OWS6.pdf All-Optical DPSK Wavelength Converter Based on MZI with Integrated SOAs and Phase Shifters B. Sartorius (1), C. Bornholdt (1), J. Slovak (1), M. Schlak (1), Ch. Schmidt (1), A. Marculescu (2), P. Vorreau (2), S. Tsadka (3), W. Freude (2), J. Leuthold (2), 1: FhG - Heinrich-Hertz-Institut, Einsteinufer 37, 10587 Berlin, Germany, [email protected] 2: University of Karlsruhe, Institute ofHigh-Frequency and Quantum Electronics, D-76131 Karlsruhe 3 : Kailigth Photonics, I- 76124 Revhot, Israel Abstract: An integrated MZI-SOA device is developed for all-optical wavelength conversion of DPSK signals. The functionality is investigated close to 40 Gb/s and error free operation with less then 1 dB penalty is demonstrated. OCIS codes: (060.45 10) Optical communications, (130.3 120) Integrated optics devices Introduction Differential Phase Shift Keying (DPSK) is increasingly becoming the communication format of choice for future networks. DPSK offers improved sensitivity and robustness to nonlinear impairments [1], which makes it particularly attractive for ultra-long haul applications. To further reduce cost in long-haul transmission networks, transparent system approaches comprising reconfigurable optical add-drop multiplexers (ROADMs) are currently investigated. In transparent networks wavelength conversion turns out to be the key to overcome wavelength contention issues [2]. In this scenario all-optical conversion appears to be very advantageous - more then for conventional Amplitude Shift Keying (ASK) formats - since DPSK receivers and transmitters are very expensive and significantly more complex then the corresponding counterparts for ASK. All-optical solutions thus can promise high benefits - if they utilize compact devices and simple structures. In this paper we present a semiconductor based wavelength converter for DPSK signals in the 40 Gb/s range. Wavelength conversion for DPSK formats A first option for wavelength conversion of phase encoded formats is to use Four Wave Mixing (FWM) [3]. The phase information is preserved using FWM, and thus the technique can be used for conversion of DPSK signals. However, FWM needs very high power, and it not really provides regeneration. Concepts for real world systems should focus on compact semiconductor devices with low power requirements. They should take into account the developed knowledge and experience in ASK conversion. The best known solutions here exploit SOAs in interferometer structures. However, control of SOAs requires ASK signals, and presently the interferometer operation is only optimised for on-off operation. The question therefore is, if there is an easy way to upgrade conventional MZI based all-optical wavelength converters for performing DPSK signal processing. Clearly, the conversion of the DPSK signal to ASK pulses (e.g. using a delay interferometer DI) is needed for controlling the SOAs, and the interferometer has to be operated for obtaining a phase modulated output. A first paper on that was presented very recently in a post deadline session at the ECOC 2005 [4]. The differential scheme was applied for controlling a hybrid interferometer, and conversion to a cw signal was demonstrated. In this paper, we present an integrated MZI-SOA device developed especially for DPSK processing. DPSK to DPSK wavelength conversion in the 40 Gb/s range (31 Gb/s) is demonstrated without applying the differential control scheme. Conversion to an optical clock signal is chosen in order to include a 3R regenerative functionality. Structure of the wavelength converter based on integrated SOA-MZI The structure of the developed DPSK converter is shown in Fig. 1. In the input stage we use a Delay Interferometer (DI) to convert the DPSK signal into ASK and inverted ASK signals. These on-off signals can be used for controlling the SOAs. They are injected with exact time correlation into the two control inputs of a Mach Zehnder Interferometer (MZI) with integrated SOAs. The SOAs are controlled either by a high level bit in the ASK or in the inverse ASK signal, very similar to the push-pull operation of electrically controlled MZ modulators in DPSK transmitters. It needs to be pointed out, that the symmetric scheme provides two ideal DPSK states with identical amplitude and a perfect 7c-phase shift between the two arms even though there is an uneven gain in the two SOA arms due to carrier depletion. OWS6.pdf All-Optical Wavelength Converter DPSK )n DPSK '-Xn in ASKkn1DPSK Xout Dl | D ~~~ASK X-in Fig. 1 Scheme of the DPSK wavelength converter. A clock signal at the new output wavelength is injected into the centre arm of the interferometer. The phase information is encoded in the MZI via the ASK / inverse ASK pulses on to the clock wavelength. The encoding of the data signal is altered in this scheme according to an XOR function between subsequent bits, similar as described in [4]. That has to be addressed in the precoding of the DPSK signal or by a post processing in the receiver. The key device of the converter is the integrated SOA-MZI module (Fig.2) which was developed in view of this application. Several challenges need to be mastered in order to get a high quality DPSK output instead of a simple on-off function. First, ASK needs a phase shift of l2 TC for on-off modulation, while the DPSK needs twice the phase shift for on-on modulation with phase inversion. Fig. 2 Photograph of the integrated MZI module. In order to improve the phase conversion efficiency, long SOAs (2 mm) are integrated into the device. While ASK has only one state of output signal (and an optimized blocking operation point), DPSK needs two equivalent output states, differing only in the phase. In order to balance the operation point of the interferometer independently of the SOA currents we integrated phase tuning sections into the interferometer. The complete device was fabricated using a polarization insensitive (<2dB) strained bulk buried heterostructure and butt coupling between SOAs and waveguide [3]. The chip with tilted, AR coated facets was packaged into a module. Functionality of the DPSK wavelength converter To test the functionality of the DPSK converter, a DPSK signal was generated (eye diagram in Fig. 3a) and injected into the converter. Fig. 3b shows the ASK and inverse ASK patterns behind the DI. The inverse nature of the sequences can clearly be noticed. These signals were injected at a power of 3 dBm (in the fibre) into the MZI. The quality of the wavelength converted DPSK signal behind the SOA-MZI was detected using a one bit DI / balanced receiver module (provided by u2t) and analysed by a sampling oscilloscope and a BER receiver. In our experiments we noticed speed limitations, caused by imperfections of the present device generation. The proof-of-concept experiments were thus performed at 31 Gb/s. Fig. 3c shows the eye diagram of the DPSK signal wavelength converted from 1545 rnm to 1560 nm. The eyes are open, indicating an error free wavelength conversion. Similar results were obtained for other input wavelengths within the C-band. OWS6.pdf 1-"'~'L~,' evaluated by '''''''w""'''vt ~,~I t. t. .s. ..F.ig. . 4 I[\l I|-*~b2;lI covre Fig. sina At 3a latEyte theX\ t was g X of the FX 3X i qultt of 3bf ASK andWttX inverse i1#11|if ASK signal behind 1gtt converted DPSK Fig. inputthDPSK Fig. 3c Eye diagram signal. the delay interferometer DI. signal. to a BR of 100 An erro fre wavele ttngXth }i 5 EWt iE 9nq XiEW- BER performance good syte pe nconvertcde o t At last the quality of the converted signal i3n was evaluated by BER measurementsc we g. 42 40 3 -32 summarizes the results. The BER curve for the | t | i 4 B p o t input ignal converted DPSK signals shows no error floor down convertdo D gnal. A error t a o of BER10n free wavelength 00. o D l w l l t t g s p o t c conversion dS obtaraed. For comparlson the BERi A e ai fe curve of the input DPSK signal is also given. r a t o f work small negative penalty of s dB at 10- (and even less for higher BER) compared to the high quality input K T s i O 2 Atl G USA indicates the ance of the perfor signal good system w avelength converter. Similar results were obtained 2003. 10 ,-pp.-48-663 M also forcLi,eY ong,from other input wavelengths C fo RSignal I 42 40 -38 -36 _34 ~-32I Fig. 4 BER performance of the input signal and the converted DPSK signal. Conclusions An all-optical DPSK waverino40G/rter has been developed, applying a DI and compact semiconductors only. Key device is an MZI with integrated long SOAs and phase shifters. Evaluation in this paper was perfo.93ed at 31 Gb/s. An error free (BER < 10-1°) wavelength conversion of DPSK signals with control power of only 3 dBm (in the fibre) was demonstrated. A low penalty of < ldB indicates the good system performance of the converter. Speed improvements on the device and investigations on regenerative features are topic of further work. References [M]A. Gnauck, "40 Gb/s RZ-Differential Phase Shift Keyed Transmission", OFC 2003, Atlanta, Georgia, USA invited paper ThEC, Proc. vol.2, pp. 450 - 45 p. [2] C. Nuzman, J. Leuthold, R. Ryf, S. Chandrasekhar, C.R. Giles, D.T. Neilson, " Design and Implementation of Wavelength-Flexible Network Nodes", J. Lightwave Technol., vol. 2 1, pp. 648-663, March 2003. [3] Z. Li, Y. Dong, J. Mo, Y. Wang, C. Lu, "Cascaded All-Optical Wavelength Conversion for R_Z-DPSK Signal Based on Four-Wave Mixing in Semiconductor Optical Amplifier", Z. Li, Y. Dong, J. Mo, Y. Wang, C. Lu, IEEE Photon. Technol. Lett. , vol. l16, pp. l1685-1l697, July 2004. [4] I. Kang, C. Dorrer, L. Zhang, M. Rasras, L. Buhl, A. Bhardwaj, S. Cabot, M. Dinu, X. Liu, M. Capuzzo, L. Gomez, A. Wong-Foy, Y.F. Chen, S. Patel, D.T. Neilson, J. Jaques, and C.R. Giles, " Regenerative All Optical Wavelength Conversion of 40 Gb/s DPSK Signals Using a Semiconductor Optical Amplifier Mach-Zehnder [5]~~~~4 T.I-- Tekin, C.- Bornoldt DP.-lvk M. -clk B. 'Ptoiu, J. Krisl S. Bauer C. Bobet W. Brnkr IB._
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