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Liebman£©Ðí¶àʱ¼äÈËÃÇËù̾ϢµÄѹÁ¦ÊÇ×Ô¼ºÇ¿¼ÓµÄÕâ¸öʱ¼ä¾ÍҪѧ»á´ÓÍ·ÄÔÉÏɨ³ý×Ô¼ºµÄѹÁ¦Ô´Õë¶ÔijЩÒÕÊõ¼ÒÓÃѹÁ¦´óÀ´Îª×Ô¼ºµÄijЩ²»Êʵ±ÐÐΪ¿ªÍѵÄ×ö·¨¸ðÓÅÏÈÉú˵£º²»¾ÍÊÇÑÝÔ±ÂðÅĸöÓ°Ï·ÍæÄÜÓÐʲôѹÁ¦ ÈôÊǸ÷È˶¼ÄÜÓÐÕâ·ÝäìÈ÷´ÓÐÄÀïжϼ縺²»Ì«ÄÃ×Ô¼ºµ±»ØÊÂÉúÑÄÖоͻáÉÙһЩ pressure, tension ºÍstress´Ó¶ø»áÈÃÈËÉú¸üÓÅÃÀЩ°É²Î¿¼ÎÄÏ×[1] Frank Wilczek, Fantastic Realities, World Scientific2006.[2] Z. X. Cao, J. Phys.:Cond.Mater. 13, 7923-7935 (2001).[3] ²ÜÔòÏÍÀ©É¢Æ«Îö·Ñ˼Á¿¡¶ÎïÀí¡·37¾í2ÆÚ128-130£¨2008£©.[4] L. D. Landau, E. M. Lifshitz, Theory of Elasticity, 3th edition, Butterworth Heinemann, 1981.[5] ²ÜÔòÏÍÖåÎÆÖ®ÃÀÓë×ðÑÏPPT (2008).[6] C. R. Li, X. N. Zhang, and Z.X.Cao, Triangular and Fibonacci number patterns driven by stress on core/shell microstructures, Science309, 909-911(2005).[7] C. R. Li, A. L. Ji , and Z. X. Cao, Stressed Fibonacci spiral patterns of definite Chirality, Appl. Phys. Lett. 90164102 (2007).[8] C. R. Li ,W. J. Dong, Gao Lei, Z. X. Cao, Stressed triangular lattices on microsized spherical surfaces and their defect management, APL93, 034108 (2008).[9] Jie Yin, Zexian Cao, Chaorong Li, Izhak Sceinman, and Xi Chen, Stress-Driven Buckling patterns in spheroidal core/shell structures, PNAS105, 19132-19135 ( 2008).ȪԴ£º·µÆÓ±à¼£ºÖعâ½üÆÚÈÈÃÅÎÄÕÂTop10¡ý µã»÷ÎÊÌâ¼´¿ÉÉó²é ¡ý1. µôÈëµØÏÂÒ»ÍòÃ×2. ÒÔǰÓиöѧÉú°¾Ò¹³Ùµ½ÁË´í°ÑÀ§ÈÅÊýѧ¼ÒµÄÄÑÌâ¿´³ÉÒµ×öÁ˳öÀ´3. Ô×Óµ¯ÖÆÔìÖ¸ÄÏ4. ÎüèһʱˬһֱÎüèһֱˬ5. Ϊʲô³¤Ê±¼ä²»Ï´Í·Ï´µÄʱ¼ä´ê²»³öÐí¶àÅÝÄ| No.1456. Ò»¸ö´ó»îÈË»¹ÄÜÈÃÄò»î»î±ïËÀ7. ÒÔÊÇWiFi ºÍ 4G ¾¿¾¹Äĸö¸üºÄµç8. ´«Ö½Ìõ±»·¢Ã÷Ò»¿´¾¹Ð´×Å...9. Ǧ±ÊÉÏÃæÄÇ¿é·Ï²ñÏðƤΪʲôÈÝÒ×°ÑÖ½²ÁÆÆ10. Ò»·ùͼ¶Á¶®Á¿×ÓÁ¦Ñ§£¨Ñ¦¶¨Ú̵Ä裩
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