We describe a method to derive, from first principles, the long-distance asymptotic behavior of
correlation functions of integrable models in the framework of the algebraic Bethe ansatz. We
apply this approach to the longitudinal spin–spin correlation function of the XXZ Heisenberg spin-
1/2
chain (with magnetic field) in the disordered regime as well as to the density–density
correlation function of the interacting one-dimensional Bose gas. At leading order, the
results confirm the Luttinger liquid and conformal field theory predictions.
The momentum-and frequency-dependent one-body correlation function of the one-dimensional interacting Bose gas (Lieb-Liniger model) in the repulsive regime is studied using the Algebraic Bethe Ansatz and numerics. We first provide a determinant representation for the field form factor which is welladapted to numerical evaluation. The correlation function is then reconstructed to high accuracy for systems with finite but large numbers of particles, for a wide range of values of the interaction parameter. Our results are extensively discussed, in particular their specialization to the static case.
We consider the XXZ spin chain with diagonal boundary conditions in the framework of algebraic Bethe Ansatz. Using the explicit computation of the scalar products of Bethe states and a revisited version of the bulk inverse problem, we calculate the elementary building blocks for the correlation functions. In the limit of half-infinite chain, they are obtained as multiple integrals of usual functions, similar to the case of periodic boundary conditions.
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