‘æ‚W‰ñ“ú‘å—HE‰vìm˜AŒgƒVƒ“ƒ|ƒWƒEƒ€
ƒvƒƒOƒ‰ƒ€ (10/25XV)
ƒvƒƒOƒ‰ƒ€iˆóü—pPDFj
11ŒŽ3“úi“yj
ŽžŠÔ | is | u‰‰ŽÒ | u‰‰ƒ^ƒCƒgƒ‹E“à—eiƒXƒ‰ƒCƒhj |
12:30 | Žó•t ŠJŽn |
êŠF‚Þ‚·‚т킴ŠÙ‚QŠKƒz[ƒ‹‘O | |
13:00-13:05 | ˆ¥ŽA | ‰vì •q‰p i‰vìmj |
|
13:05-13:10 | ˆÄ“à | ŽåÃŽÒ | ƒVƒ“ƒ|ƒWƒEƒ€‚ÉŠÖ‚·‚é˜A—Ž–€@ |
13:10-14:10 | u‰‰ | Roger Wendell
i‹ž“s‘åŠwj |
ƒjƒ…[ƒgƒŠƒm‚Æ”½ƒjƒ…[ƒgƒŠƒmU“®FŽÀŒ±“I‚ÈŠÏ“_ |
14:10-14:30 | u‰‰ | ŽR’à ’¼Ž÷ i–kŠC“¹‘åŠwj |
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–{‘åŠwj |
ƒÐƒQ[ƒWƒnƒ~ƒ‹ƒgƒjƒAƒ“‚É‚¨‚¯‚錷‚ÌU“®ƒ‚[ƒh‚ÌŠñ—^‚ɂ‚¢‚Ä |
15:25-15:45 | u‰‰ | ‘¾“c M‹` i‹ß‹E‘åŠwj |
Towards the Determination of the Dimension of Critical Surface |
15:45-16:05 | u‰‰ | ‘å’J ‘ i“ú–{‘åŠwj |
BPS Monopole in the Space of Boundary Conditions |
15:05-16:25 | u‰‰ | ‹e’n Œ’Œá i‰vìmj |
Wess-Zumino–ÍŒ^‚ɑ΂·‚éƒOƒ‰ƒfƒBƒGƒ“ƒgƒtƒ[•û’öŽ® |
16:25-16:40 | ‹xŒe | ||
16:40-17:40 | u‰‰ | ŽR˜e Kˆê i–¼ŒÃ‰®‘åŠwj |
Compositeness within/beyond the Standard Model: A Scale-invariant View, Past and Future |
17:40-18:00 | u‰‰ | “ñ•r •Žj i“ú–{‘åŠwj |
ƒXƒP[ƒ‹•s•Ï‚Èd—Í–ÍŒ^‚ƉF’ˆ˜_ |
18:00-18:20 | u‰‰ | ‹ãŒã ‘¾ˆê i‰vìmj |
^‹óƒGƒlƒ‹ƒM[‚ÌŒvŽZ‰Â”\«‚Æ¢ŠE‚̃XƒP[ƒ‹•s•Ï« |
18:30-20:00 | §e‰ï | êŠF‚Þ‚·‚т킴ŠÙ‚PŠKƒJƒtƒFKSUKSUiŽ–‘O\žŽÒ‚Ì‚Ýj |
11ŒŽ4“úi“új
ŽžŠÔ | is | u‰‰ŽÒ | u‰‰ƒ^ƒCƒgƒ‹E“à—eiƒXƒ‰ƒCƒhj |
9:30-10:30 | u‰‰ | ì’† 鑾 i‹ž“s‘åŠwj |
ÅV‚̉F’ˆüƒXƒyƒNƒgƒ‹‚Æ‚»‚̉F’ˆ•¨—Šw“I‰ðŽß |
10:30-10:50 | u‰‰ | ‹g‰ª ‹»ˆê i‹ž“s‘åŠwj |
TBA |
10:30-10:50 | u‰‰ | •½ŽR ‹M”V i’†•”‘åŠwj |
ƒzƒƒOƒ‰ƒtƒBƒbƒNQCD‚É‚æ‚é’†«Žq¯Šj•¨Ž¿‚Ìó‘Ô•û’öŽ®‚Ì“±o |
11:10-11:30 | ‹xŒe | ||
11:30-11:50 | u‰‰ | 㑺 ®•½ i‰vìmj |
Large Volume Scenario ‚Æ F-term uplifting |
11:50-12:10 | u‰‰ | ]¬ —²”V i“ú–{‘åŠwj |
Moonshine and string theory |
11:50-12:10 | u‰‰ | ¬˜H“c rŽq i“Þ—Ç—Žq‘åŠwj |
Conformal interface in Open string field theory |
12:30-13:50 | ’‹H | @‚¨•Ù“–”z•ziŽ–‘O\žŽÒ‚Ì‚Ýj | |
13:50-14:50 | u‰‰ | Œ“‘º WÆ i‘åã‘åŠwj |
ƒqƒbƒOƒX•¨—‚©‚çV•¨—‚Ö \LHC, ILC‚Æd—Í”g‚Ì‘ŠæŒø‰Ê\ |
14:50-15:10 | u‰‰ | ‘]‰äŒ© ˆè•v i‹ž“sŽY‹Æ‘åŠwj |
“’쑊ŒÝì—p‚ÌŒ´—‚ð‹‚ß‚Ä |
15:10-15:30 | ‹xŒe | ||
15:30-15:50 | u‰‰ | ’‡ Ž •¶ i“ú–{‘åŠwj |
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‘åŠwj |
’´Œ·—˜_‚É‚¨‚¯‚éƒuƒŒ[ƒ“‚ƕό`‚³‚ꂽ’´d—Í—˜_ |
16:10-16:30 | u‰‰ | –Ø‘º “NŽm i“ú–{‘åŠwj |
Semi-doubled GLSM for five-branes of codimension two |
16:30-16:50 | ‹xŒe | ||
16:50-17:10 | u‰‰ | ”~’à Œõˆê˜Y i“ú–{‘åŠwj |
Comment on a classical limit of Grover's algorithm |
17:10-17:30 | u‰‰ | ŠOŽR •¶ i‹ž“sŽY‹Æ‘åŠwj |
ƒQ[ƒgƒ‚ƒfƒ‹—ÊŽqƒRƒ“ƒsƒ…[ƒ^ã‚̎㑪’èŽÀŒ± |
17:30-17:50 | u‰‰ | oŒû ^ˆê i“ú–{‘åŠwj |
C³‚³‚ꂽBateman–ÍŒ^‚ÉŠî‚ÂŒ¸Š’²˜aU“®Žq‚Ì—ÊŽq‰» |
17:50-18:00 | ˆÄ“à | ŽåÃŽÒ | ƒVƒ“ƒ|ƒWƒEƒ€‚ÉŠÖ‚·‚é˜A—Ž–€ |