Cuspidal uu-plane formula for generalized Donaldson invariants

From papers

Let c=Hc=\operatorname{H}, let Nf=0,2,3N_f=0,2,3, and let m,n,km,n,k satisfy

2m+2n+4=(4Nf)k.2m+2n+4=(4-N_f)k.

Write Dm,2nNf\pmb{\mathrm{D}}^{N_f}_{m,2n} for the Donaldson invariant and Φk,m,2n\pmb{\Phi}_{k,m,2n} and Φk,m,2nNf,c,1\pmb{\Phi}^{N_f,c,1}_{k,m,2n} for the corresponding uu-plane invariants. The Moore–Witten type conjecture. One has

Dm,2n0=Φk,m,2n,\pmb{\mathrm{D}}^{0}_{m,2n}=\pmb{\Phi}_{k,m,2n},

and

Dm,2nNf=2(Nf+2)k20˘00pmbΦk,m,2nNf,c,1.\pmb{\mathrm{D}}^{N_f}_{m,2n}=2^{\frac{(N_f+2)k}{2}}\u000pmb{\Phi}^{N_f,c,1}_{k,m,2n}.

This is the explicit coefficient-level relation expected from the physical low-energy effective theory; the source proves only a weak version for Nf=2,3N_f=2,3, leaving the full identities conjectural.

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Sources & referencesView supporting material

Primary source

Andreas Malmendier and Ken Ono, “SO(3)-Donaldson invariants of CP^2 and Mock Theta Functions”, arXiv:0808.1442 (2012).

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