This application is a 35 U.S.C. 371 national stage filing of International Application No. PCT/GBO2/05391, filed 29 Nov. 2002, which claims priority to Great Britain Patent Application No. 0128783.8 filed on 30 Nov. 2001, in Great Britain. The contents of the aforementioned applications are hereby incorporated by reference.
This invention relates to optical communications and in particular to a method of modulating an optical carrier for use in a wavelength division multiplex (WDM) optical communications system.
In this specification the term “light” will be used in the sense that it is used generically in optical systems to mean not just visible light but also electromagnetic radiation having a wavelength between 800 nanometres (nm) and 3000 nm. Currently the principal optical communication wavelength bands are centered on 1300 nm, 1550 nm (C-Band) and 1590 nm (L-Band), with the latter bands receiving the majority of attention for commercial exploitation.
Exemplary WDM systems operating in the 1550 nm C-Band optical fibre communication band are located in the infrared spectrum with International Telecommunication Union (ITU) 200, 100 or 50 GHz channel spacing (the so called ITU Grid) spread between 191 THz and 197 THz.
With ongoing developments in optically amplified dense wavelength division multiplex (DWDM) optical links as the backbone of point-to-point information transmission and the simultaneous increase in bit rate applied to each wavelength and the simultaneous increase in the number of channels, the finite width of the erbium gain window of conventional erbium-doped optical amplifiers (EDFAs) could become a significant obstacle to further increases in capacity. Conventional EDFAs have a 35 nm gain bandwidth which corresponds to a spectral width of 4.4 THz. System demonstrations of several Tbit/s data rate are already a reality and the spectral efficiency, characterized by the value of bit/s/Hz transmitted, is becoming an important consideration. Currently, high-speed optical transmission mainly employs binary amplitude keying, using either non-return-to-zero (NRZ) or return-to-zero (RZ) signalling formats, in which data is transmitted in the form of optical pulses having a single symbol level.
In WDM several factors limit the minimum channel spacing for binary amplitude signaling, and in practice spectal efficiency is limited to ˜0.3 bits/Hz. Although increasing the per-channel bit rate tends to reduce system equipment, there are several problems that need to be overcome for transmission at bit rates above 10 Gbit/s; these being:
One technique which has been proposed which allows an improvement of spectral efficiency is the use of quadrature phase shift keying (QPSK) [S. Yamazaki and K. Emura, (1990) “Feasibility study on QPSK optical heterodyne detection system”, J. Lightwave Technol., vol. 8, pp. 1646-1653]. In optical QPSK the phase of light generated by a transmitter laser is modulated either using a single phase modulator (PM) driven by a four-level electrical signal to generate phase shifts of 0, π/2, π or 3π/2 representative of the four data states, or using two concatenated phase modulators which generate phase shifts of 0 or π/2 and π or 3π/2 respectively. A particular disadvantage of QPSK is that demodulation requires, at the demodulator, a local laser which is optically phase-locked to the transmitter laser. Typically this requires a carrier phase recovery system. For a WDM system a phase-locked laser will be required for each wavelength channel. It further requires adaptive polarisation control which, in conjunction with a phase recovery system, represents a very high degree of complexity. Furthermore, systems that require a coherent local laser are sensitive to cross-phase modulation (XPM) in the optical fibre induced by the optical Kerr non-linearity, which severely restricts the application to high capacity DWDM transmission.
It has also been proposed to use differential binary phase shift keying (DBPSK) [M. Rohde et al (2000) “Robustness of DPSK direct detection transmission format in standard fibre WDM systems”, Electron Lett., vol. 36]. In DBPSK data is encoded in the form of phase transitions of 0 or π in which the phase value depends upon the phase of the carrier during the preceding symbol interval. A Mach-Zehnder interferometer with a delay in one arm equal to the symbol interval is used to demodulate the optical signal. Although DBPSK does not require a phase-locked laser at the receiver it does not provide any significant advantages compared to conventional amplitude NRZ signalling.
U.S. Pat. No. 6,271,950 discloses a differential phase shift keying optical transmission system, comprising a laser to generate an optical signal, a delay encoder to provide a different delay for each of M input channels and an M channel phase modulator which phase modulates the optical carrier signal with each of the differently delayed M input signal channels to form a time division multiplex (TDM) phase modulated optical signal.
However, in modern communication systems, the rate of development dictates that typically data streams multiply up by a factor of 4 every few years. At the time of application the proposed standard installation will use data streams of 10 Gbit/s and systems of 40 Gbit/s have been demonstrated. In addition to the matters discussed above, the practical problem then arises that new systems operating at high speeds have to co-operate with older systems.
The present invention seeks to provide a method for pre-encoding data for use in a high data rate optical communications system that works with a decoder which is substantially the same decoder as used at a lower data rate.
According to the invention, there is provided a modulator arrangement adapted to use a differential quadrature phase shift key for use in an optical wavelength division multiplex (WDM) optical communications system, comprising a precoder, which precoder is adapted to generate drive voltages for first and second phase modulators in dependence upon first and second data streams, wherein the respective drive voltages for the first and second modulators are fed back to the precoder inputs with a delay, wherein the length of the delay is related to the line speed of the data stream.
Preferably, the length of the delay corresponds to n bits, wherein n is proportional to data stream speed. Preferably, where the data stream speed is 20 Gsymbols/s for each data stream, n is equivalent to 4 symbols or 200 ps.
In a preferred embodiment, the precoder output data streams are given by logical equations:
Ik=
Qk=
where n is the number of bits in the delay, Uk and Vk are the incoming data streams with a bit rate equal to the symbol rate, k-n being the nth bit precedent to the actual bit of information.
In a preferred embodiment where the modulator arrangement has an input of 2×n subsidiary data streams each at a bit rate of 1/n×the line symbol rate, the precoder arrangement comprises n precoders in parallel. Preferably, the precoder arrangement comprises four precoders in parallel, the outputs of which are fed to one of two respective 4:1 multiplexers, the output of each precoder also being fed via 1 bit delays to its respective inputs, wherein the output of the multiplexers is used to drive the modulators, where the bit rate is proportional to ¼ of the symbol rate, n being equal to 4.
The provision of an n bit delay in the precoder, where n is, say 4 for a 40 Gbit/s system, ensures that more time is available for the preprocessing operation and also that the decoder (also known as a demodulator) hardware can be common to systems having data streams at 10 Gbit/s thereby reducing implementation costs.
Exemplary embodiments of the precoder and decoder invention will now be described in greater detail with reference to the drawings in which:
Referring to
The modulator arrangement comprises a single frequency laser 2, for example a distributed feedback (DFB) semiconductor laser due to its stable optical output for a given wavelength, which is operated to produce an unmodulated optical output of a selected wavelength, typically a WDM wavelength channel. Light from the laser is divided by an optical splitter 4 into two parts and each part is applied to a respective phase modulator 6, 8. Each phase modulator 6, 8 is configured such that it selectively modulates the phase by 0 or π radians in dependence upon a respective binary (bipolar) NRZ drive voltage VI(t), VQ(t). In the preferred arrangement illustrated in
The optical output from the phase modulator 6 is passed through a phase shifter 10 which applies a phase shift of π/2 such that the relative phase difference between the optical signals passing along the path containing the modulator 6 and that passing along the path containing the modulator 8 is ±π/2. The optical signals from the phase shifter 10 and phase modulator 8 are recombined by an optical recombiner 12, for example a 3 dB coupler, to form an optical phase shift key (PSK) output 14. The phase shift may be substantially provided by the cooperation of MMIs forming the splitter 4 and recombiner 12, together with a control electrode to provide fine control.
The phase modulator drive voltages VI(t), VQ(t) are generated by pre-coding circuitry 16 in dependence upon the two binary data streams Uk, Vk. According to the modulator arrangement of the present invention the two data streams Uk, Vk are differentially encoded such that these data are encoded onto the optical signal 14 in the phase transitions (changes) rather than in the absolute phase value. As a result it will be appreciated that the optical signal 14 is differential quadrature phase shift key (DQPSK) encoded.
The DQPSK optical signal 14 is ideally given by E0 exp(iωt+θ+θi), where ω is the mean optical angular frequency, t is time, θ the carrier phase and θi a data dependent phase modulation for the i-th data symbol di. In the general cased diε{0, 1, . . . M−1} and for quarternary phase shift keying M=4, that is the data symbol has four values. The phase modulation term is given by θi=θi-n+Δθi(di) in which θi-1 is the phase term for the previous data symbol di-1 and Δθi the change in phase between the i-n and i-th data symbols. The relationship between data symbol di and phase shift Δθi for QPSK is tabulated below.
It is to be noted that the mapping between data, data symbol and phase change is just one example and that other mappings can be used. The pre-coding circuitry 16, a logical representation of which is shown in
VI(i)=VI(i−1)cos Δθ(di)−VQ(i−1)sin Δθ(di) Eq. 1
VQ(i)=VI(i−1)sin Δθ(di)+VQ(i−1)cos Δθ(di) Eq. 2.
The benefit of encoding the data signal as a phase difference between symbols is that the encoding has a greater resilience since much of the cross-phase modulation will be common between the respective symbols.
In a system operating at 40 Gbit/s, there is only a 50 ps separation between successive symbols in the data stream (each symbol being two bits). This duration is about at the limit of current precoder electronics ability to process due to gate delays. With reference to
The data streams Ik and Qk used to calculate the drive voltages can be derived from the logical equations:
Ik=
Qk=
where n is the number of bits in the delay, Uk and Vk are the incoming data stream, k−n being the nth bit precedent to the actual bit of information. Whilst the logic of
Incorporating a delay of n bits, where n is, say 4 bits for a 40 Gbit/s system, ensures that more time is available for the preprocessing operation and also that the decoder hardware can be common to systems having data streams at 10 Gbit/s, thereby reducing implementation costs.
Referring to
x1(t), y2(t)=cos(Δθ(di))±sin(Δθ(di))
For DQPSK where Δθ(di) takes the possible values {0, π/2, π, 3π/2} the outputs are hence binary (bipolar) signals given by:
x1(t)=Uk and y2(t)=Vk
A particular benefit of setting the MZIs 30, 32 to impart relative phase shifts between their arms of π/4 and −π/4 respectively is that this results in the de-modulated signals x1(t), y2(t) being bipolar NRZ signals. It will be appreciated that the in-phase and quadrature components of the DQPSK signal can also be demodulated using other relative phase shifts provided there is a difference of π/2 between the respective MZIs, though the resulting signals will not be symmetrical bipolar NRZ signals. In the general case, therefore, the MZI 30 is set to impart a phase shift φ and the MZI 32 set to impart a phase shift φ±π/2.
Whilst higher delay rates would be possible, it is undesirable to have too high a delay as this will make the system too sensitive to optical phase noise.
Number | Date | Country | Kind |
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0128783.8 | Nov 2001 | GB | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/GB02/05391 | 11/29/2002 | WO | 00 | 6/1/2004 |
Publishing Document | Publishing Date | Country | Kind |
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WO03/049393 | 6/12/2003 | WO | A |
Number | Name | Date | Kind |
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4893352 | Welford | Jan 1990 | A |
5222103 | Gross | Jun 1993 | A |
Number | Date | Country |
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2 370 473 | Jun 2002 | GB |
4 310038 | Nov 1992 | JP |
Number | Date | Country | |
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20050074245 A1 | Apr 2005 | US |