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Strong regularity with linearly large representative subsets and no irregular representative pair

Statement

Let ϵ0>0, let ϵ1ϵ2>0, and let k01. There are K and δ>0 such that every finite graph G of order at least k0 has an equitable partition V(G)=V1Vk,k0kK, and nonempty subsets WiVi with WiδV(G) such that

  1. every pair (Wi,Wj), including i=j, is ϵk-regular; and
  2. for all but at most ϵ0k2 ordered pairs (i,j), d(Wi,Wj)d(Vi,Vj)ϵ0.

Facts & Assumptions

Given: ϵ0, a nonincreasing positive sequence, an integer k01, and a finite graph G of order nk0.

[L1]

For any prescribed minimum coarse part count m0, strong regularity produces equitable partitions P,Q of any graph of order at least m0 with Q refining P, P being ϵ0-regular with m0P, Q being ϵP-regular, q(Q)q(P)+ϵ0, and Q bounded (Equitable strong regularity lemma: a very regular refinement that changes energy only slightly).

[L2]

A small energy increment makes almost all fine-pair densities close to their coarse densities (A small energy increment makes fine-pair densities close to their coarse densities almost everywhere).

[L3]

Every finite graph with at least one vertex contains a nonempty linearly large self-regular subset at any prescribed parameter (Every finite graph has a linearly large ϵ-self-regular vertex subset).

[L4]

Large restrictions of regular pairs stay regular and have nearby density (Slicing lemma: large subpairs remain regular and their density shifts by at most ϵ).

[L5]

If a nonnegative integer-valued random variable has expectation below 1, some outcome makes it zero (The first-moment method for avoiding or forcing a finite count of bad events).

Proof

technique · constructive
1.1

Apply [L1] with minimum coarse part count m0=k0, coarse parameter much smaller than ϵ03, and fine parameter, at a coarse part count k, much smaller than ϵk after slicing. This is legitimate because nk0. Obtain equitable P={V1,,Vk} with k0kK and a fine equitable refinement Q.

givenL1chooseconstruct
2.1

By [L2], the total ordered vertex-pair weight of fine pairs whose density differs from their coarse pair by more than ϵ0/2 is at most a chosen constant below ϵ02. The fine partition has bounded order.

step 1.1L2algebra
3.1

Independently for each i, choose a fine atom UiVi with probability proportional to its size. Choose the parameters so that the expected number I of nonregular selected ordered pairs is below 1/4, while the expected number D of pairs with d(Ui,Uj)d(Vi,Vj)>ϵ0/2 is below ϵ0k2/4.

step 1.1step 2.1algebra
4.1

Inside every selected atom Ui, apply [L3] at a much smaller parameter and obtain WiUi of size at least a fixed fraction of Ui. Because both partition orders are bounded and equitable, there is a uniform δ>0 with Wiδn.

step 3.1L3choose
4.2

Let X=I+1{D>ϵ0k2}. Since 1{D>ϵ0k2}D/(ϵ0k2), step 3.1 gives EX<1/2. By [L5] there is a selection with X=0: it has no irregular selected pair and at most ϵ0k2 density failures.

step 3.1L5algebrachoose
5.1

On every fine-regular selected cross-pair, [L4] makes (Wi,Wj) ϵk-regular and changes its density by at most ϵ0/2. Each diagonal pair is ϵk-regular by the self-regular choice in step 4.1.

step 3.1step 4.1L4algebra
6.1

For that selection, step 5.1 gives regularity for every representative pair, while step 4.2 gives the density-approximation exception bound. Step 4.1 gives the common linear lower bound and makes each Wi nonempty, and step 1.1 gives k0kK, completing the construction.

step 4.1step 5.1step 4.2discharge-construct

Depends on

Used by

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