we develop a solvability theory for the linearized operator L defined in (1.22) under suitable orthogonality conditions ,
, A.4 The reduced energy
, as ? ? 0, J ? (U ? + ? ? ) = J ? (U ? ) + h.o.t. C 1-uniformly on compact sets of (0, +?) × R n (see
, Lemma 1.A.2. Let a, b ? R + be fixed numbers such that
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