{"id":184759,"date":"2019-08-30T09:46:55","date_gmt":"2019-08-30T01:46:55","guid":{"rendered":"\/\/m.iemloyee.com\/?p=184759"},"modified":"2019-10-18T18:30:18","modified_gmt":"2019-10-18T10:30:18","slug":"%e4%bb%8a%e6%97%a5science%ef%bc%9a%e9%93%9c%e9%85%b8%e7%9b%90%e9%ab%98%e6%b8%a9%e8%b6%85%e5%af%bc%e4%bd%93%e7%9a%84%e5%8a%a8%e6%80%81%e7%94%b5%e8%8d%b7%e5%af%86%e5%ba%a6%e6%b3%a2","status":"publish","type":"post","link":"\/\/m.iemloyee.com\/?p=184759","title":{"rendered":"\u4eca\u65e5Science\uff1a\u94dc\u9178\u76d0\u9ad8\u6e29\u8d85\u5bfc\u4f53\u7684\u52a8\u6001\u7535\u8377\u5bc6\u5ea6\u6ce2"},"content":{"rendered":"<p><strong><b>\u3010\u5f15\u8a00\u3011<\/b><\/strong><\/p>\n<p>\u7531\u4e8e\u5176\u5c42\u72b6\u7ed3\u6784\u7684\u51c6\u4e8c\u7ef4\u6027\u548c\u5927\u7684\u7535\u5b50-\u7535\u5b50\u6392\u65a5\uff0c\u94dc\u9178\u76d0\u9ad8\u6e29\u8d85\u5bfc\u4f53\uff08HTSs\uff09\u504f\u79bb\u4e86\u6717\u9053\u8d39\u7c73\u6db2\u4f53\u7406\u8bba\u3002\u63ba\u6742\uff08p\uff09-\u6e29\u5ea6\uff08T\uff09\u76f8\u56fe\uff0c\u5728\u4f4eT\u5904\u7684\u53cd\u94c1\u78c1\u548c\u8d85\u5bfc\u987a\u5e8f\uff0c\u5e76\u4e14\u5728\u8f83\u9ad8\u7684T\u5904\u5305\u62ec\u8d5d\u80fd\u9699\u533a\u57df\uff0c\u5176\u7279\u5f81\u5728\u4e8e\u4e00\u4e9b\u72b6\u6001\u7684\u51c6\u7c92\u5b50\u5bc6\u5ea6\u7684\u51cf\u5c0f\u3002\u5c3d\u7ba1\u5b83\u4eec\u59cb\u7ec8\u5728\u76f8\u56fe\u7684\u4f4e\u63ba\u6742\u533a\u548c\u76f8\u5bf9\u8f83\u4f4e\u7684\u6e29\u5ea6\u4e0b\u88ab\u53d1\u73b0\uff0c\u4f46\u5b83\u4eec\u5728\u591a\u5927\u7a0b\u5ea6\u4e0a\u5f71\u54cd\u4e86\u8fd9\u4e9b\u7535\u8377\u5bc6\u5ea6\u7cfb\u7edf\u7684\u4e0d\u5bfb\u5e38\u6027\u8d28\u4ecd\u4e0d\u6e05\u695a\u3002<\/p>\n<p><strong><b>\u3010\u6210\u679c\u7b80\u4ecb\u3011<\/b><\/strong><\/p>\n<p>\u4eca\u65e5\uff0c\u5728<strong><b>\u610f\u5927\u5229\u7c73\u5170\u7406\u5de5\u5927\u5b66R. Arpaia<\/b><\/strong><strong><b>\u6559\u6388<\/b><\/strong>\u548c<strong><b>G. Ghiringhelli<\/b><\/strong><strong><b>\u6559\u6388<\/b><\/strong><strong><b>\u56e2\u961f\uff08<\/b><\/strong><strong><b>\u5171\u540c<\/b><\/strong><strong><b>\u901a\u8baf\u4f5c\u8005\uff09<\/b><\/strong>\u5e26\u9886\u4e0b\uff0c\u4e0e<strong><b>\u745e\u5178<\/b><\/strong><strong><b>\u67e5\u5c14\u59c6\u65af\u7406\u5de5\u5927\u5b66\u3001<\/b><\/strong><strong><b>\u610f\u5927\u5229CNR-ISC\u3001\u610f\u5927\u5229\u7f57\u9a6c\u5927\u5b66\u3001<\/b><\/strong><strong><b>\u6b27\u6d32\u540c\u6b65\u8f90\u5c04\u5149\u6e90\u3001<\/b><\/strong><strong><b>\u610f\u5927\u5229CNR-SPIN\u3001<\/b><\/strong><strong><b>\u610f\u5927\u5229\u90a3\u4e0d\u52d2\u65af\u8d39\u5fb7\u91cc\u79d1\u4e8c\u4e16\u5927\u5b66\u3001<\/b><\/strong><strong><b>\u5317\u4eac\u5927\u5b66<\/b><\/strong>\u5408\u4f5c\uff0c\u4f7f\u7528\u5171\u632fX\u5c04\u7ebf\u6563\u5c04\uff0c\u786e\u5b9a\u4e86\u51e0\u79cd\u63ba\u6742\u6c34\u5e73\u4e0bYBa<sub>2<\/sub>Cu<sub>3<\/sub>O<sub>7-\u03b4<\/sub>\u548cNd<sub>1+x<\/sub>Ba<sub>2-x<\/sub>Cu<sub>3<\/sub>O<sub>7-\u03b4<\/sub>\u4e2d\u968f\u6e29\u5ea6\u53d8\u5316\u7684\u7535\u8377\u5bc6\u5ea6\u6ce2\u3002\u9664\u4e86\u5df2\u77e5\u7684\u51c6\u4e34\u754c\u7535\u8377\u5bc6\u5ea6\u6ce2\u4e4b\u5916\uff0c\u56e2\u961f\u8fd8\u5206\u79bb\u4e86\u77ed\u7a0b\u52a8\u6001\u7535\u8377\u5bc6\u5ea6\u6ce2\u3002\u5b83\u4eec\u6301\u7eed\u8fdc\u9ad8\u4e8e\u8d5d\u9699\u6e29\u5ea6T*\uff0c\u4ee5\u51e0\u6beb\u4f0f\u7535\u5b50\u4f0f\u7279\u7684\u80fd\u91cf\u4e3a\u7279\u5f81\uff0c\u5e76\u5728\u76f8\u56fe\u4e2d\u5360\u636e\u5f88\u5927\u7684\u533a\u57df\u3002\u76f8\u5173\u6210\u679c\u4ee5\u9898\u4e3a<strong><b>\u201c<\/b><\/strong><strong><b>Dynamical charge density fluctuations pervading the phase diagram of a Cu-based high-Tc superconductor<\/b><\/strong><strong><b>\u201d<\/b><\/strong>\u53d1\u8868\u5728\u4e86<strong><b>Science<\/b><\/strong>\u4e0a\u3002<\/p>\n<p><strong><b>\u3010\u56fe\u6587\u5bfc\u8bfb\u3011<\/b><\/strong><\/p>\n<p><strong><b>\u56fe1<\/b><\/strong><strong><b>\u00a0<\/b><\/strong><strong><b>\u4e0d\u540c\u6c27\u63ba\u6742\u7684YBa<\/b><\/strong><strong><sub><b>2<\/b><\/sub><\/strong><strong><b>Cu<\/b><\/strong><strong><sub><b>3<\/b><\/sub><\/strong><strong><b>O<\/b><\/strong><strong><sub><b>7-\u03b4<\/b><\/sub><\/strong><strong><b>\u548cNd<\/b><\/strong><strong><sub><b>1+x<\/b><\/sub><\/strong><strong><b>Ba<\/b><\/strong><strong><sub><b>2-x<\/b><\/sub><\/strong><strong><b>Cu<\/b><\/strong><strong><sub><b>3<\/b><\/sub><\/strong><strong><b>O<\/b><\/strong><strong><sub><b>7-\u03b4<\/b><\/sub><\/strong><strong><b>\u8584\u819c\u7684\u51c6\u5f39\u6027<\/b><\/strong><strong><b>\u8868\u5f81<\/b><\/strong><strong><b><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-184760\" src=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F1.large_-1.jpg\" alt=\"\" width=\"600\" height=\"1444\" srcset=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F1.large_-1.jpg 600w, \/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F1.large_-1-125x300.jpg 125w, \/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F1.large_-1-425x1024.jpg 425w\" sizes=\"(max-width: 600px) 100vw, 600px\" \/><\/b><\/strong><\/p>\n<p><strong><b>\u56fe<\/b><\/strong><strong><b>2 <\/b><\/strong><strong><b>NBCO UD60<\/b><\/strong><strong><b>\u7684<\/b><\/strong><strong><b>\u51c6\u5f39\u6027<\/b><\/strong><strong><b>\u8868\u5f81<\/b><\/strong><strong><b><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-184761\" src=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F2.large_-1.jpg\" alt=\"\" width=\"600\" height=\"1034\" srcset=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F2.large_-1.jpg 600w, \/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F2.large_-1-174x300.jpg 174w, \/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F2.large_-1-594x1024.jpg 594w\" sizes=\"(max-width: 600px) 100vw, 600px\" \/><\/b><\/strong><\/p>\n<p><strong><b>\u56fe<\/b><\/strong><strong><b>3 <\/b><\/strong><strong><b>UD60\u548cOP90\u7684\u7535\u8377\u5bc6\u5ea6\u5cf0<\/b><\/strong><strong><b><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-184762\" src=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F3.large_-1.jpg\" alt=\"\" width=\"600\" height=\"789\" srcset=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F3.large_-1.jpg 600w, \/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F3.large_-1-228x300.jpg 228w\" sizes=\"(max-width: 600px) 100vw, 600px\" \/><\/b><\/strong><\/p>\n<p><strong><b>\u56fe<\/b><\/strong><strong><b>4 <\/b><\/strong><strong><b>HTS\u94dc\u9178\u76d0\u76f8\u56fe\u4e2d\u7684\u9759\u6001\u548c\u52a8\u6001\u7535\u8377<\/b><\/strong><strong><b>\u5206\u5e03<\/b><\/strong><strong><b><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-184763\" src=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F4.large_-1.jpg\" alt=\"\" width=\"600\" height=\"417\" srcset=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F4.large_-1.jpg 600w, \/\/m.iemloyee.com\/wp-content\/uploads\/2019\/08\/F4.large_-1-300x209.jpg 300w\" sizes=\"(max-width: 600px) 100vw, 600px\" \/><\/b><\/strong><\/p>\n<p><strong><b>\u6587\u732e\u94fe\u63a5\uff1a<\/b><\/strong><a href=\"https:\/\/science-sciencemag-org.uchile.idm.oclc.org\/content\/365\/6456\/906\" target=\"_blank\" rel=\"noopener\"><u>Dynamical charge density fluctuations pervading the phase diagram of a Cu-based high-Tc superconductor<\/u><\/a>\uff08Science\uff0c2019\uff0c\u00a0DOI:10.1126\/science.aav1315\uff09<\/p>\n<p>\u672c\u6587\u7531<strong><b>\u6728\u6587\u97ec<\/b><\/strong>\u7ffb\u8bd1\uff0c\u6750\u6599\u725b\u6574\u7406\u7f16\u8f91\u3002<\/p>\n<p>\u6b22\u8fce\u5927\u5bb6\u5230\u6750\u6599\u4eba\u5ba3\u4f20\u79d1\u6280\u6210\u679c\u5e76\u5bf9\u6587\u732e\u8fdb\u884c\u6df1\u5165\u89e3\u8bfb\uff0c\u6295\u7a3f\u90ae\u7bb1tougao@cailiaoren.com\u3002<\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>\u3010\u5f15\u8a00\u3011 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