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time
Disp
is
ersiv
ersit
e
=
estimates
e
and
in
the
,
2D
t
cubic
e
NLS
in
equation
Cedex
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the
abrice
2
Planc
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hon
x;
t
Abstract
a
W
or
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er
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d'Analyse
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place
e
globally
that
and
the
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initial
k
v
alue
u
problem
;
for
x
the
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(
cubic
this
semi-linear
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Sc
of
hr
hartz
odinger
o
equation
a
is
w
w
with
ell-p
URA
osed
et
in
75
the
(
Beso
small
v
2
space
2
_
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B
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solution,
;
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(
(2)
R
(
2
u
).
x
F
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or
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this,
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(
e
=
rely
on
:
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cal
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global
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result
ersiv
conse-
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disp
inequalities
of
deriv
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ed
suitable
from
er-
bilinear
y
restriction
o
theorems.
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In
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s
duction
Lab
W
e
189,
are
e
in
Curie,
terested
BC
in
P
the
osed
Cauc
and
h
for
y
data)
problem
L
for
([4]),
the
L
NLS
is
equation
scale-in
(1)
arian
space:
i@
u
t
a
u
then
+
u
L
u
=
=
u
k
u
2
3
where
;
u
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(
x
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0
=
(
u
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(
(
x
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in
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!
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x;
Since
)
w
u
e
x;
will
2
b
)
e
Indeed,
dealing
lo
with
in
small
(or
data,
for
the
data)
sign
is
of
direct
the
quence
non-linearit
the
y
ersiv
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estimates
irrelev
Stric
an
([16
t,
F
and
a
u
p
3
w
should
lik
b
non-linearit
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(with
understo
p
o
w
d
p
as
3),
b
ell-p
eing
holds
an
H
y
p
cubic
com
oratoire
bination
Num
of
erique,
u
CNRS
and
Univ
u
Pierre
.
Marie
Recall
4
(1)
Jussieu
is
187,
lo
252
cally
aris
w
1
ell-pR
s
the
p
,
=
p
1
what
2
exploited
p
hartz
1
of
,
emen
and
1
w
<
as
vide
obtained
rev
in
equation,
[4]
an
relying
presen
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ed
v
conjecture
arious
Definition
Stric
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hartz
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esti-
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mates.
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y
[13],
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w
the
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e
generalized
t,
these
space
results
one
to
the
w
W
ell-p
ossible.
osedness
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in
lik
the
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haracterizations
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n
space
b
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,
s
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in
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,
with
allo
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wing
estimates,
self-similar
and
solutions
,
for
as
suitable
cubic
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initial
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data.
osed-ness
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pro
in
of
ery
requires
Besides
some
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renemen
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ts
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in
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v
it
olving
situation
Loren
of
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spaces,
dimensions
as
progress
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section
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calization
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adic
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frequency
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osition
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arying
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trast
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time
ercome
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the
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lac
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alized
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for
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pieces.
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breaks
],
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them
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whenev
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in
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the
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require
transform
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in
one
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frequency
[3].
for
This
Let
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ws
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=
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results
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in
j
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+1
the
Let
self-similar
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so-
R
lutions
If
constructed
p
in
elongs
([5]),
s;q
similar
only
to
equation.
the
[3]
one
exibilit
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hiev
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ed
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in
w
[13]
time-space
in
esgue
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range
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p
pro
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mixed
3.
estimates
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v
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regularit
in
for
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to
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they
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2
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,
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tained
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tains
3D.
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or
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latter
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is
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in
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us
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oin
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v
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missing
settled
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[12
[13
using
].
argumen
W
v
e
similar
remark
the
it
that
had
ws.
b
the
een
theorem
previously
this
observ
er,
ed
e
b
e
y
t
Bourgain
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that
estimates
k
e
u
t
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b
k
of
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terest.
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e
k
v
u
stated
k
in
_
n
B
er
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w
;
p
1
In
2
the
small
is
w
v
ould
as
giv
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e
exp
global
ts
solutions
greater.
([2]).
same
Th
of
us,
v
w
ts
e
higher
are
w
remo
most
ving
ely
the
some
relation-
on
ship
restriction
b
or
et
of
w
v
een
ts.
the
o
size
this
of
w
the
recall
L
Beso
2
spaces
norm
through
and
c
the
via
size
lo
of
([1]
the
details).
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1
v
norm,
S
for
R
L
)
2
h
data.
b
The
=
k
for
ey
to
our
and
result
is
0
of
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course
j
the
2
same
as
(
in
)
[3]:
2
in
2D
j
more
)
is
S
kno
=
wn
j
ab
out
the
=
restriction
j
to
S
the
.
parab
f
oloid,
e
allo
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wing
(
for
n
greater
.
exi-
s
bilit
n
y
,
in
b
the
to
estimates
B
for
p
the
and
Sc
if
hr
odingersuch
L
The
_
partial
0
sum
(
P
+
m
regularit
m
1
;
j
assumption
(
j
f
x
)
dep
con
=
v
k
erges
e
to
2
f
t
as
over,
a
4
temp
L
ered
u
distribution.
k
"
The
L
sequence
text.
1
j
0
=
,
2
_
j
0
s
al
k
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(
j
(6)
(
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akly
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unique
k
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L
4
p
;
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elongs
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to
x
l
+
q