Abstract
For the 3d cubic nonlinear Schrodinger (NLS) equation, which has critical (scaling) norms L 3 and u H 1/2 , 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 and prove a result on the concentration of the L 3 norm at the origin. Two disparate possibilities emerge, one which coincides with solutions typically observed in numer- ical 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, i.e. those that concentrate on a sphere of radius ∼ (T −t) 1/3 , but focus towards 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.
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