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Schedule & History

2010ǯÅÙ 2011ǯÅÙ 2012ǯÅÙ 2013ǯÅÙ 2014ǯÅÙ

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4/8Á´°÷¼«¸Ê¾Ò²ð¥³¥¹¥â¥¹²ñ´Û / 13:30
4/15ÌîÂôµ®Ìé¹âÀÖÊýÊаܥ¯¥§¡¼¥µ¡¼Êì¶ä²ÏÃæ¤ÎÀ±´Ö¥À¥¹¥È¿Ê²½¤È¸º¸÷¶ÊÀþ¥³¥¹¥â¥¹²ñ´Û / 13:30
4/22¸Åß·½ÔÃæÀ­»ÒÀ±¤«¤é¥¹¥È¥ì¥ó¥¸¥¯¥©¡¼¥¯À±¤Ø¤Îdz¾Æ²áÄø¥³¥¹¥â¥¹²ñ´Û / 13:30
5/13Ä«ÈæÆàͺÂÀWesterlund 2À±ÃÄÊý¸þ¤Îʬ»Ò±À·ÁÀ®¥·¥ß¥å¥ì¡¼¥·¥ç¥ó¥³¥¹¥â¥¹²ñ´Û / 13:30
5/13ÁÄ븵ÃæÀ­»ÒÀ±¥¯¥é¥¹¥È¿¶Æ°¤ÈÅŻҼ×Êøú²Ì¥³¥¹¥â¥¹²ñ´Û / 14:10
5/20ÏÆÅÄÌ趻ÏÏÇÀ±·Ï±ßÈ×Æâ¤Î»ÀÁÇƱ°ÌÂÎÁÈÀ®Ê¬ÉÛ¥³¥¹¥â¥¹²ñ´Û / 13:30
5/27Æ£°æÄÌ»ÒÀ±ÃĤΥХꥨ¡¼¥·¥ç¥ó¤Îµ¯¸»¥³¥¹¥â¥¹²ñ´Û / 13:30
6/3¡Ê¤ªµÙ¤ß¡ËÂè3²óDTA¥·¥ó¥Ý¥¸¥¦¥à³«ºÅ¤Î¤¿¤á
6/10¡Ê¤ªµÙ¤ß¡Ë¥í¥ó¥°¥³¥í¥­¥¦¥à¤ò£²¤Ä³«ºÅ¤¹¤ë¤¿¤á
6/17¡Ê¤ªµÙ¤ß¡Ë¥í¥ó¥°¥³¥í¥­¥¦¥à¤ò£²¤Ä³«ºÅ¤¹¤ë¤¿¤á
6/24¡Ê¤ªµÙ¤ß¡Ë±§Ãè³ËʪÍý¥·¥ó¥Ý¥¸¥¦¥à³«ºÅ¤Î¤¿¤á
7/1¡Ê¤ªµÙ¤ß¡ËStar Formation Workshop³«ºÅ¤Î¤¿¤á
7/8ÉÍ̾¿ò½ÅÎÏ¥ì¥ó¥º¶ä²ÏÃķ׬¤Ë¤è¤ë±§ÃèÏÀ¥Ñ¥é¥á¡¼¥¿¡¼¿äÄꥳ¥¹¥â¥¹²ñ´Û / 13:30
7/15°ë¹¾ËãΤExoplanetary System Dynamics: Multiplicity and Planetary Mass Effects¥³¥¹¥â¥¹²ñ´Û / 13:30
7/22¹â¶¶ÇîÇ·¥Ö¥é¥Ã¥¯¥Û¡¼¥ë¶á˵¤Ç¤Î¹â²¹¥¬¥¹±À·ÁÀ®¥³¥¹¥â¥¹²ñ´Û / 13:30
10/07(no talk)
10/14(no talk)(two long-colloquium talks)
10/21Masaomi TanakaExploring Short-Timescale Transients in the UniverseConference Room, Cosmos Lodge / 13:30
10/28(no talk)(workshop of theoretical astronomy)
11/04Hiroshi KobayashiRadiation-MHD Simulation of Clumpy Outflow from Supercritical Accretion Flowlecture room / 13:30
11/11(no talk)(intensive lucture by Prof. Kotake)
11/18Shoichi OshinoTerrestrial Planet Formation around Low-Mass Stars: Effect of the Mass of Central StarsConference Room, Cosmos Lodge / 13:30
11/25Tsunehiko Katolecture room / 13:30

Abstract

4/15¡¡ÌîÂôµ®Ìé(ÍýÏÀÉô)¡¡¹âÀÖÊýÊаܥ¯¥§¡¼¥µ¡¼Êì¶ä²Ï¤ÎÀ±´Ö¥À¥¹¥È¿Ê²½¤È¸º¸÷¶ÊÀþ
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4/22¡¡¸Åß·½Ô(CfCA)¡¡ÃæÀ­»ÒÀ±¤«¤é¥¹¥È¥ì¥ó¥¸¥¯¥©¡¼¥¯À±¤Ø¤Îdz¾Æ²áÄø
Ķ¿·À±Çúȯ¸å¤Ë·ÁÀ®¤µ¤ì¤ëÃæÀ­»ÒÀ±¤Ï¡¢¥¹¥È¥ì¥ó¥¸¥¯¥©¡¼¥¯À±¤Ëž´¹¤¹¤ë²ÄǽÀ­¤¬¤¢¤ê¡¢²òÊü¤µ¤ì¤ë¥Ë¥å¡¼¥È¥ê¥Î¤¬´Ñ¬²Äǽ¤Ç¤¢¤ë¤³¤È¤â´üÂÔ¤µ¤ì¤Æ¤¤¤ë¡£²æ¡¹¤Ï¡¢£±¼¡¸µÄê¾ïή¤Ë¤ª¤±¤ë¥Ï¥É¥í¥ó¥Þ¥¿¡¼¤«¤é¥¹¥È¥ì¥ó¥¸¥¯¥©¡¼¥¯¥Þ¥¿¡¼¤Ø¤Îž´¹¤Î²áÄø¤ò¡¢¾ÜºÙ¤ËÄ´¤Ù¤¿¡£Ëֱܹé¤Ç¤ÏÉÔÄêÀ­¤Î¿¤¤¥¯¥©¡¼¥¯Êª¼Á¤Î¾õÂÖÊýÄø¼°¤ä½é´ü¤ÎÌ©Å٤ʤɤ¬¡¢Å¾´¹²áÄø¤Ë Í¿¤¨¤ë±Æ¶Á¤Ë¤Ä¤¤¤ÆµÄÏÀ¤¹¤ë¡£
5/13¡¡Ä«ÈæÆàͺÂÀ(CfCA)¡¡Westerlund 2À±ÃÄÊý¸þ¤Îʬ»Ò±À·ÁÀ®¥·¥ß¥å¥ì¡¼¥·¥ç¥ó
Westerlund 2À±ÃÄÊý¸þ¤ËľÀþ¾õ¤Ë±ä¤Ó¤¿Ê¬»Ò±À¤È±ß¸Ì¾õ¤Îʬ»Ò±À¤¬´Ñ¬¤µ¤ì¤Æ¤ª¤ê¡¢¤½¤ì¤é¤Îʬ»Ò±À¤Î´Ö¤Ë¤ÏTeV¦ÃÀþ¸»¤¬Â¸ºß¤·¤Æ¤¤¤ë¡£²æ¡¹¤Ï¤³¤ì¤é¤Îʬ»Ò±À¤¬¥¸¥§¥Ã¥È¤ÈÀ±´ÖÃæÀ­¿åÁÇ¥¬¥¹¤ÎÁê¸ßºîÍѤˤè¤Ã¤Æ·ÁÀ®¤µ¤ì¤Æ¤¤¤ë¤Î¤Ç¤Ï¤Ê¤¤¤«¤È¹Í¤¨¡¢¥¸¥§¥Ã¥È¤ÈÀ±´Ö¥¬¥¹Áê¸ßºîÍÑ¥·¥ß¥å¥ì¡¼¥·¥ç¥ó¤ò¼Â»Ü¤·¤¿¡£¤Þ¤¿¡¢Ê¬»Ò±À·Á¾õ¤Î°ã¤¤¤ÏÀ±´Ö¥¬¥¹¤ÎÌ©ÅÙʬÉۤΰ㤤¤¬¸¶°ø¤Ç¤¢¤ë¤È¹Í¤¨¡¢ÃæÀ­¿åÁÇ¥¬¥¹¤Î¥Ü¥ê¥å¡¼¥à¥Õ¥£¥ê¥ó¥°¥Õ¥¡¥¯¥¿¡¼¤òÊѲ½¤µ¤»¤¿·×»»¤ò¹Ô¤Ã¤¿¡£¥Õ¥£¥ê¥ó¥°¥Õ¥¡¥¯¥¿¡¼¤¬¾®¤µ¤¤¾ì¹ç¤Ë¤Ï¥¸¥§¥Ã¥È¤ÏÃæÀ­¿åÁÇ¥¬¥¹¤Î´Ö¤òÅÁÇŤǤ­¤ë¤Î¤Çʬ»Ò±À¤Ï¹­¤¬¤Ã¤¿¹½Â¤¤Ë¤Ê¤Ã¤¿¡£¥Õ¥£¥ê¥ó¥°¥Õ¥¡¥¯¥¿¡¼¤¬Â礭¤¤¾ì¹ç¤Ë¤Ï¥¸¥§¥Ã¥È¤ÏÃæÀ­¿åÁÇ¥¬¥¹¤òÁݤ­½¸¤áʬ»Ò±À¤Î·Á¾õ¤Ï±ß¸Ì¾õ¤Ë¶á¤Å¤¯¤³¤È¤ò¼¨¤·¤¿¡£
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7/15¡¡°ë¹¾ËãΤ(ÅìµþÂç/ÍýÏÀÉô)¡¡Exoplanetary System Dynamics: Multiplicity and Planetary Mass Effects
¶áǯ¤Î·Ï³°ÏÇÀ±Ãµºº¤Î´Ñ¬µ»½Ñ¤Î¸þ¾å¤Ëȼ¤¤¡¢Ê£¿ô¤ÎÏÇÀ±¤«¤é¤Ê¤ëÏÇÀ±·Ï¤¬Â¿¿ôȯ¸«¤µ¤ì¤Æ¤¤¤ë¡£Ëܸ¦µæ¤Ç¤Ï¡¢2014ǯ12·î¤Þ¤Ç¤Ë»ëÀþ®ÅÙË¡¤Ë¤è¤Ã¤Æ´Ñ¬¤µ¤ì¤¿375·Ï500¸Ä¤ÎÏÇÀ±¤È¡¢¥±¥×¥é¡¼Ë¾±ó¶À¤Ë¤è¤Ã¤Æȯ¸«¤µ¤ì¤¿Ê£¿ôÏÇÀ±·Ï¤Î365·Ï899ÏÇÀ±(´Þ¤àÏÇÀ±¸õÊäÅ·ÂÎ)¤òÍѤ¤¡¢ÏÇÀ±¿ô¤äÏÇÀ±¼ÁÎ̤ÈÏÇÀ±·Ï¤ÎÎϳع½Â¤¤Î´Ø·¸¤òÅý·×Ū¤ËÌÀ¤é¤«¤Ë¤¹¤ë¤³¤È¤Ç¡¢ÏÇÀ±·Ï·ÁÀ®¡¦¿Ê²½¥â¥Ç¥ë¤Ø¤Î¿·¤¿¤ÊÀ©¸Â¤Î²ÄǽÀ­¤òõ¤ë¡£ÏÇÀ±·Ï¤Ï¡¢·Ï¤ÎÏÇÀ±¿ô¡¢Ãæ¿´À±¤Î¼ÁÎ̤ǵ¬³Ê²½¤·¤¿ÏÇÀ±¼ÁÎÌ¡¢Ãæ¿´À±¤Î¿Ê²½Ãʳ¬¤Î3¸Ä¤Î¥Ñ¥é¥á¡¼¥¿¤ÇʬÎष¡¢¤½¤ì¤¾¤ì¤ÎÏÇÀ±·Ï¤Î¹½Â¤¤òÅý·×Ū¤ËÄ´¤Ù¤¿¡£º£²ó¤ÏÆäËÏÇÀ±·Ï¤Î³Ñ±¿Æ°ÎÌ·ç»(AMD)¤È¥Ò¥ëȾ·Â¤Çµ¬³Ê²½¤·¤¿ÎÙÀÜÏÇÀ±´Öµ°Æ»´Ö³Ö¤ËÃíÌܤ·¤¿¡£¤½¤Î·ë²Ì¡¢·Ï¤ÎAMD¤ÏÏÇÀ±¿ô¤ÎÁý²Ã¤Ëȼ¤¤¸º¾¯¤¹¤ë¤³¤È¤¬¤ï¤«¤Ã¤¿¡£¤³¤ì¤Ï·ÏÆâ¤ÎÏÇÀ±¤¬Â¿¤¯¤Ê¤ë¤Û¤É¡¢·Ï¤¬°ÂÄê¤Ç¤¢¤ë¤¿¤á¤Ë¤Ï¤½¤ì¤¾¤ì¤ÎÏÇÀ±¤Îµ°Æ»¤¬±ßµ°Æ»¤Ë¶á¤¯¤Ê¤±¤ì¤Ð¤Ê¤é¤Ê¤¤¤³¤È¤ò°ÕÌ£¤¹¤ë¡£¤Þ¤¿¡¢Âç¼ÁÎÌÏÇÀ±¤È¾®¼ÁÎÌÏÇÀ±¤Îµ°Æ»Î¥¿´Î¨¤ÎʬÉۤϰۤʤ뤳¤È¤¬¤ï¤«¤Ã¤¿¡£ÆäË0.4¤è¤êÂ礭¤¤µ°Æ»Î¥¿´Î¨¤ÏÂç¼ÁÎÌÏÇÀ±·Ï¤Ë¤Î¤ß¸ºß¤¹¤ë¡£¹¹¤Ë¡¢¼ç·ÏÎóÀ±¼þ¤ê¤Î¾®¼ÁÎÌÏÇÀ±·Ï¤Ç¤Ï¡¢µ°Æ»´Ö³Ö¤¬15-30¤ÎÈϰϤÇÏÇÀ±¿ô¤È¤Î´Ö¤Ë¤Ù¤­¾è¤ÎÈ¿Áê´ØÀ­¤¬¤¢¤ë¤³¤È¤¬³Îǧ¤µ¤ì¤¿¡£¤Þ¤¿¡¢Ãæ¿´À±¤Î¿Ê²½¤¬¿Ê¤à¤Ë¤Ä¤ì¡¢µ°Æ»´Ö³Ö¤¬¶¹¤¯¤Ê¤ë·¹¸þ¤¬¤¢¤ë¡£Ê£¿ôÏÇÀ±·Ï¤ÎÎϳØŪ¹½Â¤¤ÎÅý·×ŪÀ­¼Á¤Ë¤Ä¤¤¤Æ¤Þ¤È¤á¡¢¤½¤Î·ÁÀ®ÏÀŪ¤Ê°ÕÌ£¤Ë¤Ä¤¤¤ÆµÄÏÀ¤¹¤ë¡£
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10/21¡¡Masaomi Tanaka(DTA)¡¡Exploring Short-Timescale Transients in the Universe
The transient sky has been intensively explored by various surveys in the last decade. One of the important discovery spaces for time-domain astronomy is phenomena with a short timescale, ~< 1 day. To explore this frontier, we have recently started a high-cadence transient survey with Subaru telescope. We have discovered five transients showing the rising timescale shorter than 1 day. We find that the event rate of such transients is not negligible compared with supernova rate. In this talk, I will discuss the nature of these short-timescale transients and their implications.
11/4¡¡Hiroshi Kobayashi(SOKENDAI/DTA)¡¡Radiation-MHD Simulation of Clumpy Outflow from Supercritical Accretion Flow
Clumpy-shaped outflows from supercritical accretion around a stellar mass black hole are reproduced by a global Radiation-MHD simulation (Takeuchi et al. 2013). However, 2D axis symmetry is assumed in the simulations. Hence, we need to confirm the clumpy structure by 3D simulations. In this talk, I will introduce progress report toward achieving this goal.
11/18¡¡Shoichi Oshino(CfCA)¡¡Terrestrial Planet Formation around Low-Mass Stars: Effect of the Mass of Central Stars
The Kepler space telescope has detected several thousand planets and candidates. Their central stars are mainly FGK-type stars. It is difficult to observe M-stars by using visible light since M-stars have their peak radiation in the infrared region. However, recently there are several survey projects for planets around M-stars such as the InfraRed Doppler (IRD) survey of the Subaru telescope. Therefore it is expected that the number of planets around M-stars will increase in the near future. The habitable zone of M-stars is closer to the stars than that of G-stars. For this reason, the possibility of finding habitable planets is expected to be higher. Here we study the formation of close-in terrestrial planets by giant impacts of protoplanets around low-mass stars by using N-body simulations. An important parameter that controls formation processes is the ratio between the physical radius of a planet and its Hill radius, which decreases with the stellar mass. We systematically change the mass of the central stars and investigate its effects on terrestrial planet formation. We find that the mass of the maximum planet decreases with the mass of central stars, while the number of planets in the system increases. We also find that the orbital separation of adjacent planets normalized by their Hill radius increases with the stellar mass.