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## QOPSN@PQRi؁j

C_\S@A3K303
15:0015:50
I
ό\ȎȐiqf͊wnɌ^

16:0016:50
c ST
lmxpsɂlƂ̘AIf

17:1018:00
a FK
iq̌q̋Lqnɂ钴isg̑

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C_\R@w3K305
14:0014:50
c 쎁
̈ۓƌŗLl

15:0015:50

Strichartz estimates for wave equations by spherical harmonics

16:1017:00
v [
Cauchy problem of nonlinear complex Ginzburg-Landau equations in Treibel-Lizorkin spaces

17:1018:00
T
ȉ~^̔r

## QOPSN@PPUi؁j

C_\Q@A3K303
15:0015:50

EtM̉̑

16:0016:50
av mi
މڗgU̎̑IQߋ

17:1018:00
ؑ II
Uẻ̕ Lp-Lq ^]

## QOPSN@P@Xi؁j

C_\P@A3K303
15:0015:50
J Ĉꎁ
oȋԂɂփm^ɑ΂郊Er̒藝

16:0016:50
gq ݎ
OB̊ԌIÖ@LqnCubhVXe̓Il

17:1018:00
J j

## QOPRNPQPX

Fkw wȁ@A3K303

u
Z qikw w@wȁj
ʋ22̔Schr\"odingern̉̑Qߋ
v|
2ɂ2̔Schroedingern̉
Ԗł̑Qߋl.
ʂ, 2ɂ2͔̔Schroedinger̉
ԖŎRɑQ߂邩ۂ̗ՊE󋵂ł邱ƂmĂ.
ł, nɑ΂Ďʋ肵ꍇ, ̑Qߋ
RƂCRƂقȂꍇN邱Ƃ.

Fkw wȁ@w2K209

u
Ďiȑw Hwj
p(x)-aʑ̐ɂ

## QOPRN@PQ@T

Fkw wȁ@A3K303

u
rc Oikw w@wȁj
Null structure in a system for quadratic derivative nonlinear Schroedinger equations
{uł́Aɔ܂2̃VfBK[̃VXelB
܂̃VXeɑ΂AʂɊւ鋤̉A̍\Ɋւ1̏B
Ă̏̉A2ɂďȏlɑ΂鎞ԑ̑݋yт̑QߎR𓱂B
͕ЎRY(a̎R)yэG()Ƃ̋̓ełB
܂Ԃ΁AƓl̏̉A3ȏɂĂ̓XP[ՊEȃ\{tԓ
ȃf[^ɑ΂U_\zł邱ƂB
͊ݖ{W()yщ{()Ƃ̋̓ełB

## QOPRN@PP@QW

Fkw wȁ@A3K303

u
Prof. Daniel Peralta-Salas (Instituto de Ciencias Matem\'aticas)
Critical points and dynamical properties of Green's gunctions on open surfaces
v|

## QOPRN@PP@PWijj̓Z~i[

Fkw wȁ@w305

u
Fsiw Hwj
Decay estimates of the solutions to the 2D Hyperbolic Navier-Stokes equations

x

## QOPRN@PP@V

Fkw wȁ@A3K303

u
{{ liw w@Ȋwȁj
\{tDՊE̔mC}̐lΏ̉̍\ɂ
v|
̈ɂ\{tDՊE̔Neumann ^2u-u+u^p=0 ̐lΏ̉̍\lD
N(>=3)ԎƂƂCp\{tՊEw(N+2)/(N-2)菬iՊEjCiՊEjC

ułp傫ꍇiDՊEj̐lΏ̉̍\i}jlDՊEՊȄꍇ̉\
r邱ƂɂāC\{t̖ߍ݂藧ȂɓĽۂTD

## QOPRN@PORP

Fkw wȁ@A3K303

u
O iBw w@w@j
Stability of line solitons for the KP-II equation in $\mathbb{R}^2$
v|
We prove nonlinear stability of line soliton solutions of the KP-II
equation with respect to transverse perturbations
that are exponentially localized as $x\to\infty$. We find that the
amplitude of the line soliton converges to that of the
line soliton at initial time whereas jumps of the local phase shift of the
crest propagate in a finite speed toward $y=\pm\infty$.
The local amplitude and the phase shift of the crest of the line
solitons are described by a system of 1D wave equations with diffraction terms.

## QOPRN@PO@QS@x

Wu@1022?25
utFc p񎁁iHƑw w@Hwȁj
uځFc^̎ȑƑS
kb 1021()@16:00?@
uҁFc p񎁁iHƑw w@Hwȁj
uځFPƔgUɌ镡Gȉ̋
uv|

## QOPRN@POPSij?@POPVi؁j

Fkw z[

W
Workshop on Free Boundaries in Laplacian Growth Phenomena and Related Topics
@@
z[y[W

## QOPRN@PO@PO@񐔗kb

Fkw Ȋwȓ2Ku

u
_ G ikCw w@w@j
Eigenvalues of Laplacian in a domain with a thin tubular hole
v|
I deal with the eigenvalue problem of Laplacian in a singularly
perturbed domain. This domain is given by removing a thin tubular
neighborhood of a submaniforld $M$, from the original fixed domain.
I consider the asymptotic behavior of each eigenvalue of Laplacian
(Dirichlet or other boundary condition), when the thinness (small)
parameter goes to zero.

## QOPRN@PO@R

Fkw wȁ@A3K303

u
ɓ ꎁi}gw Ȋwȁj
Threshold properties of one-dimensional discrete Schr\"odinger operators
v|
$1$U$\mathbb Z$Schr\"odingerpfɑ΂C

ɓWJv$\ell^2$-$\ell^\infty$-ŗLԂ̊֌WSɕނC
ŗLԂыԂ̓tsD
]xg̓WJvZɂ Jensen-Nenciui2001j̃ASYpD
{uArne JenseniAalborgwjƂ̋ɊÂD

## QOPRN@VPW

Fkw wȍWKWOP

u҂P
v pY (kw w@w M2)
ԋԂɂwϕ^s

u҂Q
Park@Sungyong (kw w@w M2)
Local well-posedness and blow-up result for weakly dissipative Camassa-Holm equations

## QOPRN@VPP

Fkw wȍWKWOP

u
R{ Gq (kw w@w D3)
sψ}̔gUޓ_ÏWp^[ƈʒuߔ
v|
̌Ԍ̃fƂGiererMeinhardt񏥂q-}q n, lXȃp^[邪, łPȂ̂Ƃē_ÏWp^[.
͗L̓_̎̋ɂ߂ċ͈͂ɕzWp^[ł, ̋ÏW_ǂɂȂ邩ł[ł. ψ}̏ꍇɂ, ÏW
_͗̈̊􉽂猈܂邱ƂɂĂ. , ̌Ԍ lȊōs邱Ƃ. {uł, sψ}̏ꍇ̋ÏW_

## QOPRN@UQV x

Workshop on nonlinear PDEs --PDE approach to network and related topics--
627()--29(y)
z[ikw wȁjɂ
ڂ

## QOPRN@UQO 16:00--17:30

Fkw wȍWKWOP

u
J 뎡 (Rw w@RȊw)
Allen-Cahnɂ鎲Ώ̂Ȑisg
v|
Allen-Cahn[NbhԑŜōlD
̐isgɂĒׂ錤͋ߔNɕ񍐂ĂDV^isg (Ninomiya and T, 2005)C
Ώ̂Ȑisg(Hamel, Monneau and Roquejoffre, 2005, 2006) ܂p^isg(T, 2007)ȂǂD
{ł͐VȎΏ̂Ȑisgɂĕ񍐂D

## QOPRN@U@U 16:00--17:30

Fkw wȍWKWOP

u
a (kw@w {w)
The ineffectiveness of impulsive control on spatially periodic solutions to a semilinear parabolic equation
v|
ÊƂŔ^̉̋ɂčlBuԓIȐ
\impulsive controlɂɑ΂鐧JԂsƂA
ԑIɑ݂邩A邢́ALԓɔ邩ɂB
ł3ނimpulsive control^ꂼɂčl@BɁA
LԂł̔悤ȐɒڂB

Wu

## QOPRN@TQR 16:00--17:30

Fkw wȍWKWOP

u
Norbert Pozar (w w@Ȋw)
A viscosity approach to total variation flows of non-divergence type
v|
In this talk, I will introduce a notion of viscosity solutions for a general class of degenerate nonlinear parabolic problems of non-divergence form in a periodic domain of an arbitrary dimension. The characteristic feature of these problems is their very strong diffusion on the flat parts with a zero gradient, where it in fact becomes a nonlocal quantity. They are often called very singular diffusion equations. This class includes the classical (anisotropic) total variation flow as well as the motion of a graph by a crystalline mean curvature of a particular form. I will discuss a comparison principle, the stability under an approximation by regularized parabolic problems, and an existence theorem for general continuous initial data. These results extend the theory of viscosity solutions for these problems, previously available only in the one-dimensional case, to an arbitrary dimension. This is joint work with Mi-Ho Giga and Yoshikazu Giga.

## j̓Z~i[ QOPRN@TQO 14:00--15:30

Fkw w wQOP

u
ēc OY (Lw w@Hw@)
Asymptotic properties of bifurcation curves for nonlinear eigenvalue problems

Wu

## QOPRN@T@X 16:00--17:30

Fkw wȍWKWOP

u
c (kw w@w)
Optimal Strichartz estimates for rotating incompressible fluids
v|
{uł́C]Wnɂ Coriolis ͂̉el 񈳏k Euler Navier-Stokes ɂčl@D
Coriolis ͂ɂĐ^Qɑ΂āC Strichartz ]̐œKȋe͈͂𓱏oD
̉pƂ Euler ̒ԉ𐫂l@C SɌуGlM[@ɂč\ꂽԋǏC
]x\ꍇɁCCӂ̗L𒴂ĉ\ł邱ƂD
iYoungwoo Koh CSanghyuk Lee Ƃ̋j

## QOPRN@SQT 16:00--17:30

Fkw wȍWKWOP

u
l (kw WPI-AIMR)
xzɈˑÃf̒Pfɂ
v|
qñ}Nȉ^̃fƂėĂꂽxzɉ͂ˑ
ÃflD
ł͓ɒPfɒڂCɂĂ̋̓Iȗ{f
{Ɖ\ɑ΂鐔wIElIȃAv[݂D

## QOPRN@SPW 16:00--17:30

Fkw wȍWKWOP

u
r Ώ (kw w@w)
S`̔S̔r [revisited[
v|
ŚA񔭎U^iމjQKȉ~^̎ƂāA1981NɁAM. G. Crandall P.-L. LionsɂēꂽB