Cubic NLS on S6
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The theory of the
cubic NLS
on the six-dimensional sphere is as follows.
Scaling is
s
c
=
2
{\displaystyle s_{c}=2\,}
.
Uniform LWP holds in
H
s
{\displaystyle H^{s}\,}
for
s
>
5
/
2
{\displaystyle s>5/2\,}
BuGdTz-p3
.
Uniform LWP fails in the energy class
H
1
{\displaystyle H^{1}\,}
BuGdTz-p2
; indeed we have this failure for any NLS on
S
6
{\displaystyle S^{6}}
, even ones for which the energy is subcritical. This is in contrast to the Euclidean case, where one has LWP for powers
p
<
2
{\displaystyle p<2\,}
.
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