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No rapidly decaying standing wave for the defocusing cubic nonlinear Schrodinger equation
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Defocusing nonlinear Schrödinger equation
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For
ψ
=
e
−
i
Et
f
(
x
)
with real
f
, the defocusing equation
i
ψ
t
+
ψ
xx
−
2∣
ψ
∣
2
ψ
=
0
has first integral
(
f
′
)
2
=
f
4
−
E
f
2
.
(8)
A nonzero smooth function tending to zero at both infinities cannot satisfy this identity: a nonzero extremum requires
f
2
=
E
>
0
, but then the right side is negative for sufficiently small nonzero
f
.
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Defocusing nonlinear Schrödinger equation
Integrable systems
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