词条 | Gopakumar–Vafa invariant |
释义 |
In theoretical physics, Rajesh Gopakumar and Cumrun Vafa introduced in a series of papers[1][2][3][4] new topological invariants, called Gopakumar–Vafa invariants, that represent the number of BPS states on a Calabi–Yau 3-fold. They lead to the following generating function for the Gromov–Witten invariants on a Calabi–Yau 3-fold M: , where
As a partition function in topological quantum field theoryGopakumar–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: Notes1. ^{{harvnb|Gopakumar|Vafa|1998a}} 2. ^{{harvnb|Gopakumar|Vafa|1998b}} 3. ^{{harvnb|Gopakumar|Vafa|1998c}} 4. ^{{harvnb|Gopakumar|Vafa|1998d}} References
| last1 = Ionel | first1 = Eleny-Nicoleta | author1-link = Eleny Ionel | last2 = Parker | first2 = Thomas H. | doi = 10.4007/annals.2018.187.1.1 | issue = 1 | journal = Annals of Mathematics | mr = 3739228 | pages = 1–64 | series = Second Series | title = The Gopakumar–Vafa formula for symplectic manifolds | volume = 187 | year = 2018}}{{DEFAULTSORT:Gopakumar-Vafa invariant}}{{quantum-stub}} 3 : Quantum field theory|Algebraic geometry|String theory |
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