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11ŒŽ3“ú�i“y�j
| ŽžŠÔ | �i�s | �u‰‰ŽÒ | �u‰‰ƒ^ƒCƒgƒ‹�E“à—e�iƒXƒ‰ƒCƒh�j |
| 12:30 | Žó•t ŠJŽn |
�ê�Š�F‚Þ‚·‚т킴ŠÙ‚QŠKƒz�[ƒ‹‘O | |
| 13:00-13:05 | ˆ¥ŽA | ‰v�ì •q‰p �i‰v�ì�m�j |
|
| 13:05-13:10 | ˆÄ“à | Žå�ÃŽÒ | ƒVƒ“ƒ|ƒWƒEƒ€‚ÉŠÖ‚·‚é˜A—�Ž–�€�@ |
| 13:10-14:10 | �u‰‰ | Roger Wendell
�i‹ž“s‘åŠw�j |
ƒjƒ…�[ƒgƒŠƒm‚Æ”½ƒjƒ…�[ƒgƒŠƒm�U“®�FŽÀŒ±“I‚ÈŠÏ“_ |
| 14:10-14:30 | �u‰‰ | ŽR’à ’¼Ž÷ �i–kŠC“¹‘åŠw�j |
Family Unification in Special Grand Unification |
| 14:30-14:50 | �u‰‰ | “¡�ì ˜a’j �i—�Œ¤�j |
Generalized Pauli-Gursey transformation and Majorana neutrinos |
| 14:50-15:05 | ‹xŒe | ||
| 15:05-15:25 | �u‰‰ | ŽO—Ö ŒõŽk �i“ú–{‘åŠw�j |
ƒÐƒQ�[ƒWƒnƒ~ƒ‹ƒgƒjƒAƒ“‚É‚¨‚¯‚錷‚Ì�U“®ƒ‚�[ƒh‚ÌŠñ—^‚ɂ‚¢‚Ä |
| 15:25-15:45 | �u‰‰ | ‘¾“c �M‹` �i‹ß‹E‘åŠw�j |
Towards the Determination of the Dimension of Critical Surface |
| 15:45-16:05 | �u‰‰ | ‘å’J ‘� �i“ú–{‘åŠw�j |
BPS Monopole in the Space of Boundary Conditions |
| 15:05-16:25 | �u‰‰ | ‹e’n Œ’Œá �i‰v�ì�m�j |
Wess-Zumino–ÍŒ^‚ɑ΂·‚éƒOƒ‰ƒfƒBƒGƒ“ƒgƒtƒ��[•û’öŽ® |
| 16:25-16:40 | ‹xŒe | ||
| 16:40-17:40 | �u‰‰ | ŽR˜e �Kˆê �i–¼ŒÃ‰®‘åŠw�j |
Compositeness within/beyond the Standard Model: A Scale-invariant View, Past and Future |
| 17:40-18:00 | �u‰‰ | “ñ•r •�Žj �i“ú–{‘åŠw�j |
ƒXƒP�[ƒ‹•s•Ï‚È�d—Í–ÍŒ^‚ƉF’ˆ˜_ |
| 18:00-18:20 | �u‰‰ | ‹ãŒã ‘¾ˆê �i‰v�ì�m�j |
�^‹óƒGƒlƒ‹ƒM�[‚ÌŒvŽZ‰Â”\�«‚Æ�¢ŠE‚̃XƒP�[ƒ‹•s•Ï�« |
| 18:30-20:00 | �§�e‰ï | �ê�Š�F‚Þ‚·‚т킴ŠÙ‚PŠKƒJƒtƒFKSUKSU�iŽ–‘O�\�žŽÒ‚Ì‚Ý�j |
11ŒŽ4“ú�i“ú�j
| ŽžŠÔ | �i�s | �u‰‰ŽÒ | �u‰‰ƒ^ƒCƒgƒ‹�E“à—e�iƒXƒ‰ƒCƒh�j |
| 9:30-10:30 | �u‰‰ | �ì’† �鑾 �i‹ž“s‘åŠw�j |
�Å�V‚̉F’ˆ�üƒXƒyƒNƒgƒ‹‚Æ‚»‚̉F’ˆ•¨—�Šw“I‰ðŽß |
| 10:30-10:50 | �u‰‰ | ‹g‰ª ‹»ˆê �i‹ž“s‘åŠw�j |
TBA |
| 10:30-10:50 | �u‰‰ | •½ŽR ‹M”V �i’†•”‘åŠw�j |
ƒzƒ�ƒOƒ‰ƒtƒBƒbƒNQCD‚É‚æ‚é’†�«Žq�¯Šj•¨Ž¿‚Ì�ó‘Ô•û’öŽ®‚Ì“±�o |
| 11:10-11:30 | ‹xŒe | ||
| 11:30-11:50 | �u‰‰ | �㑺 �®•½ �i‰v�ì�m�j |
Large Volume Scenario ‚Æ F-term uplifting |
| 11:50-12:10 | �u‰‰ | �]�¬ —²”V �i“ú–{‘åŠw�j |
Moonshine and string theory |
| 11:50-12:10 | �u‰‰ | �¬˜H“c �rŽq �i“Þ—Ç�—Žq‘åŠw�j |
Conformal interface in Open string field theory |
| 12:30-13:50 | ’‹�H | �@‚¨•Ù“–”z•z�iŽ–‘O�\�žŽÒ‚Ì‚Ý�j | |
| 13:50-14:50 | �u‰‰ | Œ“‘º �W�Æ �i‘å�ã‘åŠw�j |
ƒqƒbƒOƒX•¨—�‚©‚ç�V•¨—�‚Ö �\LHC, ILC‚Æ�d—Í”g‚Ì‘Š�æŒø‰Ê�\ |
| 14:50-15:10 | �u‰‰ | ‘]‰äŒ© ˆè•v �i‹ž“sŽY‹Æ‘åŠw�j |
“’�쑊ŒÝ�ì—p‚ÌŒ´—�‚ð‹�‚ß‚Ä |
| 15:10-15:30 | ‹xŒe | ||
| 15:30-15:50 | �u‰‰ | ’‡ Ž •¶ �i“ú–{‘åŠw�j |
Domain Type of Field Equation in AdS5 Spacetime and Related Problem |
| 15:50-16:10 | �u‰‰ | Žð’J —Y•ô �i‹ž“s•{—§ˆã‰È‘åŠw�j |
’´Œ·—�˜_‚É‚¨‚¯‚éƒuƒŒ�[ƒ“‚ƕό`‚³‚ꂽ’´�d—Í—�˜_ |
| 16:10-16:30 | �u‰‰ | –Ø‘º “NŽm �i“ú–{‘åŠw�j |
Semi-doubled GLSM for five-branes of codimension two |
| 16:30-16:50 | ‹xŒe | ||
| 16:50-17:10 | �u‰‰ | ”~’à Œõˆê˜Y �i“ú–{‘åŠw�j |
Comment on a classical limit of Grover's algorithm |
| 17:10-17:30 | �u‰‰ | ŠOŽR �•¶ �i‹ž“sŽY‹Æ‘åŠw�j |
ƒQ�[ƒgƒ‚ƒfƒ‹—ÊŽqƒRƒ“ƒsƒ…�[ƒ^�ã‚̎㑪’èŽÀŒ± |
| 17:30-17:50 | �u‰‰ | �oŒû �^ˆê �i“ú–{‘åŠw�j |
�C�³‚³‚ꂽBateman–ÍŒ^‚ÉŠî‚ÂŒ¸�Š’²˜a�U“®Žq‚Ì—ÊŽq‰» |
| 17:50-18:00 | ˆÄ“à | Žå�ÃŽÒ | ƒVƒ“ƒ|ƒWƒEƒ€‚ÉŠÖ‚·‚é˜A—�Ž–�€ |