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Gopakumar–Vafa invariant
Topological invariants concerning BPS states From Wikipedia, the free encyclopedia
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In theoretical physics, Rajesh Gopakumar and Cumrun Vafa introduced in a series of papers[1][2][3][4] numerical invariants of Calabi-Yau threefolds, later referred to as the Gopakumar–Vafa invariants. These physically defined invariants represent the number of BPS states on a Calabi–Yau threefold. In the same papers, the authors also derived the following formula which relates the Gromov–Witten invariants and the Gopakumar-Vafa invariants.
- ,
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where
- is the class of holomorphic curves with genus g,
- is the topological string coupling, mathematically a formal variable,
- with the Kähler parameter of the curve class ,
- are the Gromov–Witten invariants of curve class at genus ,
- are the Gopakumar–Vafa invariants of curve class at genus .
Notably, Gromov-Witten invariants are generally rational numbers while Gopakumar-Vafa invariants are always integers.
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As a partition function in topological quantum field theory
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Perspective
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:
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Mathematical approaches
While Gromov-Witten invariants have rigorous mathematical definitions (both in symplectic and algebraic geometry), there is no mathematically rigorous definition of the Gopakumar-Vafa invariants, except for very special cases.
On the other hand, Gopakumar-Vafa's formula implies that Gromov-Witten invariants and Gopakumar-Vafa invariants determine each other. One can solve Gopakumar-Vafa invariants from Gromov-Witten invariants, while the solutions are a priori rational numbers. Ionel-Parker proved that these expressions are indeed integers.
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See also
Notes
References
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