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Source. Kříž, Permutation groups in Euclidean Ramsey theory, published pp. 899–902, Sections 2.1–2.4 and Definition 3.1 (publisher PDF).

Configurations and colorings

A configuration is a finite subset of a Euclidean space. We use nonempty configurations in the proofs; the empty configuration, if admitted, satisfies all the Ramsey conclusions trivially. Dimensions are nonnegative integers, and a number of colors is a positive integer. Write [m]={0,…,m−1}[m]=\{0,\ldots,m-1\}, with [0]=∅[0]=\varnothing.

An isometrical embedding is an injective map preserving all pairwise Euclidean distances. An isometry of a finite configuration onto itself is a permutation of its points preserving distance. Its group of isometries is therefore finite. A group of ambient isometries acting on a configuration may be replaced by its finite induced permutation group. A group is soluble (or solvable) if its derived series, obtained by repeatedly taking the subgroup generated by commutators, reaches the identity subgroup after finitely many steps.

Let EE be an equivalence relation on FF. The configuration is EE-Ramsey if, for every integer k≥1k\ge1, there is a dimension NN such that every coloring c:RN→[k]c:\mathbb R^N\to[k] admits an isometrical embedding ϕ:F→RN\phi:F\to\mathbb R^N with

xEy⟹c(ϕ(x))=c(ϕ(y)).xEy\quad\Longrightarrow\quad c(\phi(x))=c(\phi(y)).

Different EE-classes may receive the same color. Ordinary Ramsey means E=F×FE=F\times F. For an integer s≥1s\ge1, ss-Ramsey means that the image of some such embedding uses at most ss colors. The partition in this last definition may initially depend on the coloring; Proposition 2.4.1 removes that dependence.

If FiF_i carries EiE_i, the Euclidean product has squared distance

d((x1,x2),(y1,y2))2=d(x1,y1)2+d(x2,y2)2,d((x_1,x_2),(y_1,y_2))^2 =d(x_1,y_1)^2+d(x_2,y_2)^2,

and (x1,x2)(E1×E2)(y1,y2)(x_1,x_2)(E_1\times E_2)(y_1,y_2) means xiEiyix_iE_iy_i for both coordinates. Powers FmF^m and EmE^m use the corresponding coordinatewise definitions.

Group actions and mergers

For a group GG acting on a finite set FF, put

xEGy⟺gx=y for some g∈G.xE_Gy\quad\Longleftrightarrow\quad gx=y\text{ for some }g\in G.

A permutation bb respects EE if xEyxEy implies b(x)Eb(y)b(x)E b(y). Because bb has finite order, its inverse also respects EE, so it acts on F/EF/E. If every element of GG respects EE, define

St⁡G(E)={g∈G:gxEx for every x∈F},G/E=G/St⁡G(E).\operatorname{St}_G(E)=\{g\in G:gxEx\text{ for every }x\in F\}, \qquad G/E=G/\operatorname{St}_G(E).

The stabilizer here is the kernel of the action on F/EF/E, not the stabilizer of one point. The group G/EG/E is the induced permutation group of the equivalence classes.

Write U(E;G)U(E;G) for the equivalence relation that joins all EE-classes in each orbit of this quotient action. Explicitly,

x U(E;G) y⟺gxEy for some g∈G.(1)x\,U(E;G)\,y\quad\Longleftrightarrow\quad gxEy\text{ for some }g\in G. \tag{1}

This is an equivalence relation because it is orbit equivalence on F/EF/E, pulled back to FF.

For z∈Fz\in F, a permutation bb respecting EE, and an integer n≥0n\ge0, put

An=⋃i=0n−1[biz]E,U(E;z,b,n)=E∪(An×An).(2)A_n=\bigcup_{i=0}^{n-1}[b^iz]_E, \qquad U(E;z,b,n)=E\cup(A_n\times A_n). \tag{2}

Thus exactly the classes meeting z,bz,…,bn−1zz,bz,\ldots,b^{n-1}z are merged. For n=0n=0 or 11 the relation is EE. The merger need not be preserved by bb until an entire orbit of classes has been merged.

Source conventions

The printed norm convention on p. 900 writes ∥x∥=x⋅x\|x\|=x\cdot x. We use the ordinary Euclidean convention ∥x∥2=x⋅x\|x\|^2=x\cdot x, consistent with the distance and scalar-product arguments throughout the paper. All inequalities defining ss-Ramsey and the two-class results are inclusive: at most ss colors, at most two classes, or at most two orbits.

Related results. elementary closure properties, Proposition 2.4.1, and Theorem 4.1.

Bears on. Problem 174.