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For the 3D cubic nonlinear Schrödinger (NLS) equation, which has critical (scaling) norms L3 and Ḣ1/2, we first prove a result establishing sufficient conditions for global existence and sufficient conditions for finite-time blow-up. For the rest of the paper, we focus on the study of finite-time radial blow-up solutions, and prove a result on the concentration of the L3 norm at the origin. Two disparate possibilities emerge, one which coincides with solutions typically observed in numerical experiments that consist of a specific bump profile with maximum at the origin and focus toward the origin at rate ∼(T − t)1/2, where T > 0 is the blow-up time. For the other possibility, we propose the existence of “contracting sphere blow-up solutions,” that is, those that concentrate on a sphere of radius ∼(T − t)1/3, but focus toward this sphere at a faster rate ∼(T − t)2/3. These conjectured solutions are analyzed through heuristic arguments and shown (at this level of precision) to be consistent with all conservation laws of the equation.
Holmer et al. (Wed,) studied this question.