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2014”N11ŒŽ8“úi“yj- 9“úi“új
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ŽžŠÔ | is | u‰‰ŽÒ | u‰‰ƒ^ƒCƒgƒ‹E“à—e iƒXƒ‰ƒCƒhj |
13:00 | Žó•tŠJŽn | êŠF@‚Þ‚·‚т킴ŠÙ 3ŠK 3-B‹³Žº “üŒû | |
13:30-13:45 | ˆ¥ŽA | ‰vì •q‰p@i‰vìmj | |
13:45-13:50 | ˆÄ“à | ŽåÃŽÒ | ƒVƒ“ƒ|ƒWƒEƒ€‚ÉŠÖ‚·‚é˜A—Ž–€@ |
13:50-14:50 | u‰‰ | Â–Ø œÄ–ç@i‹ž‘åŠîŒ¤j | ŠiŽqQCD‚Ìŋ߂Ìi“W |
14:50-15:10 | ‹xŒe | ||
15:10-15:35 | u‰‰ | ‹ãŒã ‘¿ˆê˜Y@i‰vìmj | Massive supergravity |
15:35-16:00 | u‰‰ | “¡ì ˜a’j@i—Œ¤j | Neutrino-antineutrino mass splitting in the Standard Model and baryogenesis |
16:00-16:25 | u‰‰ | ”~’à Œõˆê˜Y@i“ú‘å—Hj | A hidden-variables version of Gisin's theorem |
16:25-16:50 | ‹xŒe | ||
16:50-17:50 | u‰‰ | ’Òì M“ñ@i“Œ‹ž—‰È‘åj | ˆÃ•ƒGƒlƒ‹ƒM[‚ÆC³d—Í—˜_ |
18:00-19:30 | §e‰ï | êŠF@‚Þ‚·‚т킴ŠÙ 1ŠK ƒJƒtƒF uKSUKSUv iŽ–‘O\žŽÒ‚Ì‚Ýj |
11ŒŽ9“úi“új@@‘f—±Žq‚ÆŽž‹ó^Œ»Û‚©‚ç’T‚é‘f—±Žq
ŽžŠÔ | is | u‰‰ŽÒ | u‰‰ƒ^ƒCƒgƒ‹E“à—e iƒXƒ‰ƒCƒhj |
10:00-11:00 | u‰‰ | Œã“¡ ‹œ@iKEKj | B‚Ì•¨—‚ÌŒ»ó‚Æ“W–] |
11:00-11:10 | ‹xŒe | ||
11:10-11:35 | u‰‰ | “ñ•r •Žj@i“ú‘å—Hj | ’´‘Î̈Õ•¨Ž¿‚Ì‘ÎÁ–łɂ¨‚¯‚é“dŽãE§“®•úŽË‚ÌŠñ—^ |
11:35-12:00 | u‰‰ | ™ŽR OW@i‰vìmj | Zero Higgs Doublet Model |
12:05-12:30 | u‰‰ | “nç² “ÄŽj@i‰vìmj | T2KŽÀŒ±‚É‚¨‚¯‚éd‚¢ƒjƒ…[ƒgƒŠƒm’Tõ |
12:30-14:00 | ’‹H | êŠF@‚Þ‚·‚т킴ŠÙ 1ŠK ƒJƒtƒF uKSUKSUv iŽ–‘O\žŽÒ‚Ì‚Ýj | |
14:00-15:00 | u‰‰ | ’·’Jì ‰ë–ç@iKEKj | CMB•ÎŒõŠÏ‘ªŽÀŒ±: POLARBEAR‚ÌÅV‚ÌŒ‹‰Ê‚Æ¡Œã‚Ì“W–] |
15:00-15:20 | ‹xŒe | ||
15:20-15:45 | u‰‰ | ŽO—Ö ŒõŽk@i“ú‘å—Hj | On quantum corrections of a string world sheet for a Wilson loop in the AdS/CFT correspondence |
15:45-16:10 | u‰‰ | ŽÄ ³‘¾˜Y@i‰vìmj | ê‚Ì—˜_‚É‚æ‚éƒuƒ‰ƒbƒNƒuƒŒ[ƒ“‚̉ðÍ‚Æp-soupƒ‚ƒfƒ‹ |
16:10-16:30 | ‹xŒe | ||
16:30-16:55 | u‰‰ | ’r“c Œ›–¾@i‰vìmj | ê‚Ì—˜_AŒ·—˜_‚ÉŒ»‚ê‚éLieˆŸŒQ |
16:55-17:20 | u‰‰ | oŒû ^ˆê@i“ú‘å—Hj | Gauged Twistor Models of Massless and Massive Particles |
17:20-17:45 | u‰‰ | ’‡ Ž •¶@i“ú‘å—Hj | ÕŒ‚”gŒ^”wŒiŽž‹ó‚É‚¨‚¯‚ébi-local–ÍŒ^ |
17:45-17:50 | ˆÄ“à | ŽåÃŽÒ | ƒVƒ“ƒ|ƒWƒEƒ€‚ÉŠÖ‚·‚é˜A—Ž–€ |
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