3.4. Formal reduction of the general case to the second case using smooth orbifolds [02E7]
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3.4. Formal reduction of the general case to the second case using smooth orbifolds
In order to carry out the present argument, which in essence is just a change of variables , we need to use analysis on certain smooth orbifolds. We will not give complete definitions since they are in the recent reference [BGK], section 2 pp. 560-564, see also [MO] and the references therein.
Let be a smooth orbifold pair. By this we mean that we have the prime decomposition where is an integer. We assume that is a simple normal crossing divisor. Then, a classical construction surveyed in [BGK] enables to construct an orbifold with a -morphism of orbifolds with the following properties:
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is the reduction to the coarse moduli space of .
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is an isomorphism. Hence is an open suborbifold of which is an old-fashioned manifold).
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For every open polydisk with local coordinates such that .
In this formula, the local isotropy group is , is the integer multiplicity of the divisor such that , acts on the polydisk by 99 9 The usual isomorphism of with the group of -th root of unity is used..
The orbifold -morphism is induced by .
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For sufficiently divisible , .
It is possible to define all the basic concepts of Kähler geometry on orbifolds such as smooth functions, Kähler metrics, etc… The principle is to think of as a (multivalued) smooth coordinate chart.
A continuous function on is a continuous function on . A Radon measure on is a Radon measure on .
A smooth function on is a continuous function on such that for every local chart is smooth. In particular is Hölder continuous.
A Kähler metric on is a Kähler metric on with the property that extends to a smooth Kähler metric on . In particular, it also extends as a closed Kähler current on with Hölder potentials.
The pull back of a Kähler form on to is a semi-Kähler form that is actually cohomologous to a Kähler class1010 10 Here no reference can be given. But it is easy to extend the gluing methods for Kähler forms developed in [Dem 3] and [Pa] to orbifolds. Hence [DP] extends to Kähler orbifolds. .
Observe that , hence a smooth volume form on can be interpreted as a volume form on such that
In case the pair is an orbifold pair, the equation
| (5) |
can be interpreted on as an equation of the form
The method used to analyze the case where extends with almost no changes to the orbifold case. Hence the unique continuous solution of equation (5) is smooth outside its singular locus if is an orbifold pair.
Under the more general hypothesis that and is a divisor with simple normal crossings, then we can construct an orbifold pair with and we are back to the previous case.
For the most general case, consider the ideal generated by the and fix a log resolution of . Then we are back to the previous case, with an equation on . This ends the proof of Theorem 3.6.
In certain rare circumstances, there is a finite smooth covering such that and and the argument we use here reduces to a -equivariant argument on .
Remarks 3.8.
If we start with Kähler, and the log-resolution is non trivial, is not Kähler anymore.
This method that dates back to [Ko] can be used to prove a variant of [Y], Theorem 7 p. 399 where the divisor of is a simple normal crossing divisor, under the sole assumption that .
Now, it could not have been used to prove Theorem 8 p. 403 in 1978 since log-resolutions force the use of Monge-Ampère equations with degenerate L.H.S, for which the -estimate proved here was not available then.