2016
DOI: 10.1007/s10455-015-9493-x
|View full text |Cite
|
Sign up to set email alerts
|

Uniqueness of constant scalar curvature Sasakian metrics

Abstract: Abstract. In this paper, we prove that the transverse Mabuchi K-energy functional is convex along the weak geodesic in the space of Sasakian metrics. As an application, we obtain the uniqueness of constant scalar curvature Sasakian metrics modulo automorphisms for the transverse holomorphic structure.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

0
6
0
1

Year Published

2016
2016
2020
2020

Publication Types

Select...
3
1

Relationship

0
4

Authors

Journals

citations
Cited by 4 publications
(7 citation statements)
references
References 22 publications
0
6
0
1
Order By: Relevance
“…Assume that c 2 dη − (n − 1)χ is a transverse Kähler form. Then, the Sasaki J-flow converges C ∞ to a smooth critical metric.The proof is based on the long time existence of the flow and the uniform lower bound on the second derivatives of a solution to the flow established in [23], and on the estimates developed in sections 3 and 4 of the present paper, which are obtained applying the maximum principle and a Moser iteration argument (see the proof of Prop 4.6).It is worth pointing out that as immediate corollary we get the C ∞ convergence of the flow to a critical metric on compact 5-dimensional Sasaki manifolds under the assumption c 2 dη − χ > 0.As application, we highlight the relation between the Sasaki J-flow and the Mabuchi Kenergy, introduced in the Sasakian context by [9] (see also [14]), proving a lower bound for the K-energy map under the existence of a critical metric (see Theorem 5.2 at the end of the paper).…”
mentioning
confidence: 62%
See 1 more Smart Citation
“…Assume that c 2 dη − (n − 1)χ is a transverse Kähler form. Then, the Sasaki J-flow converges C ∞ to a smooth critical metric.The proof is based on the long time existence of the flow and the uniform lower bound on the second derivatives of a solution to the flow established in [23], and on the estimates developed in sections 3 and 4 of the present paper, which are obtained applying the maximum principle and a Moser iteration argument (see the proof of Prop 4.6).It is worth pointing out that as immediate corollary we get the C ∞ convergence of the flow to a critical metric on compact 5-dimensional Sasaki manifolds under the assumption c 2 dη − χ > 0.As application, we highlight the relation between the Sasaki J-flow and the Mabuchi Kenergy, introduced in the Sasakian context by [9] (see also [14]), proving a lower bound for the K-energy map under the existence of a critical metric (see Theorem 5.2 at the end of the paper).…”
mentioning
confidence: 62%
“…As application, we highlight the relation between the Sasaki J-flow and the Mabuchi Kenergy, introduced in the Sasakian context by [9] (see also [14]), proving a lower bound for the K-energy map under the existence of a critical metric (see Theorem 5.2 at the end of the paper).…”
mentioning
confidence: 89%
“…We shall prove this theorem following the lines closely as in [24]. Given this result, one can then extend the K-energy to E 1 (M, ξ, ω T ), and keep it still convex along geodesics, see [2,41,51,5]. We actually generalize almost all related results in [24] to Sasaki setting, building up on profound results in pluripotential theory by many and geodesic equation [32].…”
Section: Introductionmentioning
confidence: 80%
“…Theorem 2 is the counterpart of main results in [30] in Sasaki setting. An important notion in the study of csck is the convexity of K-energy along C 1, 1 geodesics [3] (see also [26]), which was generalized to Sasaki setting by [51,57]. Given the results above, one can then extend K-energy to E 1 -class and keep its convexity along finite energy geodesics as in [7].…”
Section: Introductionmentioning
confidence: 99%