Abstract:
Filter-free wavelength converters for separating and rejecting an optical input signal. A first input port couples a continuous wave (CW) light. A second input port couples an optical input signal. A multimode interference semiconductor optical amplifier (MMI-SOA) determines the output port with the input port and intensity-modulation of the CW light with the optical input signal. A first output port guides the converted signal, and a second output port guides the optical input signal.

Description:
BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     The invention concerns the field of integrated optics and fiber optic telecommunications and in particular filter-free wavelength converters for rejecting the optical input signal and guiding only the converted signal to the output of the converter. 
     Operation basis of wavelength conversion are cross gain modulation (XGM) or cross phase modulation (XPM) in semiconductor optical amplifiers (SOAs). 
     XGM is the method that is intensity-modulated a continuous wave (CW) light by gain-modulation with the intensity-modulated optical input signal in the SOA. As the intensity of the optical input signal increases, the gain is decreased and the intensity of the CW light also decreases. As the intensity of the optical input signal decreases, the gain increases and the intensity of the CW light also increases. Therefore, the information in the optical input signals can be transmitted to the required wavelength by using the CW light. 
     XPM method provides the phase modulation of the CW light with the optical input signal in the SOA. When the CW light propagates into the two paths, the path difference occurs due to refractive index change in the SOAs. The combination of two paths of propagated CW light cause the interference and the intensity of the CW light is modulated. 
     Wavelength converters can be operated in two ways in accordance with the input method of the optical input signal and the CW light. 
     First, the CW light and the optical input signal are launched in opposite directions each other. This method has an advantage that no filter is required to reject the optical input signal at the output of the converter. However, at both ends of the SOA, the recombination rate also decreases due to the carrier depletion, so that the conversion speed is degraded. Therefore, the waveform is seriously distorted and the conversion speed thereof decreases. 
     Second, the CW light and the optical input signal are coupled in the same direction for high-speed conversion. However, the filter is required in order to reject the optical input signal at the output of the converter or to output only the converted signal. This method provides conversion to the same wavelength. 
     Therefore, in the above-mentioned wavelength converter, it is necessary to use the CW light and the optical input signal in the same direction in order to improve the conversion speed. Thus, in order to simplify the configuration of the optical transmission system including wavelength converters, the function capable of separating or removing the optical input signal should be included. 
     2. Description of the Prior Art 
     Hereinafter, the embodiments of the configurations of wavelength converters will be explained with reference to the accompanying figures. 
       FIG. 1  shows a configuration of the multi-mode interference (MMI) mode converter. The MMI mode converter can separate a fundamental and a higher-order mode. (See U.S. Pat. No. 5,933,554, 1999. 8. 3) In this interferometer, because an output port is determined depending on the input port, the converted signal and the optical input signal can be separated. (See “Detailed experiment investigation of all active dual-order mode Mach-Zehnder wavelength converter”, Electron. Letters, Vol. 36, No. 15) 
     The operating principle of the MMI mode converter is as follows. The optical input signal  1  is injected into the input port  3  of a first MMI coupler  5  and it is propagated to the first SOA  7 . The signal induces phase modulation of the CW light  2  and the signal  1  is absorbed in the ports  11 ,  12  of a second MMI coupler  9 . The CW light is injected into the central input port  4  and it is divided into the first MMI coupler  5  and the third MMI coupler  6 . The CW light  2  is phase-modulated in the first SOA  7  and amplified in the second SOA  8 . Thereafter, it is divided into the second MMI coupler  9  and the fourth MMI coupler  10 . Then, the two paths of light are combined in the output port  13  and only the converted signal is yielded by constructive or destructive interference. 
       FIG. 2  shows the conventional XGM method, and in this method, the SOAs  24 ,  25  are parallel connected to the input and output ports of the MMI couplers  23 ,  27 . The optical output signal  29  and the converted signal  26  are separated. (See “Monolithic Integrated Parallel Amplifier Structure for Filter-Free Wavelength Conversion”, 13 th  IPRM, 2001 International Conference on Indium Phosphide and Related Materials, Conference Proceedings FB1-5). In this structure, the injection currents into both of the SOAs  24 ,  25  are same. XGM occurs between the optical input signal  22  and CW light  21  in the SOAs  24 ,  25 . Therefore, wavelength conversion is performed. In cross state, the signal and CW lights are led to different output ports when they are coupled into the different input ports, which enables the spatial separation of the input signal and CW light, resulting in filter-free wavelength conversion. 
     The structure using the MMI mode converter of  FIG. 1  can separate the converted signal  26  and optical output signal  29 . However, the MMI coupler having multiple stages has a limitation that the employed structure is complicated. Also, there exists a problem that the performance of the wavelength converter depends on that of the MMI couplers. The structure of  FIG. 2  can separate the converted signal and optical output signal. However, the MMI coupler and the SOA should be integrated so that the structure thereof is more complicated. 
     SUMMARY OF THE INVENTION 
     Therefore, the object of the invention is to provide the simplified wavelength converter for separating and rejecting the optical input signal using multimode interference semiconductor optical amplifiers (MMI-SOAs). MMI-SOAs causes XGM and XPM and determines the output ports depending on the input ports in order to simplify the structure of the wavelength converter. 
     To achieve the above object, the invention provides an XGM based filter-free wavelength converter, which separates the optical input signal and converted signal. This consists of a first input port for coupling the CW light, a second input port for launching the optical input signal, an MMI-SOA for determining the output port depending on the input port and for modulating the CW light, a first output port for guiding the converted signal, and a second output port for transmitting the optical input signal. 
     Also, to achieve the above object, the invention provides an XPM based filter-free wavelength converter, which separates the converted signal and the optical input signals. In this configuration, the optical input signal causes phase modulation of the CW light in the MMI-SOA. This consists of an optical divider for dividing the CW light, a first MMI-SOA for occurring the phase modulation of the CW light by the optical input signal and for separating the CW light and optical input signal, a second MMI-SOA for amplifying the CW light, an optical combiner for combining the CW lights from the first and second MMI-SOA, a first output port for guiding the converted signal, and a second output port for separating the optical input signal. 
    
    
     
       BRIEF DESCRIPTION OF THE ATTACHED DRAWINGS 
         FIG. 1  shows a structure of a filter-free wavelength converter using the conventional XGM. 
         FIG. 2  shows a structure of a filter-free wavelength converter using the conventional XPM. 
         FIG. 3  shows a structure of an XGM based filter-free wavelength converter comprised of MMI-SOA in accordance with the present invention. 
         FIG. 4  shows a structure of an XPM based filter-free wavelength converter comprised of MMI-SOAs in accordance with the present invention. 
         FIG. 5  shows a spectrum for measuring transparency of MMI-SOAs of FIG.  3   
     
    
    
     DESCRIPTION OF THE PREFERRED EMBODIMENT 
     The wavelength converter according to the present invention is implemented in two types below. 
     First, the XGM based filter-free wavelength converter shown in  FIG. 3 , comprises a first input port for launching the CW light, a second input port for coupling the optical input signal, an MMI-SOA for determining the output port depending on the input port, a first output port for guiding the converted signal, and a second output port for transmitting the optical input signal. The optical input signal causes the gain modulation in the MMI-SOA so that the CW light is intensity-modulated. At this time, if the CW light and the optical input signal are injected into the different input ports each other, they are also guided to the different output ports, so that the optical input signal and the converted signal are separated. 
     The input ports and output ports may be consisted of passive or active waveguides. The second output port may be consisted of an optical absorber. 
     Second, the XPM based filter-free wavelength converter shown in  FIG. 4  comprises a first input port for coupling the CW light, a second input port for injecting the optical input signal, a first MMI-SOA for providing XPM, a second MMI-SOA for amplifying the CW light, an optical divider for dividing the CW light into the two paths, an optical combiner for combining the CW lights from the two MMI-SOAs, a first output port for guiding the converted signal, and a second output port for transmitting the optical input signal. The refractive index of the first MMI-SOA is changed due to the carrier density change with the optical input signal, so that the phase of the CW light is also changed. The converted signal is then generated due to constructive or destructive interference depending on the phase shift through the MMI-SOAs. The optical input signal from the second output port of the first MMI-SOA is separated from the converted signal. 
     The optical divider and optical combiner may be consisted of passive or active waveguides. The second output port may be consisted of an optical absorber. 
     Hereinafter, the embodiments of the present invention will be explained with reference to the accompanying drawings. 
       FIG. 3  shows the XGM based filter-free wavelength converter according to the invention. The optical input signal  32  is launched into the MMI-SOA  31  through the input port  34  and propagated to the output port  36 . The CW light  33  is coupled into the MMI-SOA  31  through the input port  35  and propagated into the output port  37 . 
     The operating principle of this structure is as follows. The gain of the MMI-SOA  31  is modulated with the optical input signal  32 . The intensity of the CW light  33  is modulated with the gain modulation. Therefore, the information of the optical input signal  32  is transmitted to the CW light  33 , resulting in wavelength conversion from the wavelength of the optical input signal to the wavelength of the CW light. Also, the optical output signal  38  is propagated to the output port  36  and the converted signal  39  is guided to the output port  37 , thereby the two signals are separated each other. 
       FIG. 4  shows the XPM based filter-free wavelength converter of the present invention. The optical input signal  41  is coupled into the MMI-SOA  45  through the input port  43  and guided to the output port  47 . The CW light  42  is injected into the input port  44  and divided into the first MMI-SOA  45  and the second MMI-SOA  46 . Thereafter, the CW lights in two paths are combined again and emerged from the output port  48 . 
     The operating principle of this structure is as follows. The optical input signal  41  induces a change in refractive index due to the change in carrier density of the MMI-SOA  45 . At this time, the phase of the CW light  42  is modulated with the change in the refractive index. Then, the optical input signal  41  is combined with the CW light  42  and is subject to the interference. Therefore, the converted signal with the phase shift in the MMI-SOA  45  is generated from the output port  48 . Also, the converted signal is separated from the optical input signal  49  and propagated to the output port  47  of the MMI-SOA  45 . 
       FIG. 5  shows a spectrum for measuring transparency of an exemplary optical amplifying converter according to an embodiment of the invention. The MMI-SOA is designed to guide an optical input signal  32  from the input port  34  to the output port  37 . To ensure the separation of the output signals, the optical powers in the output port  36  and output port  37  are measured with a spectrometer while the optical input signal  32  is coupled. The measured input signal rejection ratio is about 20 dB as shown in FIG.  5 . It means that the filter-free converter can be implemented using MMI-SOAs. 
     The wavelength converter of the invention does not require the optical filter for removing the optical input signal at the output, because the wavelength conversion is implemented while the converted signal is separated from the optical input signal. 
     Especially, owing to filter-free wavelength conversion, the use of a tunable light source is available so that the configuration of the wavelength division multiplexed (WDM) network system can be small-sized and variably employed, thereby the performance and the capacity of optical communication system can be improved. 
     Although the invention has been described in conjunction with the preferred embodiment, it is not limited to the embodiments, and it will be apparent to those skilled in the art that it can be modified in variation within the scope of the invention