3.6.1 Riemann metric, lengthDef<strong>in</strong>ition 3.23 • A Riemannian metric G on a differentiable manifoldM def<strong>in</strong>es a scalar product 〈h 1 , h 2 〉 G|c on h 1 , h 2 ∈ T c M, dependent onthe po<strong>in</strong>t c ∈ M. We assume that the scalar product varies smoothly w.r.toc.• The scalar product def<strong>in</strong>es the norm |h| c = |h| G|c = √ 〈h, h〉 G|c.Suppose γ : [0, 1] → M is a path connect<strong>in</strong>g c 0 to c 1 .∫ 1• The length is Len(γ) := | ˙γ(v)| γ(v) dv0γwhere ˙γ(v) := ∂ v γ(v).c 1∫ M1c 0• The energy (or action) is E(γ) := | ˙γ(v)| 2 γ(v) dv3.6.2 F<strong>in</strong>sler metric, lengthDef<strong>in</strong>ition 3.24 We def<strong>in</strong>e a F<strong>in</strong>sler metric to be a function F : T M → lR + ,such that• F is cont<strong>in</strong>uous <strong>and</strong>,• for all c ∈ M , v ↦→ F (c, v) is a norm on T c M.We will sometimes write |v| c := F (c, v).(Sometimes F is called a “M<strong>in</strong>kowsky norm”).As for the case <strong>of</strong> norms, a F<strong>in</strong>sler metric may be asymmetric; but, for sake<strong>of</strong> simplicity, we will only consider the symmetric case.Us<strong>in</strong>g the norm |v| c we can then aga<strong>in</strong> def<strong>in</strong>e the length <strong>of</strong> paths byLen F (γ) =<strong>and</strong> similarly the action.3.6.3 Distance∫ 10| ˙γ(t)| γ(t) dt =0∫ 10F (γ(t), ˙γ(t)) dtDef<strong>in</strong>ition 3.25 The distance d(c 0 , c 1 ) is the <strong>in</strong>fimum <strong>of</strong> Len(γ) between allC 1 paths γ connect<strong>in</strong>g c 0 , c 1 ∈ M.Remark 3.26 In the follow<strong>in</strong>g chapter, we will def<strong>in</strong>e some differentiable manifoldsM <strong>of</strong> <strong>curves</strong>, <strong>and</strong> add a Riemann (or F<strong>in</strong>sler) metric G on those; thereare two different choices for the model space,• suppose we model the differentiable manifold M on a Hilbert space U, withscalar product 〈, 〉 U ; this implies that M has a topology τ associated toit, <strong>and</strong> this topology, through the charts φ, is the same as that <strong>of</strong> U. Let28
now G be a Riemannian metric; s<strong>in</strong>ce the derivative <strong>of</strong> a chart Dφ(c)maps U onto T c M, one natural hypothesis will be to assume that 〈, 〉 U <strong>and</strong>〈, 〉 G,c be locally equivalent (uniformly w.r.to small movements <strong>of</strong> c); asa consequence, the topology generated by the Riemannian distance d willco<strong>in</strong>cide with the orig<strong>in</strong>al topology τ. A similar request will hold for thecase <strong>of</strong> a F<strong>in</strong>sler metric G, <strong>in</strong> this case U will be a Banach space with anorm equivalent to that def<strong>in</strong>ed by G on T c M.• We will though f<strong>in</strong>d out that, for technical reasons, we will <strong>in</strong>itially modelthe spaces <strong>of</strong> <strong>curves</strong> on the Fréchet space C ∞ ; but <strong>in</strong> this case there cannotbe a norm on T c M that generates the same orig<strong>in</strong>al topology (for the pro<strong>of</strong>,see I.1.46 <strong>in</strong> [48]).3.6.4 M<strong>in</strong>imal geodesicsDef<strong>in</strong>ition 3.27 If there is a path γ ∗ provid<strong>in</strong>g the m<strong>in</strong>imum <strong>of</strong> Len(γ) betweenall paths connect<strong>in</strong>g c 0 , c 1 ∈ M, then γ ∗ is called a m<strong>in</strong>imal geodesic.The m<strong>in</strong>imal geodesic is also the m<strong>in</strong>imum <strong>of</strong> the action (up to reparameterization).Proposition 3.28 Let ξ ∗ provide the m<strong>in</strong>imum m<strong>in</strong> γ E(γ) <strong>in</strong> the class <strong>of</strong> allpaths γ <strong>in</strong> M connect<strong>in</strong>g x to y. Then ξ ∗ is a m<strong>in</strong>imal geodesic <strong>and</strong> its speed| ˙ξ ∗ | is constant.Vice versa, let γ ∗ be a m<strong>in</strong>imal geodesic, then there is a reparameterizationξ ∗ = γ ∗ ◦ φ s.t. ξ ∗ provides the m<strong>in</strong>imum m<strong>in</strong> γ E(γ).A pro<strong>of</strong> may be found <strong>in</strong> [34].3.6.5 Exponential mapThe action E is a smooth <strong>in</strong>tegral, quadratic <strong>in</strong> ˙γ, <strong>and</strong> we can compute theEuler-Lagrange equations; its m<strong>in</strong>ima are more regular, s<strong>in</strong>ce they are guaranteedto have constant speed; consequently, when try<strong>in</strong>g to f<strong>in</strong>d geodesics, we will tryto m<strong>in</strong>imize the action <strong>and</strong> not the length. This also related to the idea <strong>of</strong> theexponential map.Def<strong>in</strong>ition 3.29 Let ¨γ = Γ( ˙γ, γ) be the Euler-Lagrange ODE <strong>of</strong> the actionE(γ) = ∫ 10 | ˙γ(v)|2 dv. Any solution <strong>of</strong> this ODE is a critical geodesic. Notethat any m<strong>in</strong>imal geodesic is a critical geodesic.Def<strong>in</strong>e the exponential map exp c : T c M → M as exp c (η) = γ(1), whereγ is the solution <strong>of</strong>{¨γ(v) = Γ( ˙γ(v), γ(v)), γ(0) = c, ˙γ(0) = η (3.3)Solv<strong>in</strong>g the above ODE (3.3) is <strong>in</strong>formally known as shoot<strong>in</strong>g geodesics.The exponential map is <strong>of</strong>ten used as a chart, s<strong>in</strong>ce it is the least possiblydeform<strong>in</strong>g map at the orig<strong>in</strong>.29
- Page 1 and 2: Metrics of curves in shape optimiza
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7.552.5-10 -7.5 -5 -2.5 2.5 5 7.5 1
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By using (i) and (ii) from lemma 10
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10.6.3 Existence of flow for geodes
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10.7.1 Robustness w.r.to local mini
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We already presented all the calcul
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10.9 New regularization methodsTypi
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can be solved for k (this is not so
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2. Now• at t = 1/2 it achieves th
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Definition 11.10 • The orbit is O
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y eqn. (11.3), where the terms RHS
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So Prop. 11.19 guarantees that the
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Theorem 11.23 Suppose that the Riem
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2.2.3 Examples of geometric energy
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9 Riemannian metrics of immersed cu
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contour continuation, 11convolution
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normal vector, 6objective function,
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References[1] Luigi Ambrosio, Giuse
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[30] Serge Lang. Fundamentals of di
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[57] Ganesh Sundaramoorthi, Anthony