1999
DOI: 10.1007/s002200050611
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Donaldson Invariants for Non-Simply Connected Manifolds

Abstract: We study Coulomb branch ("u-plane") integrals for N = 2 supersymmetric SU (2), SO (3) Yang-Mills theory on 4-manifolds X of b 1 (X) > 0, b + 2 (X) = 1. Using wall-crossing arguments we derive expressions for the Donaldson invariants for manifolds with b 1 (X) > 0, b + 2 (X) > 0. Explicit expressions for X = CP 1 × F g , where F g is a Riemann surface of genus g are obtained using Kronecker's double series identity. The result might be useful in future studies of quantum cohomology.

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Cited by 27 publications
(79 citation statements)
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“…The final answer for F g in these cases will be given by a sum over the different blocks. The presence of α, β leads however to nontrivial modifications of the result, as it has been already noticed in various papers [48,27,47,42,40]. We will consider these modifications when we analyze the FHSV model.…”
Section: The F G Couplings In Heterotic String Theorymentioning
confidence: 81%
See 1 more Smart Citation
“…The final answer for F g in these cases will be given by a sum over the different blocks. The presence of α, β leads however to nontrivial modifications of the result, as it has been already noticed in various papers [48,27,47,42,40]. We will consider these modifications when we analyze the FHSV model.…”
Section: The F G Couplings In Heterotic String Theorymentioning
confidence: 81%
“…More general cases can be also analyzed with the technique of lattice reduction, see [42,40] for examples.…”
Section: A Theta Functions and Modular Formsmentioning
confidence: 99%
“…Equation (4.1) generalizes Witten's expression [15] for pure Yang-Mills and was obtained in section 11 of [2]. The extension of the N f = 0 Donaldson-Witten function to non-simply connected four-manifolds was begun in [2] [16], and completed in [17].…”
Section: The Donaldson-witten Function With Massive Hypermultipletsmentioning
confidence: 99%
“…Notice that, as H 1 (Y, Z Z) ≃ Z Z, there are only two possible generators that differ in their sign. 5 To understand this dependence on the perturbation, it is useful to consider a four-dimensional version of this story, focusing again on the four manifold X = Y × S 1 , with b 1 (Y ) = 1. The structure of the cohomology ring of X is the following: We denote by S 2 a generator of H 2 (Y, Z Z) and by γ a generator…”
Section: 22b 1 (Y ) =mentioning
confidence: 99%