Twists for positroid cells

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Twists for positroid cells Greg Muller, joint with David Speyer December 0, 204

Objects of study: positroid cells The matroid of a k n matrix is the set of subsets of columns which form a basis, written as k-subsets of [n] := {, 2,..., n}. A positroid is the matroid of a totally positive matrix : a real-valued matrix whose maximal minors are all non-negative. A matroid M defines a variety in the (k, n)-grassmannian. Π(M) := {[A] Gr(k, n) the matroid of A M} Definition (Positroid cell) The positroid cell of a positroid M is Π (M) := Π(M) positroids M M Π(M ) These cells define a well-behaved stratification of Gr(k, n).

Motivation from double Bruhat cells Example (Double Bruhat cells) Double Bruhat cells in GL(n) map to positroid cells under GL(n) Gr(n, 2n), A [ ω A ] where ω is the antidiagonal matrix of ones. In a double Bruhat cell, the same data indexes two sets of subtori. Reduced words for (u, v) Products of elementary matrices in GL u,v The twist Clusters in GL u,v Berenstein-Fomin-Zelevinsky introduced a twist automorphism of the cell GL u,v which takes one type of torus to the other.

The need for a generalized twist Postnikov described a generalization to all positroid cells. Reduced graphs in the disc with positroid M Boundary measurement maps into Π (M) Conj. clusters in Π (M)? However, it wasn t proven these constructions defined tori, and the generalized twist was missing for more than a decade! Then, Marsh-Scott found the twist for the open cell in Gr(k, n). Our goal! Inspired by MS, define the twist automorphism of every Π (M). As a corollary, we prove that the constructions produce tori.

But first, we need to define... a reduced graph with positroid M, its boundary measurement map B : a torus Π (M), and its (conjectural) cluster F : Π (M) a torus. Compared to that, the definition of the twist is elementary.

Matchings of graphs in the disc Let G be a graph in the disc with a 2-coloring of its internal vertices. We assume each boundary vertex is adjacent to one white vertex, and no black or boundary vertices. A matching of G is a subset of the edges for which every internal vertex is in exactly one edge. We assume a matching exists.

The positroid of a graph Observation: Every matching of G must use k := (# of white vertices) (# of black vertices) boundary vertices. If we index the boundary vertices clockwise by [n], which k-element subsets of [n] are the boundary of matchings? Theorem (Postnikov, Talaska, Postnikov-Speyer-Williams) The k-element subsets of [n] which are the boundary of some matching of G form a positroid. Every positroid occurs this way. A graph G is reduced if it has the minimal number of faces among all graphs with the same positroid as G.

Generating functions of matchings More than asking if a subset I ( n k) is a boundary, we can encode which matchings have boundary I into a generating function D I. Example (Generating functions) 4 d a b c e f h i j 3 g 2 The ( 4 2) generating functions are: D 2 = bdgi D 4 = adfh D 24 = acgi + aegh D 3 = bdfj D 23 = begj D 34 = acfj Clearly, a generating function D I is identically zero if and only if I is not in the positroid of G.

Relations between generating functions Remarkably, the generating functions satisfy the Plücker relations! So, for a complex number at each edge of G, there is a matrix... 4 d a b c e f h 3 j i g 2 [ bd bge ] f 0 ac afh 0 gi fj b...whose I th maximal minor equals the I th generating function D I... D 2 = bdgi D 4 = adfh D 24 = acgi + aegh D 3 = bdfj D 23 = begj D 34 = acfj 2 = bdgi 4 = adfh 24 = acgi + aegh 3 = bdfj 23 = begj 34 = acfj...and this matrix determines a well-defined point in Gr(k, n).

The boundary measurement map Hence, we have a map C Edges(G) Gr(k, n) This map is invariant under gauge transformations: simultaneously scaling the numbers at each edge incident to a fixed internal vertex. Theorem (Postnikov, Talaska, M-Speyer) For reduced G, the map (C ) Edges(G) Gr(k, n) factors through B : (C ) Edges(E) /Gauge Π (M) where M is the positroid of G. The map B is called the boundary measurement map. Conjecture (essentially Postnikov) The map B is an open inclusion.

Strands in a reduced graph A strand in reduced G is a path which... 2 3 passes through the midpoints of edges, turns right around white vertices, turns left around black vertices, and 4 begins and ends at boundary vertices. 2 3 6 5 3 3 4 Index a strand by its source vertex, and label each face to the left of the strand by that label. 6 3 5

Face labels and the cluster structure Repeating this for each strand, each face of G gets labeled by a subset of [n]. Each face label is a k-element subset of [n], which determines a Plücker coordinate on Gr(k, n). Conjecture (essentially Postnikov) 2 3 25 56 23 256 24 245 456 234 The homogeneous coordinate ring of Π (M) is a cluster algebra, and the Plücker coordinates of the faces of G form a cluster. 6 345 5 4 The conjecture implies the Plückers of the faces give a rational map F : Π (M) (C ) Faces(G) /Scaling which is an isomorphism on its domain (the cluster torus).

Two conjectural tori associated to a reduced graph We now see that a reduced graph G with positroid M determines two subspaces in Π (M), which are both conjecturally tori. The image of the boundary measurement map B : (C ) Edges(G) /Gauge Π (M) The domain of definition of the cluster of Plücker coordinates F : Π (M) (C ) Faces(G) /Scaling In a simple world, they d coincide and we d have an isomorphism F B : (C ) Edges(G) /Gauge (C ) Faces(G) /Scaling In the real world, we need a twist automorphism τ of Π (M).

The twist of a matrix Let A be a k n matrix of rank k, and assume no zero columns. Denote the ith column of A by A i, with cyclic indices: A i+n = A i. Definition (The twist) The twist τ(a) of A is the k n-matrix defined on columns by τ(a) i A i = τ(a) i A j = 0, if A j is not in the span of {A i, A i+,..., A j } The columns A i and {A j } in the definition are the first basis of columns encountered when starting at column i and moving right. The vector τ(a) i is the left column of the inverse of the submatrix on these columns.

Example of a twist Twisting a matrix Consider the 3 4 matrix 0 0 A = 0 2 0 0 0 The first column τ(a) of the twist is a 3-vector v, such that... [ ] [ ] [ 0 ] [ 0 ] v 0 =, v = 0, v is already fixed, and v 2 = 0 0 0 0 [ ] We see that v =. We compute the twist matrix 2 0 0 τ(a) = 0 0 2 0 2

The twist on a positroid cell Twisting matrices descends to a well-defined map of sets Gr(k, n) τ Gr(k, n) However, this map is not continuous; the defining equations jump when A j deforms to a column in the span of {A i, A i+,..., A j }. Proposition The domains of continuity of τ are precisely the positroid cells. Theorem (M-Speyer) The twist τ restricts to a regular automorphism of Π (M). The inverse of τ is given by a virtually identical formula to τ, by reversing the order of the columns.

The induced map on tori If τ takes the image of B to the domain of F, then the composition F τ B : (C ) Edges(G) /Gauge (C ) Faces(G) /Scaling is a regular morphism. What is this map? Example: the open cell of Gr(2, 4) 4 d a b c e f h 3 B j i [ bd beg f 0 ac afh 0 gi fj b g 2? 4 ] τ [ bd acfj begj f beg aegh 3 F e dfi 0 fj adfh bdgi h bcj 0 b afh ] 2

Minimal matchings It looks like the entries are reciprocals of matchings! Which ones? Proposition (Propp) The set of matchings of G with fixed boundary I has a partial order, with a unique minimal and maximal element (if non-empty). Lemma (M-Speyer) If I is the label of a face in G, then I τ B = product of edges in M I where M I is the minimal matching with boundary I. We have two direct constructions of these minimal matchings.

The isomorphism of model tori We can collect these coordinates into a map (C ) Edges(G) (C ) Faces(G) whose coordinate at a face labeled by I is the reciprocal of the product of the edges in the minimal matching with boundary I. Lemma (M-Speyer) The above map induces an isomorphism of algebraic tori D : (C ) Edges(E) /Gauge (C ) Faces(E) /Scaling In fact, the inverse D can be induced from an explicit map (C ) Faces(G) (C ) Edges(G) whose coordinate at an edge only uses the two adjacent faces.

Putting it all together Theorem (M-Speyer) For each reduced graph G, there is a commutative diagram D (C ) Edges(G) /Gauge (C ) Faces(G) /Scaling D B Π (M) τ τ F Π (M) Corollaries: The image of B and the domain of F are open algebraic tori in Π (M), and τ takes one to the other. The (rational) inverse of B is D F τ. The (regular) inverse of F is τ B D.

Application: Inverting the boundary measurement map Let s invert B in a classic example! Example: The unipotent cell in GL(3), as a positroid cell?? 3 4????? 2 5???????? 6 B 0 0 a b c 0 0 0 d e 0 0 0 0 f

Application: Inverting the boundary measurement map Let s invert B in a classic example! Example: The unipotent cell in GL(3), as a positroid cell 0 0 a b c 0 0 0 d e 0 0 0 0 f

Application: Inverting the boundary measurement map Let s invert B in a classic example! Example: The unipotent cell in GL(3), as a positroid cell 0 0 a b c 0 0 0 d e 0 0 0 0 f τ 0 0 e a bd ce c b b c 0 0 d ad be cd e be cd be cd f 0 0 df adf

Application: Inverting the boundary measurement map Let s invert B in a classic example! Example: The unipotent cell in GL(3), as a positroid cell 3 4 c a 2 be cd b acd (adf ) ad 5 6 0 0 a b c 0 0 0 d e 0 0 0 0 f τ 0 0 e a bd ce c b b c 0 0 d ad be cd e be cd be cd f 0 0 df adf F

Application: Inverting the boundary measurement map Let s invert B in a classic example! Example: The unipotent cell in GL(3), as a positroid cell 3 a 4 ac 2 c ac 2 d a 2 cd b b ad 5 acd(be cd) b a 2 cd 2 f b be cd adf (be cd) a 2 cd 2 f b a 2 d 2 f a 2 cd 2 b adf 6 D 3 4 c a 2 be cd b acd (adf ) ad 5 6 0 0 a b c 0 0 0 d e 0 0 0 0 f τ 0 0 e a bd ce c b b c 0 0 d ad be cd e be cd be cd f 0 0 df adf F

Application: Inverting the boundary measurement map Let s invert B in a classic example! Example: The unipotent cell in GL(3), as a positroid cell a 3 4 3 4 e d d D c a 2 5 2 5 be cd cd b ae ae be cd acd ad f 6 6 (adf ) B 0 0 a b c 0 0 0 d e 0 0 0 0 f τ 0 0 e a bd ce c b b c 0 0 d ad be cd e be cd be cd f 0 0 df adf F

Relation to the Chamber Ansatz So, we have the following boundary measurement map. 3 a 4 e d 2 d 5 be cd cd ae ae f 6 B 0 0 a b c 0 0 0 d e 0 0 0 0 f This is equivalent to a factorization into elementary matrices. [ ] [ ] [ ] [ ] [ ] a b c a 0 0 cd 0 ae 0 0 be cd 0 ae e 0 d e = 0 d 0 0 0 0 d 0 0 0 0 f 0 0 f 0 0 0 0 0 0 Our computation to find this factorization is identical to the Chamber Ansatz introduced by Berenstein-Fomin-Zelevinsky.

Application: Counting matchings Corollary Let G be a reduced graph with positroid M. If A is a matrix with the matroid of A is contained in M, and for each face label I, the minor I (A) =, then the maximal minor J (τ (A)) counts matchings with boundary J. Example: Domino tilings of the Aztec diamond of order 3 Domino tilings of this shape......are the same as matchings of this graph, with boundary {4, 5, 6, 0,, 2}. 4 3 5 2 6 7 2 8 9 0

Application: Counting matchings Example: (continued) Here is an appropriate A and its inverse twist. A = τ (A) = 6 8 0 0 0 0 0 0 6 3 5 0 0 0 0 0 0 0 5 3 0 0 0 0 0 0 0 0 6 8 2 2 2 0 0 0 0 0 0 6 2 6 0 0 0 0 0 0 0 0 2 0 26 0 0 0 0 0 0 0 0 0 2 2 2 0 0 0 0 0 0 6 0 6 2 0 0 0 0 0 6 8 26 0 2 0 0 0 0 0 5 3 8 6 0 0 0 0 0 3 5 6 0 0 0 0 0 0 0 0 We compute that {4,5,6,0,,2} (τ (A)) = 64. Finding A by brute force is probably not efficient, but verifying that a matrix has the necessary properties can be faster than counting.

Further directions Directions to generalize! Positroid cells in Gr(k, n) projected Richardson cells in partial flag varieties. Reduced graphs in the disc reduced graphs in surfaces. If we label strands by their target instead of their source, we get a different cluster structure on the same algebra. How are they related? Conjecture: The twist is the decategorification of the shift functor in a categorification. Any cluster algebra with a Jacobi-finite potential has such a shift automorphism. Can this story can be extended?