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2005 Conference on Lasers and Electro-Optics Europe Effects of assist light injection at gain transparency wavelength on transmission and performances of SOAs Mohammad Amaya', Ammar Sharaiha', Frederic Ginovarr, Thierry Rampone', Sylvain Five' and Afathilde Gay2 Laboratoire RESO (EA 3380), Ecole Nationale d7ngenieurs de Brest, Technopile Brest-Iroise, CS 73 862, 29238 BREST Cedex 3, France 2Laboratoire d 'Optronique CNRS-UMR FOTON 6082, ENSSA T, 6 rue de Kerampont, BP 447, 22305 Lannion, France [email protected] Semiconductor optical amplifiers (SOAs), which are all-optical multifunctional compact components, are likely to play an important role in tomorrow's metropolitan optical network applications. However, improving the SOAs characteristics is an essential issue to deal with the increased growth of data rates in high-speed all-optical systems. Several works have studied optical beam injection effects at gain transparency in SOAs [1-2]. In this work, we experiment with the injection effects of a continuous wave (CW) assist light into the SOA cavity at the gain transparency wavelength on transmission and SOA performances. Experimental results are carried out on a 500 1Lm long low-polarization-sensitive bulk SOA having a 10.6 dB fiber-to-fiber gain at a bias current of 120 mA. The assist light beam, which has an optical power of 19 dBm at wavelength 1480 nm, has been injected into the SOA in the counter-propagative direction with respect to an optical input signal injected at wavelength 1535 nm. 14I -+ [l tho at l;_ _i.cf _ght 1-02_ I E4)2 6)4 3.5dBB\ .- 0.941 / IE-O0t X 2- Ifithassist Gigl 0.92 | Withouto susstight | a li -h o II: With at'stst hghtI E)411it asis lgh 0 Z; + 90 . . _ . iE-12 -20 -15 -10 -5 0 5 10 0 200 400 h00 800 1000 12)0 1400 160Q1 -20 -2b -24 -22 -2)1 Optical output power [dBm] Time [ps] Optical input power Figure 1: SOA gain saturation curves Figure 2: Normalized gain recovery Figure 3: Bit error rate in absence and eye diagrams for PinsIg= -10 dBm. photo-detected response, AnSig= 1535 nm. and in presence ofthe assist light. Figure 1 shows the SOA gain saturation curves and eye diagrams obtained with and without the assist light. We notice that the SOA saturation output power is improved by 3.5 dB3 in presence of the assist light while maintaining the unsaturated gain. Furthermore, the eye diagrams of the optical output signal obtained for an optical input signal power of -10 dBm modulated at 2.5 GHz, show that the assist light suppresses the overshoot time which appears when no assist light is used. Pump-probe measurements have been performed to characterize the SOA gain recovery time. Here the pump is a 5 ps pulse of about 275 fJ with a repetition rate of 454 MHz at 1540 nm. The probe signal is generated by a tunable laser set at 1535 nm with a weak cw power (-12 dBm) in order to leave the SOA gain nearly unsaturated. A filter of 0.2 nm bandwidth is used at the SOA output to select the probe signal which is detected by a fast photodiode of 32 GHz bandwidth and then displayed on a 20 GHz bandwidth oscilloscope. Figure 2 illustrates the SOA gain recovery time evolution. The injection of an assist light power of 19 dBm reduces the gain recovery time to 400 ps, which is around 750 ps without any assist light. Indeed? the pump saturates the SOA gain and the assist light will be included in the absorption region. so its absorbed power decreases the carrier lifetime which speeds up the SOA gain recovery. In addition, to evaluate the transmission performnance in presence of the assist light, the optical input signal has been modulated by PRBS signal at 2.5 GHz with an extinction ratio of 12 dB and transmitted via the SOA. The Bit Error Rate (BER) has been measured in absence and in presence of the assist light and for weak optical input signal powers. Figure 3 points out that the presence of the assist light does impose any power penalty on the optical input signal. In conclusion, we have demonstrated that the injection of a CW assist light high power into the SOA cavity at the gain transparency wavelength improves the SOA saturation output power, accelerates the dynamic gain recovery time and reduces the optical signal waveform distortion. References: [1]. R. J. Manning and D. A. . Davies, Opt. Le94., Vol. 19, (1994) pp. 889-891. [2]. M. Amaya, A. Sharaiha, and T. Rampone, (JSMO03), SPIE Vo1. 5445, August 11-15, (2003), pp. 144 - 147. 0-7803-8974-3/05/$20.00 ©2005 IEEE 561

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Page 1: [IEEE CLEO/Europe. 2005 Conference on Lasers and Electro-Optics Europe, 2005. - Munich, Germany (12-17 June 2005)] CLEO/Europe. 2005 Conference on Lasers and Electro-Optics Europe,

2005 Conference on Lasers and Electro-Optics Europe

Effects of assist light injection at gain transparency wavelengthon transmission and performances of SOAs

MohammadAmaya', Ammar Sharaiha', Frederic Ginovarr, Thierry Rampone', Sylvain Five' and Afathilde Gay2Laboratoire RESO (EA 3380), Ecole Nationale d7ngenieurs de Brest,Technopile Brest-Iroise, CS 73 862, 29238 BREST Cedex 3, France

2Laboratoire d 'Optronique CNRS-UMR FOTON 6082,ENSSA T, 6 rue de Kerampont, BP 447, 22305 Lannion, France

[email protected]

Semiconductor optical amplifiers (SOAs), which are all-optical multifunctional compact components, arelikely to play an important role in tomorrow's metropolitan optical network applications. However, improving theSOAs characteristics is an essential issue to deal with the increased growth of data rates in high-speed all-opticalsystems. Several works have studied optical beam injection effects at gain transparency in SOAs [1-2]. In this work,we experiment with the injection effects of a continuous wave (CW) assist light into the SOA cavity at the gaintransparency wavelength on transmission and SOA performances. Experimental results are carried out on a 500 1Lmlong low-polarization-sensitive bulk SOA having a 10.6 dB fiber-to-fiber gain at a bias current of 120 mA. Theassist light beam, which has an optical power of 19 dBm at wavelength 1480 nm, has been injected into the SOA inthe counter-propagative direction with respect to an optical input signal injected at wavelength 1535 nm.

14I -+ [l tho atl;_ _i.cf _ght 1-02_ I E4)2

6)4 3.5dBB\ .- 0.941 / IE-O0t X

2-Ifithassist Gigl0.92 | Withouto susstight | a li-h

o II: With at'stst hghtIE)411itasis lgh

0 Z; + 90 . . _ . iE-12

-20-15 -10 -5 0 5 10 0 200 400 h00 800 1000 12)0 1400 160Q1 -20 -2b -24 -22-2)1

Optical output power [dBm] Time [ps] Optical input powerFigure 1: SOA gain saturation curves Figure 2: Normalized gain recovery Figure 3: Bit error rate in absenceand eye diagramsfor PinsIg= -10 dBm. photo-detected response, AnSig=1535 nm. and in presence ofthe assist light.

Figure 1 shows the SOA gain saturation curves and eye diagrams obtained with and without the assistlight. We notice that the SOA saturation output power is improved by 3.5 dB3 in presence of the assist light whilemaintaining the unsaturated gain. Furthermore, the eye diagrams of the optical output signal obtained for an opticalinput signal power of-10 dBm modulated at 2.5 GHz, show that the assist light suppresses the overshoot time whichappears when no assist light is used.

Pump-probe measurements have been performed to characterize the SOA gain recovery time. Here thepump is a 5 ps pulse of about 275 fJ with a repetition rate of 454 MHz at 1540 nm. The probe signal is generated bya tunable laser set at 1535 nm with a weak cw power (-12 dBm) in order to leave the SOA gain nearly unsaturated.A filter of 0.2 nm bandwidth is used at the SOA output to select the probe signal which is detected by a fastphotodiode of 32 GHz bandwidth and then displayed on a 20 GHz bandwidth oscilloscope. Figure 2 illustrates theSOA gain recovery time evolution. The injection of an assist light power of 19 dBm reduces the gain recovery timeto 400 ps, which is around 750 ps without any assist light. Indeed? the pump saturates the SOA gain and the assistlight will be included in the absorption region. so its absorbed power decreases the carrier lifetime which speeds upthe SOA gain recovery.

In addition, to evaluate the transmission performnance in presence of the assist light, the optical input signalhas been modulated by PRBS signal at 2.5 GHz with an extinction ratio of 12 dB and transmitted via the SOA. TheBit Error Rate (BER) has been measured in absence and in presence of the assist light and for weak optical inputsignal powers. Figure 3 points out that the presence of the assist light does impose any power penalty on the opticalinput signal.

In conclusion, we have demonstrated that the injection of a CW assist light high power into the SOA cavityat the gain transparency wavelength improves the SOA saturation output power, accelerates the dynamic gainrecovery time and reduces the optical signal waveform distortion.References:[1]. R. J. Manning and D. A. . Davies, Opt. Le94., Vol. 19, (1994) pp. 889-891.[2]. M. Amaya, A. Sharaiha, and T. Rampone, (JSMO03), SPIE Vo1. 5445, August 11-15, (2003), pp. 144 - 147.

0-7803-8974-3/05/$20.00 ©2005 IEEE 561