Sub-Ensemble Correlations as a Covariance Geometry

TL;DR

This paper reveals that correlations in diffusion-coupled atomic vapors are governed by a global covariance structure, challenging the assumption of independent localized responses and establishing a geometric framework for sub-ensemble correlations.

Contribution

It introduces a unified field-theoretic approach to describe sub-ensemble correlations as projections of a single stochastic field, defining a natural geometry based on covariance operators.

Findings

Correlations are governed by the covariance of a global spin-fluctuation field.

The covariance spectrum limits the number of distinguishable sub-ensembles.

Shared access to fluctuation modes causes unavoidable statistical coupling.

Abstract

Conventional practice of spatially resolved detection in diffusion-coupled thermal atomic vapors implicitly treat localized responses as mutually independent. However, in this study, it is shown that observable correlations are governed by the intrinsic spatiotemporal covariance of a global spin-fluctuation field, such that spatial separation specifies only overlapping statistical projections rather than independent physical components. A unified field-theoretic description is established in which sub-ensembles are defined as measurement-induced statistical projections of a single stochastic field. Within this formulation, sub-ensemble correlations are determined by the covariance operator, inducing a natural geometry in which statistical independence corresponds to orthogonality of the measurement functionals. For collective spin fluctuations described by a diffusion-relaxation Ornstein-Uhlenbeck stochastic field, the covariance spectrum admits only a finite set of fluctuation modes in a bounded domain, imposing an intrinsic, field-level limit on the number of statistically distinguishable sub-ensembles. The loss of sub-ensemble independence is formalized through the notion of spatial sampling overlap, which quantifies the unavoidable statistical coupling arising from shared access to common low-order fluctuation modes. While multi-channel atomic magnetometry provides a concrete physical setting in which these constraints become explicit, the framework applies generically to diffusion-coupled stochastic fields.