Abstract:We introduce and study an integrable boundary flow possessing an infinite number of conserving charges which can be thought of as quantum counterparts of the Ablowitz, Kaup, Newell and Segur Hamiltonians. We propose an exact expression for overlap amplitudes of the boundary state with all primary states in terms of solutions of certain ordinary linear differential equation. The boundary flow is terminated at a nontrivial infrared fixed point. We identify a form of whole boundary state corresponding to this fix… Show more
“…To simplify calculations, it is convenient to trade the variable z to 45) and similarly forw. As is well known, this transformation brings MShG equation (1.5) to the conventional Sinh-Gordon (ShG) equation…”
Section: Large-θ Asymptotic Expansion and Local Immentioning
We study a family of classical solutions of modified sinh-Gordon equation, ∂ z ∂zη − e 2η + p(z) p(z) e −2η = 0 with p(z) = z 2α − s 2α . We show that certain connection coefficients for solutions of the associated linear problem coincide with the Q-function of the quantum sine-Gordon (α > 0) or sinh-Gordon (α < −1) models.
“…To simplify calculations, it is convenient to trade the variable z to 45) and similarly forw. As is well known, this transformation brings MShG equation (1.5) to the conventional Sinh-Gordon (ShG) equation…”
Section: Large-θ Asymptotic Expansion and Local Immentioning
We study a family of classical solutions of modified sinh-Gordon equation, ∂ z ∂zη − e 2η + p(z) p(z) e −2η = 0 with p(z) = z 2α − s 2α . We show that certain connection coefficients for solutions of the associated linear problem coincide with the Q-function of the quantum sine-Gordon (α > 0) or sinh-Gordon (α < −1) models.
“…The first non-trivial densities read [58], 27) where √ n = i √ 2/β is a parameter used in [58] instead of our β in (4.10). Note also that their chiral Bose fields X(u) and Y (u) are related to (4.1) as…”
Section: T-and Q-operators In Conformal Field Theorymentioning
confidence: 99%
“…(4.37) with l = 0 appeared in [74]. The full equation with arbitrary values of ℓ and r, in the regime α < −1, was recently considered in [58] in connection with the quantization of the integrable AKNS soliton hierarchy.…”
Section: Connections With the Spectral Theory Of Differential Equationsmentioning
We develop Yang-Baxter integrability structures connected with the quantum affine superalgebra U q ( sl(2|1)). Baxter's Q-operators are explicitly constructed as supertraces of certain monodromy matrices associated with (q-deformed) bosonic and fermionic oscillator algebras. There are six different Q-operators in this case, obeying a few fundamental fusion relations, which imply all functional relations between various commuting transfer matrices. The results are universal in the sense that they do not depend on the quantum space of states and apply both to lattice models and to continuous quantum field theory models as well.
“…The key observation underlying this calculation is equation (7.6) which relates the reflection amplitude to the asymptotics of the functions q p of KdV theory. These asymptotics were found in [41] based on [23]. To round off the picture, we will now briefly recall how this works.…”
Section: Explicit Calculation Of the Reflection Amplitudementioning
confidence: 92%
“…These q-functions q p (u) can be characterized as the unique solutions of the functional equations (8.7), (8.8) which have the analytic properties (8.9), the asymptotic behavior (8.11), and the additional property to be non-vanishing within the strip S u . It was shown in [23] that a solution to this set of conditions is given by the Wronskian of certain solutions to the theory -is compared to the one in [49,39], which was based on the conformal symmetry. It would be very interesting further elucidate the interplay between the integrable and the conformal structure of Liouville theory.…”
Section: Explicit Calculation Of the Reflection Amplitudementioning
Using the example of Liouville theory, we show how the separation into left-and right-moving degrees of freedom in a nonrational conformal field theory can be made explicit in terms of its integrable structure. The key observation is that there exist separate Baxter Q-operators for leftand right-moving degrees of freedom. Combining a study of the analytic properties of the Q-operators with Sklyanin's Separation of Variables Method leads to a complete characterization of the spectrum. Taking the continuum limit allows us in particular to rederive the Liouville reflection amplitude using only the integrable structure.
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