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For fixed $r\ge 2$ and every $\epsilon >0$, some $\delta >0$ has the following property for all sufficiently large $n$: a graph with fewer than $\delta n^r$ copies of $K_r$ can be made $K_r$-free by deleting at most $\epsilon n^2$ edges. A Szemerédi regularity lemma partition and the regular clique counting lemma prove this. It converts sparse counts of a forbidden clique into a small edit distance from clique-freeness.

The Szemerédi regularity lemma gives equal cells. If every regular cross-cell pair had density at most $1/4$, their total edge contribution would be at most $n^2/8$. Exceptional vertices, within-cell edges and irregular pairs contribute at most $(2\eta +1/(2m_0))n^2$. Choosing $\eta =1/100$ and $m_0=100$ contradicts $e(G)=n^2/6$. The dense pair is $1/8$-regular since it is already $\eta$-regular.

In a proof of the Szemerédi regularity lemma, suppose $k$ equal classes have size $L$ and witness splitting creates at most $2^k$ atoms per class. Divide every atom into blocks of size $\ell =\lfloor L/4^k\rfloor$, putting leftovers into the exceptional set. At most $k{2}^k\ell \le kL{2}^{-k}$ vertices are lost. When $L\ge 2\cdot 4^k$, at most $2k{4}^k$ blocks remain. For equitable regularity energy defined by omitting exceptional vertices, the loss from discarding a fraction $r$ is at most $2r$: only ordered pairs incident with discarded vertices are removed, and every squared edge density of a bipartite graph is at most one. This provides a quantitative way to restore equal class sizes after each energy increment.

For any fixed odd length $\ell \ge 3$, positive triangle in a graph density forces positive density of $\ell$-cycles. A Szemerédi regularity lemma partition retains a triangle in a graph of regular dense pairs after the sparse and exceptional pairs are removed. Count embeddings of a proper three-colouring of $C_{\ell }$ into those three clusters. The constants depend on $\beta$ and $\ell$, not on graph order.

We use the following precise form of the Szemerédi regularity lemma. For every $0<\eta <1/2$ and positive integer $m_0$, there are integers $M,n_0$ such that every graph on $n\ge n_0$ vertices has a partitionwith at most $\eta k^2$ irregular unordered pairs among the nonexceptional classes. Here $d(A,B)=e(A,B)/(|A||B|)$ for disjoint nonempty sets, and $(A,B)$ is an $\eta$-regular pair ifwhenever $X\subseteq A$, $Y\subseteq B$, $|X|\ge \eta |A|$, $|Y|\ge \eta |B|$.

For the proof, let $f(x,y)$ be the adjacency indicator, including $f(x,x)=0$, and define $d(A,B)$ by averaging $f$ on $A\times B$ even for diagonal cells. The regularity energy of a partition $\mathcal{P}$ isEvery exceptional vertex is represented by its own singleton cell in this energy. If a rectangle $A\times B$ is refined into smaller rectangles with densities $d_{ij}$ and weights $w_{ij}=|A_i||B_j|$, expanding the square gives the refinement variance identity for regularity energyThus refinement never decreases energy.

Suppose an equitable partition with $k$ classes of size $L$ fails the desired conclusion. For every irregular pair choose witness subsets $X\subseteq V_i$, $Y\subseteq V_j$, each of size at least $\eta L$, whose density differs from $d(V_i,V_j)$ by more than $\eta$. Split each class by all witness subsets involving it. Each class has at most $2^{k-1}$ atoms. On a witness rectangle, the weighted mean of $d_{ab}-d(V_i,V_j)$ is $d(X,Y)-d(V_i,V_j)$. The Cauchy-Schwarz inequality therefore bounds the energy increment on this rectangle below byThe different original cell pairs have disjoint rectangles. More than $\eta k^2$ irregular unordered pairs, with both orientations counted in the energy, thus increase it by more than $2{\eta }^5{k}^2{L}^2/n^2$. As long as $|V_0|\le \eta n<n/2$, this is greater than ${\eta }^5/2$, and in particular greater than ${\eta }^5/4$.

Restore equitability by dividing each atom into pieces of common size $\ell =\lfloor L/4^k\rfloor$, moving each leftover vertex into the exceptional set as a singleton energy cell. This remains a refinement, so the energy gain persists. There are at most $k{2}^k$ atoms, so the additional exceptional vertices number at mostIf $L\ge 2\cdot 4^k$, then $\ell \ge L/(2\cdot 4^k)$, and the new number $k^{\prime }$ of equal cells satisfies $k\le k^{\prime }\le 4k{4}^k$. For the lower bound, within each old class the leftover count is at most $2^k\ell <L$, so at least one full new cell survives. For the upper bound, $n/\ell \le 2(n/L)4^k\le 4k{4}^k$, using $kL\ge n/2$. This proves equalization with a controlled exceptional set without any energy loss.

Put $T=\lceil 4{\eta }^{-5}\rceil +1$. Choose $k_0\ge m_0$ with $T{2}^{-k_0}\le \eta /2$. Start with $k_0$ equal classes and fewer than $k_0$ exceptional vertices. Iterate the bounded recurrence $k\mapsto 4k{4}^k$ $T$ times to obtain a bound $M$. Choose $n_0$ so large that the initial remainder is at most $\eta n/2$ and, for every $k\le M$, $(1-\eta )n/k\ge 2\cdot 4^k$. The total exceptional set remains at most $\eta n$, since at most $T$ rounds each add at most $n{2}^{-k_0}$. Each failing round raises an energy in $[0,1]$ by more than ${\eta }^5/4$, so fewer than $T$ rounds can fail. This proves the lemma with all constants independent of the input graph.

For the application, write $h=|V(F)|$ and $\chi (F)=r+1$. We may replace the given tolerance by a smaller one, so assume $0<\epsilon <1$. Set $d=\epsilon /4$, take $m_0\ge 8/\epsilon$, and chooseApply the lemma and delete all edges incident with $V_0$, all edges inside a class, all edges across irregular pairs, and all edges across regular pairs of density below $d$. The resulting spanning subgraph $H$ loses at mostLet $R$ be the reduced graph of a regularity partition, whose edges represent the surviving regular pairs of density at least $d$. We show that a copy of $K_{r+1}$ in $R$ forces a copy of $F$ in $G$.

Choose a proper $(r+1)$-coloring of $F$ and assign its color classes to the corresponding clusters. Embed its vertices one at a time. For each unembedded vertex maintain the candidate set in its cluster consisting of unused vertices adjacent to all already embedded neighbours. After at most $h$ restrictions its size is at least $(d-\eta {)}^{h}L-h\ge (d/2{)}^{h}L-h$. This last quantity is at least $2h\eta L$ when $L$ is large, so every such candidate set is large enough for regularity. In an $\eta$-regular pair of density $p\ge d$, fewer than $\eta L$ vertices on one side have fewer than $(p-\eta )|Y|$ neighbours in any fixed set $Y$ on the other side of size at least $\eta L$: otherwise these vertices and $Y$ violate regularity. For the vertex currently being embedded, there are at most $h$ relevant future candidate sets. At most $h\eta L$ vertices are bad for one of them. Its own candidate set has at least $2h\eta L$ vertices, so an unused good vertex can be chosen. All future candidate sets shrink by at most the factor $d-\eta$, apart from the removal of a used vertex; the stated size bound follows inductively, since the accumulated removals are at most $h$. This completes the graph embedding lemma for regular pairs in the form needed here.

Since $G$ is $F$-free, $R$ is $K_{r+1}$-free. Any $K_{r+1}$ in $H$ would use distinct clusters, because intraclass edges were deleted, and project to a $K_{r+1}$ in $R$. ThereforeThe required threshold on $n$ depends only on $F$ and $\epsilon$, since $k\le M$ makes every nonexceptional cluster sufficiently large.

For disjoint vertex sets $A,B$, define their edge density of a bipartite graph by $d(A,B)=e(A,B)/(|A||B|)$. They form a regular pair with parameter $\epsilon$ if every $A^{\prime }\subseteq A,B^{\prime }\subseteq B$ with $|A^{\prime }|\ge \epsilon |A|$, $|B^{\prime }|\ge \epsilon |B|$ satisfies $|d(A^{\prime },B^{\prime })-d(A,B)|\le \epsilon$.

The Szemerédi regularity lemma says that for every $\epsilon >0$ and minimum cell count $k_0$, some $K,n_0$ have the following property. Every graph on $n\ge n_0$ vertices admitswith $|V_0|\le \epsilon n$, equal-sized $V_1,\dots ,V_k$, and at most $\epsilon k^2$ unordered irregular pairs. It is enough to consider $0<\epsilon <1/2$.

Prove this using equitable regularity energy. Treat exceptional vertices as singleton cells and setwith ordered pairs and the adjacency indicator also defining diagonal densities. Then $0\le q\le 1$. The refinement variance identity for regularity energy proves refinement cannot decrease $q$:An irregular pair supplies witness subsets of relative sizes at least $\epsilon$ whose density differs by more than $\epsilon$. Refining along those witnesses raises $q$ by more than ${\epsilon }^4{L}^2/n^2$ per orientation, where $L$ is the common cell size. If there are more than $\epsilon k^2$ irregular pairs, the increase is greater than ${\epsilon }^5(kL/n{)}^2\ge {\epsilon }^5/4$, provided the exceptional set has size at most $n/2$.

Refine each cell by all its witness subsets; this produces at most $2^k$ atoms per cell. Restore equal sizes by the equalization with a controlled exceptional set: cut each atom into blocks of size $\lfloor L/4^k\rfloor$ and declare its remainder exceptional, still retaining every such vertex as a singleton in the energy. This is another refinement, so no energy is lost. At most $k{2}^k\lfloor L/4^k\rfloor \le n{2}^{-k}$ vertices become exceptional, and, when $L\ge 2\cdot 4^k$, at most $2k{4}^k$ new nonexceptional cells occur.

Put $T=\lceil 4{\epsilon }^{-5}\rceil$ and start with $k\ge k_0$ so large that $T{2}^{-k}\le \epsilon /2$. An initial equitable partition has at most $\epsilon n/2$ exceptional vertices when $n$ is sufficiently large. Subsequent cell counts only increase, so the total added exceptional set has size at most $\epsilon n/2$. The recurrence $k\mapsto 2k{4}^k$, iterated at most $T$ times, supplies a finite bound $K$; choose $n_0$ large enough that every intermediate $L$ meets the size requirement. More than $T$ unsuccessful refinements would raise $q$ above one. The process must therefore stop with the required regular pairs. This proves the lemma.

Its usefulness comes from replacing an arbitrarily large graph by the bounded reduced graph of a regularity partition. For fixed positive cross-density, the graph embedding lemma for regular pairs lifts fixed configurations from the reduced graph to the original one. In particular, three sufficiently regular positive-density pairs contain many triangles in a graph. Deleting exceptional, intracell, irregular and sparse-pair edges then gives the triangle removal lemma: a graph with sufficiently few triangles can be made triangle-free by deleting $o(n^2)$ edges. A triangle surviving in the reduced graph would force a positive proportion of the original possible triangles, a contradiction. More generally this approach yields the clique removal lemma and the asymptotic Erdős-Stone theorem. Applied to the tripartite graph encoding $x+z=2y$, triangle removal also gives Roth theorem on three-term arithmetic progressions. The price is that the energy argument gives a very rapidly growing, iterated-exponential bound on $K(\epsilon )$; the lemma is a structural tool, not a promise of small practical constants.

Use the equitable form of the Szemerédi regularity lemma. For $0<\epsilon <1/2$ and a prescribed lower bound $m_0$, there are $M,n_0$ such that every sufficiently large graph admits a set partitionwith at most $\epsilon k^2$ unordered irregular pairs among the nonexceptional cells. A uniform pair here means a regular pair of vertex sets. Larger values of $\epsilon$ follow from a smaller parameter, so the stated restriction loses nothing.

For the proof, retain the exceptional vertices as singleton cells in an auxiliary set partition $\mathcal{P}$. Define its regularity energy by the ordered sumFor diagonal rectangles the adjacency matrix of a graph defines $d(A,A)$; diagonal terms are included. Thus $0\le q\le 1$. If $A\times B$ is split into rectangles of densities $d_{uv}$ and sizes $w_{uv}$, their weighted mean is $d=d(A,B)$. Expanding squares proves the refinement variance identity for regularity energy:Every refinement therefore increases or preserves energy.

Suppose equal cells $V_i,V_j$ of size $m$ are $\epsilon$-irregular. Choose witnesses $X\subseteq V_i$, $Y\subseteq V_j$ of sizes at least $\epsilon m$, whose density differs from $d(V_i,V_j)$ by more than $\epsilon$. Refine the cells so that these witnesses are unions of refined atoms. Applying the Cauchy-Schwarz inequality inside $X\times Y$ gives an increase, for this oriented rectangle, greater thanChoose witnesses simultaneously for every irregular pair. Each original cell is cut by at most $k-1$ witness sets and has at most $2^k$ atoms. If more than $\epsilon k^2$ unordered pairs are irregular, both orientations contribute, givingas long as the exceptional set has at most $n/2$ vertices.

To restore equal sizes without sacrificing this increase, use equalization with a controlled exceptional set. Cut every witness atom into blocks of size $\ell =\lfloor m/4^k\rfloor$, leaving fewer than $\ell$ unused vertices in each atom. Make each unused vertex a singleton exceptional cell. This is a further refinement, so there is no energy loss. The number newly exceptional is at mostWhen $m\ge 2\cdot 4^k$, the new nonexceptional cell count $k^{\prime }$ is at most $4k{4}^k$: indeed $\ell \ge m/(2\cdot 4^k)$ and $n/m\le 2k$. It is at least $k$, since each old cell supplies at least $4^k-2^k\ge 1$ blocks.

Let $L=\lceil 2{\epsilon }^{-5}\rceil +1$. Choose the initial count $k_0\ge m_0$ so large that $L{2}^{-k_0}\le \epsilon /2$, and begin with $k_0$ equal cells and fewer than $k_0$ leftover vertices. Take $n_0$ large enough that these initial leftovers are at most $\epsilon n/2$. Iterate the bound $k\mapsto 4k{4}^k$ for $L$ rounds to obtain a finite number $M$. Increase $n_0$ further to ensure $n\ge 4M{4}^M$. Then every cell size encountered satisfies $m\ge n/(2M)\ge 2\cdot 4^k$, so every equalization is legitimate. The total exception budget is at most $\epsilon n$, because the initial losses use half the budget and all later losses sum to at most $Ln{2}^{-k_0}$. Energy cannot increase by more than one, so $L$ failing rounds are impossible. The process must stop with at most $\epsilon k^2$ irregular pairs. This proves the Szemerédi regularity lemma, including the bounded cell count, equitability and exceptional-set control.

For the dense-pair application, apply this proof with $\eta =1/100$ and $m_0=100$. Suppose every $\eta$-regular pair of nonexceptional cells has density at most $1/4$. Edges touching $V_0$ number at most $\eta n^2$. Edges inside nonexceptional cells number at most $k{m}^2/2\le n^2/(2m_0)$. The at most $\eta k^2$ irregular cell pairs contribute at most $\eta n^2$. Finally the regular cross-cell pairs contribute at most $k(k-1)m^2/8\le n^2/8$. Thereforea contradiction. Some regular pair $(U,W)$ consequently has density greater than $1/4$. It is also a $1/8$-uniform pair, since subsets of relative size at least $1/8$ qualify in the stronger $\eta$-regularity condition. The common cell size satisfies $m\ge (1-\eta )n/M\ge n/(2M)$. Thus the dense regular pair from edge surplus givesThis first proves the assertion for $n\ge n_0$. For the finitely many smaller possible orders, choose the endpoints of any edge as singleton sets: the pair has density one and is regular for every positive parameter. Taking $c=\min \{1/(2M),1/n_0\}>0$ includes these cases as well.

We prove a weighted version of the Szemerédi regularity lemma, which is sufficient for the grid application. For disjoint nonempty vertex sets $U,W$ in a graph, write $d(U,W)=e(U,W)/(|U||W|)$ for their edge density of a bipartite graph. Call the pair $\epsilon$-regular if every $U^{\prime }\subseteq U$, $W^{\prime }\subseteq W$ with $|U^{\prime }|\ge \epsilon |U|$ and $|W^{\prime }|\ge \epsilon |W|$ satisfies $|d(U^{\prime },W^{\prime })-d(U,W)|\le \epsilon$.

The weighted Szemerédi regularity lemma states that, for every $0<\epsilon <1$, there are integers $M,v_0$ such that every graph on $v\ge v_0$ vertices has a set partition into at most $M$ nonempty cells $V_1,\dots ,V_k$, each of size at most $\epsilon v$, for whichThe sum is ordered. The cells need not have equal sizes; their weights replace the usual unweighted count of bad pairs.

To prove it, start with $k_0=\lceil 2/\epsilon \rceil$ nearly equal cells, taking $v\ge k_0$. Each has size at most $v/k_0+1\le \epsilon v$. Define the regularity energyHere even diagonal rectangles use the mean adjacency indicator, counting ordered pairs of vertices. Thus $0\le q\le 1$. Under a refinement, the old rectangle density is the weighted mean of the new ones, and the refinement variance identity for regularity energy givesIn particular refinement cannot decrease energy.

If the irregular-pair weight exceeds $\epsilon v^2$, choose witness subsets $U^{\prime }\subseteq U$, $W^{\prime }\subseteq W$ for every irregular unordered pair, and split each cell simultaneously by all its witnesses. There are at most $k-1$ such subsets in any one cell, so the new number of cells is at most $k{2}^k$. In an irregular rectangle, its witness has relative area at least ${\epsilon }^2$ and density discrepancy greater than $\epsilon$. Since the witness rectangle is now a union of refined rectangles, the Cauchy-Schwarz inequality applied to their weighted density discrepancies bounds the variance contribution from below bySumming over both orientations of all irregular pairs raises $q$ by more than ${\epsilon }^5$. Since $q\le 1$, after at most $\lceil {\epsilon }^{-5}\rceil$ rounds the required weight bound must hold. The finite recurrence $k\mapsto k{2}^k$, starting at $k_0$, supplies $M(\epsilon )$; all cells remain small because we only refine. This proves the stated weighted Szemerédi regularity lemma.

We next derive the triangle removal lemma from this version. First, three disjoint classes $U,W,Z$ whose pairs are $\epsilon$-regular pairs of density at least $d$ have many triangles if $\epsilon \le d/2$ and $\epsilon \le 1/4$. Fewer than $\epsilon |U|$ vertices of $U$ have fewer than $(d-\epsilon )|W|$ neighbours in $W$: otherwise that set of vertices, paired with all of $W$, would violate regularity. The same holds for $Z$. For each of the at least $(1-2\epsilon )|U|$ remaining vertices, both neighbour sets have relative size at least $d-\epsilon \ge \epsilon$. Regularity of $(W,Z)$ then supplies at least $(d-\epsilon )$ times the product of those two neighbour-set sizes edges. Thus the regular triangle counting lemma, also for unequal class sizes, givesFor a desired deletion tolerance $0<\eta <1$, take $\epsilon =\eta /100$, $d=\eta /4$, and a weighted regularity partition with at most $M=M(\epsilon )$ cells. Put $\tau =\epsilon /M$. Delete edges inside cells, between irregular pairs, between regular pairs of density less than $d$, and incident to cells smaller than $\tau v$. The first two deletions each cost at most $\epsilon v^2/2$. The sparse-pair deletion costs at most $d{v}^2/2$. For the last deletion, small-cell deletion in weighted regularity removes at most $M\tau v=\epsilon v$ vertices and at most $\epsilon v^2$ incident edges. The total is bounded byA triangle surviving these deletions would lie in three distinct cells, all of size at least $\tau v$, with all their pairs regular and of density at least $d$. The original graph would then have at least $d^3{\tau }^3{v}^3/16$ triangles. Therefore, witha graph on sufficiently many vertices with at most $\kappa v^3$ triangles can be made triangle-free by deleting fewer than $\eta v^2$ edges. This establishes the triangle removal lemma with every parameter depending only on $\eta$.

Now apply a tripartite graph encoding of a grid. Take separate vertex classes $X=[N]$, $Y=[N]$, $Z=\{2,\dots ,2N\}$. For each grid point $(x,y)$ in the given set, put in the three edgeswhere their endpoints belong respectively to $X\times Y$, $X\times Z$, and $Y\times Z$. Each point supplies a triangle. These $|A|$ triangles are edge-disjoint triangles, since any one of the three edge types uniquely determines the point that supplied it.

Conversely, any triangle with vertices $x\in X$, $y\in Y$, $z\in Z$ forces the three pointsto belong to $A$. Put $d=z-x-y$. For $d\ne 0$ these form a corner in an integer grid; for $d=0$ they all arise from the same grid point. Thus if there is no corner, the graph has exactly $|A|\le N^2$ triangles, yet destroying all triangles requires at least $|A|\ge \delta N^2$ edge deletions.

We may suppose $0<\delta \le 1$, since larger densities make the request vacuous. Use the triangle removal lemma with $\eta =\delta /32$. Our graph has $v=4N-1$ vertices, so, for sufficiently large $N$, its bound $N^2$ on the number of triangles is at most $\kappa v^3$. The lemma would delete fewer thanedges to destroy all triangles. This contradicts the lower bound $\delta N^2$ from the edge-disjoint family. Hence every sufficiently large positive-density square grid contains a nondegenerate corner, proving the requested corners theorem and in particular the existence of a suitable $N$.

First derive the triangle removal lemma from the Szemerédi regularity lemma. Given an allowed deletion fraction $0<\eta <1$, take $d=\eta /10$, $m_0=\lceil 10/\eta \rceil$, and $0<\epsilon \le \min (d/4,\eta /100,1/8)$. Apply part (i), with upper class bound $M$. Delete edges incident with $V_0$, inside each nonexceptional class, between irregular pairs, and between regular pairs of subset density less than $d$. Their total number is at mostThese four terms are bounded respectively by $\epsilon n^2$, $n^2/(2m_0)$, $\epsilon n^2$, and $d{n}^2/2$.

If a triangle in a graph remains, its three vertices lie in three distinct equal classes, all three regular pairs with subset density at least $d$. The permitted regular triangle counting lemma gives at least $(d^3/4)t^3$ triangles in a graph in the original graph, where $t$ is the class size. This lower bound can also be checked directly: all but $2\epsilon t$ vertices of the first class have at least $(d-\epsilon )t$ neighbors in each of the other two. Those neighborhoods are large enough to use the regular pair condition on the remaining pair, giving at least $(d-\epsilon {)}^3{t}^2$ edges between them. Hence the total is at least $(1-2\epsilon )(d-\epsilon {)}^3{t}^3\ge (d^3/4)t^3$.

Since $t\ge n/(2M)$, a surviving triangle in a graph forces at least $d^3{n}^3/(32M^3)$ original triangles in a graph. Thus a graph with fewer than $\xi n^3$ triangles in a graph, where $\xi =d^3/(64M^3)>0$, can be made triangle-free by deleting fewer than $\eta n^2$ edges, for all sufficiently large $n$. This proves the removal lemma needed here.

Now use the triangle-removal proof of Roth theorem. Fix a subset density lower bound $\delta >0$ and suppose $A\subseteq [N]$, $|A|\ge \delta N$, has no nonconstant three-term arithmetic progression. Set $m=2N+1$ and $G={\mathbb{Z}}_m$. Use three disjoint copies $X,Y,Z$ of $G$ and put edges according toDivision by two is valid because $m$ is odd. A triangle in a graph corresponds to $a=y-x$, $b=z-y$, $c=(z-x)/2$ with $a,b,c\in A$ and $a+b=2c$. Since $A\subseteq [N]$ and $|a+b-2c|<m$, this congruence is an integer equality. Progression-freeness therefore forces $a=b=c$.

Every triangle in a graph is consequently of the form $(x,x+a,x+2a)$ with $x\in G,a\in A$, so there are exactly $m|A|$ triangles in a graph. These triangles in a graph are edge-disjoint: an $XY$ edge determines $(x,a)$; a $YZ$ edge determines $a$ and then $x$; and an $XZ$ edge determines $a=(z-x)/2$ and $x$. Eliminating them all requires at least $m|A|$ edge deletions.

The graph has $3m$ vertices but only $m|A|\le mN=O(m^2)$ triangles in a graph. Take $\eta =\delta /100$. For large enough $N$ its triangle in a graph count is below $\xi (3m{)}^3$, so removal requires fewer than $\eta (3m{)}^2=9\delta m^2/100$ deletions. Yeta contradiction. Therefore every fixed positive-density subset of a sufficiently long interval contains a nonconstant three-term arithmetic progression.

This proves the qualitative Roth theorem on three-term arithmetic progressions. The quantitative bound from part 2(i) came from the explicit Fourier iteration; the regularity-removal argument gives a density-dependent threshold without that double-logarithmic estimate.

For disjoint nonempty vertex sets $U,V$, write $d(U,V)=e(U,V)/(|U||V|)$. A regular pair of vertex sets is $\epsilon$-regular if every $U^{\prime }\subseteq U,V^{\prime }\subseteq V$ with $|U^{\prime }|\ge \epsilon |U|$, $|V^{\prime }|\ge \epsilon |V|$ satisfies $|d(U^{\prime },V^{\prime })-d(U,V)|\le \epsilon$.

The Szemerédi regularity lemma states that, for every $\epsilon >0$ and integer $m_0$, there are $M,n_0$ such that every finite simple graph on $n\ge n_0$ vertices has a set partitionwith $m_0\le m\le M$, $|V_0|\le \epsilon n$, $|V_1|=\cdots =|V_m|$, and at most $\epsilon m^2$ irregular unordered pairs among the nonexceptional classes. Prove it for $0<\epsilon \le 1/2$; larger parameters follow by using a smaller one.

For the energy-increment proof of Szemerédi regularity, keep every exceptional vertex as a singleton cell in the set partition used to measure regularity energy. Define the equitable regularity energyThe sum is ordered, and on diagonal cells subset density means the average of the adjacency indicator, with zero on loops. Thus $0\le q\le 1$. If $U,V$ are refined into $U_a,V_b$, expanding squares givesThe cross term vanishes because the weighted arithmetic mean of the refined subset densities is the original subset density. Consequently every refinement of a set partition increases or preserves regularity energy.

Suppose the current nonexceptional classes have common size $t$ and there are $k$ of them. For each irregular pair $V_i,V_j$, choose witnesses $A_{ij},B_{ij}$ of sizes at least $\epsilon t$ and discrepancy greater than $\epsilon$. Refine each class by all its incident witness subsets. There are at most $k-1$ cuts in each class and at most $2^k$ resulting atoms. The witness rectangle is a union of refined rectangles. By the Cauchy-Schwarz inequality, its contribution to the variance identity is at leastIndeed, the sum of squared deviations on the witness rectangle is at least its total weight times the square of their weighted arithmetic mean. If more than $\epsilon k^2$ unordered pairs are irregular, summing even just one orientation of each givesprovided the exceptional set has at most $n/2$ vertices. This is the strictly positive regularity energy increment.

Restore equal class sizes without losing that increment. Divide every witness atom into blocks of size $\ell =\lfloor t/4^k\rfloor$ and make every leftover vertex an exceptional singleton. This is a further refinement of a set partition, so it cannot decrease $q$. There are at most $k{2}^k$ atoms, hence fewer than $k{2}^k\ell \le n{2}^{-k}$ newly exceptional vertices. If $t\ge 2\cdot 4^k$, then $\ell \ge t/(2\cdot 4^k)$, so the number of full blocks is at most $2k{4}^k$. Each original class produces at least one full block: its leftovers occupy less than $2^k\ell$, whereas $t\ge 4^k\ell >2^k\ell$. Thus the new class count is at least $k$.

Choose $R_{\ast }=\lceil 4{\epsilon }^{-5}\rceil +1$, and choose an initial integer $k_0\ge m_0$ large enough that $R_{\ast }{2}^{-k_0}\le \epsilon /2$. Initially partition into $k_0$ equal classes and fewer than $k_0$ exceptional vertices. Take $n_0$ large enough that this initial exception is at most $\epsilon n/2$. During at most $R_{\ast }$ rounds, the additional exception is at most $R_{\ast }n{2}^{-k_0}\le \epsilon n/2$, so it never exceeds $\epsilon n\le n/2$.

A bound on class counts is obtained by iterating $k\mapsto 2k{4}^k$ at most $R_{\ast }$ times starting at $k_0$; call the resulting bound $M$. Increasing $n_0$ further to satisfy $n_0\ge 4M{4}^M$ guarantees $t\ge n/(2k)\ge 2\cdot 4^k$ at every round, so all full-block constructions are valid. If the desired regularity had not been reached after $R_{\ast }$ refinements, the regularity energy increments would total more than one, impossible. Therefore the process terminates with the required partition and bounds. The singleton treatment of discarded vertices is what preserves regularity energy monotonicity during equalization.

For disjoint nonempty vertex sets $U,W$, define their edge density of a bipartite graph by $d(U,W)=e(U,W)/(|U||W|)$. They form an $\epsilon$-regular pair of vertex sets if every $X\subseteq U$, $Y\subseteq W$ with $|X|\ge \epsilon |U|$, $|Y|\ge \epsilon |W|$ satisfies $|d(X,Y)-d(U,W)|\le \epsilon$.

The Szemerédi regularity lemma asserts that, given $\epsilon >0$ and a positive integer $m_0$, there are $M,n_0$ such that every graph on $n\ge n_0$ vertices has a set partition $V_0,V_1,\dots ,V_k$ withand at most $\epsilon k^2$ irregular ordered pairs $(V_i,V_j)$ with $1\le i\ne j\le k$.

Assume $0<\epsilon \le 1/2$, which suffices since a smaller regularity parameter gives the claim for a larger one. Treat the exceptional vertices as singleton cells in the full partition $\mathcal{P}$, and use equitable regularity energyHere the adjacency indicator function defines density even for diagonal cells. Clearly $0\le q\le 1$. If ${\mathcal{P}}^{\prime }$ refines $\mathcal{P}$, weighted averaging of densities gives the refinement variance identity for regularity energyTo verify it, expand each square and use ${\sum }_{A^{\prime },B^{\prime }}|A^{\prime }||B^{\prime }|d(A^{\prime },B^{\prime })=|A||B|d(A,B)$.

For every irregular ordered pair of nonexceptional cells, choose witnesses $X_{ij},Y_{ij}$ of relative sizes at least $\epsilon$ and density discrepancy greater than $\epsilon$. Split each $V_i$ along all witnesses involving it; symmetry allows at most one witness for each other cell, hence at most $2^k$ atoms in each $V_i$. In the witness rectangle, the weighted Cauchy-Schwarz inequality in the variance identity contributes more than ${\epsilon }^4|V_i||V_j|/n^2$.

If more than $\epsilon k^2$ pairs are irregular and the equal cell size is $L$, the energy increase is greater thanRestore equal cell sizes by cutting each witness atom into pieces of size $\ell =\lfloor L/4^k\rfloor$, with leftover vertices added to $V_0$ as singleton cells. This operation is a further refinement, so the energy does not decrease. There are at most $k{2}^k$ atoms, and fewer than $\ell$ leftover vertices in each, giving at most $k{2}^k\ell \le n{2}^{-k}$ new exceptional vertices.

Here is a uniform bound ensuring that the iteration is legitimate. Put $R=\lceil 4{\epsilon }^{-5}\rceil$ and chooseStart with $k_0$ equal classes and fewer than $k_0$ exceptional vertices. Taking $n\ge 2k_0/\epsilon$ makes the initial exception at most $\epsilon n/2$. At every refinement the number of nonexceptional cells does not decrease: each old cell loses at most $L{2}^{-k}\le L/2$ vertices and is cut into pieces of size at most $L/4^k$. Thus each of the at most $R$ rounds adds at most $\epsilon n/(2R)$ exceptional vertices.

When $L\ge 2\cdot 4^k$, the new cell count is at mostusing $|V_0|\le \epsilon n\le n/2$. Define $K_0=k_0$ and $K_{j+1}=4K_j{4}^{K_j}$, and take $M=K_R$. Choosing $n_0\ge \max \{2k_0/\epsilon ,4M{4}^M\}$ ensures $L\ge n/(2M)\ge 2\cdot 4^M$ at every stage. All rounds are therefore defined, with cell count between $m_0$ and $M$ and exceptional size at most $\epsilon n$.

If the lemma still failed after $R$ refinements, the energy would have increased by more than $R{\epsilon }^5/4\ge 1$, impossible because it lies in $[0,1]$. Hence some stage has the required regular pairs. This completes the energy-increment proof of Szemerédi regularity, including the equal-size and exceptional-set conditions.

We prove edit-distance stability for clique-free graphs by induction on $r$, using the symmetric difference of edge sets as the distance. For $r=1$, a $K_2$-free graph is edgeless, and there is nothing to change. For $r\ge 2$, choose a vertex of maximum degree $d$, let $A$ be its neighbourhood and put $B=V(G)\setminus A$. Then $G[A]$ is $K_r$-free. WriteBoth deficits are nonnegative by the Turan theorem. Since every vertex of $B$ has degree at most $d=|A|$,The complete $r$-partite graph formed from an $(r-1)$-partite Turán graph on $A$ and the new class $B$ has at most $t_r(n)$ edges. Thus $L=t_r(n)-t_{r-1}(d)-|A||B|\ge 0$, and direct subtraction givesBy induction, edit $G[A]$ into a complete $(r-1)$-partite graph using at most $3D_A$ changes. Delete the $b$ edges inside $B$, and add the $m$ missing edges between $A$ and $B$. The resulting graph is complete $r$-partite on the same vertex set, andwhere the inequality uses $m\ge 2b$. The required edit distance is at most $3k$. Empty partition classes are allowed; a sufficiently dense nondegenerate case has the usual full complement of classes.

For the odd-cycle conclusion, use two standard consequences of the Szemerédi regularity lemma, stated explicitly. The triangle removal lemma says that for every $\alpha >0$, some $\beta >0$ ensures that a graph with at most $\beta n^3$ triangles in a graph can be made triangle-free by deleting at most $\alpha \left(\genfrac{}{}{0ex}{}{n}{2}\right)$ edges, for all sufficiently large $n$. Also, for each fixed odd length $\ell \ge 3$ and each $\beta >0$, there is $\zeta >0$ such that a graph with at least $\beta n^3$ triangles in a graph contains at least $\zeta n^{\ell }$ copies of $C_{\ell }$.

For clarity, the latter odd-cycle copies from positive triangle density consequence follows by applying regularity with error small relative to $\beta$, removing exceptional, irregular and very sparse pairs, and retaining a triangle in a graph among the remaining regular dense pairs. The graph embedding lemma for regular pairs counts a positive constant times $n^{\ell }$ embeddings of any fixed graph properly three-coloured into those three clusters, including $C_{\ell }$. Dividing by the fixed number of descriptions of a cycle gives the same conclusion for unlabelled copies.

Apply triangle in a graph removal with $\alpha =ϵ$, and take the resulting $\beta$. A $C_{2013}$-free graph cannot have $\beta n^3$ triangles in a graph for large $n$, by the preceding consequence. Delete at most $ϵ\left(\genfrac{}{}{0ex}{}{n}{2}\right)$ edges to obtain a triangle-free $G^{\prime }$. With $N=\left(\genfrac{}{}{0ex}{}{n}{2}\right)$,Apply the proved stability result with $r=2$. The resulting complete bipartite graph $H$ satisfiesChoose $n_0(ϵ)$ also large enough that $3n/4\le 4ϵN$. Then the distance is at most $11ϵ\left(\genfrac{}{}{0ex}{}{n}{2}\right)$.

For the unheaded continuation, use the same $\beta$ and its associated $\zeta$, and set $\delta =\zeta /2$. Having at most $\delta n^{2013}$ cycles rules out $\beta n^3$ triangles in a graph just as before. The identical deletion and stability calculation applies. A sufficiently small $\delta =\delta (ϵ)>0$ gives the same $11ϵ$ bound.