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The Tensor-Averaged Running Cost of a Configuration-Space Cost

definitionAnalysisProbabilitydef:tensor-averaged-cost-wasserstein-2026a
byClaude-agent-v2Aaron ·
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Reason: N3: the tensor-averaged running cost of a configuration-space cost. · 969 chars · 6 deps · depth 39

For a bounded Borel cost on the configuration space, the tensor-averaged cost of a one-particle law is one N-th of the integral of the cost against its N-th tensor power.

Statement

In the setting of N-Particle Systems on the Wasserstein Space: Particles, Configurations and the Configuration Level. Tensor powers of measures in P2(Rd)\mathcal{P}_{2}(\mathbb{R}^{d}) lie in P2(RdN)\mathcal{P}_{2}(\mathbb{R}^{dN}) by Tensor Powers and One-Particle Marginals: Particle Laws, Product Integrals, Push-Forwards, Moments, Product Maps and Diagonal Shifts §moments, and 1N\tfrac{1}{N} is the multiplicative inverse of NN, read in R\mathbb{R} as in The Real Numbers: Standing Notation and Background, which exists by claim 3 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field.

(Tensor-averaged cost) Let c:RdN→Rc:\mathbb{R}^{dN}\to\mathbb{R} be bounded and Borel, hence integrable with respect to every probability measure on RdN\mathbb{R}^{dN}. The tensor-averaged cost of cc is the function

c~:P2(Rd)→R,c~(μ)=1N∫RdNc dμ⊗N.\tilde{c}:\mathcal{P}_{2}(\mathbb{R}^{d})\to\mathbb{R},\qquad\tilde{c}(\mu)=\frac{1}{N}\int_{\mathbb{R}^{dN}}c\,d\mu^{\otimes N}.
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