2013
DOI: 10.1007/s12220-013-9458-x
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On the Collapsing Rate of the Kähler–Ricci Flow with Finite-Time Singularity

Abstract: Abstract. We study the collapsing behavior of the Kähler-Ricci flow on a compact Kähler manifold X admitting a holomorphic submersion X π − → Σ where Σ is a Kähler manifold with dim C Σ < dim C X. We give cohomological and curvature conditions under which the fibers π −1 (z), z ∈ Σ collapse at the optimal rate diamt(π −1 (z)) ∼ (T − t) 1/2 .

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Cited by 9 publications
(12 citation statements)
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“…Our main result is to show that the flow must also develop Type I singularities when it does not collapse and the blow-up limit is a nontrivial complete shrinking gradient Kähler-Ricci soliton. Combined with the results of Zhu [28] and Fong [7], we have the following theorem. Theorem 1.1.…”
Section: Introductionsupporting
confidence: 60%
See 1 more Smart Citation
“…Our main result is to show that the flow must also develop Type I singularities when it does not collapse and the blow-up limit is a nontrivial complete shrinking gradient Kähler-Ricci soliton. Combined with the results of Zhu [28] and Fong [7], we have the following theorem. Theorem 1.1.…”
Section: Introductionsupporting
confidence: 60%
“…is the standard flat metric on C n−1 and g F S the Fubini-Study metric on CP 1 for any sequence of points p j [7].…”
Section: Introductionmentioning
confidence: 99%
“…(2) ( [9]) If lim inf t→T (T − t) −1 V ol(X, g(t)) ∈ (0, ∞), then (X, g j (t), p j ) sub-converges in C ∞ -CGH sense to (C n−1 × CP 1 , g C n−1 ⊕ (−t)g F S ), where g C n−1 is the standard flat metric on C n−1 and g F S is the Fubini-Study metric on CP 1 for any sequence of points p j . (3) ( [31]) If lim inf t→T (T − t) −1 V ol(X, g(t)) = 0, then (X, g j (t)) converges in C ∞ -CGH sense to the unique compact shrinking Kähler Ricci soliton on CP n blown-up at one point.…”
Section: Preliminariesmentioning
confidence: 99%
“…When the initial Kähler class satisfies a 0 (n − 1) > b 0 (n + 1), the flow collapses to CP n−1 at T = (b 0 − a 0 )/2 ( [25]). It is shown in [9] that the flow must develop Type I singularities and the rescaled flow converges in Cheeger-Gromov-Hamilton sense to the ancient solution that splits isometrically as C n−1 × CP 1 . The initial Kähler class condition of a 0 (n − 1) < b 0 (n + 1), is equivalent to the limiting total volume being strictly positive at the singular time T = a 0 /(n − 1), i.e., (1.2) lim inf t→T − V ol(X, g(t)) > 0, and the flow contracts the exceptional divisor D 0 at T ( [25]).…”
Section: Introductionmentioning
confidence: 99%
“…Surprisingly, it is still an open problem to determine the precise behavior of the flow even in the case of P 1 × P 1 when one of the fibers collapses. It was shown by Song-Székelyhidi-Weinkove [59] that the diameter of the collapsing fiber is bounded above by a multiple of (T − t) 1/3 , but this falls short of the optimal rate of (T − t) 1/2 (see also [21]). It is expected that the blow-up limit is a product with a flat direction and this has been proved under symmetry conditions [20,57].…”
Section: Some Open Problemsmentioning
confidence: 99%