English

Ricci-flat manifolds of generalized ALG asymptotics

Differential Geometry 2023-02-23 v2 Mathematical Physics Algebraic Geometry math.MP

Abstract

In complex dimensions 3\geq 3, we provide a geometric existence for generalized ALG complete non-compact Ricci flat K\"ahler manifolds with Schwartz decay i.e. metric decay in any polynomial rate to an ALG model C×Y\mathbb{C}\times Y modulo finite cyclic group action, where YY is Calabi-Yau. Consequently, for any K3K3 surface with a purely non-symplectic automorphism σ\sigma of finite order, a K\"ahler crepant resolution of the orbifold C×K3σ\frac{\mathbb{C} \times K3}{\langle \sigma \rangle} admits ALG Ricci-flat K\"ahler metrics with Schwartz decay. It is known that K\"ahler crepant resolution exists in our case. Hence there are 3939 integers, such that 2π2\pi divided by each of them is the asymptotic angle of an ALG Ricci-flat K\"ahler 33-fold with Schwartz decay. We also exhibit a 1638 parameters family of ALG Ricci-flat K\"ahler 33-folds with asymptotic angle π\pi that realize 6464 distinct triples of Betti numbers. They are iso-trivially fibred by K3K3 surface with a non-symplectic Nikulin involution. A simple version of local Kunneth formula for H1,1H^{1,1}/local ii\partial\overline{\partial}-lemma plays a role in both the Schwartz decay, and the construction of ansatz that equals a Ricci flat ALG model outside a compact set (isotrivial ansatz). The proof of Schwartz decay relies on a non-concentration of the Newtonian potential, and can not be immediately generalized to fibration with higher dimensional base, due to existence of concentrating sequence of L2L^{2} normalized eigen-functions on unit round spheres of (real) dimension 2\geq 2.

Keywords

Cite

@article{arxiv.2212.11267,
  title  = {Ricci-flat manifolds of generalized ALG asymptotics},
  author = {Yuanqi Wang},
  journal= {arXiv preprint arXiv:2212.11267},
  year   = {2023}
}

Comments

47 pages. 5 figures, 3 tables. Revisions are carried out and presentation improved. Inaccuracy in Proposition 1.6 is fixed: k^2_{0} is the eigen-value, not k_{0}. Definition of weakly distinct is revised. Typos are corrected. Comments are welcome