207 research outputs found

    Bailey flows and Bose-Fermi identities for the conformal coset models (A1(1))N×(A1(1))N′/(A1(1))N+N′(A^{(1)}_1)_N\times (A^{(1)}_1)_{N'}/(A^{(1)}_1)_{N+N'}

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    We use the recently established higher-level Bailey lemma and Bose-Fermi polynomial identities for the minimal models M(p,p′)M(p,p') to demonstrate the existence of a Bailey flow from M(p,p′)M(p,p') to the coset models (A1(1))N×(A1(1))N′/(A1(1))N+N′(A^{(1)}_1)_N\times (A^{(1)}_1)_{N'}/(A^{(1)}_1)_{N+N'} where NN is a positive integer and N′N' is fractional, and to obtain Bose-Fermi identities for these models. The fermionic side of these identities is expressed in terms of the fractional-level Cartan matrix introduced in the study of M(p,p′)M(p,p'). Relations between Bailey and renormalization group flow are discussed.Comment: 28 pages, AMS-Latex, two references adde

    Supersymmetric pairing of kinks for polynomial nonlinearities

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    We show how one can obtain kink solutions of ordinary differential equations with polynomial nonlinearities by an efficient factorization procedure directly related to the factorization of their nonlinear polynomial part. We focus on reaction-diffusion equations in the travelling frame and damped-anharmonic-oscillator equations. We also report an interesting pairing of the kink solutions, a result obtained by reversing the factorization brackets in the supersymmetric quantum mechanical style. In this way, one gets ordinary differential equations with a different polynomial nonlinearity possessing kink solutions of different width but propagating at the same velocity as the kinks of the original equation. This pairing of kinks could have many applications. We illustrate the mathematical procedure with several important cases, among which the generalized Fisher equation, the FitzHugh-Nagumo equation, and the polymerization fronts of microtubulesComment: 13 pages, 2 figures, revised during the 2nd week of Dec. 200

    Riccati-parameter solutions of nonlinear second-order ODEs

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    It has been proven by Rosu and Cornejo-Perez in 2005 that for some nonlinear second-order ODEs it is a very simple task to find one particular solution once the nonlinear equation is factorized with the use of two first-order differential operators. Here, it is shown that an interesting class of parametric solutions is easy to obtain if the proposed factorization has a particular form, which happily turns out to be the case in many problems of physical interest. The method that we exemplify with a few explicitly solved cases consists in using the general solution of the Riccati equation, which contributes with one parameter to this class of parametric solutions. For these nonlinear cases, the Riccati parameter serves as a `growth' parameter from the trivial null solution up to the particular solution found through the factorization procedureComment: 5 pages, 3 figures, change of title and more tex

    Non-conformal asymptotic behavior of the time-dependent field-field correlators of 1D anyons

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    The exact large time and distance behavior of the field-field correlators has been computed for one-dimensional impenetrable anyons at finite temperatures. The result reproduces known asymptotics for impenetrable bosons and free fermions in the appropriate limits of the statistics parameter. The obtained asymptotic behavior of the correlators is dominated by the singularity in the spectral density of the quasiparticle states at the bottom of the band, and differs from the predictions of the conformal field theory. One can argue, however, that the anyonic response to the low-energy probes is still determined by the conformal terms in the asymptotic expansion.Comment: 5 pages, RevTeX

    Singular responses of spin-incoherent Luttinger liquids

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    When a local potential changes abruptly in time, an electron gas shifts to a new state which at long times is orthogonal to the one in the absence of the local potential. This is known as Anderson's orthogonality catastrophe and it is relevant for the so-called X-ray edge or Fermi edge singularity, and for tunneling into an interacting one dimensional system of fermions. It often happens that the finite frequency response of the photon absorption or the tunneling density of states exhibits a singular behavior as a function of frequency: (ωthω−ωth)αΘ(ω−ωth)(\frac{\omega_{\rm th}}{\omega-\omega_{\rm th}})^\alpha\Theta(\omega-\omega_{\rm th}) where ωth\omega_{\rm th} is a threshold frequency and α\alpha is an exponent characterizing the singular response. In this paper singular responses of spin-incoherent Luttinger liquids are reviewed. Such responses most often do not fall into the familiar form above, but instead typically exhibit logarithmic corrections and display a much higher universality in terms of the microscopic interactions in the theory. Specific predictions are made, the current experimental situation is summarized, and key outstanding theoretical issues related to spin-incoherent Luttinger liquids are highlighted.Comment: 21 pages, 3 figures. Invited Topical Review Articl

    Exact solutions of a Flat Full Causal Bulk viscous FRW cosmological model through factorization

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    We study the classical flat full causal bulk viscous FRW cosmological model through the factorization method. The method shows that there exists a relationship between the viscosity parameter ss and the parameter γ\gamma entering the equations of state of the model. Also, the factorization method allows to find some new exact parametric solutions for different values of the viscous parameter ss. Special attention is given to the well known case s=1/2s=1/2, for which the cosmological model admits scaling symmetries. Furthermore, some exact parametric solutions for s=1/2s=1/2 are obtained through the Lie group method.Comment: 18 pas. RevTeX4. New solutions. arXiv admin note: text overlap with arXiv:gr-qc/0107004 by other author

    Exceptional structure of the dilute A3_3 model: E8_8 and E7_7 Rogers--Ramanujan identities

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    The dilute A3_3 lattice model in regime 2 is in the universality class of the Ising model in a magnetic field. Here we establish directly the existence of an E8_8 structure in the dilute A3_3 model in this regime by expressing the 1-dimensional configuration sums in terms of fermionic sums which explicitly involve the E8_8 root system. In the thermodynamic limit, these polynomial identities yield a proof of the E8_8 Rogers--Ramanujan identity recently conjectured by Kedem {\em et al}. The polynomial identities also apply to regime 3, which is obtained by transforming the modular parameter by q→1/qq\to 1/q. In this case we find an A_1\times\mbox{E}_7 structure and prove a Rogers--Ramanujan identity of A_1\times\mbox{E}_7 type. Finally, in the critical q→1q\to 1 limit, we give some intriguing expressions for the number of LL-step paths on the A3_3 Dynkin diagram with tadpoles in terms of the E8_8 Cartan matrix. All our findings confirm the E8_8 and E7_7 structure of the dilute A3_3 model found recently by means of the thermodynamic Bethe Ansatz.Comment: 9 pages, 1 postscript figur

    The Yang-Baxter equation for PT invariant nineteen vertex models

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    We study the solutions of the Yang-Baxter equation associated to nineteen vertex models invariant by the parity-time symmetry from the perspective of algebraic geometry. We determine the form of the algebraic curves constraining the respective Boltzmann weights and found that they possess a universal structure. This allows us to classify the integrable manifolds in four different families reproducing three known models besides uncovering a novel nineteen vertex model in a unified way. The introduction of the spectral parameter on the weights is made via the parameterization of the fundamental algebraic curve which is a conic. The diagonalization of the transfer matrix of the new vertex model and its thermodynamic limit properties are discussed. We point out a connection between the form of the main curve and the nature of the excitations of the corresponding spin-1 chains.Comment: 43 pages, 6 figures and 5 table

    Fermionic solution of the Andrews-Baxter-Forrester model II: proof of Melzer's polynomial identities

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    We compute the one-dimensional configuration sums of the ABF model using the fermionic technique introduced in part I of this paper. Combined with the results of Andrews, Baxter and Forrester, we find proof of polynomial identities for finitizations of the Virasoro characters χb,a(r−1,r)(q)\chi_{b,a}^{(r-1,r)}(q) as conjectured by Melzer. In the thermodynamic limit these identities reproduce Rogers--Ramanujan type identities for the unitary minimal Virasoro characters, conjectured by the Stony Brook group. We also present a list of additional Virasoro character identities which follow from our proof of Melzer's identities and application of Bailey's lemma.Comment: 28 pages, Latex, 7 Postscript figure
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