11.07.2015 Views

International Congress of Mathematicians

International Congress of Mathematicians

International Congress of Mathematicians

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On the Sehrödinger Flows 287lower bound T <strong>of</strong> T f , and uniform bounds for various norms <strong>of</strong> u f _(t) in suitablespaces for t in the time interval [0,T). (Since we shall use L 2 estimates, the normsare W k ' 2 (M,N)— norms for all positive integer k.) Once we get these bounds it isclear that the u f _ subconverge to a smooth solution <strong>of</strong> (3.1) as e —¥ 0.Now let u = u f _ be a solution <strong>of</strong> (3.2), then it is easy to see that the energyE(u(tj) is uniformly bounded for t £ [0,T f ), i.e.E(u(tj) < E(u 0 ). (3.3)In the following we will make estimations on L 2 —norms <strong>of</strong> all covariant derivativesV k u (k = 2,3, •• •).Lemma 3.1 Let mo = [m/2] + 1, where [q] denotes the integral part <strong>of</strong> a positivenumber q, and let «o £ C°°(M,N). There exists a constant T = T(\\UO\\H'^O+ 1 - 2 )> 0, independent <strong>of</strong> e £ [0,1], such that ifu £ C°°(M x [0,T e ]) is a solution <strong>of</strong> (3.1)with e £ (0,1] thenT f _>T(\\Vuo\\H^o.' 2 )andfor all k > mo-IIVu(t)\\ H k,2 < C(k, ||Vuo||/r*.0 t £ [0, T]Pro<strong>of</strong> Fix a k > mo, and let I be any integer with 1 < I < k. Suppose thata be a multi-index <strong>of</strong> length I, i.e. a = (cti, • • •, aj). Then we have for t 0 always holds, such that(b, c,d,e) = h > • • • > Je, I + 1 > 3ì > 1, ii + • • • + je = l + 3, s > 3. (3.7)

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