About the definition (say in the A-model) Fg=∫Mg⟨3g−3∏i=1|∫ΣgG−zz(μi)z ˉz|2⟩ I have two questions:
- how are the CFT correlators precisely defined?
- the 3g−3 comes from dimension counting: it is equivalent to study perturbations of complex structure J↦J+ϵ, to find the conditions on Beltrami differentials; why in doing that one has to impose vanishing of Nijenhuis tensor? (isn't this automatic in 2d?)
References:
Neitzke and Vafa lectures http://arxiv.org/abs/hep-th/0410178 (correlator definition)
Collinucci lectures http://www.ulb.ac.be/sciences/ptm/pmif/Rencontres/topstrings.pdf (dimension counting)