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Lesson 9: Design of a broadband Raman amplifier using<br />

subsystems<br />

Overview<br />

The number of channels deployed in long-haul DWDM systems is rapidly increasing beyond<br />

hundreds of channels over the C-band (1528-1563 nm) and L-band (1575-1610 nm). This<br />

demand for more bandwidth is driving the search for new and more sophisticated fiber amplifiers<br />

that are flattened over a very wide spectral range for maximum bandwidth transmission over the<br />

long haul.<br />

The specifics of the stimulated Raman scattering effect allow for an interesting technique for gainflattening<br />

of broadband Raman amplifiers (Y. Emori, K. Tanaka and S. Namiki, Electron. Lett. 35,<br />

1355, 1999). It requires only a suitable multiple-pump configuration and does not rely on passive<br />

filters, gratings, etc.<br />

Definition of Multi-line source<br />

At an initial stage of the pump system lets set up a group of twelve pump laser diodes having<br />

“Parameterized” signal representations and the following wavelengths and powers:<br />

LD λ [nm] P [mW] LD λ [nm] P [mW]<br />

1 1405.0 322 7 1450.0 122<br />

2 1412.5 311 8 1457.5 113<br />

3 1420.0 311 9 1465.0 110<br />

4 1427.5 346 10 1480.0 127<br />

5 1435.0 115 11 1495.0 126<br />

6 1442.5 92 12 1510.0 219<br />

After that we multiplex their outputs using, for instance, two multiplexers and a 2x1 power<br />

combiner. The channels of the multiplexers should be accordingly adjusted to the<br />

wavelengths of the pumps, as shown for the case of the 8x1 multiplexer:<br />

Figure 87 -Adjusting multiplexer channels<br />

65

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