Vertex isoperimetry and independent set stability for tensor powers of cliques
Joshua Brakensiek

TL;DR
This paper investigates vertex isoperimetry and the stability of independent sets in tensor powers of cliques, providing recursive formulas and improved bounds that have implications for graph coloring and approximation hardness.
Contribution
It introduces a recursive method to compute vertex isoperimetric bounds and establishes near-optimal stability bounds for independent sets in tensor powers of cliques.
Findings
Recursive relation for vertex isoperimetry function ()
Improved stability bounds for independent sets with exponent _t()
Results applicable to hardness of approximation in graph problems
Abstract
The tensor power of the clique on vertices (denoted by ) is the graph on vertex set such that two vertices are connected if and only if for all . Let the density of a subset of to be , and let the vertex boundary of a set to be vertices which are incident to some vertex of , perhaps including points of . We investigate two similar problems on such graphs. First, we study the vertex isoperimetry problem. Given a density what is the smallest possible density of the vertex boundary of a subset of of density ? Let be the infimum of these minimum densities as . We find a recursive relation allows one to compute in time polynomial to the number of desired bits of precision.…
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Vertex isoperimetry and independent set stability
for tensor powers of cliques
Joshua Brakensiek
Abstract.
The tensor power of the clique on vertices (denoted by ) is the graph on vertex set such that two vertices are connected if and only if for all . Let the density of a subset of to be , and let the vertex boundary of a set to be vertices which are incident to some vertex of , perhaps including points of . We investigate two similar problems on such graphs.
First, we study the vertex isoperimetry problem. Given a density what is the smallest possible density of the vertex boundary of a subset of of density ? Let be the infimum of these minimum densities as . We find a recursive relation allows one to compute in time polynomial to the number of desired bits of precision.
Second, we study given an independent set of density , how close it is to a maximum-sized independent set of density . We show that this deviation (measured by ) is at most as long as . This substantially improves on results of Alon, Dinur, Friedgut, and Sudakov (2004) and Ghandehari and Hatami (2008) which had an upper bound. We also show the exponent is optimal assuming tending to infinity and tending to [math]. The methods have similarity to recent work by Ellis, Keller, and Lifshitz (2016) in the context of Kneser graphs and other settings.
The author hopes that these results have potential applications in hardness of approximation, particularly in approximate graph coloring and independent set problems.
Department of Mathematical Sciences, Carnegie Mellon University, Pittsburgh, PA 15213, USA. Email: jbrakens at andrew.cmu.edu. This work was partially supported by REU supplements to NSF CCF-1526092 and CCF-1422045
1. Introduction
1.1. Vertex isoperimetry
For any undirected graph and , we define the vertex boundary of to be
[TABLE]
Furthermore, we define the density of to be
[TABLE]
The relationship between and , particularly when is sufficiently small (typically at most ). Is known as a vertex isoperimetric inequality. Such relationships are captured by the isoperimetric parameter (or isoperimetric profile) of a graph
[TABLE]
Proving such inequalities for various graphs is a frequent topic in the literature (e.g., [BHT00, CEK13]). Typically such works focus on a linear or near-linear relationship between and , known as the isoperimetric constant.
[TABLE]
In this paper, we study graphs for which there is an order-of-magnitude difference between and , when is sufficiently small. For example, if for all , we would like to say that expands by a power of . Such ‘hyper-expansion’ can be captured by what we coin as the isoperimetric exponent. For all consider.
[TABLE]
where is the natural logarithm. In other words, for every subset of of density , the boundary of has density at least The larger the parameter is, the more ‘expansive’ the graph is. It is easy to see that is in general a decreasing function of . As we often work with large subsets of our graph, we let .
In this paper, we study the isoperimetric profile of the tensor powers of cliques. For undirected graphs , we define the tensor product to be the undirected graph on vertex set such that an edge connects and if and only if , and Note that up to isomorphism, the tensor product is both commutative and associative. We then denote to be the tensor product of copies of . Since this is the only graph product discussed in this article, we shorten this to . In this article, we focus on the case that , where is the complete graph on vertices. It turns out for such graphs that for all , .
In particular, we shall compute the following.
Theorem 1**.**
For all and all positive integers ,
[TABLE]
In addition to this high-level structure, we give a more-fine-tuned analysis of the behavior of . (See Theorem 10.)
1.2. Independent set stability
With these vertex isoperimetric inequalities, we apply them to the understanding the structure of near-maximum independent sets of graphs. Such results are known as stability results.
Such results are not just of interest within combinatorics, a better understanding of independent set stability of certain graphs, such as , have resulted in advances in hardness of approximation, particularly in construct dictatorship tests for approximate graph coloring and independent set problems (e.g., [ADFS04, DFR08, BG16]). In fact the investigation which led to the results in this paper was inspired by the pursuit of such results.
A landmark result of this form due to [ADFS04] is as follows.
Theorem 2** ([ADFS04]).**
For all there exist with the following property. For any positive integer , Let be an independent set such that , then there exists an independent set of maximum size () such that , where .
In other words, independent sets of near-maximum size are similar in structure to the maximum independent sets. Note that if is an independent set of maximum size, then for some and , we have that
[TABLE]
This is a well-known result due to [GL74] (see [AS04] for a proof using Fourier analysis).
Ghandehari and Hatami improved this result (Theorem 1 of [GH08]) to show that if and then can be replaced with . Both results were proven using Fourier analysis.
We improve upon this result in two steps. First, with an application of Theorem 1 we improve Theorem 2 in a black-box matter to obtain.
Theorem 3**.**
For all , there exists with the following property. For any positive integer , Let be an independent set such that , then there exists an independent set of maximum size () such that
[TABLE]
Remark 1*.*
Since ,
[TABLE]
so our result gives the optimal first-order structure for Theorem 2 assuming is sufficiently small. Furthermore, in Appendix C, we give examples of independent sets of with arbitrarily small density (assuming ) for which the exponent is optimal.
Next, using a purely combinatorial argument we pin down a precise value for .
Theorem 4**.**
In Theorem 3, for all , one may set . In other words, the theorem applies for all independent sets such that .
The choice of is not arbitrary, it corresponds to the density of the following independent set.
[TABLE]
Note that This set represents a phase transition in the independent sets from ‘dictators’ to ‘juntas,’ as the constructed above is equally influenced by coordinates (where ‘influence’ is in the sense of [ADFS04]). Such phase transitions have been studied in the literature [DFR08], but this may be the first work to highlight the exact transition point.
Additionally, to the best of the author’s knowledge, this is the first known purely combinatorial proof of Theorem 2.
1.2.1. Related work
Such stability results for independent sets have also been studied for Kneser graphs. A result similar to that of Theorem 2 was proved by [Fri08]. Numerous other works in the literature [DF09, DS05, BM08, Kee08, KM10, FKMW16, FM16] prove generalized stability results for Kneser graphs or other structures related to intersecting families.
A result which also finds a “tight” super constant exponent for the independent set stability is proved in some very recent work [EKL16b, EKL16a, EL16, KL16b, KL16a, EKL17] on Kneser graphs and related structures. (See also [EKN17] and Proposition 4.3 of [Fil16].) The techniques have high-level similarity to the ones adopted here:111The author became aware of these similar proofs only after writing major portions of the manuscript. particularly in their use of compressions to prove a isoperimetric inequality which they then bootstrap to a combinatorial independent set stability result.
1.3. Paper organization
In Section 2 we prove the claimed vertex isoperimetric inequalities. In Section 3, we prove the stability results for near-maximum independent sets in . Appendix A proves some algebraic inequalities omitted from the main text. Appendix B proves Theorem 10, which gives a refined understanding the isoperimetric profile of Kneser graphs. Appendix C shows that the exponent of in Theorems 3 and 4 is optimal.
2. Vertex isoperimetric Inequalities
In this section, we proceed to prove the isoperimetry results claimed in Section 1.1.
Identify the vertex set of with . Two vertices of are connected in if and only if for all Denote . We often write as when it is clear from context which coordinate is being inserted.
2.1. Compressions
A useful tool in our study will be the operation of the well-known technique of compressions (e.g., [Sau72, She72]). Although compressions are not strictly necessary to prove Theorem 1, they are essential in the proof of stronger isoperimetry results as well as Theorem 4, so we introduce the machinery now.
For be a subset, define the compression of in coordinate to be
[TABLE]
Informally, we ‘shift’ each element of to be as small as possible in the th direction. Note that for all . It is easy to see that is nilpotent: for all and .
We say that a set is compressed if for all . Equivalently, for all there is no such that for all .
Remark 2*.*
Note that every time a compression is applied, the quantity
[TABLE]
decreases or stays the same (in which case ). Thus, since is always positive, there must exist a finite sequence of compressions which can be applied to to make the set compressed.
Now we show that compressions respect independent sets of . This result is not needed until Section 3, but the proof does give intuition for how the compressions work.
Claim 5**.**
For all and all independent set of , is also an independent set of .
Proof.
Assume not, then there exist such that is an edge. In particular, since , we must have that or . Assume without loss of generality that . Then, by definition of , there must be . Since , there must be such that
[TABLE]
Since , we must either have that or . In the former case, is an edge of and in the latter case is an edge of . This contradicts the fact that is an independent set. ∎
Next we show that compressions can only decrease the size of the vertex boundary.
Claim 6**.**
For all and , .
Proof.
Fix . Consider .
Note that for every vertex , either has [math] or elements. Thus, . We claim that for all .
- •
If , then there are no edges between and and shifting the vertices of in the th coordinate cannot change that. Thus, .
- •
If , then the set must be constant in the th coordinate. Thus, is constant in the th coordinate, so .
- •
If , then trivially
Thus, summing across all possible , we have that . ∎
Remark 3*.*
The proof crucially uses the fact that can include elements of . If we instead had defined the vertex boundary to be , there is a simple counterexample. Consider and and Then it is not hard to check that , but .
2.2. Proof of Theorem 1
Define
[TABLE]
First, we show that . In fact, we show a whole family of equality cases.
Claim 7**.**
For all positive integers and such that , .
Proof.
For all integers , consider . Then . Thus,
[TABLE]
The lower-bound is more difficult, we first need the following inequality, proved in Appendix A.
Claim 8**.**
Let be a positive integer and let be real numbers, then
[TABLE]
Lemma 9**.**
For positive integers and and all , we have that
[TABLE]
Therefore .
Proof.
By Claim 6 and Remark 2, it suffices to consider the case that is compressed. We now proceed by induction on .
For our base case, , we must have that in which case (8) is trivial, or for some positive integer . If , then , in which case we have an equality case of (8) by the proof of Claim 7. Otherwise, if , then , so , so (8) holds.
For , assume by the induction hypothesis that (8) is true for all where . For all , let
[TABLE]
Since is compressed for all , we have that . Thus, if is nonzero, for any , there is connected to by an edge of . Thus, . Similarly, for any , there is such that is disjoint from . Therefore, . Putting these together,
[TABLE]
where we applied the inductive hypothesis in the last step. Applying Claim 8, using the fact that , we have that
[TABLE]
as desired. ∎
Claim 7 and Lemma 9 together imply Theorem 1.
2.3. A fine-tuned understanding of the isoperimetric
profile.
Recall the (vertex) isoperimetric profile of a graph to be
[TABLE]
For fixed, define
[TABLE]
Note that is non-decreasing. It is easier to work with instead of each directly to avoid complications with the discrete behavior of when is small. By Theorem 1,
[TABLE]
This is tight whenever for any integer , but ceases to be tight when is non-integral (see Figure 1).
The following recursive relationship allows one to compute to arbitrary precision.
Theorem 10**.**
For all ,
[TABLE]
Using the simple fact that and , the above equation is extremely powerful. For example,
[TABLE]
which is an exact bound compared to . This recursion is what allowed the creation of Figure 1.
Theorem 10 is proved in Appendix B. This more refined understanding of proves critical in the combinatorial proof of Theorem 4.
3. Independent set stability results
3.1. Black-box result for clique tensor powers
First, we show that if a large independent set is somewhat close to a maximum-sized independent set , then it is really close to . We fix positive integers and .
Lemma 11**.**
Let be an independent set with Assume there exists a maximum-sized independent set such that
[TABLE]
Then,
[TABLE]
Proof.
Without loss of generality, we may assume that . Pick such that but otherwise is maximal. Let . Since and are disjoint, we have that
[TABLE]
Now, consider . Recall the definition of from (9). Since has the property that every element has the same last coordinate, for all and . Thus, for all . Therefore,
[TABLE]
Applying Theorem 1, we get that
[TABLE]
Since is an independent set, is disjoint from . Since , we have that and are disjoint. Therefore,
[TABLE]
But, we also know that
[TABLE]
[TABLE]
Thus,
[TABLE]
Consider Figure 2 which has a plot of the RHS of (15) when . If is sufficiently small, then the inequality holds only when is very small (polynomial in ) or very large (about ). Since is ‘moderately’ small (), we must have that is very small. Quantitatively, note that
[TABLE]
So
[TABLE]
Therefore,
[TABLE]
where the last inequality follows from the following claim which is proved in Appendix A.
Claim 12**.**
For all ,
[TABLE]
∎
We now use this lemma to ‘amplify’ Theorem 2 to prove Theorem 3.
Proof of Theorem 3..
Set . Consider any independent set of of such that . Pick any maximum-sized guaranteed by Theorem 2 such that
[TABLE]
By Lemma 11, we have that
[TABLE]
as desired. ∎
3.2. Improved stability result for clique tensor powers
In this section we improve in Theorem 3 to an explicit expression. In fact, we may show that
[TABLE]
which corresponds to independent sets for which .
First, we try to show that if an independent set is large enough, then is either very close to or very far from a maximum-sized independent set. To do this, we show that if is ‘moderately far’ from a maximum-sized independent set, then this moderate-sized portion which is not in the maximum-sized independent set has such a large vertex boundary that it precludes a large portion of the maximum-sized independent set from being part of , forcing the density of to be at or below our threshold of .
We need a notation for the maximum sized independent sets. For all and let
[TABLE]
We say that is sorted if there exists that for all and we have that implies that
[TABLE]
Note that unlike compressions, we may assume without loss of generality that is sorted since permuting the labels so that an independent set is sorted does not change its intersection sizes with the maximum independent sets.
Claim 13**.**
Let be a sorted independent set such that (or ), then for all ,
[TABLE]
Proof.
Without loss of generality, we may let . Denote . Let . Since is an independent set
[TABLE]
Note that is [math] if but is otherwise (see the proof of Theorem 3 for more explanation). Thus, by Theorem 1,
[TABLE]
Since , we have that
[TABLE]
Thus, we obtain that
[TABLE]
Note that the two sides of the inequality are equal at and . Note that since for all , the RHS of (22) is concave for all . Thus, (22) is false when . Therefore, we have (18). ∎
From Theorem 10, we can attain a bound that is even better.
Claim 14**.**
Let be a sorted independent set such that , then for all ,
[TABLE]
Proof.
Again, we may assume without loss of generality that , let . Let . From Claim 13, we only need to consider the case that
[TABLE]
From (20)
[TABLE]
Now make the substitution
[TABLE]
where . From Theorem 10,
[TABLE]
Hence, since ,
[TABLE]
Rearranging,
[TABLE]
Like in the proof of Claim 13, we have equality when and . Furthermore, since for all , the RHS is concave when . Thus, the inequality is false for all Therefore, (24) can never hold, proving (23), as desired. ∎
The next key step is to show Theorem 4 essentially holds for compressed independent sets .
Lemma 15**.**
Let be a compressed independent set such that , then for some ,
[TABLE]
Note that by Lemma 11, we immediately have that Theorem 4 holds for compressed independent sets.
Proof.
We prove this statement by induction on . If , then the bound holds since which is clearly a maximum-sized independent set. Now assume and that the (25) holds for all compressed independent sets with .
Fix a compressed independent set with . From Claim 14, if the lemma is false, then we have that for all ,
[TABLE]
Since is compressed, this implies that for all such
[TABLE]
Recall that for all , We claim that is an independent set of . Note that in general is not an independent set of . Since is compressed, . Thus, if there were which form an edge of , then form an edge of , contradicting that is an independent set. Therefore, is indeed an independent set.
Note that which is not sharp enough of a lower bound to invoke the inductive hypothesis. But, we claim that we can find a compressed independent set such that .
Pick such that has maximal size.222To keep notation as concise as possible, we use the notation to refer to both the maximal independent sets of and . It should be clear from context which we are referring to. Note that since is not necessarily compressed, might not equal . Let . We claim that is an independent set (although it might not be compressed). As previously established is an independent set and clearly is an independent set since the last coordinate is constant. Thus, if were not an independent set then, there is and which are connected by an edge in . But, note that are connected by an edge in , contradiction. Thus, is an independent set of .
Let be a compression of . since and are already compressed and , we have that . Now,
[TABLE]
Thus, we may now invoke the induction hypothesis on . Therefore, there exists such that
[TABLE]
Since , we have that
[TABLE]
Therefore, since is compressed
[TABLE]
Hence, recalling that is very far from
[TABLE]
Likewise,
[TABLE]
Let and . Now observe that since is compressed
[TABLE]
Similarly,
[TABLE]
Since is constant in both the th and th coordinates,
[TABLE]
From Theorem 10, we have that
[TABLE]
since . Therefore, since is an independent set
[TABLE]
contradiction. Thus, the lemma is true. ∎
Now we extend this result to sorted independent sets; and thus all independent sets.
Lemma 16**.**
Let be a sorted independent set such that , then for some ,
[TABLE]
Proof.
Like in the proof of Lemma 15, by Claim 14, we may assume for sake of contradiction that for all ,
[TABLE]
It is not hard to see that for all such that ,
[TABLE]
We seek to show that for all ,
[TABLE]
By Claim 14, assume for sake of contradiction that
[TABLE]
for some . We may assume without loss of generality that . Since is sorted,
[TABLE]
Therefore,
[TABLE]
This implies that
[TABLE]
Observe that since is an independent set
[TABLE]
Therefore, if , then (because any other choice for the last coordinate would violate the above relation). Therefore,
[TABLE]
From this, we get that
[TABLE]
Next, we deduce
[TABLE]
Let . Then note that
[TABLE]
Thus, by (44)
[TABLE]
We divide the remainder of the proof into three cases depending on the value of .
Case333Recall that by (37) 1: . By Theorem 10 and the fact that for all ,
[TABLE]
Thus, by (45)
[TABLE]
Rearranging,
[TABLE]
This implies that
[TABLE]
Thus, , but this is false for , contradiction.
Case 2, .
Then . Thus, by (45)
[TABLE]
contradiction.
Case 3, .
Observe that
[TABLE]
Since is sorted, . Therefore,
[TABLE]
Thus, , but for , contradiction.
End Cases.
Therefore, our assumption that (35) failed to hold is false. Therefore
[TABLE]
for all . Applying this fact repeatedly, we can find a compressed of the same cardinality as such that for all , contradicting Lemma 15. Thus, our counterexample could have never existed. This proves the Lemma. ∎
Proof of Theorem 4.
Let be an independent set with . Assume without loss of generality that is sorted. By Lemma 16, we know that there is such that
[TABLE]
Thus, by Lemma 11, we have that
[TABLE]
as desired. ∎
Acknowledgments
The author is indebted to Venkatesan Guruswami for numerous insightful discussions and comments, in particular for pointing the author to [ADFS04].
The author would also like to thank Boris Bukh and Po-Shen Loh for helpful comments and discussions.
The 2D plots were created using Matplotlib [Hun07]. The 3D visualizations were created using Asymptote [HBP14].
Appendix A Proofs of algebraic inequalities
Proof of Claim 8.
For , let . Notice that if , then . Thus, we have that for all . Consider ; we then have that
[TABLE]
Rearranging, we obtain (7). ∎
Proof of Claim 12..
First, verify the cases and using a calculator. Notice that so
[TABLE]
Also use a calculator to verify that is less than for . Now observe that when going from to , the numerator increases by
[TABLE]
and the denominator increases by
[TABLE]
Since for all and we have by a simple inductive proof that for all . Thus, for all ,
[TABLE]
as desired. ∎
Appendix B Proof of Theorem 10
The first step in proving this theorem is to determine the structure of when is fixed but is minimized. In particular, we need to look as much like a maximal independent set (e.g., ) as possible.
Claim 17**.**
Let and be positive integers. Let be a maximum-sized independent set. Consider .
- (1)
If , then there exists such that , , and . 2. (2)
If , then there exists such that , , and .
For each , define , the level of , be the number of coordinates of not equal to (c.f., [ADFS04]).
Proof.
Without loss of generality, assume that . By Claim 6, we may assume that is compressed. This immediately resolves the case , so we may assume .
Consider the map such that
[TABLE]
Let be the indicator function of . Since is compressed, is a monotone Boolean function: whenever for all .
For all , let denote the bitwise complement of . Note that for any and , and are connected by an edge in . Therefore, because is compressed
[TABLE]
and so
[TABLE]
We now describe an algorithm which modifies into a compressed such that is maximized while keeping and . This algorithm consists of two subroutines.
Filling. See Figure 3. Let
[TABLE]
Note that but , so by (48).
Note that is compressed since is monotone.
Folding.444Note that this Folding operation is considered another form of compression in the literature, although typically used for Kneser graphs. For example see \urlhttps://gilkalai.wordpress.com/2008/10/06/extremal-combinatorics-iv-shifting/ Assume that That is, for each ,
The operator is defined for each subset .
For each let be the operator which negates the elements indexed by
[TABLE]
For any let
[TABLE]
Then, we define
[TABLE]
Figures 4 and 5 help to visualize this operator.
First, note that in the case , since is compressed. Thus, since , .
For , note that since each element of either stays the same or is replace by such that . Thus, since for all such and . we have that . Furthermore, by (48), if we know that is compressed, then .
Thus, it suffices to determine when is compressed. We claim that this is always the case when for all .
Claim 18**.**
Let be compressed and nonempty. If and for all , then is compressed and so by the above discussion and .
Proof.
This is equivalent to showing that is monotone. Assume for contradiction that there is and . such that .
First consider the case .Thus, for all and . Since , . Let .
If for some . Then, Since we assumed , we know that . Thus, since is compressed, . But, , so , contradiction.
Otherwise, Since is compressed and , we have that . Thus, since , we have that . Thus , so . Let .
Let be the coordinates for which . Then, . Since , it can be checked that . Since is compressed and , we have that . If , then this contradicts the fact that . If , then this contradicts the fact that because . ∎
Now that we have defined the operators, we finish the proof. First, set . Now, topologically sort the subsets of by inclusion. For each , in this topological order, apply to . If it so happens that applying causes for some earlier in the topological order, we go backtrack to the earliest such .
By Claim 18, we know that is still compressed after each operation. Note that each time changes, strictly increases. Thus, after some finite number of applications of these operations, we will have a compressed such that for all , , , and .
Furthermore, since , we know that either or . Now, take any such that while preserving the property that or . Since , we have that as desired. ∎
With this claim proven, we may now prove the theorem.
Proof of Theorem 10..
We divide the proof into four parts.
- •
Part 1: If then
Consider any such that . Let
[TABLE]
be the set where every element of has a appended. Note that
[TABLE]
Therefore,
[TABLE]
Thus,
[TABLE]
where
- •
Part 2: If then
Consider any such that . If , then , for which it is trivial that . Thus, assume .
If , then by Theorem 1,
[TABLE]
Thus, we may assume . By Claim 17 there is such that , and . Let
[TABLE]
Intuitively, is ‘stacked’ times. Therefore, .Then,
[TABLE]
Therefore,
[TABLE]
Thus,
[TABLE]
- •
Part 3: If then
For any such that , let be
[TABLE]
Then,
[TABLE]
Therefore,
[TABLE]
Hence,
[TABLE]
- •
Part 4: If then
For any such that , by Claim 17 there is such that , , and . Pick such that is maximal.555Note that we did not define in (9) for . In that case, define to be if and if . It is consistent to define and . Then
[TABLE]
and also
[TABLE]
Thus,
[TABLE]
Therefore,
[TABLE]
∎
Appendix C Optimality of exponent in Theorem 3
In this appendix, we show in (4) of Theorem 3 that the exponent is optimal and that the constant factor of is nearly optimal. In other words, the stability result is optimal up to a constant factor.
Lemma 19**.**
For all , there exists an infinite sequence of independent sets such that , tends to [math] as , and for any and any maximum-sized independent set of ,
[TABLE]
Proof.
For , consider and
[TABLE]
See Figure 6 for a visualization.
One may check that is an independent set of and is a maximum-sized independent set which minimizes . Furthermore,
[TABLE]
Thus,
[TABLE]
Notice that since
[TABLE]
Therefore, raising both sides to the power,
[TABLE]
as desired. ∎
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