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Directed harmonic currents near non-hyperbolic linearizable singularities
Published online by Cambridge University Press: 07 July 2022
Abstract
Let
$(\mathbb {D}^2,\mathscr {F},\{0\})$
be a singular holomorphic foliation on the unit bidisc
$\mathbb {D}^2$
defined by the linear vector field
$$ \begin{align*} z \frac{\partial}{\partial z}+ \unicode{x3bb} w \frac{\partial}{\partial w}, \end{align*} $$
where
$\unicode{x3bb} \in \mathbb {C}^*$
. Such a foliation has a non-degenerate singularity at the origin
${0:=(0,0) \in \mathbb {C}^2}$
. Let T be a harmonic current directed by
$\mathscr {F}$
which does not give mass to any of the two separatrices
$(z=0)$
and
$(w=0)$
. Assume
$T\neq 0$
. The Lelong number of T at
$0$
describes the mass distribution on the foliated space. In 2014 Nguyên (see [16]) proved that when
$\unicode{x3bb} \notin \mathbb {R}$
, that is, when
$0$
is a hyperbolic singularity, the Lelong number at
$0$
vanishes. Suppose the trivial extension
$\tilde {T}$
across
$0$
is
$dd^c$
-closed. For the non-hyperbolic case
$\unicode{x3bb} \in \mathbb {R}^*$
, we prove that the Lelong number at
$0$
:
-
(1) is strictly positive if
$\unicode{x3bb}>0$ ;
-
(2) vanishes if
$\unicode{x3bb} \in \mathbb {Q}_{<0}$ ;
-
(3) vanishes if
$\unicode{x3bb} <0$ and T is invariant under the action of some cofinite subgroup of the monodromy group.
- Type
- Original Article
- Information
- Copyright
- © The Author(s), 2022. Published by Cambridge University Press
References
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