Abstract:
There are provided a method and system for monitoring an optical transmission line. The system for monitoring the optical transmission line includes: an OTDR (optical time-domain reflectometer) transmitting a monitoring light to an optical transmission line, measuring a reflected light or backscattered light to monitor the optical transmission line; an optical amplification unit amplifying the monitoring light transmitted on the optical transmission line by using a gain clamped optical amplifier; and a filter unit removing a component having a wavelength outside a wavelength band of the monitoring light from a backward ASE (amplified spontaneous emission) generated by the optical amplification unit. Accordingly, it is possible to extend an optical transmission line monitoring distance of the OTDR. As a result, it is possible to prevent deterioration of the performance of the OTDR because of the backward ASE.

Description:
This application claims the priority of Korean Patent Application No. 2004-39985, filed on Jun. 2, 2004, in the Korean Intellectual Property Office, the disclosure of which is incorporated herein in its entirety by reference. 
     BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     The present invention relates to a method and system for monitoring an optical transmission line, and more particularly, to a method and system for monitoring an optical transmission line by using an optical time-domain reflectometer (OTDR) and an optical amplifier. 
     2. Description of Related Art 
     The optical time domain reflectometry (OTDR) is very convenient to monitor WDM transmission links. In order to solve problems in the transmission line quickly and further to prevent potential problems, online monitoring at a central office is necessary. However, the monitoring distance with a typical OTDR is limited to about 160 km of optical fiber because of the dynamic range of avalanche photo diode (˜35 dB). To further extend the monitoring length, amplified OTDR systems using optical amplifiers have been investigated, and then, the defective positions of the optical transmission line and the loss of transmission measured by the OTDR are used to improve reliability of an optical transmission system. 
     Typically, amplification of the monitoring light of the OTDR results in backward amplified spontaneous emission (ASE), which is generated by the optical amplifier. In turn, the ASE may deteriorate performance of the OTDR. In an optical transmission line monitoring system with multiple amplification stages, the performance of the OTDR may be greatly deteriorated because of ASE components outside a wavelength band of the monitoring light. Therefore, it is necessary to remove the ASE components outside a wavelength band of the monitoring light. 
     Since the monitoring light of the OTDR is a pulsed light, a signal input to the optical amplifier is periodically in on and off states. When the input signal of the optical amplifier is in the off state, the ASE from optical amplifier greatly increases. Therefore, there is a difference in the power of ASE between the on and off states of the input signal. If a pumping operation for increasing gain of the optical amplifier is intensively performed, the difference in the ASE may be further enlarged. Since the ASE generated in the off state of the input signal becomes a background noise, the operating characteristics of photo diodes in the receiver of the OTDR may be deteriorated. In addition, results of monitoring will be distorted 
       FIG. 1  is a graph showing optical spectra of outputs of an optical amplifier with or without a signal 
     The ASE without a signal is larger than that with a signal. Because of the difference in the ASE, the performance of the OTDR will be deteriorated. 
     SUMMARY OF THE INVENTION 
     The present invention provides an optical transmission line monitoring system using an optical amplifier and an OTDR (optical time-domain reflectometer) capable of monitoring a long optical transmission line, preventing deterioration of performance of the OTDR because of a backward ASE (amplified spontaneous emission) generated by the optical amplifier, and simultaneously performing signal transmission and optical transmission line monitoring. 
     According to an aspect of the present invention, there is provided an optical transmission line monitoring system comprising: an OTDR (optical time-domain reflectometer) transmitting a monitoring light to an optical transmission line, measuring a reflected light or backscattered light to monitor the optical transmission line; an optical amplification unit amplifying the monitoring light transmitted on the optical transmission line by using a gain clamped optical amplifier; and a filter unit removing a component having a wavelength outside a wavelength band of the monitoring light from a backward ASE (amplified spontaneous emission) generated by the optical amplification unit. 
     According to another aspect of the present invention, there is provided a method of monitoring an optical transmission line, comprising: transmitting an monitoring light on the optical transmission line; amplifying the monitoring light by using a gain clamped optical amplifier and maintaining an power of a backward ASE (amplified spontaneous emission) constant regardless of an power of the monitoring light; removing ASE outside a wavelength band of the monitoring light; and monitoring the optical transmission line by measuring intensities of reflected light or backscattered light generated from the monitoring light. 
     Accordingly, it is possible to extend an optical transmission line monitoring distance of the OTDR. As a result, it is possible to prevent deterioration of the performance of the OTDR because of the backward ASE. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       The above and other features and advantages of the present invention will become more apparent by describing in detail exemplary embodiments thereof with reference to the attached drawings in which: 
         FIG. 1  is a graph showing optical spectra of outputs of an optical amplifier in the on and off states of an input signal; 
         FIG. 2  is a graph showing optical spectra of outputs of a gain clamped optical amplifier in the on and off states of an input signal; 
         FIGS. 3   a  and  3   b  are view showing a structure of a gain clamped semiconductor optical amplifier using Bragg gratings; 
         FIG. 4  is a view showing a gain clamped optical amplifier in which a laser cavity provided outside a semiconductor optical amplifier; 
         FIG. 5  is a gain characteristic of a gain clamped optical amplifier; 
         FIG. 6  is a view showing an optical transmission line monitoring system according to an example of the present invention; 
         FIG. 7  is a graph showing a monitoring result of the optical transmission line monitoring system of  FIG. 6 ; 
         FIG. 8  is a view showing an optical transmission line monitoring system according to another example of the present invention; 
         FIG. 9  is a view showing an optical transmission line monitoring system using an optical amplifier for data signal on an optical transmission line according to an example of the present invention; 
         FIG. 10  is a view showing a gain clamped optical amplifier using a gain-saturated signal; and 
         FIG. 11  is a view showing a gain clamped optical amplifier using an optical grating. 
     
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     The present invention and operational advantages thereof can be fully understood by referring to the accompanying drawings and explanations thereof. 
     Now, exemplary embodiments of the present invention will be described with reference to the accompanying drawings to explain the present invention in detail. In the drawings, the same reference numerals indicate the same elements. 
     Now, an optical transmission line monitoring system using a gain clamped optical amplifier according to the present invention will be described with reference to the drawings. 
       FIG. 2  is a graph showing optical spectra of outputs of a gain clamped optical amplifier in the on and off states of an input signal; 
     As shown in  FIG. 2 , a power of an amplified spontaneous emission (ASE) does not change regardless of the on and off states of a signal within a predetermined signal wavelength band. 
       FIG. 3A ,  3 B, and  4  are views showing examples of a gain clamped optical amplifier. 
       FIGS. 3A and 3B  are view showing structures of gain clamped semiconductor optical amplifiers using Bragg gratings.  FIG. 3A  shows a gain clamped semiconductor optical amplifier having Bragg gratings at both ends of a semiconductor chip (an active section), which is called a “distributed Bragg reflector (DBR) type.”  FIG. 3B  shows a gain clamped optical amplifier having a Bragg grating under a waveguide an active region, which is called a “distributed feedback (DFB) type.” 
     More specifically, the SOA comprises the structure of a laser cavity in the optical waveguide, which a gain medium. The structure of the laser cavity is formed with Bragg gratings reflecting light in a predetermined narrow wavelength band. The laser oscillating in the laser cavity is used to saturate gain of the SOA. If the power of the input of the SOA is low, the power of the laser increases so that the gain of the SOA is saturated. If the power of the input of the SOA is high, the power of the laser decreases. But, since the power of the input is high, the gain the SOA is saturated. Therefore, the gain of the gain clamped SOA can be saturated regardless of the power of the input of the SOA, so that a constant signal gain can be obtained. In addition, since the SOA is always in a gain saturated state, the power of the ASE can be kept constant. 
       FIG. 4  is a view showing a gain clamped optical amplifier in which a laser cavity provided outside a semiconductor optical amplifier; there are provided two optical add-drop multiplexers (OADMs). A second OADM connected to the output of the SOA has three terminals A, B, and C. Having a predetermined wavelength, a portion of light input to the terminal A is output from the terminal C. The power of the light having the predetermined wavelength output from the terminal C is adjusted by a variable optical attenuator (VOA) and input to the SOA through a first OADM. In one cycle, the light output from the terminal C of the second OADM is amplified the SOA, and then, input to the terminal A of the second OADM. This cycle is repeated to generate resonance. The laser having this cavity structure is called a ring laser. 
       FIG. 5  is a gain characteristic curve of a gain clamped optical amplifier. As shown in  FIG. 5 , it can be seen that, since the SOA is kept in a constant gain saturated state, the gain is constant regardless of the power of the input signal. 
       FIG. 6  is a view showing an optical transmission line monitoring system according to an example of the present invention. 
     The optical transmission line monitoring system comprises an OTDR (optical time-domain reflectometer)  600 , optical transmission lines  610  and  640 , an optical filter  620 , and a gain clamped optical amplifier  630 . 
     A monitoring light input to the optical transmission line  610  is reflected or back-scattered. The OTDR  600  measures the reflected or back-scattered light to determine loss of transmission of the optical transmission line  610 , connection points, disconnection points, and so on. The monitoring light of the OTDR  600  is a periodical pulsed light. Since there are limitations on the output power of the monitoring light and the dynamic range of a photo diode in the receiver of the OTDR  600 , only a single OTDR  600  can not monitor over 150 km of the optical transmission line. 
     In order to extend the monitoring distance of the OTDR  600 , the gain clamped optical amplifier  630  amplifies the monitoring light (the pulsed light) of the OTDR  600 . Since the gain clamped optical amplifier  630  has a constant gain regardless of the power of the input signal thereof, the power of the ASE is constantly regardless of the power of the monitoring light. 
     Now, the gain clamped optical amplifier will be described in detail with reference to  FIGS. 2 to 5 . 
     The optical filter  620  used between the OTDR  600  and the gain clamped semiconductor optical amplifier  630  has a function of removing components outside a wavelength band of the monitoring light from the backward ASE generated by the gain clamped optical amplifier  630 . 
     The power of the ASE can be kept constant by the gain clamped optical amplifier  630  regardless of the on and off state of the monitoring light (a pulsed light). The components outside the wavelength band of the monitoring light can be removed from the backward ASE by the optical filter  620 . As a result, it is possible to prevent deterioration of the performance of the OTDR because of the ASE. 
       FIG. 7  is a graph showing a monitoring result of the optical transmission line monitoring system of  FIG. 6 . As the monitoring light proceeds along the optical transmission line, the power of the monitoring light is gradually reduced. Next, the monitoring light is amplified by the optical amplifier at about 100 km. Therefore, it is possible to extend the monitoring distance of the OTDR. 
     As seen in  FIG. 7 , it can be understood that the monitoring distance of the OTDR extends over 200 km. 
       FIG. 8  is a view showing an optical transmission line monitoring system according to another example of the present invention. 
     The optical transmission line monitoring system comprises an OTDR  800 , optical transmission lines  810  and  850 , a circulator  820 , an optical fiber grating  830 , and a gain clamped optical amplifier  840 . 
     The constructions and functions of the OTDR  800 , the gain clamped optical amplifier  840 , and the optical transmission lines  810  and  850  are the same as those of  FIG. 6 . Therefore, the detailed description is omitted. 
     Light transmitted on the optical transmission line  810  is input to the gain clamped optical amplifier  840  though the circulator  820 . A light backwardly output from the gain clamped optical amplifier  840  is input to the optical fiber grating  830  though the circulator  820 . A light reflected on the optical fiber grating  830  is input to the optical transmission line  810  through the circulator  820 . 
     The optical fiber grating  830  reflects only the components within the wavelength band of the backward monitoring light which is amplified by the gain clamped optical amplifier  840 . In other words, the circulator  820  and the optical fiber grating  830  of  FIG. 8  collectively correspond to the optical filter of  FIG. 6 . 
       FIG. 9  is a view showing an optical transmission line monitoring system using an optical amplifier for data signal on an optical transmission line according to an example of the present invention; 
     The optical transmission line monitoring system comprises an OTDR  900 , optical transmission lines  910  and  960 , a first coupler  920 , a gain clamped optical amplifier  940 , a second coupler  950 , and an optical amplifier  930 . The gain clamped optical amplifier  940  amplifies the monitoring light. The optical amplifier  930  amplifies the data signal. 
     The OTDR  900  and the gain clamped optical amplifier  940  are the same as those of  FIG. 6 . Therefore, detailed description is omitted. 
     The first coupler  920  used in front of the optical amplifier  930  demultiplexes both data signal and monitoring light output from the OTDR  900 . The first coupler  920  transmits the data signal and the monitoring light to the optical amplifier  930  and the gain clamped optical amplifier  940 , respectively. 
     The optical amplifier  930  and the gain clamped optical amplifier  940  amplify the data signal and the monitoring light, respectively. The second coupler  950  multiplexes the data signal from the optical amplifier  930  and the monitoring light from the gain clamped optical amplifier  940  and outputs the combined light to the optical transmission line  960 . 
     The backscattered monitoring light or the reflected monitoring light is backwardly input to the gain clamped optical amplifier  940  through the second coupler  950 . 
       FIG. 10  is a view showing an example of a gain clamped optical amplifier using a gain-saturated signal. 
     The gain clamped optical amplifier comprises a light source  1020  generating the gain-saturated signal, an optical amplifier  1030 , and a coupler  1010  inputting the gain-saturated signal to the optical amplifier  1030 . 
     The gain-saturated signal generated by the light source  1020  is input to the optical amplifier  1030  through the coupler  1010 . Here, the gain-saturated signal has enough high power to uniformly saturate the gain of the optical amplifier  1030  regardless of the monitoring light. Therefore, it is possible to obtain a constant signal gain at any time. 
       FIG. 11  is a view showing another example of a gain clamped optical amplifier using an optical grating. 
     The gain clamped optical amplifier comprises an optical fiber grating  1110  and an optical amplifier  1120 . The optical fiber grating  1110  has a function of reflecting a portion of ASE generated by the optical amplifier  1120  to the optical amplifier  1120 . The reflected portion of ASE is contributed to saturate the gain of the optical amplifier  1120 , so that the signal gain can be constant. 
     The reflection wavelength band of the optical fiber grating  1110  is empirically determined. Wider reflection wavelength band is preferable because sufficient reflected light has to be input to the optical amplifier  1120  in order to saturate the gain of the optical amplifier  1120 . 
     Since the light source and the coupler of  FIG. 10  can be replaced with a single optical grating, it is possible to implement a low-price gain clamped optical amplifier. 
     According to the present invention, in case of extending an optical transmission line monitoring distance of an optical time-domain reflectometer (OTDR) by using an optical amplifier, it is possible to prevent deterioration of performance of the OTDR because of backward amplified spontaneous emission (ASE) generated from the optical amplifier. In addition, since a data signal and a monitoring light have different wavelengths, it is possible to monitor the optical transmission line in real time 
     In addition, the present invention can be adapted to an optical transmission line on which a optical amplifier. In addition, a long optical transmission line can be monitored by a gain clamped optical amplifier. Therefore, it is possible to reduce time and cost in monitoring the optical transmission line. 
     While the present invention has been particularly shown and described with reference to exemplary embodiments thereof, it will be understood by those of ordinary skill in the art that various changes in form and details may be made therein without departing from the spirit and scope of the present invention as defined by the following claims.