English

Coset conformal field theory and instanton counting on C^2/Z_p

High Energy Physics - Theory 2013-09-16 v3

Abstract

We study conformal field theory with the symmetry algebra A(2,p)=gl^(n)2/gl^(np)2\mathcal{A}(2,p)=\hat{\mathfrak{gl}}(n)_{2}/\hat{\mathfrak{gl}}(n-p)_2. In order to support the conjecture that this algebra acts on the moduli space of instantons on C2/Zp\mathbb{C}^{2}/\mathbb{Z}_{p}, we calculate the characters of its representations and check their coincidence with the generating functions of the fixed points of the moduli space of instantons. We show that the algebra A(2,p)\mathcal{A}(2,p) can be realized in two ways. The first realization is connected with the cross-product of pp Virasoro and pp Heisenberg algebras: Hp×Virp\mathcal{H}^{p}\times \textrm{Vir}^{p}. The second realization is connected with: Hp×sl^(p)2×(sl^(2)p×sl^(2)np/sl^(2)n)\mathcal{H}^{p}\times \hat{\mathfrak{sl}}(p)_2\times (\hat{\mathfrak{sl}}(2)_p \times \hat{\mathfrak{sl}}(2)_{n-p}/\hat{\mathfrak{sl}}(2)_n). The equivalence of these two realizations provides the non-trivial identity for the characters of A(2,p)\mathcal{A}(2,p). The moduli space of instantons on C2/Zp\mathbb{C}^{2}/\mathbb{Z}_{p} admits two different compactifications. This leads to two different bases for the representations of A(2,p)\mathcal{A}(2,p). We use this fact to explain the existence of two forms of the instanton pure partition functions.

Keywords

Cite

@article{arxiv.1306.3938,
  title  = {Coset conformal field theory and instanton counting on C^2/Z_p},
  author = {M. N. Alfimov and A. A. Belavin and G. M. Tarnopolsky},
  journal= {arXiv preprint arXiv:1306.3938},
  year   = {2013}
}

Comments

23 pages, 1 figure