| |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
![]() | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
µo¦æ¤H¡G¶À¤ÉÀs©Òªø ½s¿è©eû¡G½²ºÍõ±Ð±Â ¥D½s¡GªLßN¤å µo¦æ¤é´Á¡G2007.12.14 | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
³Ì·s®ø®§»P¬¡°Ê¤½§i ©Ò°È¤½§i¤Î¬¡°Êªáµ¶ ¯S§O³ø¾É ÁÚ¦V³»¦y¤j¾Çpµe¬ã¨s¦¨ªG±MÄæ | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
¡@
¡@
¦b¥»©Ò´^¶©Ãv±Ð±Â¤j¤O±À°Ê¤Î¨ó§U¤U¡A¥ú¹q©Ò»P²ö´µ¬ì¤j¾Çª«²z¨t¡]FACULTY OF PHYSICS, m.v. lomOnosov moscow state university¡^ñq¤§¾Ç³N¥æ¬y¦X§@³Æ§Ñ¿ý¡A¤w©ó¥»¡]96¡^¦~11¤ë23¤é©ó³Õ²zÀ]¤C¼Ó·|ij«Ç§¹¦¨Ã±¬ù¡F¥»¦X§@³Æ§Ñ¿ý¥Dn³W¹ºÂù¤è¾Ç³N±Ð¾Ç¤Î¬ã¨s¤§¦X§@¥æ´«p¹º¡C ¡@ | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
¡@ ¡@ ¡@
®É¶¡¡G96¦~11¤ë16¤é¤U¤È4:00-6:00
Á¿ªÌ¡G½²®¶¤ô°|¤h
¡]¤¤¥¡¬ã¨s°|¡^ ½²®¶¤ô°|¤h©ó96¦~11¤ë16¤é ¡]¬P´Á¤¡^»YÁ{¥»©Ò³X°Ý¡A¨Ã©ó³Õ²zÀ]101ºtÁ¿ÆUµoªíºt»¡¡AÁ¿ÃD¬°¡uA Progress Report on Silicon-Based Ultrasonics and Photonics Research¡v¡A¥»©Ò±Ð®v¤Î¾Ç¥Í¬Ò¼ö¯P°Ñ»PºtÁ¿¬¡°Ê¡AÀò¯q¨}¦h¡C
¡@ | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
¡@ ¡ã»PÁú°êºº¸°ê¥ß¤j¾Ç¡]Seoul National University¡^ ³Õ¤h¥Í¥æ¬y¬¡°Ê 2007 ¡ã ¡iThe 2nd National Taiwan University-Seoul National University Student Workshop 2007 on Photonic Materials and Devices¡j ¡]®É¶¡¡G96¦~11¤ë17¤é¦Ü11¤ë21¤é¡F¦aÂI¡G °ê¥ß»OÆW¤j¾Ç¡^ ªáµ¶¾ã²z¡G¥ú¹q©Ò³Õ¤h¯Z¾Ç¥Íð©v¼Ý
¡@ | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
¡@ Numerical study on surface plasmon polariton behaviors in periodic metal-dielectric structures using a plane-wave-assisted boundary integral-equation method Professor Yean-Woei Kiang Graduate Institute of Photonics and Optoelectronics, National Taiwan University »OÆW¤j¾Ç¥ú¹q©Ò¦¿l°¶±Ð±Â A hybrid technique based on the boundary integral-equation method is proposed for studying the surface plasmon polariton behaviors in two-dimensional periodic structures. Considering the periodicity property of the problem, we use the plane-wave expansion concept and the periodic boundary condition instead of using the periodic Green¡¦s function. The diffraction efficiency can then be readily calculated once the equivalent electric and magnetic currents are solved that avoids invoking the numerical calculation of the radiation integral. The numerical validity is verified with the cases of highly conducting materials and practical metals. Numerical convergence can be easily achieved even in the case of a large incident angle as 80o. Based on the numerical scheme, a metal-dielectric wavy structure is designed for enhancing the transmittance of optical signal through the structure. The excitation of the coupled surface plasmon polaritons for the high transmission is demonstrated.
| |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
¡@ ¡@ | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
¡@ Small Lab---¦ó§Ó¯E±Ð±Â ¡@ ¡@¡@¥»¹êÅç«Ç©ó2007¦~¶}©l³Ð¥ß¡A¦]¦¹¡A²{¦b³B©ó¯ó³Ð®É´Á¡C¥»¹êÅç«Çªº¬ã¨s«ÂI¦b©óZnO©`¦Ìµ²ºcªºª«²z¯S©Ê¤§¬ã¨s¡A¥]¬AºUÂøì¤l¹ï¨ä¯S©Ê¤§¼vÅT¡C¤À¬°¤TÓ¥DÃD¡G ¡@ 1. µ²ºc¤§¬ã¨s¡A¥]¬A©`¦Ìµ²ºcªº³W«h©Ê¹ï¨äª«²z©Ê½è¤§¬ã¨s»P¨ä¹q¤lµ²ºc¤§¬ã¨s¡C 2. ¹q¾Ç©Ê½è¤§¬ã¨s¡A¥]¬A (1) ¹q¤l¶Ç¿é¤§¬ã¨s; (2) ¥Íª«»P¤Æ¾Ç¤À¤l»P¹q¤l¶Ç¿éªºÃö«Y¤§¬ã¨s; (3) À£¹q©Ê»P¥b¾ÉÅé©Êªº½¢¦X¤§¬ã¨s¡C 3.¥ú¾Ç¯S©Ê¤§¬ã¨s¡A¥]¬A (1) ¦Ûµo©Ê©ñ¥ú¤§¬ã¨s; (2) ®ñ¤Æ¾N©`¦Ì½uÀ³¥Î©ó¤Ó¶§¯à¹q¦Àªº¥ú¹qÀ³¥Î¡C ¡@ ¡@¡@©`¦ÌªºÁͶաA§Y¬Oµ²¦X§ó¦h¡B§ó¼sªxªº¤£¦P¡¨¬ì¾Ç¡¨I´º¡A©M¹ê»Ú¡¨¤uµ{¡¨¤è±³]pªº°õ¦æ¸gÅç¡A¨Ó¼W¥[¥¼¨Ó©`¦Ìªº¯à¶q¡C¥»¹êÅç«Ç¤§¬ã¨s¦b°ê»Ú¤W¬ÛÃö»â°ìÄÝ©ó¸û¬°«e¤©Ê¤§¬ã¨s½ÒÃD¡C§Ú̦³«ùÄòªº¿³½ì©ó§Q¥Î©`¦Ì§÷®Æªº¿W¯Sµ²ºc©Ê¡A¨Óµo®i¥i¯à¤§«e¤¤§¥ú¹qÀ³¥Î¡C§Ṳ́@¤è±µo®i»s§@¡BÆ[¹î©`¦Ìµ²ºcªº·s§Þ³N¡A¥t¤@¤è±¤]̱´°Q©`¦Ì§÷®Æ»Pµ²ºc¹ï¥ú¹q¤¸¥ó¯S©Êªº¼vÅT¡A§Æ±æ¯à°÷°µ¤@Ó¾ô¼Ù¡A¨Ï±o©`¦Ì§Þ³N»P¥ú¹q¤¸¥ó§Þ³N°µ¤@Ó§¹¬üªºµ²¦X¡C ¡@ | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
¡@ ¡X ¸ê®Æ´£¨Ñ¡G¼v¹³Åã¥Ü¥ú¹q¬ì§Þ¯S¦â¤H¤~°ö¨|¤¤¤ß¡E¼v¹³Åã¥Ü¬ì§Þª¾ÃÑ¥¥x ¡X ¡X ¾ã²z¡GªL®ÌÅɱб¡B³¯«a¦t ¡X ¡@
¡@¡@FPD International¶×¶°¤F¥ªOÅã¥Ü¾¹¡]FPD¡^³Ì·s²£«~¤Î§Þ³N¡C¥»©¡®iÄý ©ó10¤ë24¡ã26¤é¦b¾îÀØÁ|¿ì¡A¦@¦³330®a¤½¥q¡]¤é¥»269®a¡A®ü¥~91®a¡^°Ñ®i¡A®i¦ìÁ`p885Ó®i¥ÜªÅ¶¡¡C¦b¶}¹õ¦¡¤¤¡A¤é¥»¥b¾ÉÅé»s³y³]³Æ¨ó·|¡]SEAJ¡^±M°È²z¨Æ±`ªQ¬F¾iªí¥Ü¡GFPD¦b¹qµø¨Ñ³f¶q¤¤ªº¤ñ¨Ò¤£Â_ÂX¤j¡A2007¦~¦b¼Ú¬ü±N¶W¹L50¢H¡A2010¦~¦b¤¤°ê±N¶W¹L50¢H¡F¦b2009¦~FPD¨Ñ³f¶q±N¶W¹LÅã¹³ºÞ¡]CRT¡^¹qµø¡A¨ì2011¦~±N¶W¹L60¢H¡A¦Ó2011¦~ªº¹qµø¨Ñ³f¶q±N¹F¨ì2»õ¥x¡C ¡@ ¡@¡@LCDªº§Þ³Nµo®i¡A°£¤F²G´¹±ªO§Þ³Nªº¤£Â_¬ð¯}¥~¡AI¥ú§Þ³N¥ç¥²¶·¬Û¤¬·f°t¡A¤µ¦~8¤ëSharp®i¥X52 ¦T¶WÁ¡«¬¡]20 mm¡^LCD TVÂú§Î¾÷¡A¥HRGB LED¥ú·½»P½Õ¾ã«áªº±ªO·f°t¡A¦â±mÅã²{NTSC¹F¨ì150%¡A«D±`ÆvÄR¡A¦b³ÌÁ¡«p«×20 mm»P³Ì«p29 mmªº¶ZÂ÷¤§¤º¡A±N²{¦³ªº·s«¬¥ú¾Ç¨t²Î¥R¤À§Q¥Î¡C¦bFPD®iÄý·|³õ¤¤¡A¤µ¦~LCD TV¤Ø¤oº¦¸¤j´T¶W¶VPDP¡A¶W°ªµe½è¡BÁ¡«¬¤Æ¡B¬Ù¯à»PÀô«Oµ¥¶D¨D¬O¤µ¦~Åã¥Ü¾¹¼t°Ó»P§Þ³N©Ò°l¨Dªº¥Ø¼Ð¡A¨Ò¦p¡GToshiba¦b³o¦¸®iÄý¤¤¤]«Å¥Ü¤F¥¼¨Ó¶WÁ¡LCD¿Ã¹õªº¥Ø¼Ð¡A°£¤F²G´¹±ªO¬Á¼þ«p«×°¦Ü0.2 mm¥H¤U¡A¤¤¤Ø¤o¤§LEDI¥ú¼Ò²Õªº«p«×¤]°¨ì0.2-0.3 mm¥ª¥k¡A³o¤w¸g»PELÅã¥Ü¾¹ªºµo®i²£¥Í¬Û¹ïªºÄvª§©Ê¡A·í¾É¥úªO«p«×¤p©ó0.5mm®É¡A¬°¤Fºû«ùªí±¥X¥ú®Ä²v¡A·|¦³½ÆÂøªº¥X¥úµ²ºc³]p¦p¡GV-CUT»Pmicro Lensµ¥¡A¶Ç²Îªº®g¥X¦¨«¬§Þ³N¦b³o¨Ç·Lµ²ºc¦¨«¬¤W·|¹J¨ì²~ÀV¡A¨ú¦Ó¥N¤§¬O¼öÀ£¦¨«¬ªº»sµ{¡AµL½×¬O§å¦¸©Î³sÄò¼öÀ£ªº»sµ{³£¦³¼t°Ó¦b¶i¦æ¡CI¥ú¥ú¾Ç½¤¤ù¤¤±`³Q¤H©¿µøªº´N¬O¤Ï®g¤ù¡A¦ý¤Ï®g¤ù¬O¥ú¦^¦¬¾÷¨î¤¤¤£¥i©Î¯Êªº¡A¤@¯ë¬O°ª¤Ï®g²vªº»È¤Ï®g©Î¬O¦h¤Õ»Ø¥Õ¤Ï®g¤ù¡ASekisui¤Æ¾Ç§Q¥Îµoªw§Þ³N»Pthermal molding§Þ³N¡A±NPPµoªw§÷»s§@¦¨·L«¬¸Jª¬¡A¥i¥H¼W¥[LED¥¿¦V¥ú·½ªº«G«×¡A¸g¥Ñ¥ªOªº¤Ï®g¤ù¦^¦¬¤Ï®g¥i¥H¼W¥[50%«G«×¡A¦ý·L«¬¤Ï®gªM«h¥i¥H¼W¥[ªñ100¢Hªº«G«×¡CSamsung¤]®i¥X¤F¤@´Ú±Ä¥ÎLED°¼I¥úªº²G´¹¹qµø¡A±ªO«p«×¶È¦³10 mm¡C ¡@ ¡@¡@I¥ú¼Ò²Õ«p«×À£ÁYªº·N¸q¬Oªí¥Ü·s¤@¥NI¥ú¼Ò²Õªº¿n·¥µo®i¡A¨ä¤¤¥]¬A¡G¯S®íLED¥ú·½»P¥ú¾Ç´Uªº¨Ï¥Î¡A°ª¬ï³z¡B°ªÂX´²²v¤§²V¥ú¥ú¾ÇÂX´²ªO»P½Æ¦X¥ú¾Ç¼W«G½¤¡A³o¨Ç³£¥i¥H¦bFPD·|³õ¤W¨£¨ì¡A¤T¦Ê¦h®aªº°Ñ®i¼t°Ó¤¤¡A§÷®Æ¼t°Ó¬ù²¤¦³¤@¦Ê¦h®a¡A¨ä¤¤»P¥ú¾Ç½¤¬ÛÃöªº¼t°Ó´N¦û¤F1/4¥ª¥k¡A¬ÛÃöªº§Þ³NÄvª§¿E¯P¥i·Q¦Óª¾¡C
¡@¡@ ¸ê®Æ¨Ó·½¡G§÷®Æ¥@¬Éºô http://www.materialsnet.com.tw/DocView.aspx?id=6513 ¡@¡@¡@¡@¡@¡@¡@ LEDinside http://www.ledinside.com/node/1019 ¡@ | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
¡@ ¹AÃĩΦ³®`ª«½è·|º¯³z¨ì½µæ¤ôªG¸Ì±¶Ü¡H
¦³¦¹¤@»¡¡G ¦Y¤ôªG¥un¤ôªGªºªí±¬~¤@¬~¡A§âªí±ªº¹AÃĤΦ³®`ª«¬~±¼¡A´N¥i¥H¦Y©Î¬O¥´¦¨ªG¥Ä³Ü¡A¨º½µæ¬O§_¸ò¤ôªG¤@¼Ë¡A¥un½µæªºªí±¬~¤@¬~¡A§âªí±ªº¹AÃĤΦ³®`ª«¬~±¼¡A´N¥i¥H¥Í¦Y©Î¥´¦¨½µæ¥Ä³Ü¡A¦Ó¤£»Ýn°ª·Å²i½Õ¤F¡H½µæ¥i¥H¤£²i½Õ¦Ó¥Í¦Y¶Ü¡H§Úª¾¹D¤ôªG³£¬O¥Í¦Yªº¡A¨S¦³¤H·|¥h²i½Õ¤ôªG¡A¨º¦U¦¡¦U¼Ëªº½µæ¡A¦pÅÚ½³¡BµÔµæ¡B»Û£µ¥¡A©Î¬O¤@¨Ç¯S§Oªº½µæÃþ¡A³£¥i¥H¥Í¦Y¶Ü¡H¦³¨S¦³¨Ò¥~ªº©O¡H¨º¹AÃĩΦ³®`ª«·|¤£·|º¯³z¨ì½µæùØ¡A¥ú¬Oªí±²M¬~ÁÙ¤£°÷¡AÁÙ»Ýn²i½Õ³B²z¤~¦æ©O¡H
KingNet®a®xÂå¾Ç¬ìÂå®v¦^µª¡G ¤j³¡¤Àªº¹AÃij£¬O¦b«Cµæ¤ôªGªºªí±¡A¦ý¤j¦h¤£®e©ö¥u¥Î²M¤ô´N¥i¬~²b¡Cn¥Í¦Y¡A³Ì¦n¬O¥Í¾÷¶¼¹©Ò¥Í²£¡A¦]¬°¤£¨Ï¥Î¹AÃÄ¡A©ÎªÌ¦b±Ä¦¬«e´X¤Ñ¤£¥Î¹AÃÄ¡A³o¼Ë¸û¬°¦w¥þ¡I
KingNetÀç¾i«O°·¿Ô¸ßÀç¾i®v¦^µª¡G
½µæ¤¤ªº¹AÃħt¶q³Ì¦h¬°´²µæÃþ¡]¦p´µæ¡B¤p¥Õµæ¡BµÔµæµ¥¸ª¬½µæ¡^¡A¨ä¦¸¬°µ²²y¸µæ¡]¦p¥]¤ßµæ¡Bªãµæµ¥¡^¡B¨§µæÃþ¡]¥|©u¨§¡Bµæ¨§¡B½Ü¨§¡^¡BªGµæÃþ¡]¿»X¡B«C´Ôµ¥¡^¡B®ÚµæÃþ¡]°¨¹aÁ¦¡B¬õÅÚ½³¡BÅÚ½³¡^¡A§t¶q³Ì¤Ö¬°¥ÊµæÃþ¡]¤p¶À¥Ê¡Bµ·¥Ê¡BJ¥Ê¡^¡A©Ò¥HY±z·Q³Ü½µæ¥Ä¡A¥i¿ï¾Ü¹AÃħt¶q¸û¤Öªº¡C
¥»¤å¥Ñ¡iKingNet °ê®aºô¸ôÂå°|¡j´£¨Ñ ¡@ | |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
ª©Åv©Ò¦³ °ê¥ß»OÆW¤j¾Ç¹q¾÷¸ê°T¾Ç°|¥ú¹q¤uµ{¾Ç¬ã¨s©Ò http://gipo.ntu.edu.tw/ ÅwªïÂà¸ü ¦ý½Ðµù©ú¥X³B http://gipo.ntu.edu.tw/monthly.htm |