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$q$-Difference Kac-Schwarz Operators in Topological String Theory

Mathematical Physics 2017-02-22 v2 High Energy Physics - Theory math.MP Quantum Algebra Exactly Solvable and Integrable Systems

Abstract

The perspective of Kac-Schwarz operators is introduced to the authors' previous work on the quantum mirror curves of topological string theory in strip geometry and closed topological vertex. Open string amplitudes on each leg of the web diagram of such geometry can be packed into a multi-variate generating function. This generating function turns out to be a tau function of the KP hierarchy. The tau function has a fermionic expression, from which one finds a vector W|W\rangle in the fermionic Fock space that represents a point WW of the Sato Grassmannian. W|W\rangle is generated from the vacuum vector 0|0\rangle by an operator gg on the Fock space. gg determines an operator GG on the space V=C((x))V = \mathbb{C}((x)) of Laurent series in which WW is realized as a linear subspace. GG generates an admissible basis {Φj(x)}j=0\{\Phi_j(x)\}_{j=0}^\infty of WW. qq-difference analogues AA, BB of Kac-Schwarz operators are defined with the aid of GG. Φj(x)\Phi_j(x)'s satisfy the linear equations AΦj(x)=qjΦj(x)A\Phi_j(x) = q^j\Phi_j(x), BΦj(x)=Φj+1(x)B\Phi_j(x) = \Phi_{j+1}(x). The lowest equation AΦ0(x)=Φ0(x)A\Phi_0(x) = \Phi_0(x) reproduces the quantum mirror curve in the authors' previous work.

Keywords

Cite

@article{arxiv.1609.00882,
  title  = {$q$-Difference Kac-Schwarz Operators in Topological String Theory},
  author = {Kanehisa Takasaki and Toshio Nakatsu},
  journal= {arXiv preprint arXiv:1609.00882},
  year   = {2017}
}
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