<p>We propose explicit expressions for the boundary reflection matrices of the <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({\mathcal{A}}_{m}+(r, s)\)</EquationSource> </InlineEquation> series of massive scattering theories, obtained by perturbing the <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\({\mathcal{A}}_{m}\)</EquationSource> </InlineEquation> unitary minimal models with (<i>r, s</i>) boundary conditions with both bulk and boundary <i>ϕ</i><sub>1<i>,</i>3</sub> operators. We identify the vacua that live on the boundary with the allowed edges of the (<i>r, s</i>) conformal boundary conditions of the <i>A</i><sub><i>m</i></sub> Andrews-Baxter-Forrester model. The boundary reflection matrices are then “direct sums” of certain pairs of <i>A</i><sub><i>m−</i>1</sub> Behrend-Pearce solutions of the boundary Yang-Baxter equation and are consistent with the boundary bootstrap and the recently-introduced crossing, as well as the <i>Z</i><sub>2</sub> (height-reversal), Kac table and non-invertible symmetries.</p>

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Boundary reflection matrices of massive ϕ1,3-perturbed unitary minimal models

  • Zoltan Bajnok,
  • Rafael I. Nepomechie,
  • Paul A. Pearce

摘要

We propose explicit expressions for the boundary reflection matrices of the \({\mathcal{A}}_{m}+(r, s)\) series of massive scattering theories, obtained by perturbing the \({\mathcal{A}}_{m}\) unitary minimal models with (r, s) boundary conditions with both bulk and boundary ϕ1,3 operators. We identify the vacua that live on the boundary with the allowed edges of the (r, s) conformal boundary conditions of the Am Andrews-Baxter-Forrester model. The boundary reflection matrices are then “direct sums” of certain pairs of Am−1 Behrend-Pearce solutions of the boundary Yang-Baxter equation and are consistent with the boundary bootstrap and the recently-introduced crossing, as well as the Z2 (height-reversal), Kac table and non-invertible symmetries.