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This paper challenges the conventional assumption of independence in spatially resolved detection within diffusion-coupled thermal atomic vapors. It introduces a field-theoretic framework where sub-ensemble correlations are governed by a global spin-fluctuation field's spatiotemporal covariance. This leads to a new understanding of statistical independence and a limit on the number of distinguishable sub-ensembles, with implications for multi-channel atomic magnetometry and other diffusion-coupled stochastic fields.
Reference

Sub-ensemble correlations are determined by the covariance operator, inducing a natural geometry in which statistical independence corresponds to orthogonality of the measurement functionals.