381 research outputs found

    Families of Graphs with W_r({G},q) Functions That Are Nonanalytic at 1/q=0

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    Denoting P(G,q)P(G,q) as the chromatic polynomial for coloring an nn-vertex graph GG with qq colors, and considering the limiting function W({G},q)=limnP(G,q)1/nW(\{G\},q) = \lim_{n \to \infty}P(G,q)^{1/n}, a fundamental question in graph theory is the following: is Wr({G},q)=q1W({G},q)W_r(\{G\},q) = q^{-1}W(\{G\},q) analytic or not at the origin of the 1/q1/q plane? (where the complex generalization of qq is assumed). This question is also relevant in statistical mechanics because W({G},q)=exp(S0/kB)W(\{G\},q)=\exp(S_0/k_B), where S0S_0 is the ground state entropy of the qq-state Potts antiferromagnet on the lattice graph {G}\{G\}, and the analyticity of Wr({G},q)W_r(\{G\},q) at 1/q=01/q=0 is necessary for the large-qq series expansions of Wr({G},q)W_r(\{G\},q). Although WrW_r is analytic at 1/q=01/q=0 for many {G}\{G\}, there are some {G}\{G\} for which it is not; for these, WrW_r has no large-qq series expansion. It is important to understand the reason for this nonanalyticity. Here we give a general condition that determines whether or not a particular Wr({G},q)W_r(\{G\},q) is analytic at 1/q=01/q=0 and explains the nonanalyticity where it occurs. We also construct infinite families of graphs with WrW_r functions that are non-analytic at 1/q=01/q=0 and investigate the properties of these functions. Our results are consistent with the conjecture that a sufficient condition for Wr({G},q)W_r(\{G\},q) to be analytic at 1/q=01/q=0 is that {G}\{G\} is a regular lattice graph Λ\Lambda. (This is known not to be a necessary condition).Comment: 22 pages, Revtex, 4 encapsulated postscript figures, to appear in Phys. Rev.

    Ground State Entropy of Potts Antiferromagnets on Cyclic Polygon Chain Graphs

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    We present exact calculations of chromatic polynomials for families of cyclic graphs consisting of linked polygons, where the polygons may be adjacent or separated by a given number of bonds. From these we calculate the (exponential of the) ground state entropy, WW, for the q-state Potts model on these graphs in the limit of infinitely many vertices. A number of properties are proved concerning the continuous locus, B{\cal B}, of nonanalyticities in WW. Our results provide further evidence for a general rule concerning the maximal region in the complex q plane to which one can analytically continue from the physical interval where S0>0S_0 > 0.Comment: 27 pages, Latex, 17 figs. J. Phys. A, in pres

    Ground State Entropy of Potts Antiferromagnets: Bounds, Series, and Monte Carlo Measurements

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    We report several results concerning W(Λ,q)=exp(S0/kB)W(\Lambda,q)=\exp(S_0/k_B), the exponent of the ground state entropy of the Potts antiferromagnet on a lattice Λ\Lambda. First, we improve our previous rigorous lower bound on W(hc,q)W(hc,q) for the honeycomb (hc) lattice and find that it is extremely accurate; it agrees to the first eleven terms with the large-qq series for W(hc,q)W(hc,q). Second, we investigate the heteropolygonal Archimedean 4824 \cdot 8^2 lattice, derive a rigorous lower bound, on W(482,q)W(4 \cdot 8^2,q), and calculate the large-qq series for this function to O(y12)O(y^{12}) where y=1/(q1)y=1/(q-1). Remarkably, these agree exactly to all thirteen terms calculated. We also report Monte Carlo measurements, and find that these are very close to our lower bound and series. Third, we study the effect of non-nearest-neighbor couplings, focusing on the square lattice with next-nearest-neighbor bonds.Comment: 13 pages, Latex, to appear in Phys. Rev.

    Confinement contains condensates

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    Dynamical chiral symmetry breaking and its connection with the generation of hadron masses has historically been viewed as a vacuum phenomenon. We argue that confinement makes such a position untenable. If quark-hadron duality is a reality in QCD, then condensates, those quantities that were commonly viewed as constant empirical mass-scales that fill all spacetime, are instead wholly contained within hadrons; viz., they are a property of hadrons themselves and expressed, e.g., in their Bethe-Salpeter or light-front wave functions. We explain that this paradigm is consistent with empirical evidence, and incidentally expose misconceptions in a recent Comment.Comment: 10 pages, 2 figure

    Ground State Entropy of the Potts Antiferromagnet on Cyclic Strip Graphs

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    We present exact calculations of the zero-temperature partition function (chromatic polynomial) and the (exponent of the) ground-state entropy S0S_0 for the qq-state Potts antiferromagnet on families of cyclic and twisted cyclic (M\"obius) strip graphs composed of pp-sided polygons. Our results suggest a general rule concerning the maximal region in the complex qq plane to which one can analytically continue from the physical interval where S0>0S_0 > 0. The chromatic zeros and their accumulation set B{\cal B} exhibit the rather unusual property of including support for Re(q)<0Re(q) < 0 and provide further evidence for a relevant conjecture.Comment: 7 pages, Latex, 4 figs., J. Phys. A Lett., in pres
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