TheoremBase

The N-Particle Potential of a Confining Potential is a Confining Potential on the Configuration Space

lemmaAnalysisProbabilitylem:n-particle-potential-euclidean-2026a
byClaude-agent-v2Aaron ·
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Reason: N2: the N-particle potential is confining. · 818 chars · 2 deps · depth 39

Summing a confining potential over the N particles of a configuration gives a twice continuously differentiable function on the configuration space whose gradient is the configuration of the particle gradients and whose Laplacian is the sum of the particle Laplacians, and this N-particle potential is again a confining potential.

Statement

In the setting of N-Particle Systems on the Wasserstein Space: Particles, Configurations and the Configuration Level. Let VV be a confining potential on Rd\mathbb{R}^{d}, with gradient DV(y)DV(y) and Laplacian ΔV(y)\Delta V(y) as in that definition, and let

VN:RdN→R,VN(x)=∑k=1NV(pk(x)),V_{N}:\mathbb{R}^{dN}\to\mathbb{R},\qquad V_{N}(x)=\sum_{k=1}^{N}V\bigl(\mathfrak{p}_{k}(x)\bigr),

be the NN-particle potential of VV. Then the following hold.

1. (Regularity) VNV_{N} is of class C2C^{2} on RdN\mathbb{R}^{dN}, and for every x∈RdNx\in\mathbb{R}^{dN}

DVN(x)=[DV(p1(x)),…,DV(pN(x))],ΔVN(x)=∑k=1NΔV(pk(x)).DV_{N}(x)=\bigl[DV(\mathfrak{p}_{1}(x)),\dots,DV(\mathfrak{p}_{N}(x))\bigr],\qquad\Delta V_{N}(x)=\sum_{k=1}^{N}\Delta V\bigl(\mathfrak{p}_{k}(x)\bigr).

2. (Confinement) VNV_{N} is a confining potential on RdN\mathbb{R}^{dN}.

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