Abstract:
The present invention is directed towards dynamic spectral shaping. Using a grating, the spectral band is spread across a MEMS or other suitable device array. The device may be the deformable grating modulator invented by Bloom et. al. (U.S. Pat. No. 5,311,360) or other suitable device. The invention also includes the coupling in and out of the fiber and may use polarization optics to ensure the grating is used in only one polarization where the diffraction efficiency is higher.

Description:
RELATED APPLICATIONS 
     The present invention is a continuation in part of Ser. No. 09/372,712, filed Aug. 11, 1999, now abandoned and a continuation in part of Ser. No. 09,372,649, filed Aug. 11, 1999 now U.S Pat. No. 6,169,624, and a continuation in part of provisional application Ser. No. 60/171,685 filed Dec. 21, 1999, and a continuation in part of Ser. No. 09/548,788 filed Apr. 13, 2000, now U.S. Pat. No. 6,501,600, all of which applications are incorporated herein by reference. 
    
    
     BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     The present invention relates to dynamically shaping the spectral response with high resolution for fiber-optic applications. More particularly, the present invention relates to dynamic gain or channel equalization for erbium doped fiber amplifiers (EDFA) used in WDM networks. 
     2. Description of Related Art 
     The EDFA gain is highly non-uniform across the EDFA spectral band. Therefore gain flattening is an important part of good EDFA design and operation. Presently this is accomplished using a static gain flattening filter based on thin film filter technology or more recently on fiber bragg gratings. The dynamic aspect is covered by using a variable optical attenuator between the two stages of an EDFA. 
     However the previous approach is inadequate for very long links where cascading of many EDFAs and components cannot ensure adequate spectral flatness. In addition, for dynamically reconfigurable networks a static approach is inadequate. Therefore there is a need for dynamically shaping the spectral response at various points in the network for maintaining adequate end to end spectral flatness. A device for accomplishing this was invented by B. Y. Kim and others based on exciting an acoustic flexure wave along the length of a bare fiber. However this approach gives limited spectral control and the bare fiber is affected by shock and vibration. Work done at Lucent is based on spreading the wavelengths in space using a grating, followed by an array of MARS (mechanical anti-reflection switch) micromechanical modulators. This approach is limited by the fabrication difficulty and performance limitation of the MARS device. 
     Accordingly, there is a need for a simple but powerful means of dynamic spectral shaping. The ideal system should have low insertion loss, fine spectral resolution, large dynamic range, low polarization dependent loss (PDL) and simple control. 
     SUMMARY OF THE INVENTION 
     An object of the present invention is to provide controllable transmission in a communications system. 
     Another object of the present invention is to provide controllable transmission in a communications system as a function of wavelength. 
     A further object of the present invention is to provide controllable compensation for the wavelength dependent gain of EDFA&#39;s. 
     Yet another object of the present invention is to provide controllable and dynamic compensation for the dynamic wavelength dependent gain of EDFA&#39;s. 
     These and other objects of the present invention are achieved in a dynamic spectral shaping device with a controllable transmission as a function of wavelength that includes a fiber optic input port providing an input beam. A wavelength dispersive element is coupled to the input port. The wavelength dispersive element spreads the input beam in at least one dimension as a function of wavelength and generates a dispersed beam. A controllable grating reflects the dispersed beam to the wavelength dispersive element and generates a recombined beam. The controllable grating provides a controllable reflectivity as a function of wavelength. A fiber optic output port is positioned to receive the recombined beam. 
     In another embodiment of the present invention, an optical system includes an EDFA system with at least one amplifier stage. A spectral shaping device is coupled to the EDFA system. The spectral shaping device includes a fiber optic input port that provides an input beam. A wavelength dispersive element is coupled to the input port. The wavelength dispersive element spreads the input beam in at least one dimension as a function of wavelength and generates a dispersed beam. A controllable grating reflects the dispersed beam to the wavelength dispersive element and generates a recombined beam. The controllable grating provides a controllable reflectivity as a function of wavelength. A fiber optic output port is positioned to receive the recombined beam. The optical system provides a desired controllable wavelength flatness. 
     In another embodiment of the present invention, an optical system includes a fiber optic input port providing an input beam and a wavelength dispersive element coupled to the input port. The wavelength dispersive element spreads the input beam in at least one dimension as a function of wavelength and generates a dispersed beam. A controllable grating reflects the dispersed beam to the wavelength dispersive element and generates a recombined beam. The controllable grating provides a controllable reflectivity as a function of wavelength. A fiber optic output port is positioned to receive the recombined beam. An EDFA is coupled to the fiber optic input port. The optical system provides a desired controllable wavelength flatness. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIG.  1 ( a ) is a schematic top view of one embodiment of an optical system of the present invention that is utilized for dynamic spectral shaping. 
     FIG.  1 ( b ) is a schematic side view of the FIG.  1 ( a ) optical system. 
     FIG.  2 ( a ) is a schematic top view of a deformable grating, modulator array utilized in one embodiment of the present invention. 
     FIG.  2 ( b ) is a schematic side view of the FIG.  2 ( a ) deformable grating, modulator array. 
     FIG.  3 ( a ) is a schematic top view of a modified FIG.  1 ( a ) optical system that includes a circulator to extract the output light. 
     FIG.  3 ( b ) is a schematic side view of the FIG.  3 ( a ) optical system with circulator. 
     FIG.  4 ( a ) is a schematic top view of a modified FIG.  1 ( a ) optical system that includes of a quarter-wave plate to minimize PDL. 
     FIG.  4 ( b ) is a schematic side view of the FIG.  4 ( a ) optical system. 
     FIG. 5 is a schematic top view of one embodiment of an optical system of the present invention that is utilized for dynamic spectral shaping and incorporates an array waveguide grating. 
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     FIG. 1 illustrates one embodiment of an optical system  100  of the present invention for the dynamic spectral shaping. Its comprised of an input optical fiber  105 , an output optical fiber  115 , an input collimating lens  110  of focal length f 1 , an output collimating lens  120  of focal length f 1 , a walkoff birefringent plate  130  on the input side, a walkoff birefringent plate  135  on the output side, a half wave plate  140 , a grating  150  to diffract the light onto a focusing lens  160  of focal length f 2 , and then onto the device array  200 . 
     The broadband light from the input optical fiber  105  is collimated by lens  110  which may be a GRIN lens, spherical lens or any other suitable lens. The collimated light passes through a walkoff birefringent plate  130  such as YVO4, calcite or LiNbO3. The ordinary polarization goes straight through while the extraordinary polarization is displaced downwards by an amount, which if designed properly, should be greater than the beam size. The polarization of one of the displaced beams is rotated by using a half wave plate (HWP)  140  and made the same as the other beam. Now both beams are either vertically or horizontally polarized. The polarization direction is chosen to maximize the diffraction efficiency of the grating  150  which may be a holographic grating or a blazed grating. Two parallel beams impinge on the grating which diffracts the light towards the upper half of a focusing lens  160  of focal length f 2  which is placed a distance f 2  away from the grating. This telecentric use walks the focused beam across the device array  200  as a function of wavelength. The two polarization paths come together on the device array which is segmented to cover different spectral slices. The reflected light from the device goes through the bottom half of the lens  160  and impinges on the grating which puts all the wavelengths back to gather. The polarization is combined again using the HWP and the output birefringent plate  135  which is oriented opposite from the input birefringent plate. The beam is focused into the output fiber  115  using another collimating lens  120 . 
     The device array  200  may be an array of LCD elements, a suitable MEMS device array such as micro mirrors or cantilevers, an array of electro-optic modulators, an array of acousto-optic modulators or any light controlling device array. The preferred embodiment is based on using a deformable grating modulator array invented by Bloom et. al. (U.S. Pat. No. 5,311,360) as shown in FIGS.  2 A,B. The device is comprised of ribbons  199  of width w suspended above the substrate  198 . The top surface of the ribbon is a height d above the substrate. Ribbons are electrically connected and driven in pairs. Each pair controls a spectral slice.  201  controls λ 1 ,  202  controls λ 2 , and so on till  20   n  controls λn. The gap between the ribbons is also w. All ribbons and gaps are covered with a reflective layer which may be aluminum or gold. For operation at a given wavelength λ, d=mλ/2 where m is an integer. Now light reflected from the ribbons and the gaps is in phase and device looks like a mirror. By applying a voltage to the ribbons, the electrostatic force starts pulling the ribbons downwards and light starts diffracting. At a maximum deflection of λ/4, all the light is diffracted out and the element is effectively off. Two pairs of ribbon/gap provides enough isolation for a single-mode fiber. However more pairs can also be used. For a range of wavelength, λ 1 -λn, d is chosen based on the longest wavelength, λ 1 , i.e. d=mλ 1 /2. In practice, m=3 is a suitable choice. For the EDFA application λ 1 =1575 nm, therefore d=2362 nm. The shorter wavelength elements will start out with the ribbons already slightly pulled in. In FIG. 1, the choice of focal lengths f 1 , f 2  and the grating use determines the spot size on the device array which in turn determines the ribbon width w, i.e. spot size=4 w. The spectral resolution of the system is determined by f 1 , f 2 , grating pitch and the grating incident angle. The resolution should be such that going from λ 1  to λ 2  moves the spot across the device array by w. 
     An alternate embodiment of the optical system  300  is shown in FIGS.  3 A,B, which is the same as system  100  in FIG. 1, except a circulator  103  is used to separate out the light in the input fiber  101  from the output fiber  102 . 
     Yet another embodiment of the optical system  400  is shown in FIGS.  4 A,B. This is again similar to system  100  shown in FIG. 1 except that polarization splitting is not employed. Since both polarizations are impinging on the grating  150 , it is desirable that the grating have high diffraction efficiency for both polarizations. After diffracting from the grating, a quarter wave plate (QWP)  140  is employed to flip the vertical and horizontal polarizations on the return path. This reduces the polarization dependent loss (PDL) for the overall system assuming the device array  200  does not have any significant PDL. If PDL from the device array needs to be minimized further, the polarization independent grating modulator invention of Godil et. al. (include by cross-reference) can be used here configured as an array of elements. Another variation of this embodiment would be to use a circulator on the input side to separate out the output fiber from the input without creating a separate path. 
     Another embodiment of the present invention is disclosed in FIG.  5 . In this embodiment, dispersive element  150  is an arrayed waveguide grading (“AWG”). A suitable AWG  150  is manufactured by Lightwave Microsystems, San Jose, Calif. In this embodiment, device array  200  which can be a controllable, deformable grating modulator, can be placed in close proximity to the dispersed output at AWG  150 . This proximity is selected to provide good coupling efficiency back into the waveguides of AWG  150 . The maximum distance depends on the size of the waveguides of AWG  150 . In a preferred embodiment, the distance is 10 microns or less and can be butt-coupled. With this combination, AWG  150  disperses the light from the input optical fiber  105  and spreads the input beam in at least one dimension as a function of wavelength where it impinges on device array  200 . The spatially dispersed light is reflected back into AWG  150  which subsequently recombines the light into optical fiber  105  but in a counterpropagating direction to the input. The output light can be extracted by circulator  103 . Other embodiments can include a separate output port and do not require the circulator. 
     The forgoing description of the invention has been presented for purposes of illustration and description. It is not intended to be exhaustive or to limit the invention to the precise forms disclosed. Obviously, many modifications and variations will be apparent to practitioners skilled in this art.