Physics:Gopakumar–Vafa invariant

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Short description: Topological invariants concerning BPS states

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:

g=0βH2(M,)GW(g,β)qβλ2g2=g=0k=1βH2(M,)BPS(g,β)1k(2sin(kλ2))2g2qkβ ,

where

  • β is the class of pseudoholomorphic curves with genus g,
  • λ is the topological string coupling,
  • qβ=exp(2πitβ) with tβ the Kähler parameter of the curve class β,
  • GW(g,β) are the Gromov–Witten invariants of curve class β at genus g,
  • BPS(g,β) are the number of BPS states (the Gopakumar–Vafa invariants) of curve class β at genus g.

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:

Ztop=exp[g=0k=1βH2(M,)BPS(g,β)1k(2sin(kλ2))2g2qkβ] .

Notes

References