SOURCEFORGE » RALF » 2015 Evaluation and test of an optical / L-band tranceiver

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h1. 3.3 Intermodulation (IMD)

Intermodulation measures the non-linear distortions on the signal.

h2. 3.3.1 Creation of two tones for Intermodulation test

To measure the intermodulation in our system is necessary to generate two sinus at the input of the optical system and to evaluate them at the output. As the signal generator couldn't provide two sinus at the same time it has been decided to use the USRP with a Labview program to do so.

An already programmed Labview example in which one tone was generated was modified in order to do so:

p=. !{width:700px}Main_Front_Panel.png!
Figure 1. Front Panel used to generate two sinus

Then, the part of the Labview block in which the tone was generated was duplicated, adding a new output and having the result observed below:

p=. !{width:400px}Generate_Waveform.png!
Figure 2. Block modified to generate two sinus

After the Labview modifications it could be observed at the output of the USRP the two tones:

p=. !{width:500px}two_sinus.jpg!
Figure 3. Two sinus output from the USRP

h2. 3.3.2 Measurement results

In Figure 4, 5 and 6 we can observe the different intermodulation results for 0.7, 1 and 2 GHz:

p=. !{width:700px}IMD_700MHz.png!
Figure 4. 3rd order Intermodulation vs Input Power @ 700 MHz

p=. !{width:700px}IMD_1000MHz.png!
Figure 4. 3rd order Intermodulation vs Input Power @ 1000 MHz

p=. !{width:700px}IMD_2000MHz.png!
Figure 6. 3rd order Intermodulation vs Input Power @ 2000 MHz

As showed in the IMD figures, the IMD is more important as the output signal increases.

p=. !{width:700px}SFDR.png!
Figure 6. Spurious Free Dynamic Range (SFDR) @ 2000 MHz