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Nicholas B. Tufillaro

Publications and source records attributed to Nicholas B. Tufillaro.

13 recordsLinked to original sources

Symmetry and the Form of Nonlinear Behavioral Models: A Tutorial for Microwave Engineers

Behavioral models of nonlinear microwave devices -- the Cardiff model, X-parameters, the higher-order describing functions of the mechanical-systems literature -- all share a functional form that is usually presented as a modeling choice. This tutorial shows that the form follows from a single physical statement, that nothing physical depends on where the clock is started. It develops the consequences of that statement assuming phasors and harmonic balance but no group theory, and uses them to give the Cardiff model's three exponents physical interpretations. The magnitude exponent $m$ turns out to be the order of the device's load-side nonlinearity; the phase exponent $n$ is set by the drive-side harmonic; and the conjugate index $r$ obeys $r_{\max}=\lfloor K/2\rfloor$, where $K$ is the degree of the load-side nonlinearity. The familiar restriction $r\le1$ is therefore a statement about the device, exact whenever $K\le3$, and it can be tested on a bench. The final sections show that a tailored A-pull measurement displays this decomposition directly: each spectral cluster's half-width is the order of the nonlinearity that produced it. The tutorial is pedagogical: the material overlaps largely with a companion paper (arXiv:2609.35828), which states and proves the theorems in full; this tutorial starts at a more elementary level and is meant as a gentler introduction to the results treated in more detail there.

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Memory in Behavioral Models as Motion on a Slow Invariant Manifold

A single-tone large-signal operating point of a nonlinear two-port is a periodic orbit of a periodically forced circuit. When the device has memory (self-heating, trapping), the Floquet exponents of that orbit separate into fast (electrical) and slow (thermal and trapping) modes, and long-term memory is motion on the invariant manifold attached to the slow modes. An existence and uniqueness theorem for that manifold follows from the parameterization method of Cabré, Fontich and de la Llave, applied to the stroboscopic map at the orbit; the manifold is the spectral submanifold of Haller and Ponsioen, without a small-forcing parameter. The manifold is a bundle over the circle of drive phase, its fiber dimension the number of slow Floquet exponents, and the dynamic X-parameter kernel of Verspecht et al. identifies its reduced dynamics from step changes of the drive amplitude. Consequently, an exact reduced model has as many memory states as slow exponents, the memoryless X-parameter surface is the fixed-point family of the reduced dynamics, and the envelope-domain model is the reduced dynamics driven by the envelope. The hypotheses are verified and the manifold constructed for a GaN HEMT compact model with a three-pole thermal network and a drain-lag trap: the trap contributes a $14\,μ$s time constant set by the linearization and not by its $6$ ms emission time, the thermal submanifolds are nearly flat with linear reduced dynamics, and the expansion in the trap direction is valid only within a few thermal voltages ($nV_T\approx26$ mV), so trap memory needs a global representation of the manifold.

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Time Invariance, Circle Symmetry, and the Completeness of the Cardiff Behavioral Model

The functional form shared by frequency-domain behavioral models of nonlinear microwave devices (the Cardiff model, X-parameters, higher-order sinusoidal describing functions) is usually presented as a modeling choice; here it is shown to follow from time invariance. Under a shift of the time origin the $k$-th harmonic phasor rotates by $k$ times the fundamental's angle, so the spectral map of a time-invariant device is equivariant under a weighted action of the circle group, and classical invariant theory gives the general form of every such map; the three communities' phase-normalization factors are its weight-carrying factor. The result is a completeness theorem: in single-tone periodic steady state no time-invariant two-port response lies outside the Cardiff form, and the index relation $m=|n|+2r$ is the smoothness condition at zero load wave. Writing each Cardiff term as a monomial $A^{a}\bar{A}^{b}$ in the load wave gives the exponents physical interpretations -- $m$ is the order of the load-side nonlinearity, $n$ set by the drive-side harmonic, $r=\min(a,b)$ the number of conjugate pairs -- and the bound $r_{\max}=\lfloor K/2\rfloor$ for load-side polynomial degree $K$, so the familiar restriction $r\le1$ is exact for a cubic load-side nonlinearity and fails at fourth order. For a loaded device the bound becomes a measurable decay in $r$. Tailored A-pull measurement displays the decomposition directly, and two simulations reproduce its published pattern of detected terms and place the first fourth-order term near $-58$ dBc, between that measurement's $-40$ dBc spurious floor and its $-60$ dBc noise floor.

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Braid analysis of chaos

The (forced) periodic orbit spectrum is calculated for a chaotic time series (BZ reaction).

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Braid analysis of a bouncing ball

Prunning front is calculated for a bouncing ball system and the results are compared to a braid analysis. To Appear in Physical Review E.

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Teardrop and heart orbits of a swinging Atwood's Machine

An exact solution is presented for a swinging Atwood's machine. This teardrop-heart orbit is constructed using Hamilton-Jacobi theory. The example nicely illustrates the utility of the Hamilton-Jacobi method for finding solutions to nonlinear mechanical systems when more elementary techniques fail.

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Discrete Dynamical Models Showing Pattern Formation in Subaqueous Bedforms

A new class of ``toy models'' for subaqueous bedform formation are proposed and examined. These models all show a similar mechanism of wavelength selection via bedform unification, and they may have applications to bedform stratigraphy. The models are also useful for exploring general issues of pattern formation and complexity in stochastically driven far from equilibrium systems.

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Topological organization of (low-dimensional) chaos

Recent progress toward classifying low-dimensional chaos measured from time series data is described. This classification theory assigns a template to the time series once the time series is embedded in three dimensions. The template describes the primary folding and stretching mechanisms of phase space responsible for the chaotic motion. Topological invariants of the unstable periodic orbits in the closure of the strange set are calculated from the (reconstructed) template. These topological invariants must be consistent with any model put forth to describe the time series data, and are useful in invalidating (or gaining confidence in) any model intended to describe the dynamical system generating the time series.

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