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Download : 02293-01-2007-TRM-13-K.doc ( size : 1.72M ) ( Download : 1 ) ¹®¼­ °¡°Ý : 5,000 ¿ø
ÆäÀÌÁö ¼ö : 13     ¹®¼­ Á¾·ù : Research     ¾ð¾î : ÇÑ±Û     ÃâÆÇ³â : 2007
02293-12-2007-TRM-13-K [KAISTÀÇ ½Å¼ºÃ¶ ±³¼ö¿Í ·ù±¤¼ö ¹Ú»ç, ¼¼°è ¹°¸®Çаè 20³â ¼÷Á¦ÀÎ '°°Àº Â÷¿øÀÇ ÀÚ¼ºÃ¼¿¡¼­ °ÅµìÁ¦°ö¹ýÄ¢(power law) ºÐÆ÷Áö¼ö°¡ ¿Ö ´Ù¾çÇÑ °ªÀ» °®´ÂÁö'ÀÇ ÀÚ±¸º® ±¸Á¶ÀÇ °ÅµìÁ¦°ö¹ýÄ¢ ¿µÇâÀ» ±Ô¸í, ³×ÀÌó ÇÇÁ÷½º'(Nature Physics)ÀÇ 2007³â 7¿ù 15ÀÏÀÚ ÀÎÅÍ³ÝÆÇ(Advance online publication, AOP)¿¡ "°­ÀÚ¼º Çʸ§ÀÇ ¹ÚÅ©ÇÏ¿ìÁ¨ ÀӰ輺¿¡¼­ °üÂûµÈ Á¶Á¤ °¡´ÉÇÑ ºÐÆ÷Áö¼ö º¯È­ ¹ß°ß(Tunable scaling behaviour observed in Barkhausen criticality of a ferromagnetic film)"¶ó´Â ³í¹®À¸·Î °ÔÀçµÇ, ¹ÚÅ©ÇÏ¿ìÁ¨ ÀӰ輺ÀÇ ºÐÆ÷Áö¼ö´Â Â÷¿øÀÌ ¾Æ´Ï¶ó ´Ù¾çÇÑ ¿Âµµ º¯È­¿¡ ÀÇÇØ ÀÚ±¸ Á¡ÇÁ º¯È­°¡ ÀϾ, ½ºÇÉÆ®·Î´Ð½º ¹× ³ª³ë½ºÇɴнº ±â¼ú ±¸Çö½Ã Àå¾Ö°¡ µÇ´Â ¹ÚÅ©ÇÏ¿ìÁ¨ ÀâÀ½Çö»óÀ» Á¤È®È÷ ÀÌÇØÇϴµ¥ Å©°Ô ±â¿©(Barkhausen criticality. Scaling behaviour - as observed in avalanches - reveals universal behaviour dictated by the dimensionality of the system. For domain-wall motion in a ferromagnet, however, the criticality can cross over from one universality class to another depending on the temperature(24/Jul/2007)]

¿À´ÃÀÇ ÁÖÁ¦´Â ¹ÝµµÃ¼ÀÇ ÀüÇϸ¦ ÀÌ¿ëÇÑ ÀüÇÏ¿£Áö´Ï¾î¸µ½Ã´ë¿¡¼­ ¾ÕÀ¸·Î´Â ÀÚ¼ºÃ¼ÀÇ ½ºÇÉÀ» ÀÌ¿ëÇÏ´Â ½ºÇÉ¿£Áö´Ï¾î¸µ½Ã´ë¸¦ ¿­¾î°¡´Â ÀÚ¼ºÃ¼ÀÇ ¹ÚÅ©ÇÏ¿ìÁ¨ È¿°ú(¶Ç´Â ÀâÀ½È¿°ú ¶Ç´Â ÀӰ輺 ¶Ç´Â Á¡ÇÁ)¿Í À̸¦ ³ªÅ¸³»´Â °ÅµìÁ¦°ö¹ýÄ¢ ¹× ±× ºÐÆ÷Áö¼öÀÇ º¯È­¿¡ °üÇÑ ³»¿ëÀ¸·Î,
KAIST(Çѱ¹°úÇбâ¼ú¿ø)°¡ 2007³â 7¿ù 16ÀÏ ÀÌ ´ëÇÐ ¹°¸®Çаú ½ºÇÉÁ¤º¸¹°Áú ¿¬±¸½ÇÀÇ ½Å¼ºÃ¶(ãéà÷ôÍ.55) ±³¼ö¿Í ·ù±¤¼ö(׳ÎÃâª.30) ¹Ú»çÆÀÀÌ ÀÚ±¸º® ¹Ì¼¼±¸Á¶ º¯È­°¡ °ÅµìÁ¦°ö¹ýÄ¢¿¡ ¹ÌÄ¡´Â ¿µÇâÀ» ¼¼°è ÃÖÃÊ·Î ±Ô¸íÇß´Ù°í ¹àÈù ³»¿ëÀ» ¼Ò°³ÇÑ´Ù. ÀüÀÚ±âÇеµ ¾î·Á¿îµ¥ ÀÚ±âÇÐÀÇ ÀÚ¼ºÃ¼ ³»ÀÇ N±Ø°ú S±ØÀÌ ºÒ±ÔÄ¢ÀûÀ¸·Î º¯È­ÇÏ´Â ÀÌÀ¯¿¡ ´ëÇÑ ³»¿ëÀ¸·Î ÀÌÇØÇϱⰡ ¸Å¿ì ¾î·Á¿î °í³­À̵µÀÇ ³»¿ëÀ¸·Î ÇÊ¿äÇÑ ±â¼úÀûÀÎ ³»¿ëµéÀº <½ºÇÉÁ¤º¸¹°Áú ¿¬±¸½Ç> ȨÆäÀÌÁö¿¡ ¿Ã·ÁÁø ³»¿ëµéÀ» ¹ÙÅÁÀ¸·Î ¼Ò°³ÇϰíÀÚ ÇÑ´Ù.

ÀÌ ¿¬±¸ °á°ú´Â ¼¼°èÀû ÇмúÁöÀÎ '³×ÀÌó ÇÇÁ÷½º'(Nature Physics)ÀÇ 2007³â 7¿ù 15ÀÏÀÚ ÀÎÅÍ³ÝÆÇ(Advance online publication, AOP)¿¡ "°­ÀÚ¼º Çʸ§ÀÇ ¹ÚÅ©ÇÏ¿ìÁ¨ ÀӰ輺¿¡¼­ °üÂûµÈ Á¶Á¤ °¡´ÉÇÑ ºÐÆ÷Áö¼ö º¯È­ ¹ß°ß(Tunable scaling behaviour observed in Barkhausen criticality of a ferromagnetic film)"¶ó´Â ³í¹®À¸·Î °ÔÀçµÇ¾ú´Ù(³í¹® ´Ù¿î·Îµå-02293-02-2007-TRM-04-K.PDF)
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[¸ñÂ÷]

1. ½ºÇÉÆ®·Î´Ð½º(Spintronics)¶õ?
2. ³ª³ë½ºÇɴнº(Nanospinics)¶õ?
3. °ÅµìÁ¦°ö¹ýÄ¢(Power law)À̶õ? º¹ÀâÇÑ Çö»óÀ» °¡·ÎÁö¸£´Â °Å½ÃÀû Áú¼­
4. ¿Âµµ¿¡ µû¸¥ ¹ÚÅ©ÇÏ¿ìÁ¨ ÀâÀ½Çö»ó(Barkhausen avalanche or effect or noise)ÀÇ ¿ø¸®¸¦ ¹àÇô
5. ³í¹® ¿ä¾à
6. ±¤ÀÚ±â Çö¹Ì°æÀ̶õ?
7. Criticality(ÀӰ輺, °íºñ¼º)
8. ¸Þ¸ð¸®ÀÇ Á¾·ù(02250)
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1. ½ºÇÉÆ®·Î´Ð½º(Spintronics)¶õ?(½ºÇÉÁ¤º¸¹°Áú ¿¬±¸½Ç ȨÆäÀÌÁö ÂüÁ¶)

4000 ¿©³â Àü ÀÚö±¤ÀÌ Ã³À½ ¹ß°ßµÈ ÀÌÈÄ, ÀÚ¼ºÃ¼´Â ½ÅÀÌ Àΰ£¿¡°Ô Çã¶ôÇÑ ¹®¸í À̱âÀÇ Çٽɹ°Áú Áß Çϳª·Î¼­ ³ªÄ§¹Ý, ÀÚ¼®, ¸ðÅÍ»Ó ¾Æ´Ï¶ó, À½Çâ±â±âÀÇ ½ºÇÇÄ¿³ª Åë½Å±â±âÀÇ ¼Û¼öÈ­±âÀÇ À½ÆÄ¹ß»ý¿øÀ¸·Î, ÀÚµ¿Â÷¿Í Ç×°ø±âÀÇ ¼Óµµ, °¡¼Óµµ, ȸÀü ¹× ÅäÅ© µîÀÇ ¼¾¼­¹°Áú·Î, ÀÚ±â°ø¸í¿µ»óÀåÄ¡(MRI) µî ÷´Ü ÀÇ·á±â±â ¹°Áú·Î, ÄÄÇ»ÅÍ Çϵåµð½ºÅ©³ª ½Å¿ëÄ«µåÀÇ Á¤º¸ÀúÀå¹°Áú·Î, »ý»ê°øÁ¤ ºÐ¾ßÀÇ °¨Áö¼¾¼­ ¹°Áú µî ½Ç·Î ±¤¹üÀ§ÇÑ ºÐ¾ß¿¡ ÀÀ¿ëµÇ¾î ¿Ô°í, ¶ÇÇÑ Àΰ£À» ºñ·ÔÇÑ Æ÷À¯µ¿¹°ÀÇ ½ÅÁø´ë»ç¿¡ ¾ø¾î¼­´Â ¾ÈµÉ Æä¸®Æ¾(ferritin - ö°ú ¾ÆÆ÷Æä¸®Æ¾ÀÇ º¹ÇÕ¹°·Î ÀϹÝÀûÀ¸·Î À§Àå Á¡¸·, °£, ºñÀå, °ñ¼ö¿¡ ¼Ò·® Á¸ÀçÇÑ´Ù)°ú °°Àº »ýü ´Ü¹éÁú ¹°ÁúÀ̱⵵ ÇÏ´Ù.

±×·¯³ª ÀÚ¼ºÃ¼ÀÇ ¿À·£ ¿ª»ç¿Í ±¤¹üÀ§ÇÑ ÀÀ¿ë¿¡µµ ºÒ±¸Çϰí ÀÚ¼ºÃ¼ ¿¬±¸¿Í ÀÌ¿¡ ´ëÇÑ Çй®Àû ÀÌÇØ´Â ´Ù¸¥ ±Ý¼Óü³ª ¹ÝµµÃ¼¿¡ ºñÇØ µÚ¶³¾îÁ® ÀÖ´Ù. ÀÌ´Â ÀÚ¼ºÃ¼ÀÇ ÀÚ±âÀûƯ¼ºÀÌ ¼ö ³ª³ë¹ÌÅÍ(nm) °Å¸® Á¤µµ¿¡¼­ ÀÛ¿ëÇÏ´Â ¿øÀÚ½ºÇɰ£ÀÇ ¼ÒÀ§ ±³È¯»óÈ£ÀÛ¿ë(exchange interaction)¿¡ ÀÇÇÑ Çùµ¿Çö»ó(cooperative phenomena)¿¡ ÀÇÇØ Á¿ìµÇ±â ¶§¹®¿¡ ½ÇÇèÀûÀ¸·Î³ª ÀÌ·ÐÀûÀ¸·Î ¿¬±¸Çϱ⿡ ¾î·Á¿òÀÌ Àֱ⠶§¹®ÀÌ´Ù. ±×·¯³ª '90³â´ë¿¡ µé¾î¿À¸é¼­ °íÁø°ø ÁõÂø±â¼ú°ú Ç¥¸é°úÇÐÀÇ ±Þ¼ÓÇÑ ¹ßÀüÀ¸·Î ³ª³ë¹ÌÅÍ µÎ²²ÀÇ ÀÚ¼º¹Ú¸· Á¦Á¶°¡ °¡´ÉÇÏ°Ô µÇ¾ú°í, ¶ÇÇÑ À̵é ÀÎÀ§Àû Á¦Á¶ ¹°Áú¿¡¼­ ±âÁ¸ÀÇ ÀÚ¼ºÃ¼¿¡¼­ º¼ ¼ö ¾ø´Â ¼öÁ÷ÀÚ±âÀ̹漺À̳ª, °Å´ëÀÚ±âÀúÇ×(Giant magnetoresistance)µî »õ·Î¿î ÀÚ±âÇö»óµéÀÌ ¹ß°ßµÇ¾ú´Âµ¥, ÀÌ·ÎÀÎÇØ Çй®ÀûÀ¸·Î ÀÚ¼ºÃ¼¿¬±¸ÀÇ ¸£³×»ó½º¸¦ °¡Á®¿Ô°í, ƯÈ÷ ÀÀ¿ëÀûÃø¸é¿¡¼­ »õ·Î¿î ±â¼ú½Ã´ë¸¦ ¿¹°íÇÏ°Ô µÇ¾ú´Ù. ±×°ÍÀº Áö±Ý±îÁö ¹ÝµµÃ¼ÀÇ ÀüÇϸ¦ ÀÌ¿ëÇÑ ÀüÇÏ¿£Áö´Ï¾î¸µ½Ã´ë¿¡¼­ ¾ÕÀ¸·Î´Â ÀÚ¼ºÃ¼ÀÇ ½ºÇÉÀ» ÀÌ¿ëÇÏ´Â ½ºÇÉ¿£Áö´Ï¾î¸µ½Ã´ë¸¦ ¿­¾î°¡°Ô µÉ °ÍÀÌ´Ù. 1 Tb/cm2 Ãʰí¹Ðµµ/´ë¿ë·® ÀÚ±â ¹× ±¤Àڱ⠱â·Ï¸Åü, 1 GBps °í°¨µµ ÀÚ±â±â·ÏÇìµå µî ÷´Ü ½ºÇÉÁ¤º¸¼ÒÀç »Ó ¾Æ´Ï¶ó, ÇöÀçÀÇ ½Ç¸®ÄÜ(Si) ¹ÝµµÃ¼¿¡ ±âÃÊÇÑ ÀüÀÚ µð¹ÙÀ̽ºµéÀÇ ¼Óµµ ¹× ÁýÀûµµÀÇ ÇѰ踦 ÈξÀ ´É°¡ÇÏ´Â ÀÚ±âÀúÇ׸޸ð¸®(MRAM, Magnetoresistive Random Access Memory), ½ºÇÉÅͳθµ¸Þ¸ð¸®(STRAM, Spin Tunneling Random Access Memory), ½ºÇÉÆ®·£Áö½ºÅÍ µî ¼ÒÀ§ "Spintronics" ¶ó´Â »õ·Î¿î ±â¼úÇõ¸íÀ» °¡Á®¿Ã °ÍÀ¸·Î ±â´ëµÈ´Ù.

2. ³ª³ë½ºÇɴнº(Nanospinics)¶õ?(½ºÇÉÁ¤º¸¹°Áú ¿¬±¸½Ç ȨÆäÀÌÁö ÂüÁ¶)

ÀÚ¼ºÃ¼ ¼ÒÀÚµéÀÇ ÁýÀû¹Ðµµ ¹× °Åµ¿Æ¯¼ºÀº ±Ùº»ÀûÀ¸·Î ÀüÀÚ½ºÇÉ ±³È¯»óÈ£ÀÛ¿ë¿¡ ÀÇÇØ Çùµ¿Çö»óÀ» º¸ÀÌ´Â ½ºÇɵéÀÇ ÁýÇÕ, Áï ÀÚ±¸(magnetic domain)ÀÇ Å©±â¿Í µ¿·ÂÇп¡ ÀÇÁ¸Çϱ⠶§¹®¿¡, ÃʰíÁýÀûÈ­ ±â¼ú °³¹ßÀ» À§ÇØ ³ª³ë Å©±â ÀÚ±¸ÀÇ Á¦¾î¿Í ÀÌÇØ°¡ ¼±ÇàµÇ¾î¾ß ÇÑ´Ù. ±×·¯¹Ç·Î ÇöÀçÀÇ ¸¶ÀÌÅ©·ÎÀÚ¼ºÇÐ(Micromagnetism)À» ÃÊ¿ùÇÏ¿©, ³ª³ëÅ©±â ÀÚ±¸ÀÇ °Åµ¿À» ÀÌÇØÇÏ°í ¿¹ÃøÇÒ ¼ö ÀÖ´Â »õ·Î¿î ÆÄ¶ó´ÙÀÓÀÇ '³ª³ëÀÚ¼ºÇÐ(Nanomagnetism)'ÀÌ Çй®ÀûÀ¸·Î Á¤¸³µÇ¾î¾ß ÇÑ´Ù.

³ª³ëÀÚ¼ºÇÐÀÇ Çй®Àû Á¤¸³À» À§ÇØ ³ª³ëÀÚ¼ºÃ¼¿¡¼­ÀÇ ÀÚ±¸ÇüÅ ¹× ½ºÇÉ µ¿·ÂÇÐÀ» ´Ù·ç´Â ¼ÒÀ§ '³ª³ë½ºÇɴнº(Nanospinics)'¸¦ ÁßÁ¡ÀûÀ¸·Î ¿¬±¸ÇØ¾ß ÇÑ´Ù. À̸¦ À§ÇØ ³ª³ëÀÚ¼º¹Ú¸·, ³ª³ëÁ¡ ¹× ³ª³ëÁ¡ ¹è¿­(array), ºÐÀÚÀÚ¼ºÃ¼ µî ¿©·¯ °¡Áö ÇüÅÂÀÇ »õ·Î¿î ³ª³ëÀÚ¼ºÃ¼¸¦ ÀÎÀ§ÀûÀ¸·Î Á¦Á¶Çϰí, ³ª³ëÀÚ¼ºÃ¼ÀÇ ÀÚ±¸ ¹× ÀÚ±âÀû Ư¼º ÃøÁ¤À» À§ÇÑ ¿øÀÚÃþ ºÐÇØ´ÉÀÇ ÃÊ°í°¨µµ ½Ç½Ã°£ ÃøÁ¤¹æ¹ýÀ» °³¹ßÇÏ¿©, ³ª³ëÀÚ±¸ µ¿·ÂÇÐ ¸ÞÄ«´ÏÁòÀ» ±Ô¸íÇØ¾ß ÇÑ´Ù. ƯÈ÷, ÀÚ¼ºÃ¼ÀÇ 3°¡Áö ±Ù¿øÀû Àǹ®¿¡ ÃÊÁ¡À» ¸ÂÃß¾î ¿¬±¸¸¦ ¼öÇàÇØ¾ß ÇÑ´Ù. ±×°ÍÀº (1) ³ª³ëÀÚ¼ºÃ¼ÀÇ ½ºÇɹæÇâ°ú ÀÚ±¸ÇüÅÂ, (2) ÀÚ±¸¹ÝÀü°úÁ¤, (3) °Å½ÃÀû ¾çÀÚÈ¿°úÀÇ Á¸Àç¿©ºÎ¿¡ ´ëÇÑ ¿¬±¸ÀÌ´Ù. ¿Ö³ÄÇϸé ÀÌ 3°¡Áö ±Ù¿øÀû Áú¹®Àº Çй®Àû Ãø¸é¿¡¼­ ³ª³ëÀÚ¼ºÃ¼ ½ºÇɵ¿·ÂÇÐ ±Ô¸íÀÇ ÇÙ½ÉÀÏ »Ó ¾Æ´Ï¶ó ÀÀ¿ëÀû Ãø¸é¿¡¼­ ³ª³ëÀÚ¼º ½ºÇÉÁ¤º¸¹°ÁúÀ» ÀÌ¿ëÇÑ ½ºÇÉÆ®·Î´Ð½º(Spintronics) ¼ÒÀÚÀÇ ÁýÀû¹Ðµµ, Á¤º¸ÀúÀå ¼ö¸í, ±×¸®°í ÀÛµ¿½Ã°£ÀÇ ±Ã±ØÀû ÇѰ迡 ÇØ´äÀ» ÁÙ ¼ö Àֱ⠶§¹®ÀÌ´Ù.

À̸¦ À§ÇØ ½Å¼ºÃ¶ ±³¼ö°¡ À̲ô´Â ½ºÇÉÁ¤º¸¹°Áú ¿¬±¸½ÇÀº Çй®Àû Ãø¸é¿¡¼­´Â ³ª³ëÀÚ¼ºÃ¼ÀÇ ÀÚ±¸ÇüÅ ¹× ½ºÇɰŵ¿À» ±Ô¸íÇÏ´Â ³ª³ë½ºÇɴнº¶ó´Â »õ·Î¿î Çй®ºÐ¾ß¸¦ ¼±µµÀûÀ¸·Î °³Ã´ÇÏ¿© Á¤¸³Çϰí ÀÖ¾î, ³ª³ëÀÚ¼ºÃ¼ Çö»ó¿¬±¸ÀÇ ¼¼°èÀû ¿¬±¸±×·ìÀ¸·Î À§»óÀ» È®º¸ÇÒ °ÍÀ̸ç, ±â¼úÀû/°æÁ¦Àû Ãø¸é¿¡¼­´Â ¼¼°è ÃÖ°íÀÇ Ãʰí¹Ðµµ/Ãʰí¼Ó ³ª³ë½ºÇÉ Á¤º¸¹°ÁúÀ» °³¹ßÇϹǷνá Á¤º¸ÀúÀå»ê¾÷ÀÇ ¼¼°è½ÃÀå È®º¸¿Í ³ª¾Æ°¡ ½ºÇÉÆ®·Î´Ð½º ½Å»ê¾÷ âÃâ¿¡ Å©°Ô ±â¿©ÇÒ °ÍÀ¸·Î º¸ÀδÙ.

3. °ÅµìÁ¦°ö¹ýÄ¢(Power law)À̶õ? º¹ÀâÇÑ Çö»óÀ» °¡·ÎÁö¸£´Â °Å½ÃÀû Áú¼­(À±¿µ¼ö, ä½Âº´ ÁöÀ½, º¹Àâ°è °³·Ð, ¼­¿ï : »ï¼º°æÁ¦¿¬±¸¼Ò, 2005, ÆäÀÌÁö 045-054 ÂüÁ¶; Steven Strogatz, SYNC[Á¶Çö¿í ¿Å±è, µ¿½Ã¼ºÀÇ °úÇÐ, ¼­¿ï : ±è¿µ»ç, 2005, ÆäÀÌÁö 340-354 ÂüÁ¶)

¿ì¸®°¡ »ç´Â ¼¼»óÀº °³Ã¼µéÀÌ º¹ÀâÇÏ°Ô ¾ôÇô ÀÖ¾î ¾î¶² ÀÏÀÌ ¹ß»ýÇÒÁö ¸ð¸¥´Ù. ±×·±µ¥ º¹ÀâÇÑ °Íó·³ º¸À̸鼭µµ ¼¼»óÀÌ Ã¼°èÀûÀ¸·Î µ¹¾Æ°¡´Â °ÍÀ» º¸¸é ½Å±âÇϱ⸸ ÇÏ´Ù. º¹Àâ°è(Complex system)¿¡¼­ °üÂûµÇ´Â ´ëÇ¥ÀûÀÎ Áú¼­Çö»óÀ¸·Î ÀÚ¿¬°è»Ó¸¸ ¾Æ´Ï¶ó »çȸ°è¿¡¼­µµ ´Ù¾çÇÏ°Ô ³ªÅ¸³ª´Â ¹ýÄ¢ÀÌ ¹Ù·Î °ÅµìÁ¦°ö¹ýÄ¢(Power law)ÀÌ´Ù.

1934-1939³â¿¡(On Seismic Waves¿¡ 4ÆíÀÇ ³í¹® ¹ßÇ¥;1934, 1935, 1936, 1939) »ê ¾Èµå·¹¾Æ½º ´ÜÃþÀ» µû¶ó ÁöÁøÀÌ ºó¹ßÇϴ Ķ¸®Æ÷´Ï¾Æ Áö¿ªÀ» Áß½ÉÀ¸·Î ÁöÁø ¿¡³ÊÁöÀÇ Å©±â¿Í ÁöÁø ¹ß»ý ºóµµ¸¦ Á¶»çÇÏ´ø ͏®Æ÷´Ï¾Æ °ø°ú´ëÇÐÀÇ ÁöÁøÇÐÀÚ ±¸ÅÙº£¸£±×(Beno Gutenberg)¿Í ¸®È÷ÅÍ(Charles Francis Richter)´Â ÁöÁøÀÇ ¿¡³ÊÁö°¡ 10¹è°¡ µÉ ¶§¸¶´Ù ±× ¹ß»ýºóµµ´Â 1/10·Î ÁÙ¾îµç´Ù´Â »ç½ÇÀ» ¹ß°ßÇß´Ù. ÀÌ °ü°è¸¦ '±¸ÅÙº£¸£±×-¸®È÷ÅÍÀÇ ¹ýÄ¢(Gutenberg-Richter law)'À̶ó°í ÇÏ°í ±× °ø½ÄÀº ¹Ù·Î logE(S) = 11.8 + 1.5M ÀÌ´Ù.

[°ü·Ã Âü°í¹®Çå]

B. Gutenberg, C.F. Richter, Publ. Bur. Centr. Seism. Int., Travaux Scientifiques, A 15, 1937, 3.
B. Gutenberg, C.F. Richter, "P' AND THE EARTH'S CORE", Geophysical Journal International, Volume 4, Issue s5, pp. 363-372, May 1938.
B. Gutenberg, C.F. Richter, "Frequency of earthquakes in California", Bulletin of the Seismological Society of America, 1944; 34: pp. 185-188.
B. Gutenberg, C.F. Richter, Seismicity Of The Earth And Associated Phenomena, Princeton University Press, 1949.
B. Gutenberg, C.F. Richter, "Earthquake Magnitude, Intensity, Energy, and Acceleration", Bull. Seism. Soc. Am., 46, 1956, 105.

´ÙÀ½ ±×·¡ÇÁ¿¡¼­ º¸´Â ¹Ù¿Í °°ÀÌ °¡·ÎÃà°ú ¼¼·ÎÃà ¸ðµÎ ¾Æ·¡°¡ 10ÀÎ ·Î±× ´ÜÀ§·Î ±×·ÁÁ® ÀÖ´Ù. ±×·¡¼­ °ªÀÌ ¿­ ¹è Áõ°¡ÇÒ ¶§ ¸¶´Ù ±× ·Î±×°ªÀº 1¾¿ Áõ°¡ÇÏ¿©, ·Î±× ´ÜÀ§·Î ±×¸° ±×·¡ÇÁ¸¦ ÅëÇØ »ìÆìº» ÁöÁøÀÇ ÆÐÅÏÀº ±ú²ýÇÏ°í ´Ü¼øÇÑ Á÷¼±À¸·Î ³ªÅ¸³­´Ù. ÀÌ¿Í °°ÀÌ ¾î¶°ÇÑ µÎ °ªÀÇ °ü°è°¡ ·Î±× Æò¸é¿¡¼­ Á÷¼± ¸ð¾çÀÌ ³ª¿Â´Ù¸é(b=1) ÀÌ µÎ °ªÀº °ÅµìÁ¦°öÀ»¹ýÄ¢À» µû¸¥´Ù°í ÇÑ´Ù. ÀÌ´Â °Å´ëÇÑ ÁöÁøÀ̵ç ÀÛÀº ÁöÁøÀÌµç ±× Å©±â¿¡ °ü°è¾øÀÌ ¶È°°Àº ¿ø¸®¿¡ ÀÇÇØ Áö¹è ¹Þ´Â´Ù´Â °ÍÀ» ÀǹÌÇÑ´Ù. º¹ÀâÇÑ Áö±¸ÀÇ ±¸Á¶¿Í´Â °ü°è¾øÀÌ ÀÏ·üÀûÀ¸·Î ¼º¸³ÇÏ´Â ´Ü¼øÇÑ ±ÔÄ¢ÀÌ ÀÖ´Â °ÍÀÌ´Ù. º¹ÀâÇÑ ¼¼»ó¿¡¼­ ¹ß°ßµÇ´Â ÀÌ·¯ÇÑ ÀϰüµÈ ±ÔÄ¢ÀÇ Á¸Àç´Â ¿ì¸®°¡ Á¦´ë·Î ÀνÄÇÏÁö ¸øÇϰí ÀÖ´Â °Å´ëÇÑ Áú¼­°¡ ¼û¾î ÀÖÀ½À» ¾Ï½ÃÇØÁØ´Ù.

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* Winner-Take-All Society

4. ¿Âµµ¿¡ µû¸¥ ¹ÚÅ©ÇÏ¿ìÁ¨ ÀâÀ½Çö»ó(Barkhausen avalanche or effect or noise)ÀÇ ¿ø¸®¸¦ ¹àÇô

ÀÌ·± ºÒ±ÔÄ¢ÇÑ Çö»óÀÌ ÀÚ¼ºÃ¼¿¡µµ Á¸ÀçÇÑ´Ù´Â »ç½ÇÀº 1919³â µ¶ÀÏÀÇ ¹°¸®ÇÐÀÚ ¹ÚÅ©ÇÏ¿ìÁ¨(Heinrich Georg Barkhausen)ÀÌ Ã³À½ ¹ß°ßÇß´Ù. ÀÌ Çö»óÀ» '¹ÚÅ©ÇÏ¿ìÁ¨ ÀâÀ½Çö»ó(Barkhausen avalanche or effect or noise)'À̶ó°í Çϴµ¥, ÀÚ¼ºÃ¼¸¦ ÀÌ¿ëÇÑ ½ºÇÉÆ®·Î´Ð½º ±â¼ú ±¸Çö½Ã ÀâÀ½À» ¸¸µå´Â ±Ù¿øÀû ¿øÀÎÀ¸·Î Áö¸ñµÅ ¿Ô´Ù.

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±× µ¿¾È ¼ö¸¹Àº ¹°¸®ÇÐÀÚµéÀÇ ¿¬±¸·Î ¹ÚÅ©ÇÏ¿ìÁ¨ ÀâÀ½Çö»óµµ °ÅµìÁ¦°ö¹ýÄ¢ Åë°èºÐÆ÷·Î ¼³¸íµÉ ¼ö ÀÖ´Ù´Â °ÍÀÌ ÀÔÁõµÆÁö¸¸ '°ÅµìÁ¦°ö¹ýÄ¢ ºÐÆ÷Áö¼ö°¡ °°Àº Â÷¿øÀÇ ÀÚ¼ºÃ¼¿¡¼­ ¿Ö ´Ù¾çÇÑ °ªÀ» °®´ÂÁö' ÇÏ´Â Àǹ®Àº ¹ÌÇØ°á °úÁ¦·Î ³²¾Ò¾ú´Ù. À̹ø¿¡ Ä«À̽ºÆ® ¿¬±¸ÆÀÀº Ư¼ö ±â´ÉÀÇ '±¤ÀÚ±â Çö¹Ì°æ'À» Á¦ÀÛ, ÀÚ±¸¿ªÀü(Magnetization reversal, ÀÚ¼ºÃ¼ÀÇ ÀÚÈ­(Magnetization, N±Ø°ú S±Ø) ¹æÇâÀÌ ¹Ý´ë·Î ¹Ù²î´Â °Í) °úÁ¤À» 400nm(³ª³ë¹ÌÅÍ) ºÐÇØ´É(ÝÂú°Òö)À¸·Î ½Ç½Ã°£ °üÂûÇÑ °á°ú ÀÚ±¸º®(magnetic domain-wall)ÀÇ ¹Ì¼¼±¸Á¶ º¯È­°¡ °ÅµìÁ¦°ö¹ýÄ¢ ºÐÆ÷Áö¼ö º¯È­¿¡ °áÁ¤Àû ¿µÇâÀ» ¹ÌÄ£´Ù´Â »ç½ÇÀ» ¹àÇô³Â´Ù.

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¾Æ¿ï·¯ ÀÚ¼ºÃ¼ ½ºÇÉÀ» ÀÌ¿ëÇØ Çõ½ÅÀû ½Å¼ÒÀÚ¸¦ °³¹ßÇÏ´Â '½ºÇÉÆ®·Î´Ð½º' ±â¼ú±¸Çö½Ã Àå¾Ö°¡ µÇ´Â ÀâÀ½Çö»óÀ» Á¤È®È÷ ÀÌÇØÇÏ´Â µ¥µµ Å©°Ô ±â¿©ÇÒ °ÍÀ¸·Î º¸ÀδÙ. ¿¬±¸ÆÀÀÇ ½Å¼ºÃ¶ ±³¼ö´Â ÀÚ¼º ºÐ¾ß ÃÖ´ë ÇÐȸ·Î ¿À´Â 11¿ù ¹Ì±¹ Ç÷θ®´Ù¿¡¼­ ¿­¸®´Â 'ÀÚ¼º ¹× ÀÚ¼ºÃ¼ÇÐȸ'(MMM)¿¡ ÃÊû ¿¬»ç·Î Âü¼®, À̹ø ¿¬±¸ ¼º°ú¸¦ Á÷Á¢ ¼Ò°³ÇÒ ¿¹Á¤ÀÌ´Ù.
http://www.magnetism.org/


½Å¼ºÃ¶ ±³¼ö
http://physics.kaist.ac.kr/people/sungchul_shin.htm
scshin@kaist.ac.kr
TEL : +82-42-869-2528
FAX : +82-42-869-8100
web : http://cnsm.kaist.ac.kr
¿¬±¸½Ç : ÀÚ¿¬°úÇе¿ 2302È£

5. ³í¹® ¿ä¾à

°­ÀÚ¼º ¹°ÁúÀº ºÒ¿¬¼ÓÀûÀÌ°í ºÒ±ÔÄ¢ÇÑ ÀÚ±¸ Á¡ÇÁ¸¦ º¸¿©Áִµ¥ À̸¦ ¿ÜºÎ ÀÚ±âÀå ³»ÀÇ ¹ÚÅ©ÇÏ¿ìÁ¨ È¿°ú¶óÇÑ´Ù. ¹ÚÅ©ÇÏ¿ìÁ¨ ÀâÀ½Çö»ó¿¡ ´ëÇÑ ¿¬±¸µéÀº ³»ÀçµÈ ÀӰ輺À» ÀǹÌÇÏ´Â °ÅµìÁ¦°ö¹ýÄ¢ ºÐÆ÷Áö¼ö º¯È­¸¦ ¹àÈ÷°í Àִµ¥, ÀÌ´Â ÃÊÀüµµ ¼Ò¿ëµ¹ÀÌ, ¸¶ÀÌÅ©·Î Æ´»õ, ÁöÁø, Æó ÆØÃ¢, ´ë·® ¸êÁ¾, ÁÖÁ÷½ÃÀå ¹× ÀüÇÏ-ÁýÀû ÆÄÀå µîÀÇ ´Ù¾çÇÑ ½Ã½ºÅÛ¿¡¼­ °üÂûµÇ°í ÀÖ´Ù. ±×·±µ¥ Áö±Ý±îÁö ¹àÇôÁöÁö ¾ÊÀº °¡Àå ±Ùº»ÀûÀÎ Áú¹®Àº ºÐÆ÷Áö¼ö ³»ÀÇ º¸Æí¼ºÀÌ ¾î¶»°Ô ¹°ÁúÀ̳ª ¹°ÁúÀÇ ±¸Ã¼ÀûÀÎ ¹Ì¼¼±¸Á¶¿Í °ü°è¾øÀÌ Á¸ÀçÇϴ°¡ ÀÌ´Ù. ÀÌ¿¡ ¿ì¸®´Â º» ³í¹®¿¡¼­ ÁÖ¾îÁø(°°Àº Â÷¿øÀÇ) °­ÀÚ¼º Çʸ§¿¡¼­ Á¸ÀçÇÏ´Â ¹ÚÅ©ÇÏ¿ìÁ¨ ÀӰ輺ÀÇ ºÐÆ÷Áö¼ö´Â Â÷¿øÀÌ ¾Æ´Ï¶ó ´Ù¾çÇÑ ¿Âµµ º¯È­¿¡ ÀÇÇØ ½ÇÇèÀûÀ¸·Î Á¶Á¤ ¹× °üÂûÀÌ °¡´ÉÇÔÀ» ÀÔÁõÇÏ¿´´Ù. ¿ì¼± ÁÖ¾îÁø ½Ã½ºÅÛÀÇ ¹ÚÅ©ÇÏ¿ìÁ¨ ÀӰ輺 ³»ÀÇ ºÐÆ÷Áö¼ö º¯È­´Â ½Ö±Ø¼ºÀÇ »óÈ£ÀÛ¿ëÀ¸·ÎºÎÅÍ »ó´ëÀûÀÎ ±â¿©¸¦ ÇÒ ¶§ µÎ °¡ÁöÀÇ º¸Æí¼º ¼öÁØÀ» °¡·Î Áú·¯ ¶Ù¾î ³Ñ´Â´Ù´Â »ç½ÇÀ» °üÂûÇßÀ¸¸ç, ÀÌ ¶§ ÀÚ±¸º® ¿¡³ÊÁöµéÀº ÁÖ¾îÁø ½ÇÇè ÆÐ·¯¹ÌÅÍ¿¡ ÀÇÇØ º¯È­µÈ´Ù´Â »ç½ÇÀ» °üÂûÇß´Ù(A ferromagnetic material shows a sequence of discrete and jerky domain jumps, known as the Barkhausen avalanche, in the presence of an external magnetic field. Studies of Barkhausen avalanches reveal power-law scaling behaviour that suggests an underlying criticality, as observed in a wide variety of systems such as superconductor vortices, microfractures, earthquakes, lung inflations, mass extinctions, financial markets and charge-density waves. The most interesting unsolved fundamental question is whether the universality in the scaling exponent holds regardless of the material and its detailed microstructure. Here we show that the scaling behaviour of Barkhausen criticality in a given ferromagnetic film is experimentally tunable by varying the temperature(not dimensionality). We observe for the first time that the scaling behaviour in the Barkhausen criticality of a given system crosses over between two universality classes when the relative contributions from the dipolar interaction and domain-wall energies are altered by an experimental parameter).

6. ±¤ÀÚ±â Çö¹Ì°æÀ̶õ?(½ºÇÉÁ¤º¸¹°Áú ¿¬±¸½Ç ȨÆäÀÌÁö ÂüÁ¶)

º» ÀåÄ¡´Â ÀÚ¼º¹°ÁúÀÇ ½ºÇÉ(spin) µ¿·ÂÇÐ ¿¬±¸¸¦ À§ÇÏ¿© ±¤ÀÚ±â KerrÇö»óÀ» ÀÌ¿ëÇÑ °í¼º´É ±¤ÀÚ±â Çö¹Ì°æ ½Ã½ºÅÛÀÌ´Ù. °í¼º´É ±¤ÀÚ±â Çö¹Ì°æ ½Ã½ºÅÛÀº ±¤ÇÐÆí±¤Çö¹Ì°æ, ¿­ÀÚ±â±â·Ï ½Ã½ºÅÛ, ¿µ»óó¸® ½Ã½ºÅÛ°ú ÀüÀÚ¼®À¸·Î ÀÌ·ç¾îÁ® ÀÖÀ¸¸ç, ±× ÁÖ¿ä »ç¾çÀº ¾Æ·¡¿Í °°´Ù.

* °ø°£ ºÐÇØ´É: 0.3§­
* KerrȸÀü°¢ ºÐÇØ´É: 0.2¢ª
* ÃÖ´ë¹èÀ²: ¡¿1,000
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* ½Ç½Ã°£ Àڱⱸ¿ª ¿µ»óó¸®: 10 Frames/sec
* ¿­ÀÚ±â±â·Ï: Ãâ·Â-10 mWatt, ±â·Ï½Ã°£-50 ns(½Ã·áÇ¥¸é)

7. Criticality(ÀӰ輺, °íºñ¼º)

ÀÓ°èÁú·®(¶Ç´Â °íºñÁú·®, Critical mass)Àº Çٺп­À» ÀÏÀ¸Å°´Â ¹°ÁúÀº ¾î¶² Áú·® ÀÌ»óÀÌ ¸ðÀ̸é ÀÚ¹ßÀûÀÎ ¿¬¼â¹ÝÀÀÀ» ÀÏÀ¸Å°´Âµ¥, ÀÌ ¿¬¼â¹ÝÀÀ¿¡ ÇÊ¿äÇÑ ÃÖ¼ÒÀÇ Áú·®À» ÀǹÌÇÑ´Ù. ÀÓ°èÁú·®À» ³ÑÀ¸¸é ÀÛÀº Ãæ°ÝÀ¸·Îµµ ¾î¸¶¾î¸¶ÇÑ Æø¹ßÀÌ ÀϾ ¼ö ÀÖ´Ù. ÀÌ ¶§¹®¿¡ º¹Àâ°è(Complex system)¿¡¼­´Â ¾î¶°ÇÑ ±Þ°ÝÇÑ º¯È­¸¦ À¯¹ßÇÏ´Â ÇѰè Á¶°ÇÀ» ³ªÅ¸³¾ ¶§ ÀºÀ¯ÀûÀΠǥÇöÀ¸·Î ¾²ÀδÙ. ÀÓ°èÇö»ó(¶Ç´Â °íºñÇö»ó, Critical phenomenon)Àº ÀÓ°èÁ¡ ÁÖº¯¿¡¼­ ÀϾ´Â Çö»óÀ¸·Î Åë°è¹°¸®Çп¡¼­´Â »óÀüÀÌ(Phase-transition, Áï °íü¿¡¼­ ¾×ü·Î, ¾×ü¿¡¼­ °íü·Î) Çö»ó Áß Àá¿­(¼ûÀº ¿­)ÀÌ ¹ß»ýÇÏÁö ¾Ê´Â 2Â÷ »óÀüÀÌ Çö»óÀ» ´ëÇ¥ÀûÀÎ ÀÓ°èÇö»óÀ̶ó ÇÑ´Ù. Åë»óÀûÀ¸·Î ½Ã½ºÅÛÀÇ ±Þ°ÝÇÑ º¯È­¸¦ ³ªÅ¸³¾ ¶§ ÀºÀ¯ÀûÀΠǥÇöÀ¸·Î ¾²ÀδÙ. ÀÓ°èÁ¡(¶Ç´Â °íºñÁ¡, Critical point)Àº Åë°è¹°¸®Çп¡¼­ 2Â÷ »óÀüÀ̰¡ ÀϾ´Â ÁöÁ¡À» ÀǹÌÇϸç, ¼öÇп¡¼­´Â ¹ÌºÐ°ªÀÌ ¹«ÇÑ´ë ¶Ç´Â 0À̰ųª Á¤ÇØÁöÁö ¾Ê´Â Á¡À» ÀǹÌÇÑ´Ù. Åë»óÀûÀ¸·Î ±Þ°ÝÇÑ º¯È­°¡ ÀϾ´Â °íºñ°¡ µÇ´Â ÁöÁ¡À» ÀǹÌÇÏ¿©, ¶§·Î´Â ƼÇÎ Æ÷ÀÎÆ®(Tipping point), ºÐ±âÁ¡(Bifurcation), º¯°îÁ¡(Inflection), ƯÀÌÁ¡(Singularity) µîÀÇ Àǹ̷Π¾²À̱⵵ ÇÑ´Ù. ÀÓ°è»óÅÂ(¶Ç´Â °íºñ»óÅÂ, Critical state)´Â ¾î¶² ½Ã½ºÅÛÀÌ ÀÓ°èÁ¡¿¡ ³õ¿© ÀÖ´Â »óŸ¦ ÀǹÌÇÑ´Ù. Åë»óÀûÀ¸·Î ¾î¶² ±Þ°ÝÇÑ º¯È­°¡ ÀϾ±â Á÷ÀüÀÇ ºÒ¾ÈÁ¤ÇÑ »óŸ¦ ³ªÅ¸³¾ ¶§ ÀºÀ¯ÀûÀΠǥÇöÀ¸·Î ¾²ÀδÙ.

ÀӰ輺(¶Ç´Â °íºñ¼º)Àº ÀÓ°è»óÅ¿¡¼­ º¸¿©Áö´Â ½Ã½ºÅÛÀÇ Æ¯Â¡À» ÀǹÌÇÑ´Ù. ½Ã½ºÅÛÀÇ ´Ù¾çÇÑ ¹°¸®·®µéÀÌ °ÅµìÁ¦°ö¹ýÄ¢À» º¸ÀδÙ. ¸Å°³º¯¼ö°¡ ÀÓ°èÁ¡¿¡ ¸Å¿ì °¡±î¿ï ¶§ ÀÌ °ÅµìÁ¦°öÀÇ ºÐÆ÷Áö¼ö¿Í ¹Ì¼¼º¯È­´Â °°Àº Â÷¿øÀÇ ½Ã½ºÅÛ(dimensionality of the system)¿¡ ÀÇÇØ º¸Æí¼º(universality)À» ¶ì°í º¸ÆíÀû ºÐÆ÷Áö¼öº¯È­°¡ ÀϾ´Ù´Â °ÍÀÌ ±âÁ¸ Çм³À̾ú´Ù. ±×·¯³ª °ÅµìÁ¦°ö¹ýÄ¢ ºÐÆ÷Áö¼ö°¡ °°Àº Â÷¿øÀÇ ÀÚ¼ºÃ¼¿¡¼­ ¿Ö ´Ù¾çÇÑ °ªÀ» °®´ÂÁö°¡ À̹ø ½Å¼ºÃ¶ ±³¼öÆÀÀÇ ¿¬±¸·Î ¹àÇôÁø °ÍÀÌ´Ù. Áï, °­ÀÚ¼ºÃ¼ ³»ÀÇ ÀÚ±¸º® ¿îµ¿¿¡¼­´Â ¿Âµµ º¯È­¿¡ µû¶ó ÀӰ輺ÀÌ ÇϳªÀÇ º¸Æí¼º¿¡¼­ ´Ù¸¥ º¸Æí¼º ¼öÁØÀ¸·Î ¶Ù¾î ³Ñ¾î ±¸Á¶°¡ º¯È­ÇÑ´Ù´Â °ÍÀÌ´Ù(Scaling behaviour - as observed in avalanches - reveals universal behaviour dictated by the dimensionality of the system. For domain-wall motion in a ferromagnet, however, the criticality can cross over from one universality class to another depending on the temperature).

8. ¸Þ¸ð¸®ÀÇ Á¾·ù(02250)

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