Abstract:
A method and system includes a pulse reshaper for reshaping and re-amplifying optical signals in a communications network. In one embodiment, a vertical cavity semiconductor optical amplifier (VCSOA) device, comprising dual mode reflectors optically cooperating at each of an input signal wavelength (λ s ) and an offset wavelength (λ C ) proximate the input signal wavelength (λ s ) to provide thereby non-linear amplification of input signal (λ s ).

Description:
CROSS-REFERENCE TO RELATED APPLICATION 
       [0001]    This application is a divisional of pending U.S. patent application Ser. No. 11/321,151, filed on Dec. 29, 2005, entitled Semiconductor Optical Amplifier Pulse Reshaper which application is incorporated herein by reference. 
     
    
     FIELD OF THE INVENTION 
       [0002]    The invention is related to the field of optical communications, and in particular, to semiconductor optical amplifier pulse reshapers. 
       BACKGROUND OF THE INVENTION 
       [0003]    Regenerations of optical signals are essential aspects of optical communications. Regenerations may be accomplished by re-amplification, re-shaping and re-timing through the use of optic-electronic-optic (OEO) repeaters. However, optic-electronic-optic (OEO) regenerations are expensive and technologically complex. Currently, OEO regenerations are the main approach commercially available for this task. 
       SUMMARY 
       [0004]    Various deficiencies of the prior art are addressed by the present invention devices and methods for optical signal reamplification. 
         [0005]    In one embodiment, a semiconductor optical amplifier (SOA) device includes dual mode reflectors optically cooperating at an input signal wavelength (λ s ) and an offset wavelength (λ C ) proximate the input signal wavelength (λ s ) to provide thereby non-linear amplification of the input signal (XS). 
         [0006]    An embodiment of the invention provides for a semiconductor optical amplifier (SOA) pulse reshaper, including a pump for adjusting the lasing threshold and amplification of the SOA at either signal wavelength (λ s ) or offset wavelength (λ C ) which is dependent on input digital signal intensities of logical 1 and 0. The SOA includes dual mode reflectors optically cooperating at an input signal wavelength (λ s ) and an offset wavelength (λ C ) proximate the input signal wavelength (λ s ). A controller for providing thereby non-linear amplification of input signal (λ s ). 
         [0007]    The invention further provides other methods and system elements that implement various aspects, embodiments, and features of the invention, as described in further detail below. 
         [0008]    The foregoing, together with other aspects of this invention, will become more apparent when referring to the following specification, claims, and accompanying drawings. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0009]    The teachings of the present invention can be readily understood by considering the following detailed description in conjunction with the accompanying drawings, in which: 
           [0010]      FIG. 1  depicts a block diagram of a dual mode vertical cavity semiconductor optical amplifier (VCSOA) according to an embodiment of the invention; 
           [0011]      FIG. 2  depicts a block diagram of a dual mode in-plane semiconductor optical amplifier according to an embodiment of the invention; 
           [0012]      FIG. 3A  depicts a line graph depicting the relationship of small signal gains and cavity losses to two modes (or two wavelengths) without input signal according to an embodiment of the invention; 
           [0013]      FIG. 3B  depicts a line graph depicting a relationship of the gains and cavity losses to the two modes (or two wavelengths) with a logic “1” input signal with appropriate optical intensity according to an embodiment of the invention; 
           [0014]      FIG. 4  depicts a line graph of signal gain as a function of input signal intensity (signal logic “0” and logic “1”) according to an embodiment of the invention; and 
           [0015]      FIG. 5  depicts a block diagram of a semiconductor optical amplifier pulse reshaper according to an embodiment of the invention. 
       
    
    
       [0016]    To facilitate understanding, identical reference numerals have been used, where possible, to designate identical elements that are common to the figures. 
       DETAILED DESCRIPTION OF THE INVENTION 
       [0017]    The invention will be primarily described within the context of vertical cavity semiconductor optical amplifier pulse reshaper; however, those skilled in the art and informed by the teachings herein will realize that the invention is also applicable to any apparatus and method that involves regeneration of optical signals in, for example, a communication network. 
         [0018]    This invention may be utilized to replace the OEO regeneration approach with a SOA reshaper that can remarkably reduce both the cost and the complexity of the system. Embodiments of the invention can be easily integrated in front of optical receivers and/or behind other types of optical amplifiers, while providing small power consumption and footprint to improve system performance as well as simplicity. 
         [0019]      FIG. 1  depicts a block diagram of a dual mode vertical cavity semiconductor optical amplifier (VCSOA)  100  according to an embodiment of the invention. Specifically, the VCSOA  100  comprises four layers: a substrate layer  110 , a first dual mode distributed Bragg reflector (DBR) mirror  120 , an active region  130 , and a second dual mode DBR mirror  140 . 
         [0020]    Portions of the structure of the VCSOA are well known in the art, except for the “dual mode” design of this invention. The bottom layer of the four layers the substrate  110 . The next layer above the substrate is the first dual mode DBR  120  layer. The next layer above the first DBR layer is the active region  130 . The top layer is the second dual mode DBR layer  140 . The input light is transmitted into the VCSOA from the top of layer  140 . The input light enters the active region  130 . The active region  130  amplifies the input light by reflecting the light between the first and second DBR mirrors  120  and  140 , and by pumping the region with the pump light  170 . The pump light  170  transfers the pump energy into signal optical energy. The structure of the two DBRs at both ends of the active region produces wavelength-selective reflections where the light in the active region  130  is amplified. With appropriate selection of the cavity length which satisfies L=n*λ/2 (wherein L is the effective cavity length, “n” is an integer, λ is the wavelength of the specific mode), the two modes of the cavity can resonate. The amplified output light exiting the VCSOA from the top DBR layer  140  is 180 degree out of phase with respect to the part of input light that is reflected-off the surface of the top DBR layer  140 . The reflected-off input light is the portion of light that is reflected off the top DBR layer  140  without entering the VCSOA. The final output of the SOA should be the interfering result of the amplified output light and the reflected-off input light. 
         [0021]    In the present invention, DBR mirrors  120  and  140  each include two portions  180 ,  190 . A first portion reflects a first wavelength and a second portion reflects a second wavelength. Thus, the VCSOA has 2 reflective wavelengths and two modes of operation. The space between the mirrors or cavity length is selected such that the equation L=n*λ/2 (wherein L is the effective cavity length, “n” is an integer, λ is the wavelength of the specific mode) can be satisfied for both wavelengths. The dual mode VCSOA receives an input optical signal λ s    150 . The output optical signals  160  have wavelengths of λ S  and λ C . One wavelength λ S  is the same wavelength as the input signal and the other λ C  is separated by a small offset. The two wavelength outputs are amplitude modulated by each other and are interleaved in time domain with logic zeros and ones. The offset is selected to be small enough to obtain strong interaction between the two modes. In one embodiment, the wavelength offset is a value between ±0.4 nm and ±4.0 nm. In other embodiments, other amounts of offset are used. The offset values are varied by the selection of the reflective portions of the DBR mirrors as well as the effective cavity length for this offset mode. 
         [0022]      FIG. 2  depicts a block diagram of a dual-mode in-plane semiconductor optical amplifier (SOA) according to an embodiment of the invention. Specifically, the in-plane SOA has four layers: a first substrate layer  210 , an active medium layer  220 , a distributed feedback (DFB) layer  230 , and a second substrate layer  240 . 
         [0023]    The in-plane SOA receives as input an optical signal  250  and provides at an output an amplified optical signal  260 . The bottom and top layers  210 ,  240  are substrate layers, which functions as the ground and contact, respectively. The DFB layer  230  includes a wavelength selective Bragg grating. The active medium  220  is in close proximity with the DFB layer. The input optical signal resonantly diffracts back and forth in the in-plane SOA. An amplified optical signal  260  exits the in-plane SOA. 
         [0024]    In an embodiment of the present invention, the in-plane SOA has two modes that allow two wavelengths to resonate. Similar to the DBR mirrors in  FIG. 1 , the DFB layer of in-plan SOA has two reflective wavelengths or two modes of operation. The grating of the DFB will determine the two modes of the in-plane SOA. The dual mode in-plane SOA receives an input optical signal λ s    250 . The output optical signals  160  will have wavelengths of S and λ C . One wavelength λ S  is the same wavelength as the input signal and the other λ C  is separated by a small offset. The two wavelength outputs are amplitude modulated by each other (i.e. mutual modulation) and are interleaved in time domain with logic zeros and ones. In one preferred embodiment, the preferred wavelength offset is between ±0.4 nm and ±4.0 nm. In other embodiments, other amounts of offset are possible. The offset values are varied by the selection of the reflective portions of the DFB layer. 
         [0025]    The two types of SOA&#39;s can both be used as pulse reshaper. The VCSOA is use in an embodiment. The VCSOA will be used to further describe the invention. 
         [0026]      FIG. 3A  depicts a line graph depicting the relationship of small signal gains and cavity losses of two modes (or two wavelengths) without input signal according to an embodiment of the invention. The X-axis represents the wavelength; the Y-axis represents cavity loss and cavity small signal gain of the VCSOA. In one embodiment, the wavelength is measured in nanometer (nm); the loss and gain are measured in dB. In  FIG. 3A , the solid line represents the relative cavity loss over wavelength; the dotted line represents relative cavity small signal gain over wavelength. The structure as designed will have the cavity small signal gain and cavity loss characteristics as shown by the dotted line and solid line respectively. At Xs there is smaller loss, represented by a dip in the curve. At λ C  there is even smaller loss than at Xs, represented by an even bigger dip. Lasing occurs when the cavity small signal gain is greater than the cavity loss. The dotted line is substantially a horizontal line that is below the cavity loss except at the frequencies around λ C  with well controlled pumping level. Thus, the VCSOA lases at λ C  when no input signal is applied to the device. 
         [0027]    In the preferred embodiment, when there is no input signal, the wavelength λ C  has a greater gain than loss so it lases and clamps the VCSOA at deep saturation condition because the VCSOA is designed to have as small as possible cavity loss for this clamp mode (the clamp mode is equivalent to the offset mode in this document). The loss at wavelength λ S  is greater than the gain at that so the SOA does not lase at λ S . The graph of  FIG. 3A  depicts the condition equivalent to the optical input signal having a logical “0” as the input when there is only optical noise is injected. Full extinction of the signal output can be obtained by designing the two DBR mirrors so that the reflected-off input signal interferes with the amplified output signal thereby no light is produced from the VCSOA as output for logic “0”. The cavity parameters should satisfy: 
         [0000]    
       
         
           
             
               g 
               s 
             
             = 
             
               
                 
                   R 
                   t 
                 
               
               
                 
                   R 
                   b 
                 
               
             
           
         
       
       
         
           
             where: 
             g s  is single pass gain; 
             R t  is top DBR reflectivity for λ s ; 
             R b  is bottom DBR reflectivity for/λ s .
 
this full extinction condition means that the optical noise contained within the logic “0” time slot is eliminated at VCSOA output.
 
           
         
       
     
         [0032]      FIG. 3B  depicts a line graph depicting a relationship of the gains and cavity losses of the two modes (or two wavelengths) with a logic “1” input signal with appropriate optical intensity according to an embodiment of the invention. In the graph of  FIG. 3B , similar to the graph of  FIG. 3A , the X-axis represents the wavelengths of the input signal and the Y-axis represents the cavity losses and the cavity saturated gains at the respective wavelengths. The wavelength is measured in nanometer (nm) and the gain is measured in dB. The solid line represents the cavity losses at the respective wavelengths on the X-axis, and the dotted line represents the cavity saturation gains at the respective wavelengths. When there is an input signal with optical intensity above mode competition threshold, the gain is depleted by the signal thus the signal mode overwhelms the clamp mode λ C . As shown by the dotted line, λ S  saturates the gain of the VCSOA. At λ C , gain is less than the cavity loss. Thus, no lasing occurs at λ C  in the VCSOA, and the VCSOA outputs amplified signal logic “1”. 
         [0033]      FIG. 4  depicts a line graph of signal gain as a function of input signal intensity (signal logic “0” and logic “1”) according to an embodiment of the invention. The graph of  FIG. 4  illustrates that the competition between the two modes results in non-linear gain profile over input signal intensity with regard to signal logic “0” and logic “1”. The gain is graphed on the Y-axis, and input intensity is on the X-axis. The output gain will initially be flat and very low, which represents the logic “0.” As the input signal intensity approaches the threshold, the gain jumps up into a high level, representing logic “1.” After crossing the threshold, the gain flattens again representing a constant high gain, signifying logic “1.” In one embodiment, the threshold is adjusted by the reflectivities of the DBRs for the two modes and the pump level. The pump intensity is optimized according to the input intensity of the signal and the geometry of the cavity and structures. Thus, the transition between the logic “0” and logic “1” will occur at the desired point, and the optical signal pulse is reshaped. 
         [0034]    In one embodiment, the reflectivities of either the aforementioned DBR or DFB layer for the offset wavelength is higher than the input signal wavelength which results in a higher cavity loss for the signal wavelength (signal mode) than the offset wavelength (clamp mode) to implement non-linear amplification of input signal (λs) by means of competition between the two modes. Thus, the DBR or DFR obtains higher in-cavity optical resonating intensity for the clamp mode. The DBR or DFB clamps the gain medium layer of the SOA working in deep saturation condition and has higher response speed (higher data rate of the optical signal to be reamplified and reshaped). In one embodiment, the “smallest” loss design for the clamp mode and the high intensity input for optical signal “1” result in faster response. Thus, the design allows higher data rate input optical signal to be reamplified and reshaped by the VCSOA. The SOA device is activated by choosing a pumping level above clamp mode lasing threshold and under signal mode lasing threshold. 
         [0035]      FIG. 5  depicts a block diagram of a semiconductor optical amplifier pulse reshaper  500  according to an embodiment of the invention. The embodiment of  FIG. 5  depicts a module having four photodetectors  560 ,  520 ,  580 ,  547 , three taps  510 ,  570 ,  545 , a circulator  530 , a wavelength division multiplexer (WDM)  540 , a variable optical attenuator (VOA)  505 , a dual mode VCSOA with pump  550  and a controller  590 . 
         [0036]    An optical input signal  150  enters the pulse reshaper and travels to tap  510  where photo detector  520  obtains the power level of the optical input signal and transmits the characteristic data to the controller  590 . The circulator  530  circulates the input signal and passes the input signal through the WDM  540  and tap  545  into the dual mode VCSOA with pump  550 . The VCSOA  550  functions as described above. The output of the VCSOA contains two wavelengths λ S  and λ C , which enters the tap  545  with portion of the powers of the two wavelengths directed to the photo detector  547 . The photo detector  547  transmits the characteristics of the sum of the powers of the two wavelengths to the controller  590 . The output of the VCSOA then continues to the WDM  540  where the two wavelengths are separated onto two different paths. The WDM  540  directs optical signal λ C  to photo detector  560 . The power level characteristics of the optical signal λ C  are transmitted to controller  590 . The WDM  540  also directs the optical signal λ S  back to the circulator  530  where the optical signal is circulated to tap  570 . The tap  570  directs a part of the signal to photodetector  580  where the output signal power level characteristics is obtained and is sent to controller  590 . The controller, having the characteristics of the input signal, output signal, λ C  signal, and the sum of the powers of the two wavelengths from output of the VCSOA, analyzes the information and respectively adjust the pump of the VCSOA  550  and the VOA  505  in order to obtain the desired output gain profile. 
         [0037]    In one embodiment, if the fourth photodetector  547  obtains the sum of the powers of both the clamp mode output and the signal mode output as P0, and a signal is present at input port of the SOA pulse reshaper, then the input signal power is adjusted by the VOA. The adjustment to the VOA suppresses the clamp mode power level (which is obtained by photo detector  560 ). The adjustment to the VOA is P0/2 for non-return to zero data format and to d*P0/2 for return to zero data format, with insertion losses of the WDM and tap in the optical paths calibrated-out from the detected power levels, wherein “d” is the duty cycle of the return to zero data format. 
         [0038]    In one embodiment, the pulse reshaper is used in telecommunication equipment because it reamplifies and reshapes the optical pulses for both NRZ (non-return to zero) and RZ (return to zero) data format. 
         [0039]    While the foregoing is directed to various embodiments of the present invention, other and further embodiments of the invention may be devised without departing from the basic scope thereof. As such, the appropriate scope of the invention is to be determined according to the claims, which follow.