First reflection or reference arm  98   a  is also provided with a polarisation controller  102 . The laser beams reflected by mirror  100   a  and grating  100   c  interfere in first 3×3 coupler  96 , and—after passing along output fibres  102   a,b —are detected by photo-detectors  104   a,b . The outputs of the photo-detectors  104   a,b  are then converted to digital form by analogue to digital converter and associated electronics  106 . 
     Mach Zenhder interferometer  84  includes an input fibre (in the form of arm  94  of 2×2 coupler  88 ) and a beam splitter in the form of 2×2 coupler  108 . (Arm  110  of 2×2 coupler  108  is terminated by mandrel  90   b .) Light beams from2×2 coupler  108  are transmitted to a 3×3 coupler  112  along shorter and longer arms  114  and  116 , the former including polarisation controller  118 . The third input arm  120  of 3×3 coupler  112  is terminated by means of mandrel  122 . 
     Output beams from 3×3 coupler  112  are directed along first and second output arms  124   a  and  124   b  and are detected by photo-detectors  126   a,b  respectively. The outputs of the photo-detectors  126   a,b  are then converted to digital form by analogue to digital converter and associated electronics  128 . The third output arm  130  of 3×3 coupler  112  is terminated by means of mandrel  132 . 
     Further to the comment above concerning undesirable variations in wavelength modulation, tunable laser sources of this type may suffer from large changes in the wavelength amplitude (cf. the size of the probe wavelength modulation Δλ m  in the apparatus of  FIG. 2 ) for the same drive voltage applied when the centre wavelength was discretely changed (cf. the step change in Δλ m  in the apparatus of FIG.  2 ). Given that the path imbalance of the Michelson interferometer  82  will change when the wavelength of the tunable laser source  80  is stepped, the path imbalance bias and the amplitude of Δλ m  (cf.  FIG. 2 ) are chosen such that the minimum phase amplitude that results during the measurement is &gt;2π rad, so that during the demodulation process an accurate estimate of the DC point of the intensity pattern can be determined (i.e. the path imbalance of the interferometer  82  assuming that the reflection point is centred in the grating). Thus it is possible to have a long length of fibre in one arm of the interferometer to ensure that the wavelength sensitivity (the phase excursion) is large. 
     Spare leads  86   b ,  98   b ,  110 , and  120  and  130  of couplers  88 ,  96 ,  108  and  112  respectively are terminated with mandrel terminators  90   a ,  100   b ,  90   b , and  122  and  132  respectively, to minimise unwanted reflections from propagating around the optical circuit of FIG.  4 . It is also preferable to use only Angled Polished Connectors. 
     The sequence of measurement is as follows. 
     The tunable laser source  80  is instructed to step incrementally across the reflection spectrum of grating  100   c . At each wavelength step, the frequency of the laser source  80  is modulated to induce a particular intensity pattern that is proportional to the group delay. The intensity outputs from interferometers  82  and  84  are sampled at photo-detectors  104   a,b  and  126   a,b  using analog-to-digital converters  106  and  128 . This information is then written to the hard drive of the measurement PC  134 , which is connected to analog-to-digital converters  106  and  128  by data links  136   a,b  respectively. (These links also allow the remote control of analog-to-digital converters  106  and  128 , as does data link  138  of laser source  80 .) The stored intensity patterns are then demodulated electronically. The response of the Michelson interferometer  82  (with the device under test) is then divided by the response of the Mach Zehnder interferometer  84 . The resulting peak to peak phase amplitude measurements represent the mean reflection point for that particular wavelength step, that is, the average of the ensemble of reflection points for the bandwidth of wavelength modulation applied. Thus it is preferable for measurement accuracy that the wavelength modulation amplitude be very much smaller than the measurement step size. This process is then repeated for all wavelength steps, so that an array of phase amplitude measurements result that can be demodulated to yield the group delay curve of grating  100   c.    
     Thus, the measurement can be automated to minimise measurement time and to improve accuracy. The small measurement time also provides further discrimination against thermal phase drift. 
     It should be noted that while the discussion of this technique has focussed on the characterisation of chirped fibre Bragg gratings it is equally applicable to characterising the group delay characteristics of other fibre Bragg grating types. 
     Alternative High Resolution Wave-Division-Multiplexed Setup 
     To compensate directly for noise sources in the Michelson interferometer, it is also possible to have two wavelengths operating in the Michelson interferometer using wave division multiplexing. The first wavelength has both the fibre Bragg grating related dispersion measurand and the noise sources of the interferometer. The second wavelength facilitates a measure (without interaction with the fibre Bragg grating under test) of just the interferometer&#39;s noise sources that can be normalised from the original measurement wavelength channel, to yield a highly accurate measurement of the chromatic dispersion of the grating. It is also possible to dispense with the second Mach Zehnder interferometer in  FIG. 4 , if the tunable laser source can be divided to form the two Wave-Division-Multiplexed (WDM) channels: one at the original wavelength from the tunable laser source and consistent with wavelength of the grating, the other frequency shifted beyond the highest frequency response of the photo-detectors. This would facilitate the removal of both the tunable laser source variations and the thermally and acoustically induced phase noise in the measurement through normalising the measurement WDM channel by the reference WDM channel. 
     Modifications within the spirit and scope of the invention may readily be effected by persons skilled in the art. It is to be understood, therefore, that this invention is not limited to the particular embodiments described by way of example hereinabove.