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Write $[n{]}^{(r)}$ for the rank-$r$ uniform layer of the Boolean cube. For a uniform set family $\mathcal{F}\subseteq [n{]}^{(r)}$, with $1\le r\le n$, let $\partial \mathcal{F}$ be its lower shadow. The Local LYM inequality isFor its proof, count incidences $(B,A)$ with $A\in \mathcal{F}$, $B\subset A$, and $|B|=r-1$. Each member of $\mathcal{F}$ contributes $r$ incidences, while each member of the lower shadow contributes at most $n-r+1$. Thus $r|\mathcal{F}|\le (n-r+1)|\partial \mathcal{F}|$, which is the displayed bound by the ratio of consecutive binomial coefficients. Complementing every set gives the corresponding upper shadow bound, $|\nabla \mathcal{F}|/\left(\genfrac{}{}{0ex}{}{n}{r+1}\right)\ge |\mathcal{F}|/(\genfrac{}{}{0ex}{}{n}{r})$ for $r<n$.

For an antichain $\mathcal{A}$ in the Boolean lattice, the LYM inequality isHere is the proof using the Local LYM inequality. Denote the rank-$r$ part by ${\mathcal{A}}_r$, and let ${\mathcal{D}}_r$ consist of the $r$-sets containing some member of $\mathcal{A}$ of size at most $r$. These families satisfyThe union is disjoint because a member of the antichain cannot contain a strictly smaller member. Apply the upper shadow form of the Local LYM inequality to ${\mathcal{D}}_{r-1}$:Iterating gives a bound for the entire sum by $|{\mathcal{D}}_n|/(\genfrac{}{}{0ex}{}{n}{n})\le 1$. This also covers the empty antichain and an antichain containing the empty set.

For the second proof, each permutation of $[n]$ specifies a maximal chain in a Boolean lattice by taking its successive prefixes. There are $n!$ such maximal chains in a Boolean lattice, and a fixed $r$-set belongs to $r!(n-r)!$ of them. A maximal chain in a Boolean lattice meets an antichain at most once. Double counting these incidences therefore gives ${\sum }_r|{\mathcal{A}}_r|r!(n-r)!\le n!$, exactly the LYM inequality.

The Sperner theorem says that an antichain in $\mathcal{P}([n])$ has at most $\left(\genfrac{}{}{0ex}{}{n}{\lfloor n/2\rfloor }\right)$ members; a full middle rank attains this bound. Indeed, every binomial coefficient $\left(\genfrac{}{}{0ex}{}{n}{r}\right)$ is at most the central one, so the LYM inequality givesNow let $\mathcal{F}$ be an intersection-free uniform set family. If it is empty, there is nothing to prove. Fix $X\in \mathcal{F}$ and consider the tracesIf $A,B\ne X$ are distinct and $X\cap A\subseteq X\cap B$, then $X\cap A\subseteq B$. This contradicts the defining restriction on the three distinct members $X,A,B$. The intersection has size less than $r$, so it is a proper subset of $B$ even if the printed subset symbol is interpreted strictly. In particular, equal traces are impossible, and the traces form an antichain. Thus $|\mathcal{T}|=|\mathcal{F}|-1$. Applying the Sperner theorem to the $r$-element ground set $X$ proves the antichain trace bound for intersection-free familiesThe argument also handles $r=0$: a uniform set family then has at most one member.

The Kruskal-Katona theorem states that a colexicographic initial segment minimizes the lower shadow of a uniform set family of prescribed size. Its numerical form is as follows. For $m>0$, write the unique combinatorial number system expansionEvery $\mathcal{F}\subseteq [n{]}^{(r)}$ of size $m$ satisfiesThe empty family has empty lower shadow. Equality is attained by the first $m$ $r$-sets in colexicographic order, where the largest differing element belongs to the later set. Iterating the Kruskal-Katona theorem shows that the same colexicographic initial segment minimizes every iterated lower shadow.

For $1\le r<n/2$, the Erdős-Ko-Rado theorem givesfor an intersecting family $\mathcal{F}\subseteq [n{]}^{(r)}$. All $r$-sets containing one prescribed point show that the bound is sharp.

For the proof from the Kruskal-Katona theorem, put $k=n-r$ and form the complement family $\mathcal{G}=\{[n]\setminus A:A\in \mathcal{F}\}\subseteq [n{]}^{(k)}$. Let $\mathcal{S}$ be its rank-$r$ iterated lower shadow. No member $B\in \mathcal{F}$ belongs to $\mathcal{S}$: containment in $[n]\setminus A$ would give $A\cap B=\varnothing$, impossible for an intersecting family of nonempty sets. HenceSuppose $|\mathcal{F}|>\left(\genfrac{}{}{0ex}{}{n-1}{r-1}\right)=\left(\genfrac{}{}{0ex}{}{n-1}{k}\right)$. The first $\left(\genfrac{}{}{0ex}{}{n-1}{k}\right)$ members of the colexicographic order are all $k$-sets of $[n-1]$. Their rank-$r$ iterated lower shadow is all $r$-sets of $[n-1]$, since $r<k$. The next $k$-set contains $n$ and has an $r$-subset containing $n$, so taking even one more member strictly enlarges that iterated lower shadow. By the iterated Kruskal-Katona theorem, $|\mathcal{S}|>\left(\genfrac{}{}{0ex}{}{n-1}{r}\right)$. Together with $|\mathcal{F}|>\left(\genfrac{}{}{0ex}{}{n-1}{r-1}\right)$ this contradicts Pascal's identity and the preceding inequality. This proves the Erdős-Ko-Rado theorem.

For the Katona circle method proof, fix a cyclic ordering of $[n]$. A cyclic interval of length $r$ is specified by its final position. If no such interval belongs to $\mathcal{F}$, the bound below is automatic. Otherwise rotate one selected interval so that it ends at position $n$, and thus occupies positions $n-r+1,\dots ,n$. Intervals ending at positions $r,\dots ,n-r$ are disjoint from it and cannot be selected. Among the remaining endpoints, pair $j$ with $n-r+j$ for $1\le j\le r-1$. The corresponding intervals are disjoint when $n\ge 2r$, so at most one interval per pair is selected. Together with the interval ending at $n$, this gives the cyclic interval intersection bound of $r$ selected intervals.

Choose a uniformly random permutation and read its positions cyclically. A fixed $r$-set is a cyclic interval with probability $n/\left(\genfrac{}{}{0ex}{}{n}{r}\right)$: each cyclic position gives a uniformly distributed $r$-set, and for $r<n$ the $n$ intervals are distinct. Summing over $\mathcal{F}$, the expected value of the number of selected intervals is $n|\mathcal{F}|/(\genfrac{}{}{0ex}{}{n}{r})$. The cyclic interval intersection bound makes this at most $r$, giving $|\mathcal{F}|\le (r/n)\left(\genfrac{}{}{0ex}{}{n}{r}\right)=\left(\genfrac{}{}{0ex}{}{n-1}{r-1}\right)$.

Finally apply the Katona circle method to an arbitrary antichain $\mathcal{A}$. If it contains $\varnothing$ or $[n]$, it has exactly one member and the LYM inequality holds with equality. Otherwise all its members have sizes $1,\dots ,n-1$. In a fixed cyclic ordering, the cyclic intervals sharing a final position form a nested chain as their lengths increase. At most one of them can belong to the antichain. Summing over the $n$ final positions proves the cyclic interval antichain bound of $n$ intervals. Taking the expected value over a uniformly random permutation givesAfter division by $n$, this is the LYM inequality proved by cyclic intervals. The case $n=0$ consists only of the empty set and is immediate.

As printed, yes: the relation is universal. The original PDF puts the existentially quantified element in the same subset as the universally quantified element; this is not an OCR substitution. For each element of that subset, choose the element itself as witness, using reflexivity of the underlying well-quasi-ordering. For an empty subset the condition is vacuous. The truth value therefore never depends on the proposed target subset. On the power set this is a reflexive transitive relation, and every two terms of any infinite sequence are related:A well-quasi-ordering need not be antisymmetric, so universal comparability is allowed.

If the existential element is instead intended to belong to the target subset, the natural relation is the Hoare domination preorderFor arbitrary subsets the answer to that corrected question is no. Here is a complete counterexample, the Rado order. TakeThis is a partial order. Reflexivity is immediate. For transitivity, two same-row comparisons compose ordinarily. If the first comparison crosses rows and the second stays in its row, its target first coordinate is unchanged, so the cross-row inequality persists. If the first stays in its row and the second crosses, use $n\le l<k^{\prime }$; if both cross, use $n<k<l<k^{\prime }$. Antisymmetry follows because comparisons across distinct rows in both directions would require $n<k<l<m<n$.

The Rado order is a well-quasi-ordering. Given an infinite sequence $(m_i,n_i)$, if a first coordinate $m$ repeats infinitely often, its corresponding natural-number second coordinates have a nondecreasing pair, giving a same-row comparison. Otherwise each first coordinate occurs only finitely often, so the first coordinates in every tail are unbounded. In particular some later $m_j$ exceeds $n_0$, giving $(m_0,n_0){\le }_R(m_j,n_j)$.

For each $m$, take the infinite row $S_m=\{(m,n):n>m\}$. For distinct $m,k$, choose $n>\max (m,k)$. The element $(m,n)\in S_m$ is below no member $(k,l)$ of $S_k$, since its first coordinate is different and $n<k$ fails. Thus $S_m/{\le }_H{S}_k$ for every pair of distinct indices. These subsets form an infinite antichain, so the Hoare domination preorder on $\mathcal{P}(R)$ is not a well-quasi-ordering.

If only finite subsets were intended, the answer changes again: the finite-subset lifting of a well-quasi-order is a well-quasi-ordering. Enumerate each finite subset as a finite word. Higman lemma gives an earlier word embedding into a later one with every letter increased, which witnesses Hoare domination preorder comparison of the underlying subsets. The PDF specifies no finiteness restriction, so this observation supplements rather than replaces the literal answer and the arbitrary-subset counterexample.

The LYM inequality. For an antichain $\mathcal{F}$ in the Boolean lattice,To prove this by double counting, generate a maximal chain in a Boolean lattice from a permutation $\pi$ of $[n]$: its members are the first $j$ entries of $\pi$, for $0\le j\le n$. A particular $j$-set belongs to exactly $j!(n-j)!$ of the $n!$ resulting maximal chains in a Boolean lattice. Each such maximal chain in a Boolean lattice meets the antichain at most once. Counting pairs consisting of a member of $\mathcal{F}$ and a permutation whose associated maximal chain in a Boolean lattice contains it givesDivision by $n!$ proves the LYM inequality, including the empty antichain and the levels containing $\varnothing$ or $[n]$.

A symmetric chain decomposition of a Boolean lattice. A symmetric chain has one set at every size from $k$ to $n-k$, with consecutive members related by inclusion. Start with the single symmetric chain containing $\varnothing$ when $n=0$. Given a symmetric chainin a symmetric chain decomposition of a Boolean lattice on $[n]$, let $x=n+1$ and replace its two copies in the larger Boolean lattice byand, when it is nonempty, byThe endpoint sizes of the first symmetric chain sum to $n+1$; those of the second symmetric chain also sum to $n+1$. These symmetric chains partition the original symmetric chain together with its copy containing $x$. Thus this construction inductively partitions the entire Boolean lattice into symmetric chains. Each symmetric chain contains exactly one set of size $\lfloor n/2\rfloor$, so the number of symmetric chains is

The proposed sum bound for cross-intersecting families is false. Take $n=3$ andBoth are antichains, and any member of one meets any member of the other. Nevertheless,The hypothesis permits the two antichains to coincide. Even if distinct antichains were wanted, taking $\mathcal{B}=\{\{1,2\},\{1,3\}\}$ gives $5>3$.