An All-optical Metro-Access Interface for a PON System Based on NRZ to FSK Format Conversion
ABSTRACT We propose and experimentally demonstrate a novel all-optical NRZ to FSK format conversion scheme to interconnect a MAN and a PON system. Upstream data is re-modulated on downstream converted FSK format. OCIS codes: (060.2330) Fiber optics communications; (060.2630) frequency modulation; (060.4250) Networks.
- [Show abstract] [Hide abstract]
ABSTRACT: Full-duplex single fiber bidirectional transmission, using frequency-shift-keying modulation for downstream, by direct modulation of a tunable laser, and intensity modulation for upstream, in a wavelength-division-multiplexing passive optical access network is demonstrated. The optical network unit, located at the end user premises, reflects and orthogonally remodulates the received light. Rayleigh scattering effects are reported and analyzed. The system shows proper operation up to 1 Gb/s at 30-km reach.IEEE Photonics Technology Letters 04/2005; · 2.18 Impact Factor
- [Show abstract] [Hide abstract]
ABSTRACT: Employment of optical frequency shift keying (OFSK) as the downstream modulation format in a WDM passive optical network is proposed. The upstream OOK (on-off keying) transmitter at the ONU (optical network unit) can be realised by remodulating the constant-intensity downstream OFSK signal power with the upstream data. Transmission and remodulation of 2.5 Gbit/s downstream and upstream signals were successfully demonstrated.Electronics Letters 12/2003; · 1.07 Impact Factor
- [Show abstract] [Hide abstract]
ABSTRACT: We present a scalable all-optical virtual private network (VPN) in a two-stage passive optical network (PON) architecture to connect optical network units (ONUs) in different sub-PONs. It provides efficient access and VPN service covering a wider area. The scheme employs amplitude-shift keying/frequency-shift keying (FSK) orthogonal modulation formats, which are used for the VPN and upstream traffic at 625 Mb/s and 5 Gb/s, respectively. At the optical line terminal side, a fiber Bragg grating reflects one of the two frequency components in the FSK signal back to the ONUs in a same VPN. Using a bidirectional amplifier, the power budget and the scalability of the network are significantly improved, as evidenced by numerical analysis using the parameters in the experiment.IEEE Photonics Technology Letters 11/2007; · 2.18 Impact Factor
An All-optical Metro-Access Interface for a PON System
Based on NRZ to FSK Format Conversion
Yuanyuan Lu, Cishuo Yan, Qingjiang Chang, Qiang Li, Yikai Su, Weisheng Hu
State Key Lab of Advanced Optical Communication Systems and Networks, Department of Electronic Engineering
Shanghai Jiao Tong University, 800 Dongchuan Rd, Shanghai 200240, China, firstname.lastname@example.org
Abstract: We propose and experimentally demonstrate a novel all-optical NRZ to FSK format
conversion scheme to interconnect a MAN and a PON system. Upstream data is re-modulated on
downstream converted FSK format.
©2008 Optical Society of America
OCIS codes: (060.2330) Fiber optics communications; (060.2630) frequency modulation; (060.4250) Networks.
Passive optical network (PON) has become an attractive solution to provide broadband access. To reduce the cost at
the optical network units (ONUs), re-modulation on downstream data is a promising technique. The downstream
signal possesses constant intensity serving as a carrier for re-modulation at the ONU. As frequency-shift-keying
(FSK) format presents constant intensity, it has received considerable attention in PON applications [1-4]. In
addition, FSK balanced detection enables 3-dB receiver-sensitivity enhancement, and higher tolerance to fibre
nonlinear impairment and chromatic dispersion [5-7]. On the other hand, cost-effective non-return-to-zero (NRZ)
format is widely used in metropolitan area networks (MANs). Therefore, NRZ to FSK format conversion would be
desirable at an intermediate node. To the best of our knowledge, however, no demonstration has been performed on
conversions from NRZ to FSK to interface a MAN and a PON system, which is expected to be a promising
technology to provide scalable broadband access.
In this paper, we propose an all-optical metro-access interface based on NRZ to FSK conversion using a
semiconductor optical amplifier (SOA) at an optical line terminal (OLT). At the ONU, part of the FSK signal is
tapped off and detected by a balanced receiver, and the other part is fed into an optical intensity modulator for
upstream re-modulation. Error-free operation is experimentally demonstrated to show the feasibility of the proposed
scheme with a 10-Gb/s downstream data and a 1.25-Gb/s upstream data.
2. Principle of operation
Input NRZ and
Fig. 1. (a) Network topology with an NRZ to FSK format converter between a metro network and a PON system.
(b) Principle of the NRZ to FSK converter based on an SOA.
Figure 1(a) shows the network architecture with the proposed NRZ to FSK format converter at a central office (CO)
between a MAN and a PON system. The CO comprises a reconfigurable optical add/drop multiplexer (OADM) as a
metro node and an OLT for all ONUs. The format converter within the OLT acts as an all-optical interface to bridge
the MAN and the access network. The basic principle of the NRZ to FSK converter as depicted in Fig. 1(b) is
similar to a conventional wavelength converter, based on cross gain modulation (XGM) in a SOA operated in the
saturation regime . The incoming NRZ signal at wavelength λ0 and a continuous-wave (CW) light at λ1 are
launched into the SOA as a control pulse and a probe light, respectively. As shown by the dotted line in Fig. 1(b),
the power of the CW is set between the powers of “0” and “1” levels of the NRZ data. The carrier density in the
SOA is varied depending on the intensity of the control pulse. Therefore, after passing through the SOA, the probe
light carries inverted logical information as the NRZ. By adjusting the power of the NRZ and the probe, FSK signal
with a constant intensity can be obtained at the output of the SOA, and the output wavelengths are changed
depending on the input NRZ signal.
The converted FSK signal is transmitted over conventional single-mode fibre (SMF) as downstream data to an
ONU, where the chromatic dispersion between the upper and the lower sidebands (USB and LSB) is compensated
to preserve the constant intensity of the downstream FSK signal , before fed into an FSK receiver and an optical
intensity remodulator. Part of the compensated FSK is tapped and received by a balanced receiver to obtain the 3-
dB receiver-sensitivity enhancement . The rest part is then intensity modulated with the upstream on-off-keying
(OOK) data and is transmitted back to the OLT along another SMF to avoid Rayleigh backscattering.
Figure 2 depicts the experimental setup to verify the operation principle of the format conversion and to
demonstrate downstream and upstream transmissions between an OLT and an ONU. We use a commercial
polarization-independent booster SOA (SOA-NL-OEC-1550 from CIP) with a gain recovery time of ~30 ps at 300
mA drive current. This SOA has a small signal gain of 30 dB and a saturation power of 10 dBm. The NRZ signal
transmitted in a MAN is generated by modulating a CW light (LD1) at 1550.27 nm with a Mach-Zehnder
modulator (MZM) using a 10-Gb/s pseudorandom bit sequence 1 (PRBS1) of length 27-1. An erbium-doped fiber
amplifier (EDFA) amplifies the signal to 12 dBm, a tunable optical filter (TOF) with a bandwidth of 0.4 nm
suppresses amplified spontaneous emission (ASE) noise, and a variable optical attenuator (VOA) reduces the power
to 3 dBm. Another CW light at 1549.94 nm with a power of -2 dBm is coupled with the incoming NRZ signal and
launched into the SOA simultaneously. At the output of the SOA, an FSK signal with almost constant intensity is
obtained, whose eye diagram and spectrum are provided in insets (i) and (ii) of Fig. 2.
10 Gb/s PRBS1
Optical delay line
(iii) 0.5 nm/div
1.25 Gb/s PRBS2
NRZ to FSK converter
Group Delay Compensated
Fig. 2. Experimental setup. PC: Polarization controller; Cir: Circulator. Optical spectrum resolution: 0.07 nm.
The converted FSK signal is transmitted downstream through a VOA and a 12.5-km SMF to the ONU, where a
fiber Bragg grating (FBG) with an optical circulator separates the USB (1550.27 nm) and LSB (1549.94 nm) tones.
The FBG has a reflective bandwidth of 0.2 nm at 1549.94 nm. In the experiment we used an optical delay line to
compensate the group delay difference between the USB and LSB, while in practice this can be achieved using
electronic tunable delay compensation for different transmission distances. The spectra of the USB and LSB
components are illustrated in insets (iii) and (iv) of Fig. 2. Both the suppression ratios are ~15 dB. The two
sidebands are split into two parts by two 50/50 couplers. One part is received by a 10-GHz balanced photodetector
(BPD). The other part recombines and is remodulated by a 1.25-Gb/s PRBS2 of length 27-1 in a MZM. The
upstream NRZ signal is amplified and sent over a 12.5-km SMF back to the OLT, where it is detected by a 2.5-GHz
photodetector (PD). The downstream and upstream electrical NRZ signals are generated by the front and back
panels of a programmable pulse pattern generator (PPG, MP1763C from Λnritsu), respectively. To facilitate the
programming and bit error rate (BER) testing processes, we chose the pattern length of 27-1. In fact, the pattern
length is not limited to 27-1 because the gain recovery time of the SOA is as short as ~30 ps.
Figure 3 shows BER curves and eye diagrams for the format converted, downstream, and upstream signals. For
the NRZ to FSK format conversion, the power penalty of the FSK signal received by a BPD is ~1.2 dB. The
reflection ratio of the FBG is ~90%, which results in that the power of the LSB is lower than that of the USB.
Therefore, the BERs of the USB and LSB detected by a single-end PD are different, which can be avoided using an
interleaver with higher suppression ratio . The optical and electrical eye diagrams of the USB and LSB are
illustrated in Fig. 3(b). The insets of Fig. 3(c) show that the demodulated eye diagrams of the converted FSK before
and after the transmission have nearly the same shape. Yet the eye diagram after the transmission displays more
noise, which results in ~0.4-dB penalty. The eye diagrams and BER performance in Fig. 3(d) indicate that the
upstream transmission suffers ~1-dB penalty due to the dispersion between the two wavelengths of the remodulated
NRZ to FSK conversion
FSK with BPD
B to B
B to B
50 ps/div50 ps/div
Fig. 3. (a) BER curves and eye diagrams in the format conversion process; (b) Eye diagrams of the USB and LSB signals;
(c) FSK-signal transmission performance; (d) Upstream remodulated-signal performance.
We have proposed and experimentally demonstrated an all-optical NRZ to FSK format conversion scheme at an
OLT to interconnect a MAN and a PON. The constant intensity of the converted downstream FSK signal is
remodulated at the ONU to carry upstream data. Error-free conversion has been achieved at 10 Gb/s based on XGM
in an SOA with a power penalty of 1.2 dB. 1.25-Gb/s upstream remodulation and transmission are also
Acknowledgement: The authors acknowledge the help from Xinwan Li and Jianping Chen. This work was
supported by the NSFC (60777040), the 863 High-Tech Program, and the Fok Ying Tung Fund (101067).
 J. Prat, V. Polo, C. Bock, C. Arellano, J. J. V. Olmos, “Full-duplex single fiber transmission using FSK downstream and IM remote
upstream modulations for fiber-to-the-home,” IEEE Photon. Technol. Lett. 17, 702-704 (2005).
 N. Deng, C-K. Chan, L-K Chen, F. Tong, “Data remodulation on downstream OFSK signal for upstream transmission in WDM passive
optical network,” Electron. Lett. 39, 1741-1743 (2003).
 C. Arellano, V. Polo, C. Bock, J. Prat, “Bidirectional single fiber transmission based on a RSOA ONU for FTTH using FSK-IM
modulation formats,” OFC 2005, JWA46 (2005).
 Y. Tian, T. Ye, Y. Su, “Demonstration and scalability analysis of all-optical virtual private network in multiple passive optical networks
using ASK/FSK format,” IEEE Photon. Technol. Lett. 19, 1595-1597 (2007).
 T. Kawanishi, T. Sakamoto, S. Shinada, M. Izutsu, T. Fujita, K. Higuma, J. Ichikawa, “10 Gbit/s FSK transmission over 130 km SMF
using group delay compensated balance detection,” OFC 2005, OTuL1 (2005).
 A. Klekamp, W. Idler and R. Dischler, “Comparison of FSK by directly modulated DFB laser with DPSK, NRZ and RZ modulation
formats at 10 Gb/s,” ECOC 2003, We4.P.118 (2003).
 B. Wedding, R. Jung, C. Haslach, H. Söhnle, “10.7 Gbit/s FSK transmission with 61 dB power budget”, ECOC2003, TH1.5.5 (2003).
 T. Durhuus, B. Mikkelsen, C. Joergensen, S. Lykke Danielsen, and K. E. Stubkjaer, “All-optical wavelength conversion by semiconductor
optical amplifiers,” J. Lightw. Technol. 14, 942-954 (1996).