Integrable equations for the partition function of the six-vertex model

2000 ◽  
Vol 100 (2) ◽  
pp. 2141-2146 ◽  
Author(s):  
A. G. Izergin ◽  
E. Karjalainen ◽  
N. A. Kitanin
10.37236/4971 ◽  
2015 ◽  
Vol 22 (2) ◽  
Author(s):  
Angèle M. Hamel ◽  
Ronald C. King

A recent paper of Bump, McNamara and Nakasuji introduced a factorial version of Tokuyama's identity, expressing the partition function of  six vertex model as the product of a $t$-deformed Vandermonde and a Schur function. Here we provide an extension of their result by exploiting the language of primed shifted tableaux, with its proof based on the use of non-interesecting lattice paths.


2003 ◽  
Vol 315 (3-4) ◽  
pp. 231-236 ◽  
Author(s):  
F. Colomo ◽  
A.G. Pronko

2011 ◽  
Vol 844 (2) ◽  
pp. 289-307 ◽  
Author(s):  
Wen-Li Yang ◽  
Xi Chen ◽  
Jun Feng ◽  
Kun Hao ◽  
Bo-Yu Hou ◽  
...  

2011 ◽  
Vol 847 (2) ◽  
pp. 367-386 ◽  
Author(s):  
Wen-Li Yang ◽  
Xi Chen ◽  
Jun Feng ◽  
Kun Hao ◽  
Kang-Jie Shi ◽  
...  

1995 ◽  
Vol 09 (24) ◽  
pp. 3209-3217 ◽  
Author(s):  
G. ROLLET ◽  
F. Y. WU

We consider vertex models on an arbitrary graph and propose a new polynomial formulation for its gauge transformation under which the partition function is invariant. Our formulation recovers in a simple way various, previously obtained results including the condition under which the vertex model is equivalent to an Ising model.


It is shown that various cases of the Ashkin-Teller model on the square, triangular and hexagonal lattices can be transformed by the dual and star-triangle transformations and, further, that these problems can be reduced to special cases of the eight vertex model on the Kagomé lattice. In general, we can only obtain the partition function of the Ashkin-Teller model if we are on its line of fixed points, and it then turns out that it is reducible to the six vertex model. Since the partition function of the q -state Potts model at its critical point can also be related to the six vertex model, a direct connection between the Ashkin-Teller model and the Potts model can be made. It turns out that moving along the critical line of the Ashkin-Teller model corresponds to varying q for the Potts model. For the square lattice comparison is made with renormalization group calculations, and the agreement found is a satisfactory check of renormalization group theory.


2020 ◽  
Vol 2020 (6) ◽  
Author(s):  
Zoltan Bajnok ◽  
Jesper Lykke Jacobsen ◽  
Yunfeng Jiang ◽  
Rafael I. Nepomechie ◽  
Yang Zhang

2020 ◽  
Vol DMTCS Proceedings, 28th... ◽  
Author(s):  
Roger Behrend ◽  
Ilse Fischer ◽  
Matjaz Konvalinka

International audience We study the enumeration of diagonally and antidiagonally symmetric alternating sign matrices (DAS- ASMs) of fixed odd order by introducing a case of the six-vertex model whose configurations are in bijection with such matrices. The model involves a grid graph on a triangle, with bulk and boundary weights which satisfy the Yang– Baxter and reflection equations. We obtain a general expression for the partition function of this model as a sum of two determinantal terms, and show that at a certain point each of these terms reduces to a Schur function. We are then able to prove a conjecture of Robbins from the mid 1980's that the total number of (2n + 1) × (2n + 1) DASASMs is∏n (3i)! ,andaconjectureofStroganovfrom2008thattheratiobetweenthenumbersof(2n+1)×(2n+1) i=0 (n+i)! DASASMs with central entry −1 and 1 is n/(n + 1). Among the several product formulae for the enumeration of symmetric alternating sign matrices which were conjectured in the 1980's, that for odd-order DASASMs is the last to have been proved.


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