Abstract

For general Temperley–Lieb loop models, including the logarithmic minimal models LM(p,p′) with p,p′ coprime integers, we construct an infinite family of Robin boundary conditions on the strip as linear combinations of Neumann and Dirichlet boundary conditions. These boundary conditions are Yang–Baxter integrable and allow loop segments to terminate on the boundary. Algebraically, the Robin boundary conditions are described by the one-boundary Temperley–Lieb algebra. Solvable critical dense polymers is the first member LM(1,2) of the family of logarithmic minimal models and has loop fugacity β=0 and central charge c=−2. Specialising to LM(1,2) with our Robin boundary conditions, we solve the model exactly on strips of arbitrary finite size N and extract the finite-size conformal corrections using an Euler–Maclaurin formula. The key to the solution is an inversion identity satisfied by the commuting double row transfer matrices. This inversion identity is established directly in the Temperley–Lieb algebra. We classify the eigenvalues of the double row transfer matrices using the physical combinatorics of the patterns of zeros in the complex spectral parameter plane and obtain finitised characters related to spaces of coinvariants of Z4 fermions. In the continuum scaling limit, the Robin boundary conditions are associated with irreducible Virasoro Verma modules with conformal weights Δr,s−12=132(L2−4) where L=2s−1−4r, r∈Z, s∈N. These conformal weights populate a Kac table with half-integer Kac labels. Fusion of the corresponding modules with the generators of the Kac fusion algebra is examined and general fusion rules are proposed.

Highlights

  • The exactly solvable model LM(1, 2) [1, 2] of critical dense polymers [3,4,5,6,7,8,9] is the first member of the family of logarithmic minimal models LM(p, p′) [10] where 1 ≤ p < p′ and p, p′ are coprime integers

  • We introduce a family of Yang-Baxter integrable Robin boundary conditions [45] for general TL loop models, including the logarithmic minimal models LM(p, p′)

  • Similar to the construction of the bulk face operator (2.8), a boundary triangle is defined as a linear combination of the Neumann and Dirichlet boundary configurations (2.2) where the coefficients are chosen such that the triangles satisfy the boundary Yang-Baxter equation (BYBE)

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Summary

Introduction

The exactly solvable model LM(1, 2) [1, 2] of critical dense polymers [3,4,5,6,7,8,9] is the first member of the family of logarithmic minimal models LM(p, p′) [10] where 1 ≤ p < p′ and p, p′ are coprime integers. We introduce a family of Yang-Baxter integrable Robin boundary conditions [45] for general TL loop models, including the logarithmic minimal models LM(p, p′). To study in detail the properties of the Robin boundary conditions, we specialize to the case of critical dense polymers LM(1, 2) In this case, the model can be solved exactly on an arbitrary finite lattice allowing the conformal spectra to be extracted analytically using an Euler-Maclaurin formula. Jacobsen and Saleur study their model at the isotropic point allowing them to consider the situation with all boundary loops blobbed along the outer rim of the annulus By contrast, this is not possible in our scenario as the Dirichlet boundary condition alone does not provide a solution to the spectral parameter dependent boundary Yang-Baxter equations.

Statistical lattice model on a strip
Face operators and local relations
Twist boundary condition
One-boundary Temperley-Lieb algebra
General Robin boundary conditions
Link states and standard modules
Robin link states
Double row transfer tangles
Robin representations
Critical dense polymers
Hamiltonian limit
Special parameter values
Inversion identity
Exact solution for eigenvalues
Finite-size corrections
Physical combinatorics and finitized characters
Conformal data
Z4 fermions and Virasoro modules
Characters and coinvariants
Interpretation of lattice observations
Fusion rules
Discussion
A Blob algebra
B General inversion identity
C Fusion and the NGK algorithm
Full Text
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