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1d Ising model with $1/r^{1.99}$ interaction

Dario Benedetti, Edoardo Lauria, Dalimil Mazáč, Philine van Vliet

TL;DR

This work identifies a dual impurity-type description for the critical one-dimensional long-range Ising model with 1/r^{1+s} interactions, yielding a weakly coupled fixed point near the crossover s→1. The authors formulate a defect CFT Zs that couples a negative-dimension Gaussian free field to a qubit, reproduce the AYK Coulomb-gas physics, and obtain a controlled IR fixed point with g⋆ ∼ √δ and b⋆^2 ∼ 1−δ/4. They show that at s=1 the theory reduces to a conformal boundary condition for a 2d free scalar, enabling an exact spectrum and OPE data; perturbative CFT data around s=1 are then derived via both RG and analytic conformal bootstrap and shown to be in perfect agreement. The results provide a concrete, solvable framework for the 1d LRI crossover, deliver precise predictions for operator dimensions and OPE coefficients, and offer a pathway to extend these methods to related long-range and defect CFT problems.

Abstract

We study the 1d Ising model with long-range interactions decaying as $1/r^{1+s}$. The critical model corresponds to a family of 1d conformal field theories (CFTs) whose data depends nontrivially on $s$ in the range $1/2\leq s\leq 1$. The model is known to be described by a generalized free field with quartic interaction, which is weakly coupled near $s=1/2$ but strongly coupled near the short-range crossover at $s=1$. We propose a dual description which becomes weakly coupled at $s=1$. At $s=1$, our model becomes an exactly solvable conformal boundary condition for the 2d free scalar. We perform a number of consistency checks of our proposal and calculate the perturbative CFT data around $s=1$ analytically using both 1) our proposed field theory and 2) the analytic conformal bootstrap. Our results show complete agreement between the two methods.

1d Ising model with $1/r^{1.99}$ interaction

TL;DR

This work identifies a dual impurity-type description for the critical one-dimensional long-range Ising model with 1/r^{1+s} interactions, yielding a weakly coupled fixed point near the crossover s→1. The authors formulate a defect CFT Zs that couples a negative-dimension Gaussian free field to a qubit, reproduce the AYK Coulomb-gas physics, and obtain a controlled IR fixed point with g⋆ ∼ √δ and b⋆^2 ∼ 1−δ/4. They show that at s=1 the theory reduces to a conformal boundary condition for a 2d free scalar, enabling an exact spectrum and OPE data; perturbative CFT data around s=1 are then derived via both RG and analytic conformal bootstrap and shown to be in perfect agreement. The results provide a concrete, solvable framework for the 1d LRI crossover, deliver precise predictions for operator dimensions and OPE coefficients, and offer a pathway to extend these methods to related long-range and defect CFT problems.

Abstract

We study the 1d Ising model with long-range interactions decaying as . The critical model corresponds to a family of 1d conformal field theories (CFTs) whose data depends nontrivially on in the range . The model is known to be described by a generalized free field with quartic interaction, which is weakly coupled near but strongly coupled near the short-range crossover at . We propose a dual description which becomes weakly coupled at . At , our model becomes an exactly solvable conformal boundary condition for the 2d free scalar. We perform a number of consistency checks of our proposal and calculate the perturbative CFT data around analytically using both 1) our proposed field theory and 2) the analytic conformal bootstrap. Our results show complete agreement between the two methods.

Paper Structure

This paper contains 11 sections, 21 equations, 2 tables.