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Yefan Wu

Publications and source records attributed to Yefan Wu.

3 recordsLinked to original sources

Curvature-Dependent Path Concentration in Stochastic Fast-Slow Systems with Noise on the Slow Variable

We study stochastic fast-slow systems in which the noise acts exclusively on the slow variable: $dx = f(x,y)\,dt$, $dy = \varepsilon\,g(x,y)\,dt + \sigma\,h(y)\,dW_t$. While the path-concentration theory for noise on the fast variable is well developed, the complementary case of noise only on the slow variable has remained largely unexplored, with a recent exception treating the fold bifurcation. For general, uniformly normally-hyperbolic deterministic slow manifolds $x = X^*(y)$, we derive rigorous pathwise estimates showing that the deviation $z = x - X^*(y)$ concentrates with exponential tail bounds over the slow timescale $[0,T/\varepsilon]$. A central finding is that the It\^o correction arising from the curvature $D^2X^*$ of the slow manifold introduces a systematic $O(\sigma^2\|D^2X^*\|)$ bias that tightens the concentration bound beyond the classical $\sigma/\sqrt{\lambda_0}$ tube width. We identify a geometric critical noise scale $\sigma_c(\varepsilon) = C_0\min\!\bigl(\sqrt{\varepsilon},\, \varepsilon^{1/4} L_{\mathrm{geom}}/\sqrt{\lambda_0}\bigr)$, where $L_{\mathrm{geom}} = \sqrt{\lambda_0/(\|D^2X^*\|\|h\|^2)}$ is a local geometric scale of the manifold. For $\sigma \le \sigma_c$, the fast variable tracks the manifold to within $C\bigl(\varepsilon/\lambda_0 + \sigma^2\|D^2X^*\|\|h\|^2/(2\lambda_0) + \sigma/\sqrt{\lambda_0}\bigr)$ with probability at least $1 - e^{-\kappa/\varepsilon} - e^{-C_K}$, where $C_K > 0$ depends on the confinement of the slow dynamics. We also prove that the slow-variable adiabatic error is $O(\varepsilon + \sigma\sqrt{\varepsilon} + \sigma^2\|D^2X^*\|)$, which is dominated by classical terms when $\sigma \le \sigma_c$; hence curvature governs fast-variable path concentration but not adiabatic validity.

math.PR

Breakdown of Adiabatic Scaling and Noise-Induced Functional Synchronization in Deeply Quiescent Excitable Systems

Coherence resonance (CR) characterizes noise-induced regularity in excitable systems, yet its evaluation in quiescent biological media is often obscured by flattened energy landscapes and complex nonlinear dynamics. In this study, we investigate the stochastic dynamics of a 3D Sherman-Rinzel-Keizer (SRK) model driven by multiplicative Feller noise. We show that traditional extremal evaluations of CR encounter a "bathtub effect", a broad resonance valley that can lead to statistical inaccuracies. To address this, we propose a logarithmic centroid extraction method, which filters out stochastic jitter and recovers the underlying adiabatic Kramers scaling with high linearity. Furthermore, we identify the physical boundary where this adiabatic approximation breaks down under the strong-noise limit. Extending our analysis to gap-junction coupled systems, we observe a noise-induced transition from sub-threshold physiological shivering (characterized by statistical correlation but negligible functional output) to macroscopic functional synchronization. Our results provide a mathematical framework for extracting optimal noise intensities in broad energy valleys and offer insights into how quiescent biological systems utilize stochastic fluctuations for functional recovery.

cond-mat.stat-mech

Noise-Induced Transitions and Coherence Resonance in a 5D Conductance-Based Neuronal Model

Intrinsic channel noise is an important source of variability in neuronal dynamics, but its state-dependent and boundary-constrained nature can be difficult to represent numerically. Here, we investigate the effects of bounded multiplicative noise applied to the slow M-current gating variable in a five-dimensional conductance-based model of a CA1 pyramidal neuron. We employ a full-truncation semi-implicit Euler scheme to control boundary violations and perform Monte Carlo parameter sweeps, time-step checks, burst-detection sensitivity analyses, and conductance perturbations. In subthreshold regimes, noise induces firing and produces an intermediate-noise minimum in the coefficient of variation, consistent with coherence resonance. In the deep subthreshold regime, the burst rate exhibits moderate Arrhenius-like scaling over a restricted low-noise interval, supporting an interpretation in terms of noise-activated escape. Near the numerically identified onset of sustained oscillations, temporal coherence is particularly sensitive to noise intensity. In the suprathreshold regime, strong multiplicative noise accelerates firing through premature stochastic exits from the hyperpolarized recovery branch, although this behavior does not follow classical Kramers scaling. Control simulations using clipped additive Gaussian noise produce qualitatively different dynamics, indicating that the state dependence and boundary behavior of the diffusion term materially affect the observed transitions. The main trends remain robust under the tested variations in numerical resolution, burst-detection threshold, slow timescale, and M-current conductance. These results characterize model-specific effects of boundary-constrained channel noise and motivate future comparisons with discrete-state ion-channel models.

q-bio.NC