2013
DOI: 10.1109/tcsi.2013.2252452
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A Deep Investigation of the Synchronization Mechanisms in LC-CMOS Frequency Dividers

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Cited by 22 publications
(23 citation statements)
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“…However, formulas are not able to predict a constant phase offset 0 = 5 ∘ , that is, due to the reactive behavior of nonlinearities, which were here assumed to be memoryless. Finally, it should be observed that the accuracy of amplitude formula is better for small injection values as it is derived assuming small injection values and neglecting output harmonics [21][22][23][24][25][26]. Thus, we can conclude that, even if small discrepancies are present between experimental and analytical results, formulas are able to capture the main characteristics of the injectionlocking phenomenon, providing a quite good approximation to experimental results.…”
Section: Resultsmentioning
confidence: 84%
“…However, formulas are not able to predict a constant phase offset 0 = 5 ∘ , that is, due to the reactive behavior of nonlinearities, which were here assumed to be memoryless. Finally, it should be observed that the accuracy of amplitude formula is better for small injection values as it is derived assuming small injection values and neglecting output harmonics [21][22][23][24][25][26]. Thus, we can conclude that, even if small discrepancies are present between experimental and analytical results, formulas are able to capture the main characteristics of the injectionlocking phenomenon, providing a quite good approximation to experimental results.…”
Section: Resultsmentioning
confidence: 84%
“…To determine these modes, let us consider the circuit in Fig. 2 where the nonlinearity of the active part of the circuit is carefully approximated through the third-degree polynomial , where is the differential trans-conductance of MOS devices at the quiescent point, and [24]- [27]. Consequently, we get , .…”
Section: B Amplitudes Of Oscillationmentioning
confidence: 99%
“…According to this method, the amplitude and phase of the first harmonic of v are considered slowly varying quantities, that is, v ( t ) t = w ( t ) + h ( t ), where w ( t ) = W ( t )cos[ ωt + θ ( t )] denotes the first harmonic of v and h ( t ) the sum of the remaining harmonics. Thus, by using the averaging method, equation is reduced to a system of first‐order equations for the amplitude and the phase of w ( t ), which take the form (Appendix) trueW˙()t=prefix−12RCW12CIc trueθ˙()t=()ω0ω+12CWIs where the dot denotes the time derivative, and I c and I s denote the cosine and sine coefficients of the fundamental harmonic of i ( w + h , v in ), respectively. The quantity h is given by the solution of the linear equation d2hdt2+1RCdhdt+ω02h=prefix−1Cddtih(),wvitalicin where i h ( w , v in ) denotes the harmonics of i ( v , v in ) that we assume to be slightly dependent on the harmonics of v , so that i h ( w + h , v in ) ≈ i h ( w , v in ).…”
Section: Model Of Driven Oscillators Under Weak Injectionmentioning
confidence: 99%