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Radio Frequency Integrated Circuit Design - Webs

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300 <strong>Radio</strong> <strong>Frequency</strong> <strong>Integrated</strong> <strong>Circuit</strong> <strong>Design</strong><br />

R ′cap = 2�1 + C 2<br />

C 1� 2<br />

3.83 pF<br />

R cap = 2�1 +<br />

4.72 pF� 2<br />

3.1 k� = 20.3 k�<br />

Thus, the total parallel resonator resistance is R p = 843�.<br />

V tank ≈ 2I bias� C 1<br />

C 1 + C 2� R p<br />

I bias = V tank<br />

2R � p C 1 + C 2 1.6V<br />

C � =<br />

1 2(843�)�<br />

4.72 pF + 3.83 pF<br />

4.72 pF<br />

�<br />

= 1.71 mA<br />

The next thing to do is to size the transistors used in the tank. Transistors<br />

were chosen to be 25 �m.<br />

We can also estimate the phase noise of this oscillator.<br />

The re of the transistor at this bias is<br />

re = v T<br />

IC<br />

= 25 mV<br />

= 14.8�<br />

1.69 mA<br />

Since this value will seriously affect our estimate, we also take into account<br />

5� for parasitic emitter resistance (this value can be determined with a dc<br />

simulation).<br />

R re tank = 2�1 + C 1<br />

C 2� 2<br />

4.72 pF<br />

re = 2�1 +<br />

3.78 pF� 2<br />

19.8� = 200�<br />

This can be added to the existing losses of the overall resonator resistance<br />

of 843� to give 162�.<br />

Now we can compute the Q:<br />

Q = R tank√ C total<br />

L<br />

= 162� √ 1.18 pF<br />

4nH<br />

We need to estimate the available power:<br />

PS =<br />

2<br />

V tank (1.6V)2<br />

= = 7.9 mW<br />

2R tank 2(162�)<br />

= 2.78<br />

We can now estimate the phase noise of the oscillator. We will assume<br />

that the phase noise due to K VCO is not important.

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