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Some kind of Besov spaces related to non-linear PDEs
by
Tosinobu Muramatu
Chuo University
Besov-type spaces related to linear parts of non-linear PDEs give good existence rusults for Cauchy problems.
The Besov spaces reported here are defined as follows: For an infinitely differentialble real-valued function P(\xi), a weight \rho on R+, a real number b, 1 <= p <= \infty, and 1 <= q <= \infty the space Bp, q, P(\rho, b)(Rd+1) is the space of tempered distributions f such that the norm
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||f||B(\rho, b)p, q, P : = ||{\rho(2j)2bk||fjk, P(x, t)||Lp(Rd+1)}||lq |
| (\theequation) |
is finite. We write the space by Bp, q, P(s, b)(Rd+1) when \rho(t)=ts. Here, [^f] denotes the Fourier transform of f,
|
|
^
f
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jk, P
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(\xi, \tau) = jj(|\xi|)jk(\tau-P(\xi)) |
^
f
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(\xi, \tau), |
| (\theequation) |
and jj(z), j=0, 1, ... , are infinitely differentiable functions of a real variable z having the following properties:
jj(z)=jj(-z), suppj0 subset {z;|z| < 2},
supp j1 subset {z;1 < |z| < 4},
jk(z)=j1(2-k+1z) ( for , k >= 1), \sumj=0\inftyjj(z)=1.
This norm is a Besov analogue of that given by
|
||f||Xs, b= |
æ è
|
|
ó õ
|
|
ó õ
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R2
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(1+|\xi|)2s (1+|\tau-P(\xi)|)2b| |
^
f
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(\xi, \tau)|2d\xid\tau |
ö ø
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1/2
|
, |
| (\theequation) |
which has been employed by Kenig-Ponce-Vega (J. A. M. S. 9, 1996, Trans. A. M. S. 348, 1996).
They proved the existence of time-local solutions to the KdV equation
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\labelkdvequation\partialtu+\partialx3u+\partialx(u2)=0, |
| (\theequation) |
with u(x, 0)=u0(x) in Hs(R), s > -3/4, by making use of the estimate
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\labelestderfgcapx||\partialx(fg)||Xs, b-1 <= c||f||Xs, b||g||Xs, b with P=\xi3, |
| (\theequation) |
which holds for any s > -3/4 and some b > 1/2, and fails for any s < -3/4 and any b in R. Nakanishi-Takaoka-Tsutsumi showed that () fails also when s=-3/4.
The corresponding estimates by means of our norm are the following inequalities:
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||\partialx(fg)||B(\rho, -1/2)2, 1, \xi3 |
|
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c||f||B(\rho, 1/2)2, 1, \xi3||g||B(\rho, 1/2)2, 1, \xi3, if -3/4 <= s < 0, |
| |
||\partialx(fg)||B(\rho, -1/2)2, 1, \xi3 |
|
| | c||f||B(s, b)2, 1, \xi3||g||B(s, 1/2)2, 1, \xi3, if -3/4 <= s < 0, b > 1/2, |
|
|
where \rho(t)=log(2+t)ts, which make it possible to improve Kenig-Ponce-Vega's result, i. e., it can be proved that there exists T=T(||u0||B2, 1-3/4(R)) and u(x, t) in B2, 1, \xi3(-3/4, 1/2)(R2) which satisfies the equation () when |t| <= T and the initial condition u(x, 0)=u0(x) in B2, 1-3/4(R).
Our method is very general. It gives not only an improvement of Kenig-Ponce-Vega's result for one-dimensional nonlinear Schrödinger equation with nonlinear terms of the form c1u2+c2u[`u]+c3[`u]2, but it also is applicable to many kind of nonlinear PDEs.
Department of Mathematics, Chuo University
Date received: August 10, 2001
Copyright © 2001 by the author(s).
The author(s) of this document and the organizers of the conference
have granted their consent to include this abstract in
Atlas Conferences Inc.
Document # cahz-98.