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Complex Optical Spectrum Analysis

Since their origins, optical transmission systems have been improving in terms of transmission capacity at an amazing pace. The introduction of WDM enabled a huge increase of capacity but actual networks are saturated and need to increase their capacity while maintaining their costly DWDM infrastructure. The only way out has been increasing the spectral efficiency of the optical signals, which have been reluctant to abandon the traditional on-off keying format, in which the power of an optical carrier was modulated to have light (a logical ‘1’) or darkness (a logical ‘0’). In addition to being spectrally very inefficient (OOK signals occupy a spectral bandwidth of twice their data rate), they are also suboptimal against chromatic dispersion and many non-linear effects. In this scenario, more advanced modulation formats, most of them inherited from radio communications, that combine power and phase to encode information are being rapidly introduced. 40G systems already experienced a strong introduction of DPSK systems, and much more complex modulation formats are being proposed for 100G networks.

The use of the optical phase to encode information has given a boost for the development of new measurement techniques, a step beyond the technology of traditional optical oscilloscopes. For most of them that work in the time domain, the measurement of the phase has become a challenge. This evolution of the transmission systems has generated a demand for new technologies to enable the characterization and performance evaluation of these signals and subsystems.

Phase Modulation Characterization

The measurement of the phase shift keyed (PSK) signals is normally performed by using balanced detection following a Mach-Zehnder differential interferometer (MZDI). For modulations with more symbols, such as quadrature phase-shift keying (QPSK), two signals must be acquired, the in-phase (I) and the in-quadrature signals (Q). Considering the fact that BOSA PHASE provides the possibility of directly obtaining the instantaneous Phase, an alternative representation is possible: the phase eye diagram, which comprises all the information in a very intuitive graph.

Optical Signal-to-Noise (OSNR) Measurement

OSNR is one of the key parameters to measure the quality of the signals in a DWDM system. Its value is related to the BER of the channel and represents a direct way to monitor the status of the network.

Due to the evolution of new optical networks, OSNR measurement has become a new challenge. The addition of ROADMs to the existing infrastructure, plus the increasing data bit rates, has made the standard measurement processes obsolete.

Two "in-band" OSNR measurement techniques can be supported using the optical spectrum analyzer. Spectral measurements of a 40Gbps P-DPSK commercial transmission signal permit direct measurement of  the noise level made accessible through the polarization nulling method.  This method takes advantage of the fact that the signal under investigation has a defined state of polarization, while the noise is unpolarized.  Polarization nulling provides a maximum and minimum power value: at the maximum, the noise below the signal corresponds to half the power of the total depolarized noise. In the corresponding minimum position the noise level can be measured directly.  An application note, referenced below, can provide detailed measurement information.