English

Toda Darboux transformations and vacuum expectation values

Exactly Solvable and Integrable Systems 2024-08-20 v1 Mathematical Physics math.MP

Abstract

Determinant formulas for vacuum expectation values s+k+nm,seH(t)βmβ1βnβ1gk\langle s+k+n-m,-s|e^{H(\mathbf{t})}\beta_m^{*}\cdots\beta_1^{*}\beta_n\cdots\beta_1g|k\rangle are given by using Toda Darboux transformations. Firstly notice that 2--Toda hierarchy can be viewed as the 2--component bosonizations of fermionic KP hierarchy, then two elementary Toda Darboux transformation operators T+(q)=Λ(q)Δq1T_{+}(q)=\Lambda(q)\cdot\Delta\cdot q^{-1} and T(r)=Λ1(r)1Δ1rT_{-}(r)=\Lambda^{-1}(r)^{-1}\cdot\Delta^{-1}\cdot r are constructed from the changes of Toda (adjoint) wave functions by using 2--component boson--fermion correspondence. Based on this, the above vacuum expectation values now can be realized as the successive applications of Toda Darboux transformations. So the corresponding determinant formulas can be derived from the determinant representations of Toda Darboux transformations. Finally by similar methods, we also give the determinant formulas for nmeH(x)βmβ1βnβ1gk\langle n-m|e^{\mathcal{H}(\mathbf{x})}\beta_m^{*}\cdots\beta_1^{*}\beta_n\cdots\beta_1g|k\rangle related with KP tau functions.

Keywords

Cite

@article{arxiv.2408.09457,
  title  = {Toda Darboux transformations and vacuum expectation values},
  author = {Chengwei Wang and Mengyao Chen and Jipeng Cheng},
  journal= {arXiv preprint arXiv:2408.09457},
  year   = {2024}
}

Comments

18 pages

R2 v1 2026-06-28T18:15:54.868Z