Quintic NLS on T

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The theory of the quintic NLS on the circle is as follows.

  • This equation may be viewed as a simpler version of cubic DNLS, and is always at least as well-behaved.
  • Scaling is s_c = 0\,.
  • LWP is known for s > 0\, Bo1993.
    • For s < 0\, the solution map is not uniformly continuous from C^k\, to C^{-k}\, for any k\, CtCoTa-p3.
  • GWP is known in the defocusing case for s > 4/9\, (De Silva, Pavlovic, Staffilani, Tzirakis)
    • For s > 2/3\, this is commented upon in Bo-p2 and is a minor modification of CoKeStTkTa-p.
    • For s \ge 1\, one has GWP in the defocusing case, or in the focusing case with small L^2\, norm, by Hamiltonian conservation.
      • In the defocusing case one has GWP for random data whose Fourier coefficients decay like 1/|k|\, (times a Gaussian random variable) Bo1995c; this is roughly of the regularity of H^{1/2}\,. Indeed one has an invariant measure. In the focusing case the same result holds assuming the L^2\, norm is sufficiently small.
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