English

Complex Monge-Ampere operators via pseudo-isomorphisms: the well-defined cases

Complex Variables 2014-04-01 v2 Dynamical Systems

Abstract

Let XX and YY be compact K\"ahler manifolds of dimension 33. A bimeromorphic map f:XYf:X\rightarrow Y is pseudo-isomorphic if f:XI(f)YI(f1)f:X-I(f)\rightarrow Y-I(f^{-1}) is an isomorphism. Let T=T+TT=T^+-T^- be a current on YY, where T±T^{\pm} are positive closed (1,1)(1,1) currents which are smooth outside a finite number of points. We assume that the following condition is satisfied: {\bf Condition 1.} For every curve CC in I(f1)I(f^{-1}), then in cohomology {T}.{C}=0\{T\}.\{C\}=0. Then, we define a natural push-forward f(φddcuf(T))f_*(\varphi dd^cu\wedge f^*(T)) for a quasi-psh function uu and a smooth function φ\varphi on YY. We show that this pushforward satisfies a Bedford-Taylor's monotone convergence type. Assume moreover that the following two conditions are satisfied {\bf Condition 2.} The signed measure TTTT\wedge T\wedge T has no mass on I(f1)I(f^{-1}). {\bf Condition 3.} For every curve CC in I(f1)I(f^{-1}), the measure T[C]T\wedge [C] has no Dirac mass. Then, we define a Monge-Ampere operator MA(f(T))=f(T)f(T)f(T)MA(f^*(T))=f^*(T)\wedge f^*(T)\wedge f^*(T) for f(T)f^*(T). We show that this Monge-Ampere operator satisfies several continuous properties, including a Bedford-Taylor's monotone convergence type when TT is positive. The measures MA(f(T))MA(f^*(T)) are in general quite singular. Also, note that it may be not possible to define f(T±)f(T±)f(T±)f^*(T^{\pm})\wedge f^*(T^{\pm})\wedge f^*(T^{\pm}).

Keywords

Cite

@article{arxiv.1403.6425,
  title  = {Complex Monge-Ampere operators via pseudo-isomorphisms: the well-defined cases},
  author = {Tuyen Trung Truong},
  journal= {arXiv preprint arXiv:1403.6425},
  year   = {2014}
}

Comments

13 pages. Some materials added. Typos and minor inaccuracies are corrected. The introduction and references to relevant literature will be added later, when this and arXiv:1403.5235 will be combined

R2 v1 2026-06-22T03:34:11.482Z