.
Gopakumar–Vafa invariant
In theoretical physics Rajesh Gopakumar and Cumrun Vafa introduced new topological invariants, which named Gopakumar–Vafa invariant, that represent the number of BPS states on Calabi–Yau 3-fold, in a series of papers. (see Gopakumar & Vafa (1998a),Gopakumar & Vafa (1998b) and also see Gopakumar & Vafa (1998c), Gopakumar & Vafa (1998d).) They lead the following formula generating function for the Gromov–Witten invariant on Calabi–Yau 3-fold M.
\( \sum_{g\ge0,n\ge1,\beta\in H^2(M,\mathbb{Z})} GW(g,\beta)q^{-\beta}\lambda^{2g-2}=\sum_{k>0,r\ge0,\beta\in H^2(M,\mathbb{Z})}BPS(r,\beta)\frac{1}{k}\left(2\sin\left(\frac{k\lambda}{2}\right)^{2r-2}q^{k\beta}\right) \)
where \( GW(g,\beta) \) is Gromov–Witten invariant, \( \beta \)the number of pseudoholomorphic curves with genus g and BPS(r,\beta) the number of the BPS states.
As a partition function in topological quantum field theory
Gopakumar–Vafa invariants can be viewed as a partition function in topological quantum field theory. They are proposed to be the partition function in Gopakumar–Vafa form:
\( Z_{top}=\exp\left[\sum_{\begin{smallmatrix} k>0,\ r\ge0,\\ \beta\in H^2(M,\mathbb{Z})\end{smallmatrix}}BPS(r,\beta)\frac{1}{k}\left(2\sin\left(\frac{k\lambda}{2}\right)^{2r-2}q^{k\beta\cdot t}\right)\right]\ . \)
References
Gopakumar, Rajesh; Vafa, Cumrun (1998a), M-Theory and Topological strings-I
Gopakumar, Rajesh; Vafa, Cumrun (1998b), M-Theory and Topological strings-II
Gopakumar, Rajesh; Vafa, Cumrun (1998c), On the Gauge Theory/Geometry Correspondence
Gopakumar, Rajesh; Vafa, Cumrun (1998d), Topological Gravity as Large N Topological Gauge Theory
Retrieved from "http://en.wikipedia.org/"
All text is available under the terms of the GNU Free Documentation License
