SearcharxivSearch

arXiv · 2407.16817

Kuramoto model on Sierpinski Gasket I: Harmonic maps

Abstract

Motivated by the study of attractors in the Kuramoto model (KM) on graphs approximating the Sierpinski gasket (SG), we revisit the problem of harmonic maps (HMs) from SG to the circle, first considered by Strichartz. We provide a geometric proof of Strichartz's theorem, which states that for a prescribed degree and suitable boundary conditions, there exists a unique HM from SG to the circle. We extend this result to HMs on post-critically finite (p.c.f.) fractals. For continuous functions on SG, we define a degree given by vector of integers of arbitrary finite length. We show that the degree determines a homotopy class on SG with values in the circle. This provides an analog of the Hopf degree theorem on SG. We move on to analyze HMs. At the heart of our method lies an original construction of covering spaces. After lifting continuous functions on SG with values in the unit circle to continuous real-valued functions on the covering space, we use the harmonic extension algorithm to obtain a harmonic function on the covering space. The desired HM is obtained by restricting the domain of the harmonic function to the fundamental domain and projecting the range to the circle. Each covering space is constructed separately for HMs of a given homotopy class, capturing its intrinsic topology. We show that with suitable modifications the method applies to p.c.f. fractals, a large class of self-similar domains. We illustrate our method using numerical examples of HMs from SG to the circle and discuss the construction of covering spaces for several representative p.c.f. fractals, including the 3-level SG, hexagasket, and pentagasket. The results of this paper provide the foundation for a follow-up work where we give a complete description of attractors in the KM on graphs approximating p.c.f. fractals. Specifically, we show that all HMs identified in this paper are stable steady states of the KM.

Explore related subjects

Keep this discovery

BibTeXRIS

Georgi S. Medvedev, Matthew S. Mizuhara. 2024-07-23. Kuramoto model on Sierpinski Gasket I: Harmonic maps. https://arxiv.org/abs/2407.16817

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Why we should condition denoising diffusion generative models on windows of past observations

Data assimilation (DA) is, traditionally, a cycling process that relies on time-dependent priors to propagate information from past observations to future cycles. Using denoising diffusion generative modeling for DA is challenging because standard approaches use a fixed training data set, which in turn leads to a static prior that ignores information from past observations. Because past observations are ignored, DA systems with static priors lead to larger posterior errors than cycling DA systems. Incorporating time-dependent priors into generative models, however, requires expensive and frequent retraining. Motivated by linear systems theory - where the dependence of a prediction of a Kalman filter on past observations decays exponentially - we condition diffusion models on short windows of past observations. Specifically, we describe training procedures for two frameworks: a diffusion DA system predicting the current state given a set of past observations, and a diffusion ``direct observation prediction'' (DOP) system, predicting future observations given a set of past observations. Using a canonical linear system, we show that both systems can achieve the minimal posterior error characteristic of a fully-cycled DA/DOP system, without re-training, provided the time windows are long enough. The linear setup ensures analytical tractability, avoids confounding neural network training errors, and confirms that conditioning on windows of past observations is required for efficient and accurate diffusion-based DA or DOP.

math-ph

The kinematic structures and the inertial geometry of a moving charge

We ask how much of the geometry a charged particle moves in is fixed by its motion, and how much a particle must bring. We ask of a symplectic structure only that it relate velocity to momentum as Hamilton's equations do, and we ask it of every energy at once. In particular, we show that the structures meeting that demand are the canonical one and its twists by a closed two-form of the base. A field provides the two-form, a particle the multiplier before it, which we identify constitutively with its charge. Thus, a single energy governs a family of structures, and each particle takes the one its charge fixes. We then ask what a particle must bring to be given a momentum, and we show that the degree of that map settles the degree at which a field enters Newton's Second Law. An antisymmetric bilinear form returns no Lorentz force, whilst a Randers metric returns one --- a length whose difference from a Riemannian one is linear in the velocity. Moreover, we find that metric already within the twisted structure, as its primitive over a level of the free energy, and its law of transport to be nonlinear, no affine connection being known to serve. Under an indefinite signature the length parts from the dynamics, and the extremals turn from shortest to longest. On the round sphere a monopole flux leaves no such metric, whilst the transport remains and prequantisation, given a unit of action, restricts the charge to a lattice. In this manner, we conclude that each charge-to-mass ratio receives a geometry of its own, so that by a functionalist criterion none of them is the spacetime of a charged particle.

math-ph