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Shards and noncrossing tree partitions Alexander Clifton and Peter Dillery August 4, 2016 Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 1 / 48

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Shards and noncrossing tree partitions

Alexander Clifton and Peter Dillery

August 4, 2016

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 1 / 48

Outline

1 Broad overview

2 What is a noncrossing tree partition?

3 Lattice theory4 The structure of noncrossing tree partitions

1 Grading2 Self-duality3 Enumerative results

5 Defining a CU-labeling of BicpT q6 Shard intersection order of BicpT q

1 Describing ψpBq2 Describing ψpCq X ψpDq3 Putting it all together

7 Further enumerative results

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 2 / 48

Broad Overview

Fix a tree T embedded in a disk with exactly its leaves on theboundary and whose interior vertices (the vertices not on theboundary) have degree at least 3.

T =

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 3 / 48

Broad Overview

We obtain the following diagram of posets defined from T :

Bic(T ) Ψ(Bic(T ))

−→FG(T ) Ψ(

−→FG(T ))

ψ

ψ

φ ?

NCP(T )∼

Goal: Understand the combinatorics of NCPpT q

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 4 / 48

Noncrossing tree partitions: Overview

The poset NCPpT q is called the noncrossing tree partitions of T . Inthis part of the talk, we will discuss our research of the followingproperties of NCPpT q:

1 NCPpT q is a lattice

2 NCPpT q is graded (conjecture)

3 NCPpT q is not self-dual

4 How to count the maximal chains in NCPpT q

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 5 / 48

What is NCPpT q?

For a tree T , a segment s “ pv0, . . . , vtq “ rv0, vts with t ě 1 is asequence of interior vertices of T that takes a “sharp” turn at each vi.In particular, the interior vertices of T are not segments.

Example

In the tree below, p1, 5q and p2, 4, 6q are segments. The sequence p1, 3qis not a segment.

2

3

4

5

6

1

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 6 / 48

A noncrossing partition B “ pB1, . . . , Bkq is a set partition of the interior vertices of Twhere

the vertices in Bi can be connected by red admissible curves (i.e. curves whoseendpoints define segments of T and leave their endpoints to the right), where any pairof such curves can only agree at their endpoints, andred admissible curves connecting vertices of Bi do not cross those of Bj for i ‰ j.

We let NCPpT q denote the poset of noncrossing tree partitions ordered by refinement.

ExampleB “ tt1, 4, 6u, t2, 3u, t5uu is an element of NCPpT q.

2

3

4

5

6

1

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 7 / 48

Theorem (Garver-McConville)

The poset NCPpT q is a lattice.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 8 / 48

Lattice Theory

Before we talk about the structural properties of NCPpT q, we need todiscuss the relevant lattice theory.

Definition

A lattice is called congruence-uniform if it can be constructed from asingle point using interval doublings.

Here is an example of a lattice constructed from interval doublings:

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 9 / 48

Lattice Theory

Theorem

A lattice is congruence-uniform if and only if it admits an edge labelingknown as a CU-labeling.

In fact, the colors on the edges of the picture above form aCU-labeling, where the color set is ordered s ď t if the color s appearsbefore t in the sequence of doublings.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 10 / 48

Lattice Theory

L a latticeλ a CU-labeling of Lx ∈ L

Ψ(L)Shard intersection order

ΨpLq consists of sets

ψpxq “ tlabels appearing betweenk

ľ

i“1

yi and xu

where tyiuki“1 is the set of elements immediately below x in L. The

partial ordering on ΨpLq is inclusion. We call the interval rŹki“1 yi, xs

the facial interval corresponding to x.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 11 / 48

Back to NCPpT q

Theorem (Garver-McConville)

For a tree T , NCPpT q is isomorphic to ΨpÝÝÑFGpT qq.

This brings us to one of the main objects in our project:

Conjecture

The lattice NCPpT q is graded by the number of blocks in a partition.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 12 / 48

Conjecture

The lattice NCPpT q is graded by the number of blocks in a partition.

How we want to prove this conjecture:

Show that every covering relation in NCPpT q is given by mergingtwo blocks of a partition (which is what happens with NCpnq).

To do this, it suffices to show that if we can merge m blocks of B,m ě 3, then we can merge m´ 1 blocks.

To show the above, we work withÝÝÑFGpT q. We know that B

corresponds to a facial interval inÝÝÑFGpT q. We want to show that it

is contained in a facial interval “one dimension lower” than theentire lattice.

B ÞÑ ψpxq „ ra, xs Ĺ ra1, x1s ĹÝÝÑFGpT q

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 13 / 48

Corollaries of conjecture and further structure

Garver and McConville defined a bijection NCPpT q called theKreweras Complement. The Kreweras complement sends a partitionwith m blocks to a partition with #V opT q ` 1´m blocks. A corollaryof this map and the previous conjecture is the following:

Corollary

The lattice NCPpT q is rank-symmetric.

The above property is shared by NCpnq. A natural question to ask is:How many of the nice properties of NCpnq carry over to NCPpT q? Weprovide a partial answer here:

Theorem

In general, NCPpT q is not self-dual.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 14 / 48

We conclude our discussion of NCPpT q with a method of calculatingthe number of maximal chains, denoted mcpT q.

We will exploit the following fact in order to obtain recursions: lettaiu

ni“1 be the set of coatoms of NCPpT q; then

mcpT q “n

ÿ

i“1

mcpr0̂, aisq.

From here, we can note that r0̂, ais is isomorphic to the product of twononcrossing tree partitions of smaller trees, as shown by the followingpicture:

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 15 / 48

2

3

4

5

6

1ai =

We have that r0̂, ais – NCPpT1q ˆNCPpT2q, where

T1 = T2 =

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 16 / 48

Using this method, we can count the maximal chains of the kthstar-graph, denoted Sk, which is the family of trees of the followingform:

S5

k = # of edgesattached to central vertex

We get that mcpSkq “k!Fk`1

2 , where Fk`1 is the pk ` 1qth fibonaccinumber.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 17 / 48

Segments S1, S2 P SegpT q whose composition is also in SegpT q arecomposable.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 18 / 48

A subset B Ă SegpT q is closed if for any composable S1, S2 P B, wehave S1

9S2 P B.

A subset B Ă SegpT q is biclosed if both B and BC are closed.

BicpT q is a poset who elements are biclosed sets B Ă SegpT q, partiallyordered by inclusion.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 19 / 48

A subset B Ă SegpT q is closed if for any composable S1, S2 P B, wehave S1

9S2 P B.

A subset B Ă SegpT q is biclosed if both B and BC are closed.

BicpT q is a poset who elements are biclosed sets B Ă SegpT q, partiallyordered by inclusion.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 19 / 48

A subset B Ă SegpT q is closed if for any composable S1, S2 P B, wehave S1

9S2 P B.

A subset B Ă SegpT q is biclosed if both B and BC are closed.

BicpT q is a poset who elements are biclosed sets B Ă SegpT q, partiallyordered by inclusion.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 19 / 48

We will explicitly demonstrate the CU-labeling for BicpT q.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 20 / 48

For a segment ra, cs with vertex b in between, we say that ra, bs andrb, cs constitute a break of ra, cs

Each of ra, bs and rb, cs is a split of ra, cs corresponding to that break.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 21 / 48

For a segment ra, cs with vertex b in between, we say that ra, bs andrb, cs constitute a break of ra, cs

Each of ra, bs and rb, cs is a split of ra, cs corresponding to that break.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 21 / 48

Recall that a CU-labeling is a map λ : tcovering relations ofBicpT qu Ñ P for some poset P of labels.

We choose P with elements of the form S∆ where S P SegpT q and ∆ isa set of splits of S. The partial ordering is given by S∆ ě Qµ if Scontains Q.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 22 / 48

Recall that a CU-labeling is a map λ : tcovering relations ofBicpT qu Ñ P for some poset P of labels.

We choose P with elements of the form S∆ where S P SegpT q and ∆ isa set of splits of S. The partial ordering is given by S∆ ě Qµ if Scontains Q.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 22 / 48

Covering relations in BicpT q look like:

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 23 / 48

Covering relations in BicpT q look like:

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 24 / 48

Example:

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 25 / 48

Example:

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 26 / 48

Example:

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 27 / 48

Example:

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 28 / 48

Example:

Covering relations look like

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 29 / 48

Example:

Covering relations look like

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 29 / 48

Example:

Covering relations look like

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 30 / 48

Example:

Covering relations look like

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 31 / 48

Example:

Covering relations look like

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 32 / 48

ΨpBicpT qq has a maximum element.

If we can show that for all C,D P BicpT q, there exists someB P BicpT q such that ψpCq X ψpDq “ ψpBq, then we can conclude thatΨpBicpT qq is a lattice.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 33 / 48

Elements of ψpBq are those of the form S∆ where S is a composition ofsome of S1, S2, . . . , Sm and ∆ is a set of splits of S with certainstipulations.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 34 / 48

Vertices within S which are endpoints of some Si correspond tofaultline breaks.

Other vertices correspond to non-faultline breaks.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 35 / 48

Vertices within S which are endpoints of some Si correspond tofaultline breaks.

Other vertices correspond to non-faultline breaks.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 36 / 48

What splits of S are in ∆?

For non-faultline breaks, these are predetermined by ∆1,∆2, . . . ,∆m.For each faultline break, there is an independent choice.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 37 / 48

What splits of S are in ∆?

For non-faultline breaks, these are predetermined by ∆1,∆2, . . . ,∆m.

For each faultline break, there is an independent choice.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 37 / 48

What splits of S are in ∆?

For non-faultline breaks, these are predetermined by ∆1,∆2, . . . ,∆m.For each faultline break, there is an independent choice.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 37 / 48

Labels in ψpCq X ψpDq are of the form S∆ where:

S must simultaneously be a composition of Si’s and Qi’s.Furthermore, the splits determined by the corresponding ∆i’s and µi’smust be compatible.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 38 / 48

Labels in ψpCq X ψpDq are of the form S∆ where:S must simultaneously be a composition of Si’s and Qi’s.

Furthermore, the splits determined by the corresponding ∆i’s and µi’smust be compatible.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 38 / 48

Labels in ψpCq X ψpDq are of the form S∆ where:S must simultaneously be a composition of Si’s and Qi’s.Furthermore, the splits determined by the corresponding ∆i’s and µi’smust be compatible.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 38 / 48

S must simultaneously be a composition of Si’s and Qi’s:

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 39 / 48

The only breaks for which there is a choice of what split of S to includein ∆ are when the break is a faultline for S viewed as a composition ofSi’s and S viewed as a composition of Qi’s.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 40 / 48

The only breaks for which there is a choice of what split of S to includein ∆ are when the break is a faultline for S viewed as a composition ofSi’s and S viewed as a composition of Qi’s.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 41 / 48

The only breaks for which there is a choice of what split of S to includein ∆ are when the break is a faultline for S viewed as a composition ofSi’s and S viewed as a composition of Qi’s.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 42 / 48

Call an element of ψpCq XψpDq pseudominimal if it does not containany double faultlines in its composition pair.

Pseudominimal elements generate all of ψpCq X ψpDq in the sense thatany S∆ P ψpCq X ψpDq satisfies

1 S is a composition of the segment parts of pseudominimal labels.

2 The only choices for which splits of S to include in ∆ occur atbreaks where two such pseudominimal lables are joined together.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 43 / 48

Call an element of ψpCq XψpDq pseudominimal if it does not containany double faultlines in its composition pair.

Pseudominimal elements generate all of ψpCq X ψpDq in the sense thatany S∆ P ψpCq X ψpDq satisfies

1 S is a composition of the segment parts of pseudominimal labels.

2 The only choices for which splits of S to include in ∆ occur atbreaks where two such pseudominimal lables are joined together.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 43 / 48

Call an element of ψpCq XψpDq pseudominimal if it does not containany double faultlines in its composition pair.

Pseudominimal elements generate all of ψpCq X ψpDq in the sense thatany S∆ P ψpCq X ψpDq satisfies

1 S is a composition of the segment parts of pseudominimal labels.

2 The only choices for which splits of S to include in ∆ occur atbreaks where two such pseudominimal lables are joined together.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 43 / 48

Call an element of ψpCq XψpDq pseudominimal if it does not containany double faultlines in its composition pair.

Pseudominimal elements generate all of ψpCq X ψpDq in the sense thatany S∆ P ψpCq X ψpDq satisfies

1 S is a composition of the segment parts of pseudominimal labels.

2 The only choices for which splits of S to include in ∆ occur atbreaks where two such pseudominimal lables are joined together.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 43 / 48

Pseudominimal elements of ψpCq X ψpDq generate ψpCq X ψpDq thesame way ψpBq is generated by the labels on its covering relations.

We can conceivably takeB “ _t pseudominimal elements of ψpCq X ψpDqu to obtainψpBq “ ψpCq X ψpDq.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 44 / 48

For the star graph Sk:

|NCP pSkq| “

2|NCP pSk´1q| ` |NCP pSk´2q|

with |NCP pS3q| “ 14, |NCP pS4q| “ 34

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 45 / 48

For the star graph Sk:

|NCP pSkq| “2|NCP pSk´1q| ` |NCP pSk´2q|

with |NCP pS3q| “ 14, |NCP pS4q| “ 34

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 45 / 48

For the star graph Sk:

|NCP pSkq| “2|NCP pSk´1q| ` |NCP pSk´2q|

with |NCP pS3q| “ 14, |NCP pS4q| “ 34

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 45 / 48

Straight trees like

are analagous to classical non-crossing partitions.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 46 / 48

Thank you to project mentor Al Garver,project TA Craig Corsi, ThomasMcConville, Vic Reiner, the University ofMinnesota, and the National ScienceFoundation.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 47 / 48

References

A. Garver and T. McConville. Oriented flip graphs and noncrossingtree partitions. arXiv: 1604.06009, 2016.

N. Reading. Noncrossing partitions and the shard intersectionorder. Journal of Algebraic Combinatorics, 2011.

R. Simion and D. Ullman. On the structure of the lattice ofnoncrossing partitions. Discrete Mathematics, 1989.

Alexander Clifton and Peter Dillery Shards and noncrossing tree partitions August 4, 2016 48 / 48