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Futaki Invariant and CM Polarization

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Book cover Geometry and Topology of Manifolds

Part of the book series: Springer Proceedings in Mathematics & Statistics ((PROMS,volume 154))

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Abstract

This is an expository paper. We will discuss various formulations of Futaki invariant and its relation to the CM line bundle. We will discuss their connections to the K-energy. We will also include proof for certain known results which may not have been well presented or less accessible in the literature. We always assume that M is a compact Kähler manifold. By a polarization, we mean a positive line bundle L over M, then we call (ML) a polarized manifold.

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Notes

  1. 1.

    In [21], the integrand is given in a different but equivalent form.

  2. 2.

    In [6], we assume that \(M_0\) is a \({\mathbb Q}\)-Fano variety with \(L_0\) being the anti-canonical bundle \(K_{M_0}^{-1}\). However, as one can see in the subsequent discussion, the general cases can be done by following similar arguments.

  3. 3.

    We refer the readers to [12] for definition of the twisted K-energy which extends the usual K-energy to conic cases.

  4. 4.

    Our presentation here differs slightly from that in [7], but they are equivalent.

  5. 5.

    One can even have an \({\mathbf G}_0\)-equivaraint resolution, but it is not needed here.

  6. 6.

    This is a pointwise version of the adjunction formula.

  7. 7.

    Here the \({\mathbf G}_0\)-action on \(M_0'\) is given by \(v'\) which covers the m-multiple of the action generated by v on \(M_0\), so we need to add m when using \(\hat{\theta }\) et al. in the subsequent computations.

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Correspondence to Gang Tian .

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Tian, G. (2016). Futaki Invariant and CM Polarization. In: Futaki, A., Miyaoka, R., Tang, Z., Zhang, W. (eds) Geometry and Topology of Manifolds. Springer Proceedings in Mathematics & Statistics, vol 154. Springer, Tokyo. https://doi.org/10.1007/978-4-431-56021-0_18

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