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Proofs and Confirmations: the Story of the Alternating Sign Matrix Conjecture

Authors:
Proofs & Confirmations!
The story of the !
alternating sign matrix conjecture!
David M. Bressoud
Macalester College
Arizona State University
Tempe, AZ
March 19, 2009!
These slides are available at !
www.macalester.edu/~bressoud/talks!
Artwork by Greg Kuperberg!
0 0 1 0 0
0 1 1 0 1
1 1 0 1 0
0 1 0 0 0
0 0 1 0 0
Square matrix:!
Entries are 0, 1, –1!
Row and column sums
are +1!
Non-zero entries
alternate in sign in each
row!
Bill Mills!
Howard Rumsey!
IDA-CCR!
David Robbins
(1942–2003)!
MAA Robbins Prize in
algebra, combinatorics, or
discrete math!
Charles L. Dodgson!
aka Lewis Carroll!
“Condensation of Determinants,”
Proceedings of the Royal Society, London
1866!
Desnanot-Jacobi adjoint matrix theorem (Desnanot for
n 6 in 1819, Jacobi for general case in 1833!
M
j
i
is matrix M with row i and column j removed.!
det M =
det M
1
1
det M
n
n
det M
n
1
det M
1
n
det M
1,n
1,n
Given that the determinant of the empty
matrix is 1 and the determinant of a 1×1
is the entry in that matrix, this uniquely
defines the determinant for all square
matrices.!
Carl Jacobi (1804–1851)!
det M =
det M
1
1
det M
n
n
det M
n
1
det M
1
n
det M
1,n
1,n
det
λ
M =
det
λ
M
1
1
det
λ
M
n
n
+
λ
det
λ
M
n
1
det
λ
M
1
n
det
λ
M
1,n
1,n
det
1
M = det M
( )
det
λ
a
j
i 1
( )
i, j =1
n
= a
i
+
λ
a
j
( )
1i < j n
det
λ
a b
c d
= ad +
λ
bc
det
λ
a b c
d e f
g h j
= aej +
λ
bdj + afh
( )
+
λ
2
bfg + cdh
( )
+
λ
3
ceg
+
λ
1 +
λ
( )
bde
1
fh
det M =
det M
1
1
det M
n
n
det M
n
1
det M
1
n
det M
1,n
1,n
det
λ
M =
det
λ
M
1
1
det
λ
M
n
n
+
λ
det
λ
M
n
1
det
λ
M
1
n
det
λ
M
1,n
1,n
0 1 0 0
1 1 1 0
0 1 1 1
0 0 1 0
0 1 0 0
1 1 1 0
0 0 0 1
0 1 0 0
det
λ
x
i, j
( )
=
λ
Inv A
( )
A= a
i , j
( )
1 +
λ
1
( )
N A
( )
x
i, j
a
i , j
i, j
Sum is over all alternating sign matrices, N(A) = # of –1’s!
n!
1!
2!
3!
4!
5!
6!
7!
8!
9!
A
n!
1!
2!
7!
42!
429!
7436!
218348!
10850216!
911835460!
0 0 1 0 0
0 1 1 0 1
1 1 0 1 0
0 1 0 0 0
0 0 1 0 0
n!
1!
2!
3!
4!
5!
6!
7!
8!
9!
A
n!
1!
2!
7!
42 !
429!
7436!
218348!
10850216!
911835460!
= 3 × 11 × 13!
= 2
2
× 11 × 13
2!
= 2
2
× 13
2
× 17 × 19!
= 2
3
× 13 × 17
2
× 19
2!
= 2
2
× 5 × 17
2
× 19
3
× 23!
= 2 × 3 × 7!
How many n × n alternating sign
matrices?!
n!
1!
2!
3!
4!
5!
6!
7!
8!
9!
A
n!
1!
2!
7!
42!
429!
7436!
218348!
10850216!
911835460!
0 0 1 0 0
0 1 1 0 1
1 1 0 1 0
0 1 0 0 0
0 0 1 0 0
There is exactly one 1
in the first row!
n!
1!
2!
3!
4!
5!
6!
7!
8!
9!
A
n!
1!
1+1!
2+3+2!
7+14+14+7!
42+105+…!
0 0 1 0 0
0 1 1 0 1
1 1 0 1 0
0 1 0 0 0
0 0 1 0 0
There is exactly one 1
in the first row!
1!
1 1!
2 3 2!
7 14 14 7!
42 105 135 105 42!
429 1287 2002 2002 1287 429!
1!
1 1!
2 3 2!
7 14 14 7!
42 105 135 105 42!
429 1287 2002 2002 1287 429!
+! +! +!
1!
1 1!
2 3 2!
7 14 14 7!
42 105 135 105 42!
429 1287 2002 2002 1287 429!
+! +! +!
1!
1 2/2 1!
2 2/3 3 3/2 2!
7 2/4 14 14 4/2 7!
42 2/5 105 135 105 5/2 42!
429 2/6 1287 2002 2002 1287 6/2 429!
1!
1 2/2 1!
2 2/3 3 3/2 2!
7 2/4 14 5/5 14 4/2 7!
42 2/5 105 7/9 135 9/7 105 5/2 42!
429 2/6 1287 9/14 2002 16/16 2002 14/9 1287 6/2 429!
2/2!
2/3 3/2 !
2/4 5/5 4/2 !
2/5 7/9 9/7 5/2!
2/6 9/14 16/16 14/9 6/2!
1+1 !
1+1 1+2 !
1+1 2+3 1+3 !
1+1 3+4 3+6 1+4 !
1+1 4+5 6+10 4+10 1+5 !
Numerators:!
1+1 !
1+1 1+2 !
1+1 2+3 1+3 !
1+1 3+4 3+6 1+4 !
1+1 4+5 6+10 4+10 1+5 !
Conjecture 1:!
Numerators:!
A
n,k
A
n,k +1
=
n 2
k 1
+
n 1
k 1
n 2
n k 1
+
n 1
n k 1
Conjecture 1:!
Conjecture 2 (corollary of Conjecture 1):!
A
n,k
A
n,k +1
=
n 2
k 1
+
n 1
k 1
n 2
n k 1
+
n 1
n k 1
A
n
=
3 j + 1
( )
!
n + j
( )
!
j = 0
n1
=
1!4!7! 3n 2
( )
!
n! n + 1
( )
! 2n 1
( )
!
Richard Stanley!
Richard Stanley!
George Andrews!
Andrews’ Theorem: the number
of descending plane partitions
of size n is!
A
n
=
3 j + 1
( )
!
n + j
( )
!
j = 0
n1
=
1!4!7! 3n 2
( )
!
n! n + 1
( )
! 2n 1
( )
!
What is a
descending
plane partition?!
Percy A. MacMahon!
Plane Partition
Work begun in!
1897!
6 5 5 4 3 3!
Plane partition of 75
# of pp’s of 75 = pp(75)
6 5 5 4 3 3!
Plane partition of 75
# of pp’s of 75 = pp(75) = 37,745,732,428,153
Generating function:!
1 + pp j
( )
j =1
q
j
= 1 + q + 3q
2
+ 6q
3
+ 13q
4
+
=
1
1 q
k
( )
k
k =1
=
1
1 q
( )
1 q
2
( )
2
1 q
3
( )
3
1912 MacMahon proves that the generating function for
plane partitions in an n × n × n box is
1 q
i + j + k 1
1 q
i + j + k 2
1i, j, k n
Symmetric Plane Partition
4 3 2 1 1
3 2 2 1
2 2 1
1 1
1
At the same time, he conjectures that the
generating function for symmetric plane
partitions is
1 q
i + j + k 1
1 q
i + j + k 2
1i = j n
1k n
1 q
2 i+ j + k 1
( )
1 q
2 i+ j + k 2
( )
1i < j n
1k n
“The reader must be warned that, although there
is little doubt that this result is correct, … the
result has not been rigorously established. …
Further investigations in regard to these matters
would be sure to lead to valuable work.’ (1916)!
1971 Basil Gordon
proves case for n = infinity
1971 Basil Gordon
proves case for n = infinity
1977 George Andrews and Ian Macdonald
independently prove general case
Cyclically Symmetric Plane Partition
Macdonald’s Conjecture (1979): The
generating function for cyclically
symmetric plane partitions in B(n,n,n) is!
“If I had to single out the most interesting open
problem in all of enumerative combinatorics, this
would be it.” Richard Stanley, review of
Symmetric Functions and Hall Polynomials,
Bulletin of the AMS, March, 1981.!
1 q
η
1+ ht
η
( )
( )
1 q
η
ht
η
( )
η
B /C
3
1979, Andrews counts cyclically symmetric
plane partitions
1979, Andrews counts cyclically symmetric
plane partitions
1979, Andrews counts cyclically symmetric
plane partitions
1979, Andrews counts cyclically symmetric
plane partitions
1979, Andrews counts cyclically symmetric
plane partitions
length!
width!
L
1
= W
1
> L
2
= W
2
> L
3
= W
3
> …!
1979, Andrews counts descending plane
partitions
length!
width!
L
1
> W
1
L
2
> W
2
L
3
> W
3
!
6 6 6 4 3!
3 3!
2!
length!
width!
6 6 6 4 3!
3 3!
2!
Mills, Robbins, Rumsey Conjecture: # of n × n
ASM’s with 1 at top of column j equals # of
DPP’s n with exactly j–1 parts of size n.!
Discovered an easier proof of Andrews’
formula, using induction on j and n.!
Used this inductive argument to prove
Macdonald’s conjecture!
“Proof of the Macdonald Conjecture,” Inv. Math.,
1982!
But they still didn’t have a
proof of their conjecture!!
1983!
Totally Symmetric Self-Complementary
Plane Partitions!
Vertical flip of ASM = complement of DPP ?!
David Robbins!
Totally Symmetric Self-Complementary
Plane Partitions!
Robbins’ Conjecture: The number of
TSSCPP’s in a 2n X 2n X 2n box is
3 j + 1
( )
!
n + j
( )
!
j = 0
n1
=
1!4!7! 3n 2
( )
!
n! n + 1
( )
! 2n 1
( )
!
Robbins’ Conjecture: The number of
TSSCPP’s in a 2n X 2n X 2n box is
1989: William Doran shows equivalent to
counting lattice paths!
1990: John Stembridge represents the counting
function as a Pfaffian (built on insights of
Gordon and Okada)!
1992: George Andrews evaluates the Pfaffian,
proves Robbins’ Conjecture!
3 j + 1
( )
!
n + j
( )
!
j = 0
n1
=
1!4!7! 3n 2
( )
!
n! n + 1
( )
! 2n 1
( )
!
December, 1992!
Doron Zeilberger
announces a proof that
# of ASM’s of size n
equals of TSSCPP’s in
box of size 2n.!
December, 1992!
Doron Zeilberger
announces a proof that
# of ASM’s of size n
equals of TSSCPP’s in
box of size 2n.!
1995 all gaps removed, published as “Proof of
the Alternating Sign Matrix Conjecture,” Elect. J.
of Combinatorics, 1996.!
Zeilbergers proof is an 84-page
tour de force, but it still left open
the original conjecture:!
A
n, k
A
n, k +1
=
n 2
k 1
+
n 1
k 1
n 2
n k 1
+
n 1
n k 1
1996 Kuperberg
announces a simple proof
“Another proof of the alternating
sign matrix conjecture,”
International Mathematics
Research Notices!
Greg Kuperberg!
UC Davis!
1996 Kuperberg
announces a simple proof
“Another proof of the alternating
sign matrix conjecture,”
International Mathematics
Research Notices!
Greg Kuperberg!
UC Davis!
Physicists had been studying ASM’s
for decades, only they called them the
six-vertex model.!
Horizontal = 1!
Vertical = –1!
0 0 1 0 0
0 1 1 0 1
1 1 0 1 0
0 1 0 0 0
0 0 1 0 0
1960’s
Anatoli Izergin
Vladimir Korepin
1980’s
Rodney Baxters
Triangle-to-
triangle relation!
det
1
x
i
y
j
( )
ax
i
y
j
( )
x
i
y
j
( )
ax
i
y
j
( )
i, j =1
n
x
i
x
j
( )
y
i
y
j
( )
1i < j n
= 1 a
( )
2 N A
( )
a
n(n1)/2 Inv A
( )
A
A
n
× x
i
vert
y
j
ax
i
y
j
( )
SW, NE
x
i
y
j
( )
NW, SE
a = z
4
, x
i
= z
2
, y
i
= 1
RHS = z z
1
( )
n n 1
( )
z + z
1
( )
2 N A
( )
A
A
n
z = e
π
i /3
RHS = 3
( )
n n 1
( )
/2
A
n
det
1
x
i
y
j
( )
ax
i
y
j
( )
x
i
y
j
( )
ax
i
y
j
( )
i, j =1
n
x
i
x
j
( )
y
i
y
j
( )
1i < j n
= 1 a
( )
2 N A
( )
a
n(n1)/2 Inv A
( )
A
A
n
× x
i
vert
y
j
ax
i
y
j
( )
SW, NE
x
i
y
j
( )
NW, SE
1996
Doron Zeilberger
uses this
determinant to
prove the original
conjecture
“Proof of the refined alternating sign matrix
conjecture,” New York Journal of Mathematics!
!e End"
(which is really just the beginning)!
These slides can be downloaded from
www.macalester.edu/~bressoud/talks!
... The seminal work of Razumov and Stroganov [1] revealed a remarkable combinatorial structure of the periodic Heisenberg XXZ spin chain with anisotropy ∆ = −1/2. They investigated the ground state of the Hamiltonian for chains of odd length N = 2n + 1 and observed that in a suitable normalisation, many components and scalar products are given by integer sequences in n which appear in the enumeration of alternating sign matrices (ASMs) and plane partitions [2]. Similar connections were found for chains of even length with twisted boundary conditions, as well as for open chains with boundary magnetic fields [3][4][5]. ...
... Each such matrix is assigned the weight t k where k is the number of orbits of negative entries, or equivalently the number of negative entries in one quadrant. Their generating function is denoted by A QT (2N ; t) and was found by Kuperberg [23] to factorise as the product of two polynomials in t, A (1) QT (2N ; t) and A (2) QT (2N ; t). Theorem 2.10. ...
... Following Kuperberg's notation, we denote by A UU (4n; t, y, z) the corresponding generating function for 2n × 2n UUASMs. He proved that [23] A (2) UU (4n; t, y, z) = ...
Preprint
The nineteen-vertex model on a periodic lattice with an anti-diagonal twist is investigated. Its inhomogeneous transfer matrix is shown to have a simple eigenvalue, with the corresponding eigenstate displaying intriguing combinatorial features. Similar results were previously found for the same model with a diagonal twist. The eigenstate for the anti-diagonal twist is explicitly constructed using the quantum separation of variables technique. A number of sum rules and special components are computed and expressed in terms of Kuperberg's determinants for partition functions of the inhomogeneous six-vertex model. The computations of some components of the special eigenstate for the diagonal twist are also presented. In the homogeneous limit, the special eigenstates become eigenvectors of the Hamiltonians of the integrable spin-one XXZ chain with twisted boundary conditions. Their sum rules and special components for both twists are expressed in terms of generating functions arising in the weighted enumeration of various symmetry classes of alternating sign matrices (ASMs). These include half-turn symmetric ASMs, quarter-turn symmetric ASMs, vertically symmetric ASMs, vertically and horizontally perverse ASMs and double U-turn ASMs. As side results, new determinant and pfaffian formulas for the weighted enumeration of various symmetry classes of alternating sign matrices are obtained.
... Alternating Sign Matrices (ASM), i.e. matrices with entries 0, 1, −1, such that 1 and −1's alternate along each row and column, possibly separated by arbitrarily many 0's, and such that row and column sums are all 1, have attracted much attention over the years and seem to be a Leitmotiv of modern combinatorics, hidden in many apparently unrelated problems, involving among others various types of plane partitions or the rhombus tilings of domains of the plane (see the beautiful book by Bressoud [1] and references therein). The intrusion first of physics and then of physicists in the subject was due to the fundamental remark that the ASM of size n × n may be identified with configurations of the six-vertex model, that consist of putting arrows on the edges of a n × n square grid, subject to the ice rule (there are exactly two incoming and two outgoing arrows at each vertex of the grid), with so-called domain wall boundary conditions. ...
... A case of particular interest is when the model is defined on a square n×n grid, with socalled domain wall boundary conditions (DWBC), namely with horizontal external edges pointing inwards and vertical external edges pointing outwards. Moreover, we consider the fully inhomogeneous case where we pick n arbitrary horizontal spectral parameters, 1 Note that we use a slightly unusual sign convention for q, which is however convenient here. ...
... We may now repeat the whole process with the removal of pairs of arches with numbers (n − 2, n − 1), (n − 3, n − 2), . . . , (1,2). This yields the invariance of α n under the interchange of any two of its consecutive arguments, henceforth α n is fully symmetric in its n arguments. ...
Preprint
We prove that the sum of entries of the suitably normalized groundstate vector of the O(1) loop model with periodic boundary conditions on a periodic strip of size 2n is equal to the total number of n x n alternating sign matrices. This is done by identifying the state sum of a multi-parameter inhomogeneous version of the O(1) model with the partition function of the inhomogeneous six-vertex model on a n x n square grid with domain wall boundary conditions.
... Using a second guise of ASMs, the six vertex model, Kuperberg [8] could find a different proof for their enumeration. A more detailed account on the history of the ASM Theorem can be found in [2]. ...
... FurtherΨ n (t) is independent of t and uniquely determined by (2). ...
... Using again the induction hypothesis for the D τ 's with τ ≤σ proofs the claim. (d) Let a = 0, b = 1 and letσ be the noncrossing matching whose Young diagram consists of λ(σ ) and the boxes labelled with α i for 1 ≤ i ≤ A. Lemma 12 (2,3) implies ...
Preprint
This article proves a conjecture by Zuber about the enumeration of fully packed loops (FPLs). The conjecture states that the number of FPLs whose link pattern consists of two noncrossing matchings which are separated by m nested arches is a polynomial function in m of certain degree and with certain leading coefficient. Contrary to the approach of Caselli, Krattenthaler, Lass and Nadeau (who proved a partial result) we make use of the theory of wheel polynomials developed by Di Francesco, Fonseca and Zinn-Justin. We present a new basis for the vector space of wheel polynomials and a polynomiality theorem in a more general setting. This allows us to finish the proof of Zubers conjecture.
... The problem of enumerating alternating sign matrices has led to many deep results and difficult conjectures. For a history of alternating sign matrices see [1]. There are several combinatorial and physical structures equivalent to alternating sign matrices. ...
... One of the most fertile has been the square-ice model originally used in statistical mechanics. The square ice graph corresponding to (1) is ...
Preprint
We settle a question of Bressoud concerning the existence of an explicit bijection from a class of oriented square-ice graphs to a class of tournaments. We give an algorithm constructing such a bijection.
... The domain wall boundary partition functions is one of the most well-studied class of partition functions. It was first introduced and investigated by Korepin [4], and later Izergin found its determinant representation [5] based on his analysis, which have been used for applications to the enumeration of the alternating sign matrices [6,7,8,9] in later years. The most important step for the analysis of the domain wall boundary partition functions was the work by Korepin [4], in which he presented a way how to view partition functions as multivariable polynomials of spectral parameters by using the quantum inverse scattering method, which was crucial for the Izergin-Korepin determinant formula [5] to be found. ...
... 6) when x N = M .Let us show (5.1) satisfies Property(4). See[21] for case of the simpler wavefunctions without reflecting boundary. ...
Preprint
We extend the recently developed Izergin-Korepin analysis on the wavefunctions of the Uq(sl2)U_q(sl_2) six-vertex model to the reflecting boundary conditions. Based on the Izergin-Korepin analysis, we determine the exact forms of the symmetric functions which represent the wavefunctions and its dual. Comparison of the symmetric functions with the coordinate Bethe ansatz wavefunctions for the open XXZ chain by Alcaraz-Barber-Batchelor-Baxter-Quispel is also made. As an application, we derive algebraic identities for the symmetric functions by combining the results with the determinant formula of the domain wall boundary partition function of the six-vertex model with reflecting end.
... Connections to fields such as statistical mechanics [2] and enumerative combinatorics [3] were subsequently discovered, and ASMs continue to attract sustained interest from diverse viewpoints. We refer to Bressoud's book [4], for a comprehensive account of the emergence of attention to ASMs and the mathematical developments that ensued. ...
Article
We investigate multiplicative groups consisting entirely of singular alternating sign matrices (ASMs) and present several constructions of such groups. It is shown that every finite group is isomorphic to a group of singular ASMs, with a singular idempotent ASM as its identity element. The relationship between the size, the rank, and the possible multiplicative orders of singular ASMs is explored.
... The conjecture was first resolved by Zeilberger [Zei96], with subsequent proofs provided by Kuperberg [Kup96], Fischer [Fis06,Fis07,Fis16], and Fischer and Konvalinka [FK20a,FK20b,FK22]. For a history of ASMs, see [Bre99]. ...
Preprint
A diagonally symmetric alternating sign matrix (DSASM) is a symmetric matrix with entries 1-1, 0 and 1, where the nonzero entries alternate in sign along each row and column, and the sum of the entries in each row and column equals 1. An off-diagonally symmetric alternating sign matrix (OSASM) is a DSASM, where the number of nonzero diagonal entries is 0 for even-order matrices and 1 for odd-order matrices. Kuperberg (Ann. Math., 2002) studied even-order OSASMs and derived a product formula for counting the number of OSASMs of any fixed even order. In this work, we provide a product formula for the number of odd-order OSASMs of any fixed order. Additionally, we present an algebraic proof of a symmetry property for even-order OSASMs. This resolves all the three conjectures of Behrend, Fischer, and Koutschan (arXiv, 2023) regarding the exact enumeration of OSASMs.
... The author acknowledges support from the Austrian Science Foundation FWF, START grant Y463 and SFB grant F50. Alternating sign matrices (ASMs), on the other hand, were introduced more than 35 years ago [RR86,MRR82,Bre99] and are defined as square matrices with entries in {0, 1, −1} such that, along each row and each column, the non-zero elements alternate and add up to 1. It is no coincidence that there are also 7 ASMs of order 3 as it was shown in [ABF] that, for any positive integer n, there is the same number of order n ASMs as there is of order n ASTs. ...
Preprint
Alternating sign triangles (ASTs) have recently been introduced by Ayyer, Behrend and the author, and it was proven that there is the same number of ASTs with n rows as there is of nxn alternating sign matrices (ASMs). We prove a conjecture by Behrend on a refined enumeration of ASTs with respect to a statistic that is shown to have the same distribution as the column of the unique 1 in the top row of an ASM. The proof of the conjecture is based on a certain multivariate generating function of ASTs that takes the positions of the columns with sum 1 (1-columns) into account. We also prove a curious identity on the cyclic rotation of the 1-columns of ASTs. Furthermore, we discuss a relation of our multivariate generating function to a formula of Di Francesco and Zinn-Justin for the number of fully packed loop configurations associated with a given link pattern. The proofs of our results employ the author's operator formula for the number of monotone triangles with prescribed bottom row. This is opposed to the six-vertex model approach that was used by Ayyer, Behrend and the author to enumerate ASTs, and since the refined enumeration implies the unrefined enumeration, the present paper also provides an alternative proof of the enumeration of ASTs.
... We will be discussing a type of square matrix called an alternating sign matrix. These matrices were introduced in [5], and subsequently linked to many other topics in Combinatorics; see [1] for an overview. In [4] the alternating sign matrices are linked to partially ordered sets in the following way. ...
Preprint
For an integer n1n\geq 1, we display a poset Φn\Phi_n whose maximal chains are in bijection with the n×nn\times n alternating sign matrices. The Hasse diagram Φ^n\widehat \Phi_n is obtained from the n-cube by adding some edges. We show that the dihedral group D2nD_{2n} acts on Φ^n\widehat \Phi_n as a group of automorphisms.
... In recent years it has become clear that some exactly integrable models present a deep and somehow unexpected combinatorial structure, related to various enumerations of alternating sign matrices (ASM). Such matrices appeared for the first time in the work of Mills, Robbins and Rumsey [1], and from that moment on they have played a fundamental role in modern developments of combinatorics [2]. An ASM is a matrix with only 0, 1, −1 entries, such that on each row and on each column 1s and −1s appear alternately, possibly separated by zeroes and the sum on each row and each column is equal to 1. ...
Preprint
In this paper we study the Rotor Model of Martins and Nienhuis. After introducing spectral parameters, a combined use of integrability, polynomiality of the ground state wave function and a mapping into the fully-packed O(1)-model allows us to determine the sum rule and a family of maximally nested components for different boundary conditions. We see in this way the appearance of 3-enumerations of Alternating Sign Matrices.
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