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The Canonical Expanding Soliton and Harnack inequalities for Ricci flow (2009)

by Esther Cabezas-rivas
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A Lie algebraic approach to Ricci flow invariant curvature conditions and Harnack inequalities

by Burkhard Wilking
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The canonical shrinking soliton associated to a Ricci flow

by Esther Cabezas-Rivas , Peter M Topping - Calc. Var
"... Abstract To every Ricci flow on a manifold M over a time interval I ⊂ R−, we associate a shrinking Ricci soliton on the space-time M×I. We relate properties of the original Ricci flow to properties of the new higher-dimensional Ricci flow equipped with its own time-parameter. This geometric constru ..."
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Abstract To every Ricci flow on a manifold M over a time interval I ⊂ R−, we associate a shrinking Ricci soliton on the space-time M×I. We relate properties of the original Ricci flow to properties of the new higher-dimensional Ricci flow equipped with its own time-parameter. This geometric construction was discovered by consideration of the theory of optimal transportation, and in particular the results of the second author
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...[8, 13] after setting t = −τ. One advantage of the notion of Canonical Soliton over the construction of Perelman is that we can use it to find and prove new (and old) Harnack inequalities. Indeed, in =-=[1]-=- we will extend the ideas of this paper to give Canonical Expanding Solitons in order to achieve this. A notion of Canonical Steady Soliton, discussed in Section 5, completes the picture. In Section 6...

The Geometry of Differential Harnack Estimates

by Sebastian Helmensdorfer , 2013
"... In this short note, we hope to give a rapid induction for non-experts into the world of Differential Harnack inequalities, which have been so influential in geometric analysis and probability theory over the past few decades. At the coarsest level, these are often mysterious-looking inequalities tha ..."
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In this short note, we hope to give a rapid induction for non-experts into the world of Differential Harnack inequalities, which have been so influential in geometric analysis and probability theory over the past few decades. At the coarsest level, these are often mysterious-looking inequalities that hold for ‘positive ’ solutions of some parabolic PDE, and can be verified quickly by grinding out a computation and applying a maximum principle. In this note we emphasise the geometry behind the Harnack inequalities, which typically turn out to be assertions of the convexity of some natural object. As an application, we explain how Hamilton’s Differential Harnack inequality for mean curvature flow of a n-dimensional submanifold of R n+1 can be viewed as following directly from the wellknown preservation of convexity under mean curvature flow, but this time of a (n + 1)-dimensional submanifold of R n+2. We also briefly survey the earlier work that led us to these observations. 1
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...e correspondence between the relevant Harnack quantity and the curvature of a degenerate space-time construction (see [CK] for further details). E. CabezasRivas and P. Topping extended these ideas in =-=[CT]-=- by constructing a nondegenerate expanding space-time approximate Ricci soliton, the limit of whose curvatures gave the existing, and new, Harnack quantities. Thus Harnack inequalities correspond to t...

Sharp differential estimates of Li-Yau-Hamilton type for positive (p, p)-forms on Kähler manifolds

by Lei Ni, Yanyan Niu - COMMUN. PURE APPL. MATH , 2011
"... In this paper we study the heat equation (of Hodge Laplacian) deformation of.p; p/-forms on a Kähler manifold. After identifying the condition and establishing that the positivity of a.p; p/-form solution is preserved under such an invariant condition, we prove the sharp differential Harnack (in the ..."
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In this paper we study the heat equation (of Hodge Laplacian) deformation of.p; p/-forms on a Kähler manifold. After identifying the condition and establishing that the positivity of a.p; p/-form solution is preserved under such an invariant condition, we prove the sharp differential Harnack (in the sense of Li-Yau-Hamilton) estimates for the positive solutions of the Hodge Laplacian heat equation. We also prove a nonlinear version coupled with the Kähler-Ricci flow and some interpolating matrix differential Harnack-type estimates for both the Kähler-Ricci flow and the Ricci flow.

Sur la regularite du . . .

by Chih-wei Chen , 2012
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Preface 2

by unknown authors , 2009
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... is a calculation. Some parts of that calculation are given in the proposition below; more involved calculations will be required in Chapter 4 for the Canonical Expanding Soliton, and can be found in =-=[5]-=-. Proposition 3.1.2. (See [4].) Fixing τ > 0, a time at which the Ricci flow exists, and fixing local coordinates {x i } in a neighbourhood U of some p ∈ M, then in any neighbourhood V ⊂⊂ U × (a, b) o...

Preface 2

by unknown authors , 2009
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... is a calculation. Some parts of that calculation are given in the proposition below; more involved calculations will be required in Chapter 4 for the Canonical Expanding Soliton, and can be found in =-=[5]-=-. Proposition 3.1.2. (See [4].) Fixing τ > 0, a time at which the Ricci flow exists, and fixing local coordinates {x i } in a neighbourhood U of some p ∈ M, then in any neighbourhood V ⊂⊂ U × I of (p,...

Preface 2

by unknown authors , 2010
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... is a calculation. Some parts of that calculation are given in the proposition below; more involved calculations will be required in Chapter 4 for the Canonical Expanding Soliton, and can be found in =-=[5]-=-. Proposition 3.1.2. (See [4].) Fixing τ > 0, a time at which the Ricci flow exists, and fixing local coordinates {x i } in a neighbourhood U of some p ∈ M, then in any neighbourhood V ⊂⊂ U × I of (p,...

:0

by Esther Cabezas-rivas , 2009
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...ies. More precisely, the components of the (4, 0) curvature tensor τRm(ĝ) coincide (up to errors of order 1 N ) with the components of Perelman’s version of the matrix Harnack expression [8, 13]. In =-=[1]-=- we will explain how a variant of these ideas can be used to prove new Harnack inequalities. Remark 1.3. Although each side of (1.2) evaluated on the pair ( ∂ ∂τ , ∂ ∂τ ) will have magnitude of order ...

unknown title

by unknown authors , 2014
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...erate Harnack quantities. The general idea is that a differential Harnack estimate corresponds to a preserved curvature condition on a canonical soliton. E. Cabezas-Rivas and P. Topping have shown in =-=[CT2]-=- that this procedure works for the Ricci flow. The Ricci curvature of the canonical expanding Ricci soliton converges as N → ∞ to Hamilton’s matrix Harnack quantity for the Ricci flow (see [HA]). More...

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