2000 IEEE MTT-S International Microwave Symposium Digest (Cat. No.00CH37017)
DOI: 10.1109/mwsym.2000.861046
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A unified approach of PM noise calculation in large RF multitone autonomous circuits

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Cited by 14 publications
(9 citation statements)
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“…Equation (25) can be solved by resorting to a Newton-iteration scheme. So doing, at each step a linear equation must be solved whose coefficients matrix is (26) and the partial derivatives in (26) are evaluated at the current approximation (for the -th iteration). If the Newton-iteration scheme converges, both an initial condition on the limit cycle and the cycle period are found and the matrix (27) is the correct sensitivity matrix exhibiting at least one eigenvalue equal to 1.…”
Section: A Shooting Methodsmentioning
confidence: 99%
“…Equation (25) can be solved by resorting to a Newton-iteration scheme. So doing, at each step a linear equation must be solved whose coefficients matrix is (26) and the partial derivatives in (26) are evaluated at the current approximation (for the -th iteration). If the Newton-iteration scheme converges, both an initial condition on the limit cycle and the cycle period are found and the matrix (27) is the correct sensitivity matrix exhibiting at least one eigenvalue equal to 1.…”
Section: A Shooting Methodsmentioning
confidence: 99%
“…In this case, during the simulation of the PLL with the VCO-DIV, the additional equation (13) is solved for ∆θ noise,vco (t) by the simulator, with ∆θ 1 (t) obtained as in (11).…”
Section: B Device-noise Analysismentioning
confidence: 99%
“…We are motivated in creating a phase model just for the VCO and divider (seen as a single oscillator) since the perturbation theory on oscillators is robust [13], while doing so for the other PLL's blocks might require simplifications on the circuit's behavioral model, resulting in a loss of accuracy with respect to transistor-level simulations. Besides, our methodology is based on well-known analyses in the circuit simulation area, i.e., SST computation-based methods (Harmonic Balance (HB) [9] or the Shooting method [10]) and SST noise analyses (the conversion matrix method [11], [12] or the perturbation projection vector (PPV) [13], [14]) for the construction of the phase macromodel, so that designers could be able to validate it with a little effort. The creation of the phase model can be done, e.g., in Verilog-A language, enriching it with equations and input parameters we provide here, together with guidelines for our procedure, with some remarks on how to automate it.…”
mentioning
confidence: 99%
“…Circuit simulations have been successively carried out with a time domain Monte Carlo (TDMC) simulator, which avoid linearization [25], and a frequency domain simulator developed in our laboratory which performs the phase noise calculation using the Conversion Matrices Method (C.M.M.) [20], [26], [27]. The noise analysis in the frequency domain is derived from HB method by a linearization of the nonlinear network equation around the steady state solution to construct a linear periodically time varying model of the oscillator circuit.…”
Section: Oscillator Phase Noise Analysismentioning
confidence: 99%
“…Be careful, an inaccurate steady state solution can lead to inaccurate phase noise simulation results near the carrier [27]. Ignoring this numerical problem of steady state solution accuracy on the phase noise calculation has been a great source of confusion in the past!…”
Section: Oscillator Phase Noise Calculation By Means Of Cmmmentioning
confidence: 99%