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98.05.13 | ß·ÅÄ Å¯Íº(ÆüÂç¡¡Íý¹©) | mgnetic monopole¤¬Â¸ºß¤¹¤ë¤È¡¤¤³¤ÎÀ¤³¦¤ÎÉ÷·Ê¤Ï¤É¤¦¤Ê¤ë¤«¡© |
98.05.20 | ½ÐÞ¼ Âî(ÃÞÇÈÂç) | Constructive approach to the massless lattice fermions |
98.06.03 | ¹õÌÚ ·Ð½¨(ÅìÂç¡¡Áí¹çʸ²½) | Master Field on Fuzzy Sphere |
98.06.10 | ÎëÌÚ ·ò»Ê(Å칩Âç¡¡Íý) | Black¡¡Hole entropy as T-duality invariant |
98.06.17 | ³û²¼ ½ß°ì(¤ªÃã¤Î¿åÂç¡¡Íý) | NLC/JLC¤Ë¤ª¤±¤ëĶÂоÎÀÌÏ·¿¤Î¥Ò¥Ã¥°¥¹Î³»Ò¤Î¸½¾ÝÏÀ |
98.07.15 | °ÀÀ¸ÅÄ ·ò°ì(ÆüÂç¡¡Íý¹©) | Berry's Phase and Protective Measurement |
98.09.30 | Ê¡Åç ¾»¹¨¡ÊÂçºåÂç¡¡Íý¡Ë | Monopole Clustering and Color Confinement in the Multi-Instanton System |
98.10.09 | L.H.Ryder(University of Kent) | The Geometric Phase |
98.10.14 | ÃæȪ ²í¹Ô(ÅìÂ籧ÃèÀþ¸¦¡Ë | ¥¹¡¼¥Ñ¡¼¥«¥ß¥ª¥«¥ó¥Ç¤Ë¤è¤ë¥Ë¥å¡¼¥È¥ê¥Î¿¶Æ°¤Îȯ¸« |
98.10.21 | B.P.Mandal(SIoNP,CALCUTTA) | SUPERSPACE FORMULATIONS OF GAUGE THEORIES |
98.10.28 | ÃöÌÚ ·Ä¼£(¿ÀÆàÀîÂç¡¡Íý) | Another Look at ¦Ð¡¼¦ÐScattering in the Scalar Channel and sigma Model¡¡ |
98.11.10 (½ÙÇî²ñ) | Arno Bohm(¥Æ¥¥µ¥¹Âç¡Ë | »þ´ÖÈóÂоΤÊÎÌ»ÒÍýÏÀ |
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98.11.18 | ¤ªµÙ¤ß | |
98.11.25 | ÃæÅç Í£¿Î(ÆüÂç¡¡¸¶¸¦) | Anomalies,branes, and currents¤ÎReview talk |
98.12.02 | ë°æ µÁ¾´(ºë¶ÌÂç¡¡Íý) | Supersymmetry in the AdS/CFT Correspondence |
98.12.09 | ¾®ÅÄ Î´°ì¡ÊÆüÂç¡¡Íý¹©¡Ë | ¥¯¥©¡¼¥¯¡¦È¿¥¯¥©¡¼¥¯Ãæ´Ö»Ò·Ï¤Î¼ÁÎÌ¥¹¥Ú¥¯¥È¥ë¤È¹½Â¤ |
98.12.16 | º´Æ£ Îɹ§¡ÊÆüÂç Íý¹©¡Ë | Bethe-SalpeterÊýÄø¼°¤Î¹½Â¤¤È bi-local·¿ÊýÄø¼°¤Ø¤ÎReduction |
99.01.13 | ¶áÆ£ ·Ä°ì¡ÊÀéÍÕÂç¡¡Íý¡Ë | Topological derivation of quark confinement in QCD |
99.01.20 | ÃæÌî Çî¾Ï¡Ê¿·³ãÂç¡¡Íý¡Ë | Effective Superpotential Approach to Anomalous U(1) Supersymmetry Breaking |
99.01.27 | °ë ¶Ç¡ÊKEK.ÁÇγ»ÒÍýÏÀÉô¡Ë | 1Éô¡¡stringÍýÏÀÆþÌç(ºÇ¾®Ä¹¤µ¤È»þ¶õ¤Î¹½Â¤) 2Éô¡¡Ä¶¸¹ÍýÏÀ¤Î¹½À®ÏÀŪÄêµÁ(¶B¹ÔÎóÌÏ·¿)¤È»þ¶õ¤ÎÀ¸À® |
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99.02.16.17 | ¸¦µæ¼¼Æ⽤ÏÀȯɽ²ñ | |
99.02.24 | ¥³¥¾¥í¥Õ | Introduction to (super) rare decay processes of an extra gauge Z¡Ç boson |
99.03.03,04 | ʪÍý¡¦ÎÌ»ÒÀ칶½¤ÏÀȯɽ²ñ | |
99.03.26 | ºÙë ͵¡¡¡Ê¥ß¥Í¥½¥¿Âç¡Ë | The Hamiltonian-Jacobi Formalism for Strings and p-branes |