1 May 2006 Waveband routed optical packet switch: implementation and performance evaluation
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Optical Engineering, 45(5), 050504 (2006). doi:10.1117/1.2195369
An optical packet switch based on wavelength routing and optical waveband conversion is demonstrated. The switch performs header extraction, packet routing, and regeneration and exhibits very good physical performance.
Politi, Klonidis, Tzanakaki, O’Mahony, and Tomkos: Waveband routed optical packet switch: implementation and performance evaluation



Optical packet switching (OPS) is seen as a promising solution offering high spectral efficiency through fine switching granularity.1, 2 Various OPS architectures have been proposed addressing a variety of issues including packet and header format and appropriate switching techniques.1 However, a number of issues are still unresolved such as buffering, physical performance, complexity, and cost.

This work examines the performance of an OPS architecture based on waveband converters, a waveband-routed OPS.3 A serial header-payload format is utilized with a phase-modulated header and non-return-to-zero amplitude modulated payload. The switching fabric relies on wavelength routing using a set of waveband converters (WBCs) followed by an arrayed waveguide grating (AWG). Waveband routing has been discussed in Ref. 3. WBCs are used to minimize the requirements in terms of wavelength converters, while at the output of the switching subsystem (WBCs and AWG) a single-wavelength conversion (SWC) stage provides flexible wavelength assignment, contention resolution, regeneration, and header deletion. These features significantly reduce the overall component count, cost, and power consumption of a node, supporting reduced capital and operational expenditure in practical networks.3


OPS Architecture

The generic structure of the optical packet switch is illustrated in Fig. 1. Synchronous optical packets of the same length enter the switch through a band demultiplexer. The bank of WBCs that follows converts and routes the optical packets to the appropriate output ports through the AWG according to their wavelength. The architecture utilizes grouping of packets in wavebands (group of wavelengths) to enable the use of WBCs; however, this does not impose a banded wavelength channel plan at the transport network level. In particular, although simultaneous switching of all packets at the same waveband is performed, each of the packets is routed individually and independently of the others. The design rules for the application of this scheme are explained in Ref. 3. In the experiment presented here, a packet waveband comprises two packets at different wavelengths. The switch control can be implemented in parallel to the packet routing path, utilizing technology similar to that in Ref. 2. At the input of the switch a 10% of the signal is tapped for band header decoding (BHD) using differential phase shift keying (DPSK) based decoding through a passive one-bit delayed interferometer (DI). This translates the phase encoded header into the equivalent DPSK intensity variations, which then can be detected and processed by the control.2 Header reinsertion (HR) is performed after the SWC by means of a phase modulator.

Fig. 1

N×N waveband-based optical packet switch.


In this paper a widely tunable four wave mixing (FWM) converter using a semiconductor optical amplifier (SOA) in dual pump configuration2 is deployed for the WBC. To enable nonblocking operation of the packet switch, minimizing the number of output wavelength converters, the AWG output ports are combined in a predetermined fashion through passive coupling.3 This introduces an increased requirement in AWG dimensions compared to the case with SWC. However, these requirements can be accommodated by existing AWG technology that scales up to 256×256 ,1 while multistage configurations can also be utilized.4 The output conversion stage operates in tunable-input–fixed-output mode and is used to assign appropriate wavelengths to the output packets. This assists the contention resolution and minimizes the buffering requirements. In addition to wavelength assignment and contention resolution, the SWC offers regeneration and power equalization, as well as header deletion.


Experimental Configuration

The experimental configuration shown in Fig. 2 is implemented in order to evaluate the performance of the proposed OPS design. The OPS demonstrator comprises packet generation, header extraction, waveband conversion, switching, regeneration, and header reinsertion.

Fig. 2

Experimental setup.


Two packet sequences at λA=1561.25nm and λB=1562.05nm are modulated at 10Gbs . Each packet consists of 4096bits . The first 128bits of the total packet length are set to ‘one’ (high) and provide a power level on top of which the header bits are encoded on the phase of the carrier at 2.5Gbs . This scheme, previously presented in Ref. 2, offers optimum header encoding, maintaining the extinction ratio of the propagated payload bits at maximum. The guard band between the header and the payload is 12.8ns in duration, while the guard band between consecutive packets is 72.6ns . Both packets are modulated with the same header information, and coupled with a fixed pump at λ0=1560.25nm and a second wavelength selectable pump. This is obtained through a laser array that selects the appropriate pump required to convert the input waveband packets to the selected output wavelengths. The two laser pumps are at λP1=1547.85nm and λP2=1555.3nm and are switched appropriately using a pulse generator. They are then introduced into a multi-quantum-well SOA 1mm in length, operated at 220mA .2 This enables the simultaneous conversion of the two input packet streams into different wavebands (on a packet-by-packet basis) and eventually their routing to different outputs of the AWG. As a result, copies of the initial packets at λA and λB are produced at λ1=1554.3nm and λ2=1553.5nm or λ3=1546.85nm and λ4=1546.05nm depending on the second pump’s wavelength ( λP1 or λP2 ). After routing through the AWG, the packets are converted by a SWC at an output wavelength λout=1540.8nm . The SWC is based on cross-phase modulation (XPM) in a 2×2 integrated Mach-Zehnder interferometer utilizing SOAs. Each arm consists of two SOAs in a row, each 1mm in length. The initial packet sequence at λA is illustrated in Fig. 3a. The 1st, 3rd, 4th, and 5th packets of the two input packet sequences at λA and λB are converted to λ1 and λ2 , respectively. The 2nd packet of the two input packet sequences is converted to λ3 and λ4 , respectively. The traces of the four converted packets at λ1 , at the output of the AWG, are shown in Fig. 3b, while the same packets at the output of the XPM converter are illustrated in Fig. 3c. Similar, Fig. 3d and 3e illustrate the converted packet at λ3 and the same one after the XPM converter. Therefore, specific packets are routed to different AWG ports. Additionally, the cross-talk and cross-gain modulation effects, as well as the poor OSNR introduced by the FWM converter, are compensated through the regenerating XPM stage of the SWC at the output. The bit error rate (BER) curves show that the penalty induced at 109 BER is 2.6dB for packet 1 and increases to 2.9dB for packet 4, due to the wavelength dependent performance of the two converters. The system power penalty was also measured for continuous data operation and was observed to be identical to that of the packet case.

Fig. 3

Packets traces with arbitrary units for comparison and evaluation of the BER measurements as explained in the text.


Simultaneous header extraction for both packets with the same characteristics and excellent performance is achieved. An example of the extracted header after the DI is shown in Fig. 4a. The header payload separation is 6.2dB and a clear threshold can be applied by the control. Figure 4b shows the header’s level after deletion regeneration and reinsertion in phase. Note that small ripples (<1dB) appear at the header’s level due to the effect of the AWG on the phase-encoded bits and the imperfect regeneration after the XPM processing. However the phase information is fully deleted. These ripples may cause amplitude variations of the DPSK decoded header, especially when packets are routed through a large number of nodes. Phase modulation of the header was arbitrary and no comparative study of the extracted information before and after the reinsertion could be performed due to the differential nature of the coding.

Fig. 4

(a) Decoded header and (b) header’s level after XPM SWC.


In conclusion, this paper presents a demonstration of an OPS architecture using waveband routing. The switch is based on widely tunable WBCs, an AWG, and regenerative SWCs and minimizes the required component count.


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Christina Politi, Dimitris Klonidis, Anna Tzanakaki, Michael J. O'Mahony, Ioannis Tomkos, "Waveband routed optical packet switch: implementation and performance evaluation," Optical Engineering 45(5), 050504 (1 May 2006). http://dx.doi.org/10.1117/1.2195369




Integrated optics

Phase shift keying

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