{"id":27045,"date":"2021-06-18T19:49:40","date_gmt":"2021-06-18T11:49:40","guid":{"rendered":"https:\/\/swarma.org\/?p=27045"},"modified":"2021-06-18T19:49:40","modified_gmt":"2021-06-18T11:49:40","slug":"%e5%89%8d%e6%b2%bf%e9%80%9f%e9%80%92%ef%bc%9a%e9%ba%a6%e5%85%8b%e6%96%af%e9%9f%a6%e5%a6%96%e7%9a%84%e6%96%b0%e6%b6%a8%e8%90%bd%e5%ae%9a%e7%90%86","status":"publish","type":"post","link":"https:\/\/swarma.org\/?p=27045","title":{"rendered":"\u524d\u6cbf\u901f\u9012\uff1a\u9ea6\u514b\u65af\u97e6\u5996\u7684\u65b0\u6da8\u843d\u5b9a\u7406"},"content":{"rendered":"
\n
\n
\n

<\/p>\n

\n
\n
\n
\n
\n
\n

<\/section>\n<\/section>\n
\n
\n

\u5bfc\u8bed<\/strong><\/p>\n<\/section>\n<\/section>\n

\n

<\/section>\n<\/section>\n<\/section>\n<\/section>\n<\/section>\n
\n
\n
\n

\u7531\u4e8e\u7814\u7a76\u4eba\u5458\u5bf9\u7eb3\u7c73\u5c3a\u5ea6\u548c\u4ecb\u89c2\u5c3a\u5ea6\u7cfb\u7edf\u63a7\u5236\u7684\u5174\u8da3\uff0c\u6709\u4e00\u4e9b\u7814\u7a76\u901a\u8fc7\u6539\u8fdb\u9ea6\u514b\u65af\u97e6\u5996\uff08Maxwell’s demon\uff09\u7684\u6982\u5ff5\u6765\u5173\u6ce8\u5f00\u653e\u7cfb\u7edf\u4e2d\u80fd\u91cf\u8017\u6563\u7684\u6781\u9650\u3002\u5728\u6700\u8fd1\u53d1\u8868\u5728 Science Advances <\/em>\u7684\u4e00\u7bc7\u6587\u7ae0\u4e2d\uff0c\u4e3a\u4e86\u63ed\u793a\u9ea6\u514b\u65af\u97e6\u5996\u63a7\u5236\u7684\u7cfb\u7edf\u80cc\u540e\u7684\u57fa\u672c\u7269\u7406\u539f\u7406\uff0c\u7814\u7a76\u4eba\u5458\u8bc1\u660e\u4e86\u4e00\u7ec4\u4ee5\u524d\u672a\u63a2\u7d22\u8fc7\u7684\u6da8\u843d\u5b9a\u7406\u3002\u8fd9\u4e9b\u6da8\u843d\u5b9a\u7406\u610f\u5473\u7740\u7cfb\u7edf\u5b58\u5728\u4e00\u4e2a\u5185\u5728\u7684\u975e\u5e73\u8861\u72b6\u6001\uff0c\u53d7\u9ea6\u514b\u65af\u97e6\u5996\u5f15\u8d77\u7684\u8017\u6563\u4fe1\u606f\u5f71\u54cd\u3002
<\/strong><\/p>\n


<\/strong><\/p>\n

\u7814\u7a76\u9886\u57df\uff1a<\/strong><\/strong>\u975e\u5e73\u8861\u6001\u70ed\u529b\u5b66<\/span><\/strong><\/span><\/p>\n<\/section>\n<\/section>\n<\/section>\n

\n
<\/svg><\/section>\n<\/section>\n<\/section>\n<\/section>\n<\/section>\n<\/section>\n
\n
<\/section>\n<\/section>\n
\n

\u6f58\u4f73\u680b | \u4f5c\u8005<\/span><\/strong><\/strong><\/p>\n

\u9093\u4e00\u96ea | \u7f16\u8f91<\/strong><\/span><\/p>\n<\/section>\n


<\/p>\n


<\/p>\n

<\/p>\n

\n
\n
\n

\u539f\u6587\u9898\u76ee\uff1a<\/span><\/p>\n

New fluctuation theorems on Maxwell\u2019s demon<\/span><\/p>\n

\u539f\u6587\u5730\u5740\uff1a<\/span><\/p>\n

https:\/\/advances.sciencemag.org\/content\/7\/23\/eabf1807<\/span><\/p>\n<\/section>\n<\/section>\n<\/blockquote>\n


<\/p>\n

\u5728\u7269\u7406\u5b66\u53f2\u4e0a\uff0c\u8457\u540d\u7684\u9ea6\u514b\u65af\u97e6\u5996\u88ab\u63d0\u51fa\u7528\u6765\u53cd\u5bf9\u70ed\u529b\u5b66\u7b2c\u4e8c\u5b9a\u5f8b[1]\u3002\u5b83\u964d\u4f4e\u4e86\u7edd\u70ed\u7cfb\u7edf\u4e2d\u7684\u71b5\uff0c\u6700\u7ec8\u5c06\u6574\u4e2a\u5b87\u5b99\u4ece\u70ed\u5bc2<\/span>\uff08heat death\uff09<\/span>\u4e2d\u62ef\u6551\u51fa\u6765\u3002\u5c3d\u7ba1\u542c\u8d77\u6765\u662f\u795e\u8bdd[2-3]\uff0c\u4f46\u662f\u9ea6\u514b\u65af\u97e6\u5996\u53cd\u6620\u4e86\u666e\u9002\u7cfb\u7edf\u7684\u6027\u8d28\uff0c\u5c24\u5176\u662f\u5728\u5fae\u89c2\u5c3a\u5ea6\u4e0a\uff1a\u4e0e\u9ea6\u514b\u65af\u97e6\u5996\u76f8\u4e92\u4f5c\u7528\u7684\u7cfb\u7edf\u53d8\u5f97\u5f00\u653e\u5e76\u56e0\u6b64\u8fdc\u79bb\u70ed\u5e73\u8861\u72b6\u6001\u3002<\/span><\/p>\n


<\/p>\n

\u9ea6\u514b\u65af\u97e6\u5996\u6240\u6d89\u53ca\u7684\u975e\u5e73\u8861\u70ed\u529b\u5b66\u4e0e\u4fe1\u606f\u8bba\u4e4b\u95f4\u5b58\u5728\u7740\u6df1\u523b\u7684\u8054\u7cfb\u3002\u4fe1\u606f\u7684\u7269\u7406\u6027\u8d28\u53ef\u4ee5\u901a\u8fc7\u5bf9\u9ea6\u514b\u65af\u97e6\u5996\u7684\u7814\u7a76\u6765\u63ed\u793a\u3002\u51fa\u4e8e\u8be5\u539f\u56e0\uff0c\u7814\u7a76\u4eba\u5458\u5728\u8be5\u65b9\u5411\u505a\u51fa\u4e86\u5927\u91cf\u52aa\u529b\u3002\u5728\u7eb3\u7c73\u548c\u4ecb\u89c2\u7cfb\u7edf\u7684\u5206\u6790\u548c\u63a7\u5236\u7684\u7406\u8bba\u548c\u5b9e\u9a8c\u9886\u57df\uff0c\u7814\u7a76\u4eba\u5458\u7684\u76f8\u5173\u5de5\u4f5c\u90fd\u663e\u793a\u51fa\u9ea6\u514b\u65af\u97e6\u5996\u7684\u91cd\u8981\u6027[7-15]\u3002<\/span><\/p>\n


<\/p>\n

\u4f5c\u4e3a\u73b0\u4ee3\u70ed\u529b\u5b66\u7684\u6838\u5fc3\u6982\u5ff5\uff0c\u71b5\u4ea7\u751f<\/span>\uff08entropy production\uff09<\/span>\u91cf\u5316\u4e86\u968f\u673a\u7cfb\u7edf\u4e2d\u7684\u80fd\u91cf\u8017\u6563\u3002\u71b5\u4ea7\u751f\u7684\u57fa\u672c\u6027\u8d28\u4e4b\u4e00\u662f\u5b83\u9075\u5faaJarzynski\u6052\u7b49\u5f0f[16]\u548c\u79ef\u5206\u6da8\u843d\u5b9a\u7406\uff0c\u4ece\u5fae\u89c2\u89d2\u5ea6\u53ef\u4ee5\u5c06\u5176\u89c6\u4e3a\u5e7f\u4e49\u7b2c\u4e8c\u5b9a\u5f8b\u3002\u4e3a\u4e86\u5206\u6790\u9ea6\u514b\u65af\u97e6\u5996\u7684\u5f71\u54cd\uff0c\u4e00\u4e9b\u5f00\u521b\u6027\u7684\u5de5\u4f5c\u8bd5\u56fe\u6784\u5efa\u4e00\u4e2a\u4e0d\u7b26\u5408Jarzynski\u7b49\u5f0f [17-22]\u7684\u71b5\u4ea7\u751f\u3002Sagawa\u548cUeda[23-24]\u7ed9\u51fa\u4e86\u4e00\u4e2a\u8fd9\u6837\u7684\u6784\u9020\uff0c\u5176\u4e2d\u8003\u8651\u5230\u9ea6\u514b\u65af\u97e6\u5996\u83b7\u5f97\u7684\u4fe1\u606f\uff0c\u63d0\u51fa\u4e86\u6da8\u843d\u5b9a\u7406<\/span>\uff08Sagawa-Ueda\u5b9a\u7406\uff09<\/span>\u3002\u76f8\u5e94\u5730\uff0c\u8fd9\u4e2a\u6da8\u843d\u5b9a\u7406\u4ea7\u751f\u4e86\u4e00\u4e2a\u5e7f\u4e49\u7684\u7b2c\u4e8c\u5b9a\u5f8b\uff1a\u9ea6\u514b\u65af\u97e6\u5996\u63d0\u53d6\u7684\u529f\u4e0d\u80fd\u8d85\u8fc7\u5176\u5e73\u5747\u83b7\u5f97\u7684\u4fe1\u606f\u3002\u8fd9\u4e00\u7ed3\u679c\u4e3a\u8bb8\u591a\u6a21\u578b\u63d0\u4f9b\u4e86\u5408\u7406\u7684\u89e3\u91ca\u3002<\/span><\/p>\n


<\/p>\n

\u7531\u4e8e\u4e00\u4e9b\u539f\u56e0\uff0c\u8be5\u6846\u67b6\u4e2d\u4ecd\u7136\u5b58\u5728\u672a\u89e3\u51b3\u7684\u95ee\u9898\u3002\u9996\u5148\uff0c\u975e\u6b63\u5e38\u7684\u71b5\u4ea7\u751f\u662f\u56e0\u4e3a\u7cfb\u7edf\u52a8\u529b\u5b66\u88ab\u4f7f\u7528\u4e0d\u4e00\u81f4\u7684\u65b9\u5f0f\u6d4b\u91cf\uff0c\u5176\u4e2d\u7f3a\u5c11\u90e8\u5206\u9ea6\u514b\u65af\u97e6\u5996\u7684\u8d21\u732e\u3002\u56e0\u6b64\uff0c\u975e\u6b63\u5e38\u7684\u71b5\u4ea7\u751f\u9519\u8bef\u5730\u6d4b\u91cf\u4e86\u80fd\u91cf\u8017\u6563\u3002\u76f4\u89c2\u4e0a\uff0c\u9ea6\u514b\u65af\u97e6\u5996\u4e0d\u4ec5\u63a7\u5236\u7cfb\u7edf\u72b6\u6001\uff0c\u8fd8\u63a7\u5236\u80fd\u91cf\u4ea4\u6362\uff0c\u4f8b\u5982\u70ed\u6e90\u548c\u7cfb\u7edf\u7684\u529f\u548c\u70ed\u3002\u56e0\u6b64\uff0c\u9ea6\u514b\u65af\u97e6\u5996\u5bf9\u70ed\u6e90\u548c\u7cfb\u7edf\u7684\u71b5\u5747\u6709\u8d21\u732e\u3002\u6709\u4e86\u8fd9\u4e2a\u60f3\u6cd5\uff0c\u7814\u7a76\u4eba\u5458\u53ef\u4ee5\u901a\u8fc7\u5ffd\u7565\u9ea6\u514b\u65af\u97e6\u5996\u8d21\u732e\u7684\u4e00\u4e9b\u90e8\u5206\u6765\u6784\u5efa\u4e0d\u540c\u7684\u975e\u6b63\u5e38\u71b5\u4ea7\u751f\u3002\u76f8\u5e94\u5730\uff0c\u8fd9\u4e9b\u71b5\u4ea7\u751f\u5b58\u5728\u4e0d\u540c\u7684\u6da8\u843d\u5b9a\u7406\uff0c\u8fd9\u4f1a\u5bfc\u81f4\u529f\u6216\u70ed\u7684\u4e0d\u540c\u7684\u7b2c\u4e8c\u5b9a\u5f8b\u4e0d\u7b49\u5f0f\u3002\u56e0\u6b64\uff0c\u7b2c\u4e00\u4e2a\u95ee\u9898\u662f\u54ea\u4e2a\u4e0d\u7b49\u5f0f\u66f4\u5408\u9002\u3002<\/span><\/p>\n


<\/p>\n

\u5176\u6b21\uff0c\u7b2c\u4e8c\u5b9a\u5f8b\u4e0d\u7b49\u5f0f\u53d6\u7b49\u65f6\u4ee3\u8868\u7cfb\u7edf\u5904\u4e8e\u70ed\u5e73\u8861\u72b6\u6001\u3002\u7136\u800c\uff0c\u7cfb\u7edf\u5728\u88ab\u9ea6\u514b\u65af\u97e6\u5996\u63a7\u5236\u65f6\u5e94\u8be5\u5904\u4e8e\u975e\u5e73\u8861\u72b6\u6001\u3002\u8fd9\u8868\u660e\uff0c\u5982\u679c\u9ea6\u514b\u65af\u97e6\u5996\u6709\u6548\u5730\u5de5\u4f5c\uff0c\u90a3\u4e48\u5148\u524d\u6846\u67b6\u4e2d\u7b2c\u4e8c\u5b9a\u5f8b\u4e2d\u7684\u7b49\u5f0f\u5e76\u4e0d\u603b\u662f\u6210\u7acb\u3002\u7814\u7a76\u4eba\u5458\u7684\u4e00\u4e9b\u5de5\u4f5c\u8868\u660e\uff0c\u5f53\u7cfb\u7edf\u5904\u4e8e\u53d7\u63a7\u7684\u975e\u5e73\u8861\u72b6\u6001\u65f6\uff0c\u5b58\u5728\u989d\u5916\u7684\u80fd\u91cf\u8017\u6563[25-28]\u3002\u56e0\u6b64\uff0c\u7b2c\u4e8c\u4e2a\u95ee\u9898\u662f\u8fd9\u79cd\u80fd\u91cf\u8017\u6563\u4ece\u4f55\u800c\u6765\u3002<\/span><\/p>\n


<\/p>\n

<\/p>\n

\u56fe\uff1a\u9ea6\u514b\u65af\u97e6\u5996\u5bf9\u7cfb\u7edf\u548c\u73af\u5883\u71b5\u53d8\u7684\u8d21\u732e<\/span><\/p>\n


<\/p>\n

\u5728\u8be5\u6587\u7ae0\u4e2d\uff0c\u7814\u7a76\u4eba\u5458\u66f4\u6e05\u6670\u5730\u63cf\u7ed8\u4e86\u9ea6\u514b\u65af\u97e6\u5996\u3002\u4ed6\u4eec\u6ce8\u610f\u5230\u4e00\u4e2a\u4e8b\u5b9e\uff0c\u5373\u5f53\u6b63\u786e\u6d4b\u91cf\u7cfb\u7edf\u72b6\u6001\u65f6\uff0c\u53d7\u63a7\u7684\u7cfb\u7edf\u5b9e\u9645\u4e0a\u9075\u5faa\u7b2c\u4e8c\u5b9a\u5f8b\u3002\u9ea6\u514b\u65af\u97e6\u5996\u9047\u5230\u7684\u95ee\u9898\u6d89\u53ca\u6574\u4e2a\u52a8\u529b\u5b66\u8fc7\u7a0b\u4e2d\u7cfb\u7edf\u4e0e\u9ea6\u514b\u65af\u97e6\u5996\u4e4b\u95f4\u7684\u76f8\u4e92\u4f5c\u7528\u3002\u7814\u7a76\u4eba\u5458\u53ef\u4ee5\u91cf\u5316\u4e0d\u540c\u7c97\u7c92\u5ea6\u7ea7\u522b\u7684\u6b63\u786e\u7684\u71b5\u4ea7\u751f\uff0c\u4ee5\u4f9b\u9ea6\u514b\u65af\u97e6\u5996\u63a7\u5236\u3002\u7814\u7a76\u4eba\u5458\u901a\u8fc7\u4ed6\u4eec\u8003\u8651\u71b5\u4ea7\u751f\u7684\u603b\u8d21\u732e\uff0c\u4ece\u800c\u5b8c\u6210\u5bf9\u9ea6\u514b\u65af\u97e6\u5996\u8fdb\u884c\u5b8c\u6574\u8868\u5f81\u7684\u4efb\u52a1\u3002\u5bf9\u4e8e\u5b8c\u6574\u7684\u70ed\u529b\u5b66\u63cf\u8ff0\uff0c\u5e94\u8be5\u53d1\u5c55\u4e00\u5957\u6da8\u843d\u5b9a\u7406\uff0c\u5b83\u4e0d\u4ec5\u5305\u62ec\u7cfb\u7edf\u4e2d\u7684\u71b5\u4ea7\u751f\uff0c\u8fd8\u5305\u62ec\u8017\u6563\u4fe1\u606f<\/span>\uff08dissipative information\uff09<\/span>\u3002\u8017\u6563\u4fe1\u606f\u7684\u6da8\u843d\u5b9a\u7406\u91cf\u5316\u4e86\u975e\u5e73\u8861\u76f8\u4e92\u4f5c\u7528\u3002\u5f53\u9ea6\u514b\u65af\u97e6\u5996\u6709\u6548\u5730\u5de5\u4f5c\u65f6\uff0c\u5b58\u5728\u4ee5\u6b63\u5e73\u5747\u8017\u6563\u4fe1\u606f\u4e3a\u7279\u5f81\u7684\u5185\u5728\u975e\u5e73\u8861\u72b6\u6001\uff0c\u8fd9\u5c31\u662f\u9ea6\u514b\u65af\u97e6\u5996\u5728\u5f88\u591a\u60c5\u51b5\u4e0b\u80fd\u91cf\u8017\u6563\u7684\u6765\u6e90\u3002<\/span><\/p>\n


<\/section>\n
\n
\n
\n

\u53c2\u8003\u6587\u732e<\/strong><\/p>\n<\/section>\n<\/section>\n<\/section>\n

\n
\n
\n
\n
<\/span><\/section>\n

1. J. C. Maxwell, Theory of Heat (Greenwood Press, ed. 3, 1970).<\/span><\/p>\n

2. O. R. Shenker, Maxwell\u2019s Demon 2: Entropy, classical and quantum information computing. Stud. Hist. Philos. Sci. B 35, 537\u2013540 (2004).<\/span><\/p>\n

3. K. Maruyama, F. Nori, V. Vedral, Colloquium: The physics of Maxwell\u2019s demon and information. Rev. Mod. Phys. 81, 1\u201323 (2009).<\/span><\/p>\n

4. L. Szilard, u\u0308ber die entropieverminderung in einem thermodynamischen system bei eingriffen intelligenter Wesen. Z. Physik 53, 840\u2013856 (1929).<\/span><\/p>\n

5. R. Landauer, Irreversibility and heat generation in the computing process. IBM J. Res. Dev. 5, 183\u2013191 (1961).<\/span><\/p>\n

6. M. Esposito, C. Van den Broeck, Second law and Landauer principle far from equilibrium. Europhys. Lett. 95, 40004 (2011).<\/span><\/p>\n

7. S. Deffner, C. Jarzynski, Information processing and the second law of thermodynamics: An inclusive, Hamiltonian approach. Phys. Rev. X 3, 041003 (2013).<\/span><\/p>\n

8. S. Toyabe, T. Sagawa, M. Ueda, E. Muneyuki, M. Sano, Experimental demonstration of information-to-energy conversion and validation of the generalized Jarzynski equality. Nat. Phys. 6, 988\u2013992 (2010).<\/span><\/p>\n

9. D. Mandal, C. Jarzynski, Work and information processing in a solvable model of Maxwell\u2019s demon. Proc. Natl. Acad. Sci. U.S.A. 109, 11641\u201311645 (2012).<\/span><\/p>\n

10. J. V. Koski, A. Kutvonen, I. M. Khaymovich, T. Ala-Nissila, J. P. Pekola, On-chip Maxwell\u2019s demon as an information-powered refrigerator. Phys. Rev. Lett. 115, 260602 (2015).<\/span><\/p>\n

11. V. Serreli, C. F. Lee, E. R. Kay, D. A. Leigh, A molecular information ratchet. Nature 445, 523\u2013527 (2007).<\/span><\/p>\n

12. M. Alvarez-Perez, S. M. Goldup, D. A. Leigh, A. M. Z. Slawin, A chemically driven molecular information ratchet. J. Am. Chem. Soc. 130, 1836\u20131838 (2008).<\/span><\/p>\n

13. A. B. Boyd, J. P. Crutchfield, Maxwell demon dynamics: Deterministic chaos, the Szilard map, and the intelligence of thermodynamic systems. Phys. Rev. Lett. 116, 190601 (2016).<\/span><\/p>\n

14. T. McGrath, N. S. Jones, P. R. ten Wolde, T. E. Ouldridge, Biochemical machines for the interconversion of mutual information and work. Phys. Rev. Lett. 118, 028101 (2017).<\/span><\/p>\n

15. P. P. Potts, P. Samuelsson, Thermodynamic uncertainty relations including measurement and feedback. Phys. Rev. E 100, 052137 (2019).<\/span><\/p>\n

16. C. Jarzynski, Nonequilibrium equality for free energy differences. Phys. Rev. Lett. 78, 2690\u20132693 (1997).<\/span><\/p>\n

17. M. Esposito, G. Schaller, Stochastic thermodynamics for \u201cMaxwell demon\u201d feedbacks. Europhys. lett. 99, 30003 (2012).<\/span><\/p>\n

18. P. Strasberg, G. Schaller, T. Brandes, M. Esposito, Quantum and information thermodynamics: A unifying framework based on repeated interactions. Phys. Rev. X 7, 021003 (2017).<\/span><\/p>\n

19. J. M. Horowitz, M. Esposito, Thermodynamics with continuous information flow. Phys. Rev. X 4, 031015 (2014).<\/span><\/p>\n

20. K. Ptaszynski, M. Esposito, Thermodynamics of quantum information flows. Phys. Rev. Lett. 122, 150603 (2019).<\/span><\/p>\n

21. J. M. Horowitz, H. Sandberg, Second-law-like inequalities with information and their interpretations. New J. Phys. 16, 125007 (2014).<\/span><\/p>\n

22. D. Hartich, A. C. Barato, U. Seifert, Stochastic thermodynamics of bipartite systems: Transfer entropy inequalities and a Maxwell\u2019s demon interpretation. J. Stat. Mech. Theory Exp. 2014, P02016 (2014).<\/span><\/p>\n

23. T. Sagawa, M. Ueda, Generalized Jarzynski equality under nonequilibrium feedback control. Phys. Rev. Lett. 104, 090602 (2010).<\/span><\/p>\n

24. J. M. R. Parrondo, J. M. Horowitz, T. Sagawa, Thermodynamics of information. Nat. Phys. 11, 131\u2013139 (2015).<\/span><\/p>\n

25. A. C. Barato, U. Seifert, Unifying three perspectives on information processing in stochastic thermodynamics. Phys. Rev. Lett. 112, 090601 (2014).<\/span><\/p>\n

26. A. B. Boyd, D. Mandal, J. P. Crutchfield, Identifying functional thermodynamics in autonomous Maxwellian ratchets. New J. Phys. 18, 023049 (2016).<\/span><\/p>\n

27. C. Aghamohammadi, J. P. Crutchfield, Thermodynamics of random number generation. Phys. Rev. E 95, 062139 (2017).<\/span><\/p>\n

28. A. B. Boyd, M. Dibyendu, J. P. Crutchfield, Thermodynamics of modularity: Structural costs beyond the Landauer bound. Phys. Rev. X 8, 031036 (2018).<\/span><\/p>\n


<\/span>
<\/section>\n


<\/p>\n<\/section>\n<\/section>\n<\/section>\n<\/section>\n

\n
\n

\uff08\u53c2\u8003\u6587\u732e\u53ef\u4e0a\u4e0b\u6ed1\u52a8<\/strong>\u67e5\u770b\uff09<\/p>\n<\/section>\n<\/section>\n


<\/section>\n

<\/section>\n
\n
\n
\n
\n

\u590d\u6742\u79d1\u5b66\u6700\u65b0\u8bba\u6587<\/strong><\/p>\n<\/section>\n<\/section>\n<\/section>\n<\/section>\n

\n


<\/p>\n<\/section>\n

\u96c6\u667a\u6591\u56fe\u9876\u520a\u8bba\u6587\u901f\u9012\u680f\u76ee\u4e0a\u7ebf\u4ee5\u6765\uff0c\u6301\u7eed\u6536\u5f55\u6765\u81eaNature\u3001Science<\/span>\u7b49\u9876\u520a\u7684\u6700\u65b0\u8bba\u6587\uff0c\u8ffd\u8e2a\u590d\u6742\u7cfb\u7edf\u3001\u7f51\u7edc\u79d1\u5b66\u3001\u8ba1\u7b97\u793e\u4f1a\u79d1\u5b66\u7b49\u9886\u57df\u7684\u524d\u6cbf\u8fdb\u5c55\u3002\u73b0\u5728\u6b63\u5f0f\u63a8\u51fa\u8ba2\u9605\u529f\u80fd\uff0c\u6bcf\u5468\u901a\u8fc7\u5fae\u4fe1\u670d\u52a1\u53f7\u300c\u96c6\u667a\u6591\u56fe\u300d\u63a8\u9001\u8bba\u6587\u4fe1\u606f\u3002\u626b\u63cf\u4e0b\u65b9\u4e8c\u7ef4\u7801\u5373\u53ef\u4e00\u952e\u8ba2\u9605\uff1a<\/span>
<\/p>\n

<\/p>\n

\n


<\/p>\n<\/section>\n


<\/p>\n

\n

\u63a8\u8350\u9605\u8bfb<\/span><\/strong><\/strong><\/p>\n