Alternating sign matrix

Mathematical model From Wikipedia, the free encyclopedia

In mathematics, an alternating sign matrix is a square matrix of 0s, 1s, and −1s such that the sum of each row and column is 1 and the nonzero entries in each row and column alternate in sign. These matrices generalize permutation matrices and arise naturally when using Dodgson condensation to compute a determinant.[1] They are also closely related to the six-vertex model with domain wall boundary conditions from statistical mechanics. They were first defined by William Mills, David Robbins, and Howard Rumsey in the former context.

The seven alternating sign matrices of size 3

Examples

The permutation matrices are precisely the alternating sign matrices that don't contain −1.

An example of an alternating sign matrix that is not a permutation matrix is

Puzzle picture corresponding to the 4x4 alternating sign matrix shown to the left. Green pieces represent zeros, vertical yellow pieces are 1 and horizontal yellow pieces are -1.

Alternating sign matrix theorem

The alternating sign matrix theorem states that the number of alternating sign matrices is

The first few terms in this sequence for n = 0, 1, 2, 3, … are

1, 1, 2, 7, 42, 429, 7436, 218348, … (sequence A005130 in the OEIS).

This theorem was first proved by Doron Zeilberger in 1992.[2] In 1995, Greg Kuperberg gave a short proof[3] based on the Yang–Baxter equation for the six-vertex model with domain-wall boundary conditions, that uses a determinant calculation due to Anatoli Izergin.[4] In 2005, a third proof was given by Ilse Fischer using what is called the operator method.[5]

Razumov–Stroganov problem

In 2001, A. Razumov and Y. Stroganov conjectured a connection between O(1) loop model, fully packed loop model and alternating sign matrices.[6] This conjecture was proved in 2010 by Cantini and Sportiello.[7]

References

Further reading

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