ScalingStacks

Verified tagged author-source HTML · 2007.01384v1 · cited publication edition alignment unverified.

009E

Notation. Our convention is d=∂+∂¯d=\partial+\bar{\partial}, dc=−12​π(−∂+∂¯)d^{c}=\frac{\sqrt{-1}}{2\pi}(-\partial+\bar{\partial}), so d​dc=−1π​∂∂¯dd^{c}=\frac{\sqrt{-1}}{\pi}\partial\bar{\partial}. The relation between Kähler potentials and Kähler metrics is ωϕ=ω+d​dc​ϕ\omega_{\phi}=\omega+dd^{c}\phi. Alternatively, we think of a Kähler metric in terms of local absolute potentials, meaning ω=d​dc​φ\omega=dd^{c}\varphi for locally defined psh functions φ\varphi. Given a Hermitian metric hh on a line bundle LL, its curvature form is −d​dc​log⁡h1/2-dd^{c}\log h^{1/2} in the class c1​(L)c_{1}(L).

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