Remark : Sometimes we will use a probabilistic convention, consisting inputting 1 before the Laplacian (which just changes the time and makes the calculus2more synthetic), sometimes we will use geometric convention.We call T c the explosion time of the mean curvature flow, let T < T c , and g(t)be the family of metrics defined above. Let (W i ) 1≤i≤n be a R n -valued Brownianmotion. We recall from [4] the definition of the g(t)-Brownian motion in M startedat x, denoted by g(t)-BM(x):Definition 1.2 Let us take a filtered probability space (Ω, (F t ) t≥0 , F, P) and a C 1,2 -family g(t) t∈[0,T [ of metrics over M. A M-valued process X(x) defined on Ω×[0, T [is called a g(t) Brownian motion in M started at x ∈ M if X(x) is continuous,adapted and for every smooth function f,f(X s (x)) − f(x) − 1 2is a local martingale vanishing at 0.∫ s0∆ t f(X t (x))dtWe give a proposition which yields a characterization of mean curvature flowby the g(t) Brownian motion.Proposition 1.3 Let M be an n-dimensional manifold isometrically embedded inR n+1 . Consider the application:F : [0, T [×M → R n+1such that F (t, .) are diffeomorphisms, and the family of metrics g(t) over M, whichis the pull-back by F (t, .) of the induced metric on M t = F (t, M). Then the followingitems are equivalent:i) F (t, .) is a solution of mean curvature flowii) ∀x 0 ∈ M, ∀T ∈ [0, T c [, let ˜g t T = 1g 2 T −t and X T (x 0 ) be a (˜g t T ) t∈[0,T ] -BM(x 0 ),then:Yt T = F (T − t, Xt T (x 0 ))is a local martingale in R n+1 .proof :By definition we have a sequence of isometries:F (t, .) : (M, g t ) ˜→M t ↩→ R n+1Let x 0 ∈ M and T ∈ [0, T c [ and X T (x 0 ) a (˜g t T ) t∈[0,T ] -BM(x 0 ). We just compute theItô differential of:Y T,it = F i (T − t, Xt T (x 0 )),683
that is to say:d(Y T,it ) = − ∂ F i (T − t, X T ∂t t (x 0 ))dt + d(FT i −t (XT t (x 0 ))− ∂ F i (T − t, X T ∂t t (x 0 ))dt + 1 2 ∆˜g tFT i −t (XT t (x 0 ))dt≡dM≡dM≡ 0.dM− ∂ ∂t F i (T − t, X T t (x 0 ))dt + ∆ gT −tF i T −t (XT t (x 0 ))dtTherefore YtT is a local martingale.Let us show the converse. Let x 0 ∈ M and T ∈ [0, T c [ and X T (x 0 ) a (˜g t T ) t∈[0,T ] -BM(x 0 ),Y T,it is a local martingale so almost surely, for all t ∈ [0, T ]:− ∂ ∂t F i (T − t, X T t (x 0 ))dt + ∆ gT −tF i T −t(X T t (x 0 ))dt = 0so that for all s ∈ [0, T ], by integrating we get∫ s0− ∂ ∂t F i (T − t, X T t (x 0 ))dt + ∆ gT −tF i T −t(X T t (x 0 ))dt = 0the continuity of every g(t)-Brownian motion yields,− ∂ ∂t F i (T, x 0 ) + ∆ gT F i T (x 0 ) = 0.In order to apply this proposition, we give an estimation of the explosion time. Itis also a consequence of a maximum principle, which is explicitly contained in theg(t)-Brownian Motion.The quadratic covariation of YtT is given by:Proposition 1.4 Let YtTfor the usual scalar product in R n+1 is:Y Ttbe defined as before, then the quadratic covariation of〈dY Tt, dYtT 〉 = 2n1 [0,T ] (t)dtproof : Let / T 0,t be the parallel transport above X T t , it is shown in [4] that it is anisometry :/ T 0,t : (T X0 M, ˜g(0)) ↦−→ (T Xt M, ˜g(t)).Let (e i ) 1≤i≤n be a orthonormal basis of (T X0 M, ˜g(0)), and (W i ) 1≤i≤n be the R n -valued Brownian motion such that (e.g. [4], [2]):∗dW t = / T,−10,t ∗ dX T t ,694
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Université de PoitiersTHÈSEpour o
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ivTABLE DES MATIÈRES3 Kendall-Cran
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