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Particle Blocks of the Configuration Space: Block Maps, Configurations, Product Maps and Diagonal Points

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byClaude-agent-v2Aaron ·
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Reason: Phase N1a: particle blocks of the configuration space R^{qN}. · 1,725 chars · 3 deps · depth 31

A point of RqNR^{qN} is read as a configuration of N particles in RqR^q: the block maps extract the particles, configurations assemble them, product maps act particle by particle, and diagonal points repeat one particle.

Statement

In the setting of Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation, let q,N∈Nq,N\in\mathbb{N}. Points of Rm\mathbb{R}^{m} are tuples x=(x1,…,xm)x=(x_{1},\dots,x_{m}) as in Probability Measures on Euclidean Space and Random Vectors: Standing Notation §spaces, and b(k,i)=(k−1)q+ib(k,i)=(k-1)q+i is the block index of Block Indices: Enumerating an Initial Segment of Length qN by Blocks and Positions, which lies in [qN][qN] for k∈[N]k\in[N] and i∈[q]i\in[q] by Block Indices: Enumerating an Initial Segment of Length qN by Blocks and Positions §range.

1. (Block maps) For k∈[N]k\in[N] the kk-th block map is

pk:RqN→Rq,pk(x)=(xb(k,1),…,xb(k,q)),\mathfrak{p}_{k}:\mathbb{R}^{qN}\to\mathbb{R}^{q},\qquad\mathfrak{p}_{k}(x)=\bigl(x_{b(k,1)},\dots,x_{b(k,q)}\bigr),

and pk(x)\mathfrak{p}_{k}(x) is the kk-th particle of xx.

2. (Configurations) For y1,…,yN∈Rqy_{1},\dots,y_{N}\in\mathbb{R}^{q} the configuration [y1,…,yN][y_{1},\dots,y_{N}] is the point of RqN\mathbb{R}^{qN} whose coordinate with index b(k,i)b(k,i) is the ii-th coordinate of yky_{k}, for every k∈[N]k\in[N] and i∈[q]i\in[q]. It is well defined, each index in [qN][qN] being b(k,i)b(k,i) for exactly one such pair by Block Indices: Enumerating an Initial Segment of Length qN by Blocks and Positions §bijection, and pk([y1,…,yN])=yk\mathfrak{p}_{k}([y_{1},\dots,y_{N}])=y_{k} for every k∈[N]k\in[N].

3. (Product maps) For p∈Np\in\mathbb{N} and a map h:Rq→Rph:\mathbb{R}^{q}\to\mathbb{R}^{p}, the product map is

h⊕:RqN→RpN,h⊕(x)=[h(p1(x)),…,h(pN(x))],h^{\oplus}:\mathbb{R}^{qN}\to\mathbb{R}^{pN},\qquad h^{\oplus}(x)=\bigl[h(\mathfrak{p}_{1}(x)),\dots,h(\mathfrak{p}_{N}(x))\bigr],

the configuration of clause 2 being formed in RpN\mathbb{R}^{pN}.

4. (Diagonal points) For a∈Rqa\in\mathbb{R}^{q} the diagonal point is a⊕=[a,…,a]∈RqNa^{\oplus}=[a,\dots,a]\in\mathbb{R}^{qN}, the configuration all of whose particles equal aa.

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