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Log truncated threshold and zero mass conjecture

Fusheng Deng, Yinji Li, Qunhuan Liu, Zhiwei Wang, Xiangyu Zhou

TL;DR

This work analyzes singularities of plurisubharmonic functions in the Cegrell class by introducing the log truncated threshold $lt(\varphi,0)$ and linking higher Lelong numbers $\nu_j(\varphi)$ to the residual Monge–Ampère mass $\nu_n(\varphi)$. It proves that if $\nu_1(\varphi)=0$, then for almost every linear map $A$, the residual mass $\nu_n(\max\{\varphi, A^*\psi\})$ vanishes, using a dimension-enlargement approach with $\Phi(z,w)=\max\{\varphi(z),\psi(w)\}$ together with Teissier-type inequalities and Crofton formulas. A sharp bound is established: for finite $lt(\varphi,0)=\gamma$, $\nu_n(\varphi)$ is controlled by the first $n-1$ Lelong numbers and $\gamma$, yielding $\nu_n(\varphi)=0$ when $\nu_1(\varphi)=0$ and providing several corollaries for $S^1$-invariant and uniformly directional Lipschitz PSH functions. The results unite and strengthen known zero-mass statements, offer a new quantitative framework, and illuminate the interplay between directional Lelong numbers and residual Monge–Ampère mass in several complex variables.

Abstract

For plurisubharmonic functions $\varphi$ and $ψ$ lying in the Cegrell class of $\mathbb{B}^n$ and $\mathbb{B}^m$ respectively such that the Lelong number of $\varphi$ at the origin vanishes, we show that the mass of the origin with respect to the measure $(dd^c\max\{\varphi(z), ψ(Az)\})^n$ on $\mathbb{C}^n$ is zero for $A\in \mbox{Hom}(\mathbb{C}^n,\mathbb{C}^m)=\mathbb{C}^{nm}$ outside a pluripolar set. For a plurisubharmonic function $\varphi$ near the origin in $\mathbb{C}^n$, we introduce a new concept coined the log truncated threshold of $\varphi$ at $0$ which reflects a singular property of $\varphi$ via a log function near the origin (denoted by $lt(\varphi,0)$) and derive an optimal estimate of the residual Monge-Ampère mass of $\varphi$ at $0$ in terms of its higher order Lelong numbers $ν_j(\varphi)$ at $0$ for $1\leq j\leq n-1$, in the case that $lt(\varphi,0)<\infty$. These results provide a new approach to the zero mass conjecture of Guedj and Rashkovskii, and unify and strengthen well-known results about this conjecture.

Log truncated threshold and zero mass conjecture

TL;DR

This work analyzes singularities of plurisubharmonic functions in the Cegrell class by introducing the log truncated threshold and linking higher Lelong numbers to the residual Monge–Ampère mass . It proves that if , then for almost every linear map , the residual mass vanishes, using a dimension-enlargement approach with together with Teissier-type inequalities and Crofton formulas. A sharp bound is established: for finite , is controlled by the first Lelong numbers and , yielding when and providing several corollaries for -invariant and uniformly directional Lipschitz PSH functions. The results unite and strengthen known zero-mass statements, offer a new quantitative framework, and illuminate the interplay between directional Lelong numbers and residual Monge–Ampère mass in several complex variables.

Abstract

For plurisubharmonic functions and lying in the Cegrell class of and respectively such that the Lelong number of at the origin vanishes, we show that the mass of the origin with respect to the measure on is zero for outside a pluripolar set. For a plurisubharmonic function near the origin in , we introduce a new concept coined the log truncated threshold of at which reflects a singular property of via a log function near the origin (denoted by ) and derive an optimal estimate of the residual Monge-Ampère mass of at in terms of its higher order Lelong numbers at for , in the case that . These results provide a new approach to the zero mass conjecture of Guedj and Rashkovskii, and unify and strengthen well-known results about this conjecture.

Paper Structure

This paper contains 4 sections, 16 theorems, 107 equations.

Key Result

Theorem 1.1

Suppose $\varphi\in\mathcal{E}(\mathbb{B}^n)$, $\psi\in\mathcal{E}(\mathbb{B}^m)$, where $n,m\geq 1$. If $\nu_1(\varphi)=0$, then for outside a pluripolar set, it holds that where $A^*\psi$ is the compostion of $\psi$ and $A$ given by

Theorems & Definitions (36)

  • Definition 1.1
  • Theorem 1.1
  • Remark 1.1
  • Theorem 1.2
  • Definition 1.2
  • Remark 1.2
  • Theorem 1.3
  • Corollary 1.4
  • Corollary 1.5
  • Theorem 2.1
  • ...and 26 more