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Edwin Jan Klein - Universiteit Twente

Edwin Jan Klein - Universiteit Twente

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Chapter 7<br />

Figure 7.12. Measured eye patterns of the<br />

input signal (top) and the signal at IDrop1<br />

(bottom). The resonator is tuned “on<br />

resonance”.<br />

168<br />

Figure 7.13. The Measured eye patterns of<br />

the signal at IDrop1 when the resonator is tuned<br />

“off resonance”.<br />

The multicasting feature of the OADM as it was shown in Figure 7.4 (for customers 1<br />

and 5) was tested by tuning the first two resonators in the OADM such that each drops<br />

an equal part of the input signal as is illustrated in Figure 7.14 (the figure is idealized,<br />

typically MR1 is tuned so that it drops 50 % while MR2 is tuned to be on-resonance<br />

to drop the rest of the signal). Figure 7.15 shows the two eye patters that were<br />

measured at IDrop1 and IDrop2 and for this configuration. Although the amplitude of the<br />

measured signals was lower compared to a single dropped signal, as can be expected,<br />

the eye-patterns are still open. This shows that, at a bitrate of 40 Gbit/s, this OADM is<br />

indeed capable of multicasting.<br />

Dropped power (dB)<br />

0<br />

-3<br />

-6<br />

-9<br />

-12<br />

-15<br />

MR1<br />

MR 2<br />

-18<br />

1548 1549 1550<br />

Wavelength (nm)<br />

1551 1552<br />

Figure 7.14. Multicasting principle: Each<br />

resonator is tuned such that only part of the<br />

signal (at λ=1550 nm) is dropped.<br />

Figure 7.15. Multicasting principle: Each<br />

resonator is tuned such that only part of the<br />

signal (at λ=1550 nm) is dropped.

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