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Correlation functions of charged free boson and fermion systems

Published 9 Dec 2019 in math.QA, hep-th, math-ph, math.MP, and quant-ph | (1912.03870v2)

Abstract: Using the idea of the quantum inverse scattering method, we introduce the operators B(x),C(x)\mathbf{B}(x), \mathbf{C}(x) and B~(x),C~(x)\mathbf{\tilde{B}}(x), \mathbf{\tilde{C}}(x) corresponding to the off-diagonal entries of the monodromy matrix TT for the phase model and ii-boson model in terms of bc fermions and neutral fermions respectively, thus giving alternative treatment of the KP and BKP hierarchies. We also introduce analogous operators B<sup>∗(x)\mathbf{B}<sup>{*}(x) and C<sup>∗(x)\mathbf{C}<sup>{*}(x) for the charged free boson system and show that they are in complete analogy to those of bcbc fermionic fields. It is proved that the correlation function ⟨0∣C(xN)⋯C(x1)B(y1)⋯\langle 0|\mathbf{C}(x_N)\cdots\mathbf{C}(x_1)\mathbf{B}(y_1)\cdots B(yN)∣0⟩\mathbf{B}(y_N)|0\rangle in the bcbc fermionic fields is the inverse of the correlation function ⟨0∣C<sup><em>(xN)⋯C<sup></sup></em>(x1)B<sup>∗(y1)⋯</sup></sup>B<sup>∗(yN)∣0⟩\langle 0|\mathbf{C}<sup>{<em>}(x_N)\cdots\mathbf{C}<sup>{</sup></em>}(x_1)\mathbf{B}<sup>{*}(y_1)\cdots</sup></sup> \mathbf{B}<sup>{*}(y_N)|0\rangle in the charged free bosons.

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