Abstract
We consider the non-unitary Lee-Yang minimal model ${\cal M}(2,5)$ in three different finite geometries: (i) on the interval with integrable boundary conditions labelled by the Kac labels $(r,s)=(1,1),(1,2)$, (ii) on the circle with periodic boundary conditions and (iii) on the periodic circle including an integrable purely transmitting defect. We apply $\varphi_{1,3}$ integrable perturbations on the boundary and on the defect and describe the flow of the spectrum. Adding a $\Phi_{1,3}$ integrable perturbation to move off-criticality in the bulk, we determine the finite size spectrum of the massive scattering theory in the three geometries via Thermodynamic Bethe Ansatz (TBA) equations. We derive these integral equations for all excitations by solving, in the continuum scaling limit, the TBA functional equations satisfied by the transfer matrices of the associated $A_{4}$ RSOS lattice model of Forrester and Baxter in Regime III. The excitations are classified in terms of $(m,n)$ systems. The excited state TBA equations agree with the previously conjectured equations in the boundary and periodic cases. In the defect case, new TBA equations confirm previously conjectured transmission factors.
Highlights
The determination of the full spectrum of a 1+1 dimensional Quantum Field Theory (QFT) in finite volume is a highly non-trivial and usually intractable task
Adding a Φ1,3 integrable perturbation to move off-criticality in the bulk, we determine the finite size spectrum of the massive scattering theory in the three geometries via Thermodynamic Bethe Ansatz (TBA) equations. We derive these integral equations for all excitations by solving, in the continuum scaling limit, the TBA functional equations satisfied by the transfer matrices of the associated A4 Restricted Solid-On-Solid (RSOS) lattice model of Forrester and Baxter in Regime III
The TBA method exploits the fact that, for large Euclidean time, the partition function is dominated by the contribution of the ground state
Summary
The determination of the full spectrum of a 1+1 dimensional Quantum Field Theory (QFT) in finite volume is a highly non-trivial and usually intractable task. The key difference, compared to the ground-state equation, is in the appearance of so called source terms, or equivalently, in choosing a different contour for integrations Such a program using analytic continuation has not been successfully carried out to obtain TBA equations for the full excitation spectrum even for the simple non-unitary scaling Lee-Yang model [8, 9]. Of the Lee-Yang model has been recast [24] as an integral equation by assuming the analytic properties of the Y -function providing a conjectured exact finite volume spectrum for periodic boundary conditions. We investigate the analytic structure of the transfer matrix eigenvalues and classify all excited states We do this first for the trigonometric theory whose scaling limit corresponds to the conformal Lee-Yang model.
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