See discussions, stats, and author profiles for this publication at: https://www.researchgate.net/publication/232634140 Frequency Chirp Characteristics on WDM Direct Modulation Article · March 2010 DOI: 10.1109/ICCEA.2010.32 CITATIONS READS 3 260 1 author: Zaiton Abdul Mutalip Technical University of Malaysia Malacca 14 PUBLICATIONS 23 CITATIONS SEE PROFILE Some of the authors of this publication are also working on these related projects: fiber optic modulation View project All content following this page was uploaded by Zaiton Abdul Mutalip on 28 May 2014. The user has requested enhancement of the downloaded file. 2010 Second International Conference on Computer Engineering and Applications Frequency Chirp Characteristics on WDM Direct Modulation Zaiton Binti Abdul Mutalip Faculty of Electronics and Computer Engineering Universiti Teknikal Malaysia Melaka Malacca, Malaysia zaiton@utem.edu.my Abstract — The paper studies the characteristic of frequency chirp in optical communication network as well as the association of the chirp and BER intended for utilization of directly modulated wavelength division multiplexing (WDM). The research was made based on a simulation of a direct modulated link for different bit rates and fiber lengths to evaluate the effect of those parameters on frequency chirp. The result shows that the performance of the WDM direct modulation link is affected by the transmission bit rates and the distance. r = ER= INTRODUCTION Optical fiber communication provides tremendously high transmission capacity needed aligned with the development of FTTH which moving directly to the user. This need has leaded the research of transmitting high capacity of information in a longer distance. However transmission of shorter link can fully utilized the use of direct modulation DWM technique. In optical communication system, the modulation operation is the key functionality, where it converting the high bit rate electrical data signals into an optical carrier frequency. Thus, light modulation is one of the main issues in order to provide larger bandwidth over a longer distance transmission. Optical modulation is referred as the process of adding information to an optical signal carrier, which is transmitted by an optical source. There are two options for modulating an optical signal, which is through direct modulation and external modulation. [1][2]. The parameters which being modulated can either be the amplitude, frequency, phase and polarization. Thus, two types of optical modulation available, named: Analogue - AM, FM, PM and PoIM Digital - ASK, FSK, PSK, PoISK Figure 1. Appearance of chirp in signal [2] In optical modulation, ASK is the simplest and widely used method of modulating an optical signal. This ASK is also referred to as On-Off Keying (OOK) as the lasers used is turns on and off in order to transmit the “0” and “1” bits. Although it is the most preferable modulation methods, it is not perfectly accurate as the laser light is not totally turned off during the transmission of “0” bit. The quotient of “0” bit power over “1” bit power is called Extinction Ratio (ER) and is represented by Equation (1). [1][6][4] 978-0-7695-3982-9/10 $26.00 © 2010 IEEE DOI 10.1109/ICCEA.2010.32 (1) As the laser is turned off and on, a chirp appears when the current represents the “0” bit (I0) is smaller than the current for the laser to works linearly (Ith) as in Fig. 1. Chirp is described as an incident which forces the transmitted spectrum to broaden due to variations of the carrier frequency with time, as in Fig. 2. The appearance of chirp limits the transmission distances and bit rates. [6][2] Keywords- chirp, direct modulation I. P0 <1 P1 Figure 2. Chirp effect [2] 125 The appearance of chirp in directly modulated link normally is considered as the limiting factor for high speed transmission where at higher bit rates, it leads to a broadening linewidth and thus limiting the transmission distance. However the simplicity of direct modulation technique is an advantage that can be manipulated in transmission of high speed capacity at shorter range [7]. output is connected to an optical attenuator, which its output is then feed to an optical receiver (PIN Photodiode). A data recovery module is connected at the end of the link, in order to observe and measure the quality of the link through its eye diagram and bit-error rate (BER) characteristics. The binary signal input of the data recovery module is connected to the PRBS output and the electrical signal input is connected to the sequence generator. This is to enable the data recovery module to compare the transmitted and received signal for BER analysis. The optical power meter is connected to the attenuator output to measure the received optical power (known as sensitivity as BER = 10-9). An optical spectrum analyzer (OSA) and optical time domain visualizer (OTDV) were also connected to the laser output to observe the emitted optical signal. As direct modulation is the simplest and cost-effective and widely used modulation category in optical communication system. In this modulation technique, the light is modulated inside the light source. Unfortunately, due to the physics of laser action and finite response of lasing levels, the light output in direct modulation could not immediately response to the input electrical signal. Furthermore, the delays in turning on-off laser source occur, similar as ASK method discussed earlier. As a result, several undesirable effects such as chirping and pulse width broadening occur. The process of turning on and off cycle of the laser source makes the output spectrum and wavelength changed over time. The pulse width broadening results from the process of measuring the time-integrated optical spectrum. Since the spectral width of the light source varies quickly over time, a measurement of the optical spectrum over a time interval which is long compared to the instantaneous frequency changes results in broadening the spectral width. Although this unwanted effects become more obvious in multigigabit-per-second speeds of transmission but it still can be useful in short range transmission. [1][2][5]. II. OBJECTIVES In this paper, a simulation approach is used to determine the channel capacity in the presence of frequency chirping. The aim of this research is to investigate how chirp effect directly modulated link and how it can be limited in order to make full use of the advantage of direct modulation WDM technique. Thus, three objectives has been outlined as (1) find out the receiver sensitivity, (2) investigate observe the effect of varying the bit rates on the transmitted signal, and (3) investigate the effect of varying the fiber length on the transmitted signal. III. Figure 3. Direct modulation set up B. Experimental The simulation is been conducted in three different setting. The first setting is to investigate the receiver sensitivity. The optical attenuator value in the simulation set up is varied to obtain the BER of 10-9. Second setting is to investigate the effect of chip as the bit rates is varied. In this part, the bit rate of the laser modulating data is increased in order to identify the maximum modulating bit rate for a realistic degradation in BER due to chirp. The optical time domain visualiser is used to measure the amount of chirp in the optical modulated signal. The maximum chirp is measured and recorded in Table 1. The next step is to decrease the attenuation value by 3dB to 29.8dB and the bit rate is increased by 1 Gbit/s steps. This procedure is repeated until the BER reached 10-9 again. Last setup is used to investigate the effect of increasing the fiber length as the chirp contributes to signal spectrum broadening and chromatic dispersion will limits the distance of the transmission. The first step is to set the simulation bit rates and attenuation to its initial condition (2.5 Gbit/s and SIMULATION A. Simulation Set up The simulation setup is based on Fig. 3, performed with Optiwave simulation software. In this setup the Distributed Feedback Laser (DFB) operating at 1550nm is used. A Non Return Zero (NRZ) pulse generator which operates as a laser driver is modulated by a pseudo-random bit sequence (PRBS) generator. The output of the NRZ generator is connected to a low-pass filter which limits the bandwidth to 0.75*bit rate before applying the filter output to the bias input of the bias input of the DFB laser. The laser is then been connected to the single mode fiber (SMF). The fiber 126 32.8 dB respectively). The length is set to 40km and simulation is repeated by varying the attenuation value in order to achieve the BER of 10-9. The procedure is repeated by increasing the fiber length by the step of 20km. IV. diagrams for various but rates. The power at the receiver does not give any impact on the changes of bit rate. The value of the attenuation is decreased by 3 dB to allow for loss in signal strength or light power that occurs as light pulses propagate through the fiber. Thus, by using approximately -26.9 dB receiver sensitivity, only 4.95 Gbit/s signal can be transmitted in order to have minimum error (BER 10-9 in this case). Unfortunately, the amount of chirp detected is too high. RESULT AND DISCUSSION The results for the simulation are as discussed as follows: A. Receiver Sensitivity The attenuation value used to obtain minimum BER of 10-9 is 32.8 dB. The power measured at the optical receiver at this BER is known the sensitivity. This is the minimum power at the receiver in order to have an error free transmission. The sensitivity measured is -29.907 dBm. The resulting eye diagram is as Fig. 4. 2.50 Gbps 3.50 Gbps 4.50 Gbps 5.00 Gbps 5.30 Gbps 5.50 Gbps Figure 4. Eye diagram at BER of 10-9 B. Chirp versus Bit Rates TABLE I. Figure 5. Eye diagram for various bit rates CHIRP VERSUS BIT RATE MEASUREMENT Fibre length = 20 km C. Chirp versus Fiber Length From the results in Table II and the eye diagram on Fig. 6, it shows that as the fiber length is increased, the attenuation and receiver sensitivity is decreased. This finding proved that the attenuation limits the transmission distance. The power penalty is the difference in receiver sensitivity in dB, used to measure signal degradations. Higher receiver input power were required as the quality of the signal degraded. Bit Rate (Gbit/s) Attenuation 32.8dB Attenuation 29.8 dB Bit rate (Gb/s) 2.50 3.50 4.50 4.95 5.00 5.30 5.50 Sensitivity (dBm) -29.9 26.9 26.9 26.9 26.9 26.9 26.9 Chirp (GHz) 36 70 96 74 70 162 150 1.4*10-9 4.7* 10-21 5.3* 10-18 1.8* 10-9 1.8* 10-8 1.2* 10-5 1.0* 10-4 BER From Table I, it can be concluded that the amount of chirp measured is increased as the bit rate is increase with the same receiver sensitivity. Figure 5. shows the eye 127 TABLE II. CHIRP VERSUS FIBER LENGTH MEASUREMENT V. The completion of the simulation experiment enables detail investigation on the influence of chirp in WDM direct modulation. Generally, it was proven the frequency chirp affected both the transmission bit rates and distance. With the presence of frequency chirp, the best transmission bit rates is 5.00 Gbits/s. For longer transmission distance, the bit rates must be reduced for better performances. Therefore, it is useful to know the transmission bit rates and the distance before selecting the modulation technique going to be used. Bit Rate = 2.5 Gbit/s BER = 10-9 Fiber Length (km) Attenuation (dB) Sensitivity (dBm) 20 32.8 -29.907 40 28.5 -29.607 0.3 60 23.2 -28.307 1.6 80 18.3 -27.407 2.5 100 12.5 -25.607 4.3 120 1 -18.107 11.8 20 km CONCLUSION Penalty (dB) ACKNOWLEDGMENT To every special people at Universiti Teknikal Malaysia Melaka (UTeM) who provided necessity, fund and enthusiastic assistance, thank you. 40 km REFERENCES [1] 60 km 80 km [2] [3] [4] [5] 100 km 120 km [6] [7] Figure 6. Eye diagram for various transmission distance 128 View publication stats Breed, G. (2007, May). A Tutorial to Optical Modulation Techniques. High Frequency Electronics Magazine . Optical Society of America, Fiber Optics Handbook: Fiber, Devices, and Systems for Optical Communications, McGraw-Hill Professional, 2001 Green, P. (1994). Fiber Optic Networks. New Jersey: Prentice Hall. R. 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