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         �������u��̗ʎq�_ 2000�v\\
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         --- ���F����L�O�� �R�K ��u���� ---}
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%%%%%%%%%%%%%%%%%%%%% reviews %%%%%%%%%%%%%%%%%%%%%%
\newcommand{\kato}{%
\talk{�������T}{���呍��}
{�������ƌ����_�i����j$\!\mbox{}^*$}
{50}}

\newcommand{\hayakawa}{%
\talk{�����i}{KEK}
{�����ԏ�̏�̗��_�̐����Ɖ��p�i����j$\!\mbox{}^*$}
{50}}

\newcommand{\takahashi}{%
\talk{�����q�F}{�ޗǏ��q��}
{�^�L�I���Ïk�ƌ��̏�̗��_$\!\mbox{}^*$}
{50}}

\newcommand{\fukuma}{%
\talk{���ԏ���}{�}
{Comments on the Holographic Renormalization Group�i����j$\!\mbox{}^*$}
{50}}

\newcommand{\tachibana}{%
\talk{�k�@��}{�}
{Extra Dimension �̕����i����j$\!\mbox{}^*$}
{50}}

\newcommand{\sugimoto}{%
\talk{���{�Ύ�}{�}
{Non BPS brane �� K ���_�Ɋւ���ŋ߂̔��W�i����j$\!\mbox{}^*$}
{50}}


%%%%%%%%%%%%%%%%%%%%% talks %%%%%%%%%%%%%%%%%%%%%%%%
\newcommand{\murakami}{%
\talk{�������}{���}
{Worldsheet and Spacetime Properties of D$p$-D$p'$ System with
$B$ Field and Noncommutative Geometry}
{20}}

\newcommand{\hashiba}{%
\talk{�H�Ď��Y}{�}
{String Junctions in $B$ Field Background}
{20}}

\newcommand{\skawamoto}{%
\talk{�͖{�ˈ�}{���嗝}
{Open membranes in a constant $C$-field background and
noncommutative boundary strings}
{20}}

\newcommand{\terashima}{%
\talk{��������}{���嗝}
{On the Equivalence between Noncommutative and
Ordinary Gauge Theories}
{20}}

\newcommand{\okawa}{%
\talk{���S�i}{���}
{Constraints on effective Lagrangian of D-branes from
non-commutative gauge theory}
{20}}

\newcommand{\hashimoto}{%
\talk{���{�K�m}{�}
{Non-linear electrodynamics in curved background}
{20}}

\newcommand{\furuta}{%
\talk{�Óc�@��}{������}
{Wess-Zumino-Witten model �̔���Ȋg���Ƃ��̎��O���U�̐���}
{20}}

\newcommand{\moriyama}{%
\talk{�X�R�ĕ�}{���嗝}
{Noncommutative Monopole from Nonlinear Monopole}
{20}}

\newcommand{\goto}{%
\talk{�㓡����}{���嗝}
{Noncommutative Monopole at the Second Order in theta}
{20}}

\newcommand{\asakawa}{%
\talk{���k�F}{���嗝}
{Noncommutative Gauge Theories from Deformation Quantization}
{20}}

\newcommand{\naganuma}{%
\talk{�i����j}{���H��}
{Nonnormalizable Zero Modes on BPS Junctions}
{20}}

\newcommand{\yamashita}{%
\talk{�R���T�V}{�_�ˑ�}
{A simple proof of nonrenormalization for the Chern-Simons
coupling and Seiberg's trick}
{20}}

\newcommand{\uesugi}{%
\talk{�㐙����}{���嗝}
{Boundary State �ƃ^�L�I���Ïk}
{20}}

\newcommand{\nakamura}{%
\talk{�����@�^}{���嗝}
{��ʉ�����Liouville���_�ɂ�����Dirichlet���E����}
{20}}

\newcommand{\naitoh}{%
\talk{��������}{���s��}
{Quantum string field theories of type 2 and heterotic type}
{20}}

\newcommand{\sugiyama}{%
\talk{���R���V}{���呍�l}
{Central Charge of Topological Sigma Model with Calabi-Yau
Target Spaces}
{20}}

\newcommand{\sako}{%
\talk{���Ï��j}{�L����}
{Euler number of Instanton moduli space and Seiberg-Witten
invariants}
{20}}

\newcommand{\masuda}{%
\talk{���c�M�G}{�É���}
{Six dimensional gauge theories and integrable systems}
{20}}

\newcommand{\horata}{%
\talk{���c�T��}{KEK}
{Numerical Analysis of the Double Scaling Limit in the IIB Matrix
Model}
{20}}

\newcommand{\muramatsu}{%
\talk{�����N�s}{���呍��}
{Matrix theory �ɂ����� supersymmetry}
{20}}

\newcommand{\fuji}{%
\talk{���@���V}{���嗝}
{Open String on Symmetric Product}
{20}}

\newcommand{\nitta}{%
\talk{�V�c�@�y}{���H��}
{Auxiliary Field Formulation of Supersymmetric Nonlinear Sigma
Models}
{20}}

\newcommand{\yamamoto}{%
\talk{�R�{��`}{������}
{Three-dimensional nonlinear sigma models with extended
supersymmetry}
{20}}

\newcommand{\onishi}{%
\talk{�吼���F}{�_�ˑ�}
{Novel Phase Structure of Twisted $O(N)$ $\phi^4$ model on
$M^{D-1} \times S^1$}
{20}}

\newcommand{\fujii}{%
\talk{����@��}{���}
{Instantons, Monopoles and the Flux Quantization in the
Faddeev-Niemi Decomposition}
{20}}

\newcommand{\tanimura}{%
\talk{�J���Ȍ�}{����H}
{Dressing field method and Screeing Potential in QCD}
{20}}

\newcommand{\shinohara}{%
\talk{���@�O}{��t��}
{Renormalizable Abelian-projected effective gauge theory derived
from Quantum Chromodynamics}
{20}}

\newcommand{\ogushi}{%
\talk{�����K�q}{������}
{$c$-function from AdS/CFT correspondence}
{20}}

\newcommand{\okuyama}{%
\talk{���R�a��}{KEK}
{Path Integral Approach to String Theory on $AdS_3$}
{20}}

\newcommand{\hikida}{%
\talk{�D�c�׏�}{���嗝}
{$AdS_3$ ��ԏ�̌����_�Ƃ��̎��R��\��}
{20}}

\newcommand{\takayanagi}{%
\talk{�����@��}{���嗝}
{ALE ��Ԃɂ����� String Creation �� Quiver �Q�[�W���_��
Renormalization flow}
{20}}

\newcommand{\yokoi}{%
\talk{���䒼�l}{���}
{Three-Dimensional Extremal Black Holes and the Maldacena
Duality}
{20}}

\newcommand{\nojiri}{%
\talk{��K�L��}{�h�q��}
{Dilatonic Brane World}
{20}}

\newcommand{\hatanaka}{%
\talk{�����v��}{����F������}
{Many-Brane Extension of the Randall-Sundrum Solution}
{20}}

\newcommand{\ohashi}{%
\talk{�勴�\��}{���嗝}
{Supergravity Tensor Calculus in 5D from 6D}
{20}}

\newcommand{\ejiri}{%
\talk{�]�K�M�i}{�}�g��}
{Extra Dimension �������� Yang-Mills ���_�̑��݉\���ɂ���}
{20}}

\newcommand{\nakayama}{%
\talk{���R�m��}{����}
{�i�q��̓d�㗝�_�ɂ�����A�m�}���[���E}
{20}}

\newcommand{\igarashi}{%
\talk{�܏\�� �ޓ�}{�V����}
{���肱�݌Q�ƑΏ̐�}
{20}}

\newcommand{\ichinose}{%
\talk{��m�� �ˈ�}{�É�������}
{Renormalization using Domain Wall Regularization}
{20}}

\newcommand{\ishikawa}{%
\talk{�ΐ쌒�O}{�k��}
{�ʎq�z�[���K�X�̏�̗��_}
{40}}

\newcommand{\maeda}{%
\talk{�O�c�W��}{�k��}
{U(1) Symmetry Breaking in the Quantum Hall System}
{20}}

\newcommand{\nkawamoto}{%
\talk{�͖{�@��}{�k��}
{��ʉ����ꂽ�Q�[�W���_�� Weinberg-Salam �͌^}
{30}}

\newcommand{\kuwano}{%
\talk{�K��׍G}{�鎭��ÉȊw��}
{Difference equations for correlation functions of Belavin's
$Z_n$-symmetric model with boundary reflection}
{20}}

\newcommand{\higuchi}{%
\talk{����O�Y}{���呍��}
{��G���~�[�g�ȓ]���s��ɑ΂��閧�x�s�񂭂肱�݌Q}
{20}}

\newcommand{\abe}{%
\talk{�������Y}{������}
{Perturbative or Path-Integral Approach versus
Operator-Formalism Approach}
{25}}

\newcommand{\shiokawa}{%
\talk{���� ��o��}{�A���o�[�^��}
{���]�X�R�s�b�N�n�Ƃ��Ă̋Ȃ�������Ԃ̏�̗��_�i����j}
{20}}

\newcommand{\hyakutake}{%
\talk{�S���c��}{�}
{Orientifold-plane, non-BPS D-brane and Wilson line in type I
theory}
{20}}

\newcommand{\nozaki}{%
\talk{���^��}{���嗝}
{Gepner ���f���� boundary state �̍\���Ƃ��̉��p}
{20}}



%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{document}

\noindent
\title

\begin{day}{4��}
\begin{session}{�ߑO1}{9:00-10:00}
\kato
\end{session}

\begin{session}{�ߑO2}{10:15-11:30}
\murakami
\hashiba
\skawamoto
\end{session}

\begin{session}{�ߑO3}{11:45-13:00}
\terashima
\okawa
\hashimoto
\end{session}

\lunch

\begin{session}{�ߌ�1}{14:15-15:15}
\hayakawa
\end{session}

\begin{session}{�ߌ�2}{15:45-17:00}
\furuta
\moriyama
\goto
\end{session}

\begin{session}{�ߌ�3}{17:15-18:30}
\asakawa
\fujii
\naganuma
\end{session}
\end{day}
\newpage

\usebox{\headskip}

\begin{day}{5��}
\begin{session}{�ߑO1}{9:30-10:40}
\ishikawa
\maeda
\end{session}

\begin{session}{�ߑO2}{10:55-11:45}
\kuwano
\higuchi
\end{session}

\begin{session}{�ߑO3}{12:00-13:00}
\nkawamoto
\shiokawa
\end{session}

\lunch

\begin{session}{�ߌ�1}{14:15-15:30}
\sako
\masuda
\yamashita
\end{session}

\begin{session}{�ߌ�2}{16:00-17:15}
\sugiyama
\nitta
\yamamoto
\end{session}

\begin{session}{�ߌ�3}{17:30-18:45}
\onishi
\tanimura
\shinohara
\end{session}
\end{day}
\newpage

\usebox{\headskip}

\begin{day}{6��}
\begin{session}{�ߑO1}{9:00-10:00}
\fukuma
\end{session}

\begin{session}{�ߑO2}{10:15-11:30}
\ogushi
\okuyama
\hikida
\end{session}

\begin{session}{�ߑO3}{11:45-13:00}
\takayanagi
\igarashi
\ichinose
\end{session}

\lunch

\begin{session}{�ߌ�1}{14:15-15:15}
\tachibana
\end{session}

\begin{session}{�ߌ�2}{15:45-17:00}
\hatanaka
\ohashi
\nojiri
\end{session}

\begin{session}{�ߌ�3}{17:15-18:30}
\ejiri
\nakayama
\yokoi
\end{session}
\end{day}
\newpage

\usebox{\headskip}

\begin{day}{7��}
\begin{session}{�ߑO1}{9:00-10:00}
\takahashi
\end{session}

\begin{session}{�ߑO2}{10:15-11:30}
\uesugi
\nakamura
\naitoh
\end{session}

\begin{session}{�ߑO3}{11:45-13:00}
\horata
\muramatsu
\fuji
\end{session}

\lunch

\begin{session}{�ߌ�1}{14:15-15:15}
\sugimoto
\end{session}

\begin{session}{�ߌ�2}{15:25-16:15}
\hyakutake
\nozaki
\end{session}
\end{day}

���ʓ��̐����͍u�����ԁi���j�A$*$ ���������̂̓��r���[���܂ލu���ł��B

\end{document}
