697 research outputs found

    The continuum limit of aN−1(2)a_{N-1}^{(2)} spin chains

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    Building on our previous work for a2(2)a_2^{(2)} and a3(2)a_3^{(2)} we explore systematically the continuum limit of gapless aN−1(2)a_{N-1}^{(2)} vertex models and spin chains. We find the existence of three possible regimes. Regimes I and II for a2n−1(2)a_{2n-1}^{(2)} are related with a2n−1(2)a_{2n-1}^{(2)} Toda, and described by nn compact bosons. Regime I for a2n(2)a_{2n}^{(2)} is related with a2n(2)a_{2n}^{(2)} Toda and involves nn compact bosons, while regime II is related instead with B(1)(0,n)B^{(1)}(0,n) super Toda, and involves in addition a single Majorana fermion. The most interesting is regime III, where {\sl non-compact} degrees of freedom appear, generalising the emergence of the Euclidean black hole CFT in the a2(2)a_{2}^{(2)} case. For a2n(2)a_{2n}^{(2)} we find a continuum limit made of nn compact and nn non-compact bosons, while for a2n−1(2)a_{2n-1}^{(2)} we find nn compact and n−1n-1 non-compact bosons. We also find deep relations between aN−1(2)a_{N-1}^{(2)} in regime III and the gauged WZW models SO(N)/SO(N−1)SO(N)/SO(N-1).Comment: 43 pages, 4 figure

    A new look at the collapse of two-dimensional polymers

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    We study the collapse of two-dimensional polymers, via an O(nn) model on the square lattice that allows for dilution, bending rigidity and short-range monomer attractions. This model contains two candidates for the theta point, ΘBN\Theta_{\rm BN} and ΘDS\Theta_{\rm DS}, both exactly solvable. The relative stability of these points, and the question of which one describes the `generic' theta point, have been the source of a long-standing debate. Moreover, the analytically predicted exponents of ΘBN\Theta_{\rm BN} have never been convincingly observed in numerical simulations. In the present paper, we shed a new light on this confusing situation. We show in particular that the continuum limit of ΘBN\Theta_{\rm BN} is an unusual conformal field theory, made in fact of a simple dense polymer decorated with {\sl non-compact degrees of freedom}. This implies in particular that the critical exponents take continuous rather than discrete values, and that corrections to scaling lead to an unusual integral form. Furthermore, discrete states may emerge from the continuum, but the latter are only normalizable---and hence observable---for appropriate values of the model's parameters. We check these findings numerically. We also probe the non-compact degrees of freedom in various ways, and establish that they are related to fluctuations of the density of monomers. Finally, we construct a field theoretic model of the vicinity of ΘBN\Theta_{\rm BN} and examine the flow along the multicritical line between ΘBN\Theta_{\rm BN} and ΘDS\Theta_{\rm DS}.Comment: v2 : references adde

    Non compact continuum limit of two coupled Potts models

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    We study two QQ-state Potts models coupled by the product of their energy operators, in the regime 2<Q≤42 < Q \le 4 where the coupling is relevant. A particular choice of weights on the square lattice is shown to be equivalent to the integrable a3(2)a_3^{(2)} vertex model. It corresponds to a selfdual system of two antiferromagnetic Potts models, coupled ferromagnetically. We derive the Bethe Ansatz equations and study them numerically for two arbitrary twist angles. The continuum limit is shown to involve two compact bosons and one non compact boson, with discrete states emerging from the continuum at appropriate twists. The non compact boson entails strong logarithmic corrections to the finite-size behaviour of the scaling levels, the understanding of which allows us to correct an earlier proposal for some of the critical exponents. In particular, we infer the full set of magnetic scaling dimensions (watermelon operators) of the Potts model.Comment: 33 pages, 10 figures v2: reference added, minor typo corrected v3: revised version for publication in JSTAT: section 3.1 added, some technical content moved to appendi

    Non compact conformal field theory and the a_2^{(2)} (Izergin-Korepin) model in regime III

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    The so-called regime III of the a_2^{(2)} Izergin-Korepin 19-vertex model has defied understanding for many years. We show in this paper that its continuum limit involves in fact a non compact conformal field theory (the so-called Witten Euclidian black hole CFT), which leads to a continuous spectrum of critical exponents, as well as very strong corrections to scaling. Detailed numerical evidence based on the Bethe ansatz analysis is presented, involving in particular the observation of discrete states in the spectrum, in full agreement with the string theory prediction for the black hole CFT. Our results have important consequences for the physics of the O(n) model, which will be discussed elsewhere.Comment: 57 pages, 19 figures; v2: reference adde
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