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Online proceedings - EDA Publishing Association

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The simulation output phase noise has been compared with the<br />

theoretical phase noise from Leeson effect.<br />

11-13 May 2011, Aix-en-Provence, France<br />

One can calculate the phase noise of such an oscillator with<br />

the Leeson effect [5], and examine the phase noise variations<br />

with the resonator physical parameters. The Leeson equation<br />

between the oscillator and the feedback amplifier [6] phase<br />

spectral densities follows relation (8):<br />

Leeson frequency<br />

17Hz<br />

1 ν<br />

0 2<br />

Sϕ<br />

( f ) = [1 + ( ) ] S ( f )<br />

2 φ<br />

(8)<br />

f 2Q<br />

S ϕ<br />

( f ) is the phase spectral density of the oscillator<br />

S φ<br />

( f ) is the phase spectral density of the amplifier<br />

ν<br />

0 is the resonance frequency and Q is the quality factor of<br />

the resonator.<br />

f is the offset frequency from the carrier.<br />

The cut-off frequency, called Leeson’s frequency, is:<br />

ω<br />

f L<br />

= 0<br />

(9)<br />

2Q<br />

Simulations are run taking the physical quantities of the VIA<br />

(table 1) into account. The quality factor of the characteristic<br />

equation (1) is:<br />

Fig. 8. phase noise output<br />

This Leeson's model theoretical value matches the verilog-A<br />

model simulation described above. Leeson’s frequency varies<br />

only with the damping coefficient and the mass.<br />

In the next simulations, only the mass of the<br />

resonator is changed. The theoretical Leeson's frequency is<br />

proportional to m -1 . We have previously shown that the<br />

Leeson's frequency was 15.5 Hz with a mass of 1.10 -8 kg. For<br />

1.10 -9 kg and 1.10 -10 kg, we have respectively frequencies of<br />

155Hz and 1.55 kHz, as verified by the following simulation<br />

on figure 9:<br />

ω m<br />

Q = 0<br />

(10)<br />

ρ<br />

x<br />

The Leeson’s frequency is:<br />

ρ<br />

x<br />

f<br />

L<br />

= (11)<br />

2m<br />

f L<br />

= 15. 5Hz<br />

Phase noise analysis is performed with Virtuoso simulator and<br />

the output signal is selected to create the phase noise output. It<br />

becomes possible to read the Leeson’s frequency (figure 8).<br />

Fig. 9. phase noise output depends on the mass<br />

C. Influence of the transconductance amplifier noise<br />

The white noise and flicker noise can be added to this<br />

model and particularly to the transconductance amplifier<br />

block.<br />

1. White noise<br />

White noise function is added to the the transconductance<br />

amplifier plus pin. Therefore, we add a VerilogA block. A<br />

Cadence special function is used : white_noise().<br />

395

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