This application is a national stage application of PCT/EP2007/052005, filed Mar. 2, 2007, which claims the benefit of priority to German Application No. 10 2006 009 990.7, filed Mar. 3, 2006, the contents of which hereby incorporated by reference.
The invention relates to a modulator device for generating an optical transfer signal modulated by a binary signal.
A laser having a downstream amplitude modulator (intensity modulator) generates an optical spectrum with a spectral line at the carrier frequency and a bandwidth which is wider than the bandwidth of the information signal. Such an emission spectrum reduces the amount of information which can be transferred overall in a wavelength-division multiplex system. On account of the non-linear properties of the transmission fiber, a wider bandwidth results in greater distortion of the transfer signal. One method for reducing the bandwidth is duobinary coding. Such a method is described in IEEE Photonics Technology Letters, 1998, Vol. 10, Issue 8, pp. 1159-1161: “Prechirped Duobinary Modulation” by A. Djupsjöbacka (Ericsson Components, Sweden). However, this type of coding is very complicated.
The invention discloses a modulation device which can be implemented in a simple manner and is intended to generate a high-quality transfer signal.
One advantage of the invention is that the optical carrier signal is frequency-modulated such that the optical carrier is suppressed at least to a large extent. The drive signal for the frequency modulator is pre-coded such that frequency shift keying is respectively carried out in the case of a 10 or 01 change. This frequency shift keying is required in the case of 101 sequences. In contrast, in the case of longer 11 sequences or 00 sequences, no frequency shift keying is carried out. An amplitude modulator which suppresses the broad signal spectrum produced during frequency shift keying is connected downstream of the frequency modulator. As a result, further spectral lines, apart from the spectral lines adjacent to the original carrier frequency, disappear in the case of a 1010 signal sequence. The spectrum remains narrow even in the case of a real data signal.
The circuit can be constructed in a particularly cost-effective manner if a directly modulated laser is used as the source of the carrier signal and as the frequency modulator.
A suitably designed drive circuit makes it possible to compensate for asymmetry in the amplitude, to optimize the transfer signal with regard to a desired chirp, and to compensate for delay time differences.
The invention is described in more detail using figures, in which:
The method of operation of the modulator device is now explained in more detail using a timing diagram which is illustrated in
The third row shows a sinusoidal frequency modulation signal FMS which is at half the fundamental frequency of the binary signal in the case of a 10 sequence. It is shaped (if necessary) by the first filter arrangement 35 which also provides the required drive voltage for the frequency modulator in this case.
The fourth row illustrates a frequency modulation voltage FMS1 for an advantageous variant of the modulation device, in which unnecessary frequency shift keying is avoided. Frequency shift keying is carried out whenever there is a 101 sequence. For this purpose, a further input signal is supplied to the logic circuit via the dashed connection in
In the fifth row, frequency shift keying is no longer carried out by a sinusoidal frequency modulation voltage but rather takes place in the half period before it. For the rest, the FM modulation voltage FMS2 corresponds to the modulation voltage in the third row.
The binary signal is impressed in the amplitude modulator 4. It takes place for the correct temporal assignment of an amplitude modulation signal AMS to the frequency modulation signal or at the times during which frequency shift keying is carried out. The second row shows a square-wave (dashed) modulation signal, which, apart from a necessary time delay, corresponds to the binary signal BS, and the sinusoidal amplitude modulation signal AMS. During frequency shift keying, the frequency-modulated signal FTS must be suppressed as far as possible and the amplitude of the transfer signal LS must thus be zero as far as possible so that the interfering frequency components are masked. This is the case with a combination of the frequency modulation signal FMS and the amplitude modulation signal AMS. The time function in the lowest, sixth row shows the amplitude profile of the transfer signal for this combination of sinusoidal amplitude modulation and frequency modulation FMS.
If, in contrast, the variant is implemented with frequency shift keying for 101 sequences according to row 4 or 5, the amplitude modulation voltage is delayed by the duration of one bit, as illustrated in
| Number | Date | Country | Kind |
|---|---|---|---|
| 10 2006 009 990 | Mar 2006 | DE | national |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/EP2007/052005 | 3/2/2007 | WO | 00 | 8/28/2008 |
| Publishing Document | Publishing Date | Country | Kind |
|---|---|---|---|
| WO2007/099165 | 9/7/2007 | WO | A |
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| 6592274 | Kahn et al. | Jul 2003 | B2 |
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| 20030002121 | Miyamoto et al. | Jan 2003 | A1 |
| 20030043931 | Fullerton et al. | Mar 2003 | A1 |
| Number | Date | Country |
|---|---|---|
| 0825733 | Feb 1998 | EP |
| 2237469 | May 1991 | GB |
| WO-2005084268 | Sep 2005 | WO |
| Number | Date | Country | |
|---|---|---|---|
| 20100245967 A1 | Sep 2010 | US |