SearcharxivSearch

arXiv · 2112.12730

Almost everywhere ergodicity in quantum lattice models

Abstract

We rigorously examine the ergodic properties of quantum lattice models with short range interactions, in the C* algebra formulation of statistical mechanics. Ergodicity results, in the context of group actions on C* algebras, assume that the algebra is asymptotically abelian, which is not the case for time evolution. The Lieb-Robinson bound tells us that the spatial extent of the time evolution of operators is exponentially small outside a light-cone, defined by the Lieb-Robinson velocity. More precisely, this means that the algebra of observables is asymptotically abelian only in a space-like region. This implies a form of ergodicity outside the light-cone, but what happens within it? We show that the long-time average of connected correlation functions of observables, along space-time rays of almost every speed, vanishes. This holds in any state that is invariant under space-time translations and that satisfies weak clustering properties in space. Further, we show that the long-time limit of the n-th moment, with respect to the state, of a ray-averaged observable converges to the n-th power of its ensemble average, which means that there are no fluctuations of ray averages in the long time limit. This is a statement of ergodicity. The ray averages can also be performed in a way that accounts for oscillations, showing that correlations (and moments) of the ray averaged observables cannot sustainably oscillate in the long time limit. Finally, we show that in the GNS representation of the algebra of observables, for any KMS state with the above properties, the long-time limit of the ray averaged commutator converges (in the strong operator topology (SOT)) to 0 and the ray average of any observable converges (in the SOT) to a multiple of the identity. This indicates that observables get "thinner" almost everywhere within the light-cone.

Explore related subjects

Keep this discovery

BibTeXRIS

Dimitrios Ampelogiannis, Benjamin Doyon. 2021-12-23. Almost everywhere ergodicity in quantum lattice models. https://doi.org/10.1007/s00220-023-04849-9

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