arXiv:2610.35933v1 Announce Type: new Abstract: We study deterministic causal quantization with pathwise error at most $\varepsilon$, using $\omega$ shared representatives updated from transmitted addresses alone. For a midpoint realization with first-in, first-out replacement, we compare address entropy rates with process $\varepsilon$-entropy, the least entropy rate of any block quantizer meeting the same constraint. From $\varepsilon$-separated initialization, the gap is at most two bits per sample for every stationary source with finite scalar $\varepsilon$-entropy, without density, independence or mixing assumptions. A causal address-tree argument extends this comparison to any synchronized quantizer with cell overlap $m$, giving $\log_2 m$ bits. Lattice initialization with consistent boundary ownership realizes uniform grids with sharp one-bit scalar and process comparisons. Under an entropy condition and finite Fisher information rate $J$, the gap is at most $2J\varepsilon^2/(\pi^2\ln 2)$; general initializations add a term of order $\omega\varepsilon\sqrt{J}$. The scalar grid estimate gives a nonasymptotic form of R\'enyi's theorem. Since a grid is causal, the price of causality is at most $\min\{1,2J\varepsilon^2/(\pi^2\ln 2)\}$ bits per sample, versus the high-resolution squared-error loss $\tfrac12\log_2(\pi e/6)$. These bounds certify $\varepsilon$-entropy brackets for autoregressive Laplace and Gaussian sources. For memoryless sources, the optimal causal rate equals the scalar $\varepsilon$-entropy. For a stationary process on finitely many $2\varepsilon$-separated centers, adding independent uniform noise of width $2\varepsilon$ gives exact Shannon lower-bound equality at every block length, attained by storing those centers. This includes histograms with finitely many bins. Storing two non-lattice centers beats every uniform grid of the same cell width by half a bit per sample.
Continue to arXiv Mathematics →You are being forwarded in 6s — stay on this page