Structural properties of Potts model partition functions and chromatic polynomials for lattice strips

Citation
Sc. Chang et R. Shrock, Structural properties of Potts model partition functions and chromatic polynomials for lattice strips, PHYSICA A, 296(1-2), 2001, pp. 131-182
Citations number
91
Categorie Soggetti
Physics
Journal title
PHYSICA A
ISSN journal
03784371 → ACNP
Volume
296
Issue
1-2
Year of publication
2001
Pages
131 - 182
Database
ISI
SICI code
0378-4371(20010701)296:1-2<131:SPOPMP>2.0.ZU;2-M
Abstract
The q-state Potts model partition function (equivalent to the Tutte polynom ial) for a lattice strip of fixed width L-y and arbitrary length L-x has th e form Z(G, q, v) = Sigma (NZ,j)(j=1) c(Z,G,j)(lambda (Z,G,j))(Lx), where L ; is a temperature-dependent variable. The special case of the zero-tempera ture antiferromagnet (v = -1) is the chromatic polynomial P(G, q). Using co loring and transfer matrix methods, we give general formulas for C-X,C-G = Sigma (NX,j)(j=1) c(X,G,j) for X = Z,P on cyclic and Mobius strip graphs of the square and triangular lattice. Combining these with a general expressi on for the (unique) coefficient c(Z,G,j) of degree d in q: c((d)) = U-2d(ro otq/2), where U-n(x) is the Chebyshev polynomial of the second kind, we det ermine the number of lambda (Z,G,j)'s with coefficient c((d)) in Z(G,q,v) f or these cyclic strips of width L-y to be n(Z)(L-y,d)=(2d + 1)(L-y + d + 1) (-1) ((2Lx)(Ly-d)) for 0 less than or equal to d less than or equal to L-y and zero otherwise, For both cyclic and Mobius strips of these lattices, th e total number of distinct eigenvalues lambda (Z,G,j) is calculated to be N -Z,N-L,N-lambda=((2Lx)(Ly)). Results are also presented for the analogous n umbers n(P)(L-y, d) and N(P,Ly,)lambda for P(G,q). We find that n(P)(L-y, 0 )=n(P)(L-y- 1,1)=MLx-1 (Motzkin number), n(Z)(L-y,0)= C-Lx (the Catalan num ber), and give an exact expression for N-P,N-Ly,N-lambda. Our results for N -Z,N-Ly,N-lambda and N-P,N-Ly,N-lambda apply for both the cyclic and Mobius strips of both the square and triangular lattices; we also point out the i nteresting relations N-Z,N-Ly,N-lambda = 2N(DA,tri.Ly) and N-P,N-Ly,N-lambd a = 2N(DA,sq,Ly,) where N-DA,N-A,N-n denotes the number of directed lattice animals on the lattice Lambda. We find the asymptotic growths N-Z,N-Ly,N-l ambda similar to L-y(-1.2) 4(Ly) and N-P,N-Ly,N-lambda similar to L(y)(-1.2 )3(Ly) as L-y --> infinity. Some general geometric identities for Potts mod el partition functions are also presented. 0 2001 Published by Elsevier Sci ence B.V.