“…In Appendix B we explain how one can deduce from this expression the result obtained in [29] in the case of free fermions.…”
Section: Thermodynamic Limitmentioning
confidence: 99%
“…These lemmas are used in Sections 4 and 5. In Appendix B we compare the representation (6.16) for the dynamical σ z correlation function at ∆ = 0 with the one obtained in [29] in the case of free fermions.…”
Section: Introductionmentioning
confidence: 99%
“…[10,11,12,13,14,15,16,17,18,19,20,21]). As for the dynamical correlation functions, up to now, the only known exact results concern the case of free fermions ∆ = 0 [22,23,24,25,26,27,28,29].…”
We derive a master equation for the dynamical spin-spin correlation functions of the XXZ spin-1 2 Heisenberg finite chain in an external magnetic field. In the thermodynamic limit, we obtain their multiple integral representation.
“…In Appendix B we explain how one can deduce from this expression the result obtained in [29] in the case of free fermions.…”
Section: Thermodynamic Limitmentioning
confidence: 99%
“…These lemmas are used in Sections 4 and 5. In Appendix B we compare the representation (6.16) for the dynamical σ z correlation function at ∆ = 0 with the one obtained in [29] in the case of free fermions.…”
Section: Introductionmentioning
confidence: 99%
“…[10,11,12,13,14,15,16,17,18,19,20,21]). As for the dynamical correlation functions, up to now, the only known exact results concern the case of free fermions ∆ = 0 [22,23,24,25,26,27,28,29].…”
We derive a master equation for the dynamical spin-spin correlation functions of the XXZ spin-1 2 Heisenberg finite chain in an external magnetic field. In the thermodynamic limit, we obtain their multiple integral representation.
“…Finally, to evaluate the expectation value (3.1), it remains to compute scalar products of the type 10) where N j=1 B(λ j )|0 is an eigenstate of the transfer matrix, while the parameters {µ j } 1≤j≤N are arbitrary. The result for (3.10) is given by [19,22] (see [14] for another proof):…”
Section: From Theorem 31 and Remark 32 One Obtainsmentioning
confidence: 99%
“…Although the method to compute eigenstates and energy levels goes back to H. Bethe in 1931 [1,2,3,4], the knowledge of its spin correlation functions has been for a long time restricted to the free fermion point ∆ = 0, a case for which nevertheless tremendous works have been necessary to obtain full answers [5,6,7,8,9,10].…”
Using algebraic Bethe ansatz and the solution of the quantum inverse scattering problem, we compute compact representations of the spin-spin correlation functions of the XXZ-1 2 Heisenberg chain in a magnetic field. At lattice distance m, they are typically given as the sum of m terms. Each term n of this sum, n = 1, . . . m, is represented in the thermodynamic limit as a multiple integral of order 2n + 1; the integrand depends on the distance as the power m of some simple function. The root of these results is the derivation of a compact formula for the multiple action on a general quantum state of the chain of transfer matrix operators for arbitrary values of their spectral parameters.
Realizing bosonic field v(x) as current of massless (chiral) fermions we derive hierarchy of quantum polynomial interactions of the field v(x) that are completely integrable and lead to linear evolutions for the fermionic field. It is proved that in the classical limit this hierarchy reduces to the dispersionless KdV hierarchy. Application of our construction to quantization of generic completely integrable interaction is demonstrated by example of the mKdV equation.
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