ScalingStacks

Example 1.10 . [03Z5]

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Example 1.10.

(Negative vertex) By a similar argument, in the negative vertex setting (cf. Section 1.1.5) the curvature 2-form FF satisfies

(1.18) −12​π​d​F=−−14​π​(∂2Wp​q¯∂μ​∂μ+4​∂2V∂ηp​∂η¯q)​d​μ∧d​ηp∧d​η¯q=S,-\frac{1}{2\pi}dF=-\frac{\sqrt{-1}}{4\pi}\left(\frac{\partial^{2}W^{p\bar{q}}}{\partial\mu\partial\mu}+4\frac{\partial^{2}V}{\partial\eta_{p}\partial\bar{\eta}_{q}}\right)d\mu\wedge d\eta_{p}\wedge d\bar{\eta}_{q}=S,

where S={z1+z2=1}={e2​π​i​η1+e2​π​i​η2=1}⊂ℂz1∗×ℂz2∗×{0}⊂ℂz1∗×ℂz2∗×ℝμS=\{z_{1}+z_{2}=1\}=\{e^{2\pi i\eta_{1}}+e^{2\pi i\eta_{2}}=1\}\subset\mathbb{C}^{*}_{z_{1}}\times\mathbb{C}^{*}_{z_{2}}\times\{0\}\subset\mathbb{C}^{*}_{z_{1}}\times\mathbb{C}^{*}_{z_{2}}\times\mathbb{R}_{\mu} defines a codimension 3 cycle. Here SS is endowed with the complex orientation, and the orientation on ℂz2∗×ℝμ\mathbb{C}^{*}_{z_{2}}\times\mathbb{R}_{\mu} is defined by the form d​μ∧d​Re​η1∧d​Im​η1∧d​Re​η2∧d​Im​η2d\mu\wedge d\text{Re}\eta_{1}\wedge d\text{Im}\eta_{1}\wedge d\text{Re}\eta_{2}\wedge d\text{Im}\eta_{2}.

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