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The edge-density form of Rödl's theorem implies the maximum-degree form, with ϵ and δ each shrunk by a constant factor

Statement

Assume the edge-density form of Rödl's theorem holds at parameter ϵ/4 with constant δ0. Then the maximum-degree form holds at parameter ϵ with constant δ0/2.

Facts & Assumptions

Given: A graph H, a real ϵ∈(0,12), and the edge-density form of Rödl's theorem at parameter ϵ/4 with constant δ0.

[L1]

The edge-density form supplies, in every nonempty H-free graph G, a set X of size at least δ0∣V(G)∣ with dG(X,X)≤ϵ/4 or dG(X,X)≥1−ϵ/4 (The edge-density form of Rödl's theorem: every nonempty H-free graph has a linearly large set of self-density at most ϵ or at least 1−ϵ).

[L2]

If dG(X,X)≤c, then some subset X′⊆X with ∣X′∣≥∣X∣/2 is 4c-sparse (A set of self-density at most c has a subset of at least half its size that is 4c-sparse).

Proof

technique · direct
1.1L1choose

Let G be a nonempty H-free graph. By [L1], choose X⊆V(G) with ∣X∣≥δ0∣V(G)∣ and either dG(X,X)≤ϵ/4 or dG(X,X)≥1−ϵ/4.

2.1step 1.1L2

In the sparse branch, [L2] applied with c=ϵ/4 gives a subset X′⊆X with ∣X′∣≥∣X∣/2 that is ϵ-sparse, hence ϵ-restricted.

2.2step 1.1L2L3algebra

In the dense branch, the diagonal convention gives dG‾(X,X)=1−1/∣X∣−dG(X,X)≤ϵ/4; applying [L2] to G‾ yields a subset X′⊆X with ∣X′∣≥∣X∣/2 that is ϵ-sparse in G‾, and [L3] turns this into ϵ-dense, hence ϵ-restricted, in G.

3.1step 2.1step 2.2∎

In either branch ∣X′∣≥(δ0/2)∣V(G)∣, so the maximum-degree form holds with constant δ0/2.

Depends on

Used by

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