{"id":158689,"date":"2018-11-12T06:13:10","date_gmt":"2018-11-11T22:13:10","guid":{"rendered":"\/\/m.iemloyee.com\/?p=158689"},"modified":"2018-11-11T19:14:40","modified_gmt":"2018-11-11T11:14:40","slug":"%e6%a2%b3%e7%90%86%ef%bc%9a%e6%9d%90%e6%96%99%e7%83%ad%e5%8a%9b%e5%ad%a6%e7%a0%94%e7%a9%b6%e6%96%b9%e9%9d%a2%e5%80%bc%e5%be%97%e9%98%85%e8%af%bb%e7%9a%84%e7%bb%bc%e8%bf%b0","status":"publish","type":"post","link":"\/\/m.iemloyee.com\/?p=158689","title":{"rendered":"\u68b3\u7406\uff1a\u6750\u6599\u70ed\u529b\u5b66\u7814\u7a76\u65b9\u9762\u503c\u5f97\u9605\u8bfb\u7684\u7efc\u8ff0"},"content":{"rendered":"<p>\u5728\u5f53\u4eca\u6750\u6599\u79d1\u5b66\u7684\u7814\u7a76\u548c\u53d1\u5c55\u4e2d\uff0c\u57fa\u4e8e\u70ed\u529b\u5b66\u7684\u63a2\u7d22\u5df2\u7ecf\u975e\u5e38\u5e7f\u6cdb\uff0c\u5176\u4e2d\uff0c\u6709\u4e9b\u662f\u4ece\u8ba1\u7b97\u6a21\u62df\u7684\u89d2\u5ea6\u5f00\u53d1\u548c\u6539\u5584\u6750\u6599\uff0c\u6709\u4e9b\u662f\u5bf9\u4ee5\u524d\u7684\u7406\u8bba\u6216\u8ba1\u7b97\u6a21\u578b\u7684\u4fee\u6b63\uff0c\u6709\u4e9b\u5219\u662f\u5bf9\u7406\u8bba\u672c\u8eab\u7684\u6269\u5145\u548c\u53d1\u5c55\uff0c\u5448\u73b0\u51fa\u5bf9\u7279\u5b9a\u9886\u57df\u7684\u67d0\u4e9b\u5177\u6709\u7c7b\u4f3c\u5173\u7cfb\u7684\u7ed3\u6784\u91c7\u7528\u76f8\u4f3c\u7684\u7406\u8bba\u6a21\u578b\u548c\u7814\u7a76\u65b9\u6cd5\u3002\u672c\u6587\u6c47\u603b\u4e86\u8fd1\u671f\u4e00\u4e9b\u6750\u6599\u70ed\u529b\u5b66\u65b9\u9762\u7684\u7efc\u8ff0\u548c\u6bd4\u8f83\u65b0\u9896\u7684\u7814\u7a76\u8bba\u6587\uff0c\u5305\u62ec\u4f4e\u6e29\u4e0b\u7b2c\u4e09\u5b9a\u5f8b\u7684\u7ea6\u675f\u95ee\u9898\u3001\u6676\u4f53\u751f\u957f\u7684\u70ed\u529b\u5b66\u8ba1\u7b97\u3001\u67d0\u4e9b\u7cfb\u7edf\u7684\u70ed\u529b\u5b66\u7406\u8bba\u8ba1\u7b97\u548c\u6df7\u5408\u5206\u5b50\u52a8\u529b\u5b66\/\u8499\u7279\u5361\u7f57\u6a21\u62df\u8ba1\u7b97\uff0c\u4ee5\u53ca\u7eb3\u7c73\u7ed3\u6784\u751f\u957f\u7b49\u65b9\u9762\u3002<\/p>\n<p><strong><b>\u6676\u4f53\u751f\u957f<\/b><\/strong><\/p>\n<p>Tatau Nishinaga\u3001R.F. Sekerka\u7b49\u4eba\u5728\u70ed\u529b\u5b66\u89d2\u5ea6\u63ed\u793a\u4e86\u6676\u4f53\u751f\u957f\u7684\u673a\u7406\uff0cTatau Nishinaga\u4ece\u5b9a\u4e49\u7684\u4ea5\u59c6\u970d\u5179\u3001\u73bb\u5c14\u5179\u66fc\u7684\u71b5\u516c\u5f0f\u548c\u5409\u5e03\u65af\u81ea\u7531\u80fd\u51fa\u53d1\uff0c\u63a2\u8ba8\u4e86\u4ee5Toschev\u65b9\u6cd5\u4e3a\u4f8b\u7684\u5f62\u6210\u5e73\u8861\u6838\u548c\u975e\u5e73\u8861\u7c07\u7684\u81ea\u7531\u80fd\u4e0e\u534a\u5f84\u7684\u5173\u7cfb\uff0c\u8bc1\u660e\u4e86\u5f62\u6210\u7c07\u7684\u81ea\u7531\u80fd\u6700\u5927\u503c\u5904\u5bf9\u5e94\u4e8e\u4e34\u754c\u6838\uff0c\u5c0f\u4e8e\u4e34\u754c\u6838\u7684\u7c07\u6d88\u5931\u800c\u8f83\u5927\u7684\u7c07\u5219\u8fde\u7eed\u751f\u957f\u3002\u6700\u540e\uff0c\u901a\u8fc7\u6c42\u89e3\u8d28\u91cf\u4f5c\u7528\u5b9a\u5f8b\u548c\u521d\u59cb\u6761\u4ef6\uff0c\u8ba1\u7b97\u4e86\u6240\u6709\u6c14\u6001\u7269\u8d28\u7684\u5206\u538b\uff0c\u91c7\u7528\u672a\u6c89\u79ef\u5728\u7cfb\u7edf\u4e2d\u7684\u5143\u7d20\u5b88\u6052\u5b9a\u5f8b\u6765\u63a8\u5bfc\u5c01\u95ed\u7cfb\u7edf\u4e2d\u7684\u5c42\u6d41\u901f\u7387\u548c\u6c14\u6d41\u7cfb\u7edf\u4e2d\u7684\u751f\u957f\u901f\u7387\uff0c\u5e76\u5229\u7528\u751f\u957f\u5143\u7d20\u4e0e\u975e\u6c89\u79ef\u5143\u7d20\u7684\u901a\u91cf\u6bd4\u6765\u6d88\u9664\u751f\u957f\u7cfb\u7edf\u4e2d\u51e0\u4f55\u53d8\u5316\u7684\u5f71\u54cd\u3002<\/p>\n<p>\u56fe1 \u5409\u5e03\u65af\u81ea\u7531\u80fd\u5728\u84b8\u6c14\u538bp\u4e0b\u4ea7\u751f\u534a\u5f84\u4e3ar\u7684\u56e2\u7c07<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-158706 size-full aligncenter\" src=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72472-6.png\" alt=\"\" width=\"240\" height=\"217\" \/>Tatau Nishinaga\uff0cThermodynamics-for understanding crystal growth[J]\uff0cProgress in Crystal Growth and Characterization of Materials 62 (2016) 43\u201357<\/p>\n<p>\u6587\u732e\u94fe\u63a5\uff1a<a href=\"http:\/\/dx.doi.org\/10.1016\/j.pcrysgrow.2016.04.001\"><u>http:\/\/dx.doi.org\/10.1016\/j.pcrysgrow.2016.04.001<\/u><\/a><\/p>\n<p>F. Sekerka, W.J. Boettinger, G.B. McFadden\uff0cSurface morphologies due to grooves at moving grainboundaries having stress-driven fluxes\u00a0[J]\u00a0\uff0cActa Materialia 61 (2013) 7216\u20137226<\/p>\n<p>\u6587\u732e\u94fe\u63a5\uff1a<a href=\"http:\/\/dx.doi.org\/10.1016\/j.actamat.2013.08.026\"><u>http:\/\/dx.doi.org\/10.1016\/j.actamat.2013.08.026<\/u><\/a><\/p>\n<p><strong><b>\u70ed\u529b\u5b66\u7b2c\u4e09\u5b9a\u5f8b\uff1a\u4f4e\u6e29\u4e0b\u7684\u76f8\u5e73\u8861\u548c\u76f8\u56fe<\/b><\/strong><\/p>\n<p>\u70ed\u529b\u5b66\u7b2c\u4e09\u5b9a\u5f8b\u7684\u80fd\u65af\u7279-\u666e\u6717\u514b-\u897f\u8499\u8868\u8ff0\u4e3a\uff1a\u7edd\u5bf9\u96f6\u5ea6\uff080 K\uff09\u4e3a\u7269\u8d28\u6e29\u5ea6\u7684\u57fa\u672c\u4e0b\u9650\uff0c\u4ee5\u53ca\u6d4b\u91cf\u548c\u8ba1\u7b97\u7269\u8d28\u7edd\u5bf9\u71b5\u7684\u81ea\u7136\u539f\u70b9\uff1b\u70ed\u529b\u5b66\u5e73\u8861\u4e2d\u6240\u6709\u7269\u8d28\u7684\u71b5\u5728T = 0 K\u65f6\u4e3a\u96f6\uff0c\u5373\uff0cS<sub>0<\/sub>\u00a0= 0\u72ec\u7acb\u4e8e\u538b\u529b\u3001\u5916\u90e8\u573a\u6216\u805a\u96c6\u72b6\u6001\uff1b\u53ea\u8981\u5904\u4e8e\u70ed\u529b\u5b66\u5e73\u8861\u72b6\u6001\uff0c\u70ed\u529b\u5b66\u7b2c\u4e09\u5b9a\u5f8b\u53ef\u4ee5\u5355\u72ec\u5e94\u7528\u4e8e\u6750\u6599\u7684\u5404\u4e2a\u65b9\u9762\u6216\u5b50\u7cfb\u7edf\uff0c\u4f8b\u5982\uff0c\u65cb\u8f6c\u7cfb\u7edf\u3001\u632f\u52a8\u548c\u65cb\u8f6c\u72b6\u6001\u7b49\u3002<\/p>\n<p>\u5728\u7b2c\u4e09\u5b9a\u5f8b\u7684\u65e9\u671f\u8ba8\u8bba\u4e2d\uff0c\u7231\u56e0\u65af\u5766\u8ba4\u4e3a\u4e25\u683c\u7684\u7b2c\u4e09\u5b9a\u5f8b\u7684\u8868\u8ff0\u9700\u8981\u63a5\u89e6\u7269\u8d28\u7684\u91cf\u5b50\u7406\u8bba\u3002\u666e\u6717\u514b\u5bf9\u71b5\u7684\u7edf\u8ba1\u89e3\u91ca\u4f7f\u7528\u73bb\u5c14\u5179\u66fc\u7684\u71b5\u63cf\u8ff0\uff0c\u65ad\u8a00\u5904\u4e8eT = 0 K\u7684\u5e73\u8861\u72b6\u6001\u4e0b\u7684\u5404\u4e2a\u76f8\u4f4d\u72b6\u6001\u662f\u975e\u7b80\u5e76\u7684\uff0c\u5bf9\u4e8e\u6750\u6599\u7cfb\u7edf\u6216\u5b50\u7cfb\u7edf\u4e2d\u4efb\u4f55\u7c92\u5b50\uff08\u6216\u51c6\u7c92\u5b50\uff09\u7684\u7ec4\u5408\uff0c\u5373\u4f7f\u975e\u5e38\u5fae\u5f31\u7684\u76f8\u4e92\u4f5c\u7528\uff0c\u7c92\u5b50\u5c06\u5728T = 0 K\u5904\u6709\u5e8f\uff0c\u4ece\u800c\u4ea7\u751f\u5177\u6709S<sub>0<\/sub>\u7684\u6700\u4f4e\u80fd\u91cf\u57fa\u6001\u3002<\/p>\n<p>\u897f\u8499\u5f3a\u8c03\u70ed\u529b\u5b66\u7cfb\u7edf\u901a\u5e38\u662f\u5404\u79cd\u70ed\u7cfb\u7edf\u6216\u5b50\u7cfb\u7edf\u7684\u590d\u5408\u7269\uff0c\u6bcf\u4e00\u4e2a\u90fd\u53ef\u4ee5\u5728\u70ed\u529b\u5b66\u5e73\u8861\u4e0b\u5355\u72ec\u5904\u7406\u3002\u6750\u6599\u7684\u67d0\u4e9b\u5b50\u7cfb\u7edf\u53ef\u4ee5\u5728\u7ed9\u5b9a\u7684\u70ed\u65f6\u95f4\u5185\u51b7\u5374\u81f30K\u671f\u95f4\u8f83\u5bb9\u6613\u5730\u5efa\u7acb\u5e73\u8861\uff0c\u800c\u5176\u4ed6\u5b50\u7cfb\u7edf\u76f8\u5bf9\u70ed\u5f1b\u8c6b\u800c\u53ef\u80fd\u65e0\u6cd5\u5728\u4f4e\u6e29\u4e0b\u8fbe\u5230\u5e73\u8861\u3002\u6839\u636e\u7b2c\u4e09\u5b9a\u5f8b\uff0c\u5e73\u8861\u5b50\u7cfb\u7edf\u7684\u71b5\u5728T = 0 K\u5904\u6d88\u5931\uff0c\u800c\u53d7\u7ea6\u675f\u7684\u5b50\u7cfb\u7edf\u5c06\u6b8b\u4f59\u71b5\u5e26\u52300 K\uff0c\u5f3a\u8c03\u7b2c\u4e09\u5b9a\u5f8b\u4ec5\u9002\u7528\u4e8e\u70ed\u529b\u5b66\u5e73\u8861\u4e2d\u7684\u7cfb\u7edf\u6216\u5b50\u7cfb\u7edf\u3002\u5bf9\u4e8e\u5728T = 0 K\u7684\u70ed\u529b\u5b66\u5e73\u8861\u7684\u6750\u6599\uff0c\u7cfb\u7edf\u5e94\u8be5\u7531\u7eaf\u76f8\u53ca\u5176\u6df7\u5408\u7269\u548c\u5177\u6709\u96f6\u71b5\u7684\u6709\u5e8f\u76f8\u7ec4\u6210\u3002<\/p>\n<p>\u8fd1\u51e0\u5341\u5e74\u6765\uff0c\u5728\u8ba1\u7b97\u70ed\u529b\u5b66\uff08Calphad\uff09\u548c\u7406\u8bba\u65b9\u6cd5\uff08CVM\uff09\u7684\u5e94\u7528\u65b9\u9762\u53d6\u5f97\u4e86\u91cd\u5927\u8fdb\u5c55\uff0c\u5305\u62ec\u6240\u8c13\u7684\u7b2c\u4e00\u539f\u7406\u65b9\u6cd5\uff0c\u7528\u4e8e\u70ed\u529b\u5b66\u6027\u8d28\u5efa\u6a21\u548c\u8ba1\u7b97\u6750\u6599\u76f8\u56fe\u3002David E. Laughlin\u7b49\u4eba\u9610\u660e\u4e86\u70ed\u529b\u5b66\u7b2c\u4e09\u5b9a\u5f8b\u7684\u5185\u5bb9\u53ca\u5176\u5728\u70ed\u529b\u5b66\u5e94\u7528\u4e8e\u6750\u6599\u79d1\u5b66\u76f8\u5e73\u8861\u4e2d\u7684\u4f5c\u7528\uff0c\u63d0\u51fa\u5728\u8bc4\u4f30\u4f4e\u6e29\u76f8\u5e73\u8861\u53ca\u5176\u70ed\u529b\u5b66\u6027\u8d28\u65f6\u5e94\u8003\u8651\u70ed\u529b\u5b66\u7b2c\u4e09\u5b9a\u5f8b\u7684\u7ea6\u675f\uff0c\u8fd9\u5bf9\u4e8e\u9884\u6d4b\u53ef\u80fd\u7684\u4f4e\u6e29\u76f8\u573a\u548c\u8fb9\u754c\u4ee5\u53ca\u9884\u6d4b\u70ed\u529b\u5b66\u4e0a\u4e00\u81f4\u7684\u76f8\u56fe\u914d\u7f6e\u662f\u6709\u4ef7\u503c\u7684\u3002<\/p>\n<p>\u56fe2 \u4e0d\u540c\u76f8\u4e92\u4f5c\u7528\u4e0bCVM\u548c\u8499\u7279\u5361\u7f57\u65b9\u6cd5\u7684\u7ed3\u679c\u6bd4\u8f83<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-158707 size-full aligncenter\" src=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72473-5.png\" alt=\"\" width=\"414\" height=\"614\" srcset=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72473-5.png 414w, \/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72473-5-202x300.png 202w\" sizes=\"(max-width: 414px) 100vw, 414px\" \/>David E. Laughlin, William A. Soffa\uff0cThe Third Law of Thermodynamics: Phase equilibria and phasediagrams at low temperatures\u00a0[J]\u00a0\uff0cActa Materialia 145 (2018) 49-61<\/p>\n<p>\u6587\u732e\u94fe\u63a5\uff1a<a href=\"https:\/\/doi.org\/10.1016\/j.actamat.2017.11.037\"><u>https:\/\/doi.org\/10.1016\/j.actamat.2017.11.037<\/u><\/a><\/p>\n<p>Jose\u2032\u00a0P. Abriataa\u7b49\u4eba\u6307\u51fa\uff0c\u5bf9\u4e8e\u666e\u901a\u6750\u6599\uff0c0 K\u7684\u5e73\u8861\u72b6\u6001\u540c\u65f6\u6ee1\u8db3\u80fd\u91cf\u548c\u71b5\u5904\u4e8e\u6700\u4f4e\u53ef\u80fd\u503c\u7684\u4e24\u4e2a\u6761\u4ef6\uff0c\u5982\u5bf9\u72b6\u6001\u53d8\u91cf\u65bd\u52a0\u7684\u8fdb\u5316\u7ea6\u675f\u6240\u5141\u8bb8\u7684\u3002\u6b64\u5916\uff0c\u81ea\u7531\u5185\u90e8\u72b6\u6001\u53d8\u91cf\uff08\u4f8b\u5982\u5171\u5b58\u76f8\u7684\u5e73\u8861\u7ec4\u6210\uff09\u5fc5\u987b\u4f7f\u5f97\u5b83\u4eec\u4f5c\u4e3a\u6e29\u5ea6\u51fd\u6570\u7684\u5e73\u8861\u503c\u7684\u53d8\u5316\u7387\u57280K\u65f6\u4e3a\u96f6\u3002<\/p>\n<p>\u56fe3 \u71b5\u3001\u5185\u90e8\u80fd\u91cf\u548c\u8868\u9762\u4e0e\u7b2c\u4e09\u5b9a\u5f8b\u7684\u4e0d\u53ef\u83b7\u5f97\u6027\u9648\u8ff0\u548c\u80fd\u65af\u7279\u9648\u8ff0\u4e0d\u4e00\u81f4<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-158708 size-full aligncenter\" src=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72474-5.png\" alt=\"\" width=\"428\" height=\"286\" srcset=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72474-5.png 428w, \/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72474-5-300x200.png 300w\" sizes=\"(max-width: 428px) 100vw, 428px\" \/>Jose\u2032 Abriataa, David E. Laughlin\uff0cThe Third Law of Thermodynamics and lowtemperature phase stability\u00a0[J]\uff0cProgress in Materials Science 49 (2004) 367\u2013387<\/p>\n<p>doi:10.1016\/S0079-6425(03)00030-6<\/p>\n<p><strong><b>\u6c22\u5316\u77f3\u58a8\u70ef<\/b><\/strong><\/p>\n<p>Kumar\u7b49\u4eba\u901a\u8fc7\u57fa\u4e8e\u5bc6\u5ea6\u6cdb\u51fd\u7406\u8bba\u7684\u5e73\u9762\u6ce2\u8d5d\u52bf\u65b9\u6cd5\u8ba1\u7b97\u4e86\u6905\u5b50\uff0c\u8239\u548c\u4e09\u8f6e\u8f66\u7b49\u4e09\u79cd\u7a33\u5b9a\u7ed3\u6784\u4e2d\u6c22\u5316\u77f3\u58a8\u70ef\u7684\u7ed3\u6784\u3001\u7535\u5b50\u3001\u5149\u5b66\u548c\u70ed\u5b66\u6027\u8d28\u3002\u8ba1\u7b97\u4e8619\u4e2a\u53c2\u6570\u7684\u503c\uff0c\u5e76\u9996\u6b21\u7814\u7a76\u4e86\u4ecb\u7535\u5e38\u6570\uff0c\u53cc\u6298\u5c04\uff0c\u7b49\u79bb\u5b50\u4f53\u80fd\u91cf\u548c\u5fb7\u62dc\u6e29\u5ea6\u7b49\u56db\u4e2a\u53c2\u6570\uff0c\u53d1\u73b0\u6676\u683c\u5e38\u6570\u3001\u952e\u957f\u3001\u952e\u89d2\u3001\u80fd\u9699\u3001\u7ed3\u5408\u80fd\u548c\u539f\u5b50\u79cd\u7fa4\u7b49\u65b9\u9762\u7684\u8ba1\u7b97\u503c\u4e0e\u8bd5\u9a8c\u503c\u4e00\u81f4\uff0c\u5bf9\u80fd\u5e26\u7ed3\u6784\u548c\u72b6\u6001\u5bc6\u5ea6\u7684\u7814\u7a76\u8868\u660eC-2p\u548cH-s\u6001\u5728s-p\u6742\u5316\u4ea7\u751f\u80fd\u9699\u65b9\u9762\u8d77\u91cd\u8981\u4f5c\u7528\uff0c\u800c\u8fd9\u4e9b\u53c2\u6570\u7684\u4fe1\u606f\u5bf9\u4e8e\u5728IC\u8bbe\u8ba1\u4e2d\u9009\u62e9\u886c\u5e95\u6750\u6599\u548c\u8bbe\u8ba1\u5404\u79cd\u7ebf\u6027\u548c\u975e\u7ebf\u6027\u5149\u7535\u5668\u4ef6\u975e\u5e38\u91cd\u8981\u3002<\/p>\n<p>\u56fe4 \u4e09\u79cd\u4e0d\u540c\u7684\u7ed3\u6784\u548cEnergy-Volume\u66f2\u7ebf\uff1a\uff08a\uff09\u6905\u5b50\uff0c\uff08b\uff09\u8239\u548c\uff08c\uff09\u4e09\u8f6e\u8f66<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-158709 size-full aligncenter\" src=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72475-5.png\" alt=\"\" width=\"659\" height=\"520\" srcset=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72475-5.png 659w, \/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72475-5-300x237.png 300w\" sizes=\"(max-width: 659px) 100vw, 659px\" \/>Kumar, R. Santosh, S. Chandra\uff0cFirst-principle calculations of structural, electronic, optical and thermalproperties of hydrogenated graphene\u00a0[J]\uff0cMaterials Science &amp; Engineering B 226 (2017) 64\u201371<\/p>\n<p>\u6587\u732e\u94fe\u63a5\uff1a<a href=\"http:\/\/dx.doi.org\/10.1016\/j.mseb.2017.09.005\"><u>http:\/\/dx.doi.org\/10.1016\/j.mseb.2017.09.005<\/u><\/a><\/p>\n<p><strong><b>Cr-S\u7cfb\u7edf<\/b><\/strong><\/p>\n<p>Minoru Arita\u7b49\u4eba\u5229\u7528\u516c\u5e03\u7684Cr-S\u7cfb\u7edf\u7684\u84b8\u6c7d\u538b\u529b\u6d4b\u91cf\u503c\u7528\u4e8e\u786e\u5b9a\u76f8\u5173\u7684\u70ed\u529b\u5b66\u6027\u8d28\uff0c\u5e76\u91c7\u7528\u7edf\u8ba1\u70ed\u529b\u5b66\u6765\u6c42\u5f97\u914d\u5206\u51fd\u6570\u3001\u76f8\u4e92\u4f5c\u7528\u80fd\u548c\u81ea\u7531\u80fd\uff0c\u4ee5\u8868\u5f81\u6d4b\u91cf\u4e2d\u51fa\u73b0\u7684\u751f\u6210\u76f8\uff0c\u8ba1\u7b97\u51fa\u83f1\u5f62Cr<sub>2<\/sub>S<sub>3<\/sub>\u7684\u751f\u6210\u7113\u548c\u6cbfCr\u5c42\u7684Cr-Cr\u76f8\u4e92\u4f5c\u7528\u80fd\uff0c\u4ee5\u53ca\u5728873-1364K\u4e4b\u95f4\u7684\u76f8\u7a33\u5b9a\u6027\u7684\u53d8\u5316\uff0c\u901a\u8fc7\u4e00\u79cd\u51c6\u5316\u5b66\u65b9\u6cd5\u63ed\u793a\u4e86Cr\u539f\u5b50\u5728\u539f\u5b50\u5c42\u548c\u76f8\u90bb\u5c42\u4e4b\u95f4\u7684\u504f\u6790\u3002<\/p>\n<p>\u56fe5 \u201cCr3S4\u201d\u3001\u201cCr2S3\u201d\u548c\u516d\u65b9\u5bc6\u5806\u79efCr\u5c42\u4e2d\u539f\u5b50\u7684\u6392\u5217<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-158710 size-full aligncenter\" src=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72476-5.png\" alt=\"\" width=\"631\" height=\"858\" srcset=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72476-5.png 631w, \/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72476-5-221x300.png 221w\" sizes=\"(max-width: 631px) 100vw, 631px\" \/><\/p>\n<p>Minoru Arita\uff0cThermodynamics of the Cr\u2013S System\u00a0[J]\uff0cActa Materialia 53 (2005) 5241\u20135255<\/p>\n<p>\u6587\u732e\u94fe\u63a5\uff1a<a href=\"http:\/\/dx.doi:10.1016\/j.actamat.2005.07.037\"><u>http:\/\/dx.doi:10.1016\/j.actamat.2005.07.037<\/u><\/a><\/p>\n<p><strong><b>Pb-Sn\u7cfb\u7edf<\/b><\/strong><\/p>\n<p>Seyed Alireza Etesami\u7b49\u4eba\u63d0\u51fa\u4e86\u4e00\u5957\u65b0\u6539\u8fdb\u7684\u5d4c\u5165\u5f0f\u539f\u5b50\u65b9\u6cd5\u53c2\u6570\uff0c\u7528\u6765\u63cf\u8ff0Pb-Sn\u7cfb\u7edf\u7684\u7194\u70b9\u3001\u5f39\u6027\u5e38\u6570\u548c\u6df7\u5408\u7113\u7b49\uff0c\u5e76\u5229\u7528\u6df7\u5408\u5206\u5b50\u52a8\u529b\u5b66\/\u8499\u7279\u5361\u7f57\u6a21\u62df\u8ba1\u7b97\u4e86Pb-Sn\u5408\u91d1\u7684\u5bccSn\u4fa7\u7684\u76f8\u56fe\uff0c\u6b64\u5916\u8fd8\u4ecb\u7ecd\u4e86Pb-Sn\u6db2\u6001\u5408\u91d1\u7684\u7ed3\u6784\u56e0\u7d20\u4ee5\u53ca\u4e0e\u6e29\u5ea6\u76f8\u5173\u7684\u70ed\u81a8\u80c0\u7cfb\u6570\u548c\u70ed\u5bb9\u91cf\u3002<\/p>\n<p>\u56fe6 MEAM\u539f\u5b50\u4f5c\u7528\u52bf\u548c\u6df7\u5408\u5206\u5b50\u52a8\u529b\u5b66\/\u8499\u7279\u5361\u7f57\u6a21\u62df<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-158711 size-full aligncenter\" src=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72477-4.png\" alt=\"\" width=\"681\" height=\"538\" srcset=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72477-4.png 681w, \/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72477-4-300x237.png 300w\" sizes=\"(max-width: 681px) 100vw, 681px\" \/>Seyed Alireza Etesami, Michael I. Baskes, Mohamed Laradji, and Ebrahim Asadi\uff0cThermodynamics of Solid Sn and Pb-Sn Liquid Mixtures using Molecular DynamicsSimulations\u00a0[J]\uff0cActa Materialia (2018)\uff0c<\/p>\n<p>doi: https:\/\/\u00a0doi.org\/10.1016\/j.actamat.2018.09.036.<\/p>\n<p><strong><b>\u81ea\u6d3d\u7684\u51c6\u8c10\u6ce2\u8fd1\u4f3c\uff08SC-QHA\uff09<\/b><\/strong><\/p>\n<p>\u81ea\u6d3d\u7684\u51c6\u8c10\u6ce2\u8fd1\u4f3c\uff08SC-QHA\uff09\u65b9\u6cd5\u7528\u4e8e\u8ba1\u7b97\u56fa\u4f53\u5728\u6709\u9650\u6e29\u5ea6\u4e0b\u7684\u70ed\u81a8\u80c0\u548c\u70ed\u529b\u5b66\u51fd\u6570\u7b49\u65b9\u9762\u5177\u6709\u9ad8\u6548\u7387\u548c\u9ad8\u7cbe\u5ea6\uff0c\u5b83\u6bd4\u4f20\u7edf\u7684QHA\u65b9\u6cd5\u9700\u8981\u66f4\u5c11\u7684\u58f0\u5b50\u8ba1\u7b97\uff0c\u5e76\u4e14\u8fd8\u4fbf\u4e8e\u5206\u6790\u5b8f\u89c2\u70ed\u73b0\u8c61\u7684\u5fae\u89c2\u8d77\u6e90\uff0c\u65e2\u662f\u4e00\u79cd\u6709\u6548\u7684\u8ba1\u7b97\u548c\u6709\u7528\u7684\u7406\u8bba\u5de5\u5177\uff0c\u4e5f\u53ef\u4ee5\u7406\u89e3\u5b9e\u9a8c\u786e\u5b9a\u7684\u6750\u6599\u7684\u975e\u8c10\u6027\u8d28\u3002<\/p>\n<p>Huang\u7b49\u4eba\u8bc4\u4f30\u4e86SC-QHA\u65b9\u6cd5\uff0c\u5e76\u5c06\u5176\u5e94\u7528\u4e8e\u7814\u7a76Ca<sub>3<\/sub>Ti<sub>2<\/sub>O<sub>7<\/sub>\u7684\u70ed\u81a8\u80c0\u548c\u70ed\u529b\u5b66\uff0c\u8fd9\u5bf9\u4e8e\u4f20\u7edf\u7684QHA\u65b9\u6cd5\u6765\u8bf4\u5b58\u5728\u4e00\u5b9a\u7684\u6311\u6218\u6027\u3002\u901a\u8fc7\u57fa\u4e8e\u7845\uff0c\u91d1\u521a\u77f3\u548c\u6c27\u5316\u94dd\u7684SC-QHA\u65b9\u6cd5\u7684\u6548\u7387\u548c\u51c6\u786e\u5ea6\u6821\u51c6\u8868\u660e\uff0c\u4e8c\u9636SC-QHA\u65b9\u6cd5\u6bd4\u4e00\u9636SC-QHA\u5b9e\u65bd\u7cfb\u7edf\u66f4\u51c6\u786e\uff0c\u4f461st-SC-QHA\u65b9\u6cd5\u662f\u7528\u4e8e\u6d4b\u8bd5\u5bc6\u5ea6\u6cdb\u51fd\u7406\u8bba\u8ba1\u7b97\u4e2d\u6240\u9700\u7684\u8ba1\u7b97\u53c2\u6570\u3002<\/p>\n<p>SC-QHA\u65b9\u6cd5\u53ef\u4ee5\u663e\u8457\u964d\u4f4e\u5404\u79cd\u51c6\u8c10\u6ce2\u70ed\u6027\u8d28\u7684\u8ba1\u7b97\u5f00\u9500\uff0c\u7279\u522b\u662f\u5f53\u9700\u8981\u8003\u8651\u5927\u91cf\u7ed3\u6784\u6216\u56fa\u4f53\u7ed3\u6784\u590d\u6742\u65f6\u3002\u9884\u8ba1\u8be5\u7b97\u6cd5\u5c06\u9002\u7528\u4e8e\u5404\u79cd\u9886\u57df\uff0c\u5305\u62ec\u6c27\u5316\uff0c\u8150\u8680\uff0c\u9ad8\u538b\u7269\u7406\uff0c\u94c1\u7535\u4f53\u548c\u9ad8\u901a\u91cf\u7ed3\u6784\u7b5b\u9009\u7b49\u65b9\u9762\u9700\u8981\u6e29\u5ea6\u6548\u5e94\u6765\u63cf\u8ff0\u771f\u5b9e\u6027\u8d28\u65f6\uff0c\u53ef\u4ee5\u6269\u5c55\u5230\u91d1\u5c5e\u548c\u78c1\u6027\u56fa\u4f53\uff0c\u6b64\u5916\uff0c\u57fa\u672c\u7684SC-QHA\u7b97\u6cd5\u53ef\u4ee5\u8f6c\u79fb\u5230\u8d85\u51fa\u51c6\u8c10\u6ce2\u8fd1\u4f3c\u7684\u8303\u56f4\uff0c\u5e76\u51cf\u5c11\u7528\u4e8e\u6a21\u62df\u9ad8\u9636\u975e\u8c10\u6027\u8d28\u7684\u8ba1\u7b97\u5f00\u9500\u3002<\/p>\n<p>\u56fe7 SC-QHA\u65b9\u6cd5\u7684\u5de5\u4f5c\u6d41\u7a0b\uff08\u5de6\uff09\u4e0e\u4f20\u7edf\u7684QHA\u65b9\u6cd5\uff08\u53f3\uff09\u7684\u6bd4\u8f83<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-158712 size-full aligncenter\" src=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72478-3.png\" alt=\"\" width=\"423\" height=\"531\" srcset=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72478-3.png 423w, \/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72478-3-239x300.png 239w\" sizes=\"(max-width: 423px) 100vw, 423px\" \/>Liang-Feng Huang, Xue-Zeng Lu, Emrys Tennessen, James M. Rondinelli\uff0cAn efficient ab-initio quasiharmonic approach for the thermodynamicsof solids\u00a0[J]\uff0cComputational Materials Science 120 (2016) 84\u201393\uff0c<\/p>\n<p>\u6587\u732e\u94fe\u63a5\uff1a<a href=\"http:\/\/dx.doi.org\/10.1016\/j.commatsci.2016.04.012\"><u>http:\/\/dx.doi.org\/10.1016\/j.commatsci.2016.04.012<\/u><\/a>.<\/p>\n<p><strong><b>\u7eb3\u7c73\u7ed3\u6784\u751f\u957f<\/b><\/strong><\/p>\n<p>\u81ea\u7ec4\u88c5\u7eb3\u7c73\u7ed3\u6784\uff0c\u4f8b\u5982\u91cf\u5b50\u70b9\uff08QD\uff09\uff0c\u91cf\u5b50\u73af\uff08QRs\uff09\u548c\u7eb3\u7c73\u7ebf\uff08NW\uff09\uff0c\u4e3a\u4e86\u6539\u5584\u5b83\u4eec\u7684\u7269\u7406\u6027\u8d28\u548c\u5668\u4ef6\u5e94\u7528\uff0c\u5728\u7eb3\u7c73\u6280\u672f\u4e2d\u9700\u8981\u5236\u9020\u5177\u6709\u5747\u5300\u5c3a\u5bf8\uff0c\u9002\u5f53\u5f62\u72b6\u548c\u89c4\u5219\u4f4d\u7f6e\u7684\u7eb3\u7c73\u7ed3\u6784\u3002\u56e0\u6b64\uff0c\u7814\u7a76\u7eb3\u7c73\u7ed3\u6784\u7684\u751f\u957f\u8fc7\u7a0b\u5bf9\u4e8e\u7075\u6d3b\u63a7\u5236\u7eb3\u7c73\u7ed3\u6784\u7684\u81ea\u7ec4\u88c5\u548c\u5408\u6210\u8fc7\u7a0b\u975e\u5e38\u91cd\u8981\u3002\u70ed\u529b\u5b66\u7406\u8bba\u4f5c\u4e3a\u7814\u7a76\u6750\u6599\u751f\u957f\u7684\u901a\u7528\u65b9\u6cd5\u800c\u88ab\u7528\u4e8e\u7814\u7a76\u7eb3\u7c73\u7ed3\u6784\u7684\u751f\u957f\u3002<\/p>\n<p>Li\u7b49\u4eba\u7efc\u8ff0\u4e86\u7eb3\u7c73\u7ed3\u6784\u751f\u957f\u7684\u70ed\u529b\u5b66\u7406\u8bba\u5904\u7406\u3001\u5916\u5ef6\u751f\u957f\u7684QDs\u3001\u6db2\u6ef4\u5916\u5ef6\u751f\u957f\u7684QRs\uff0c\u4ee5\u53caVLS\u673a\u5236\u7684NWs\u7b49\u3002\u9996\u5148\uff0c\u4ed6\u4eec\u901a\u8fc7\u81ea\u7ec4\u88c5\u5916\u5ef6\u6280\u672f\u4ecb\u7ecd\u4e86\u91cf\u5b50\u70b9\u751f\u957f\u673a\u5236\u7684\u70ed\u529b\u5b66\u6a21\u578b\uff0c\u5e76\u8ba8\u8bba\u4e86\u91cf\u5b50\u70b9\u7684\u5f62\u6210\u3001\u7a33\u5b9a\u6027\u3001\u5f62\u72b6\u548c\u4f4d\u7f6e\u3002\u5176\u6b21\uff0c\u901a\u8fc7\u6db2\u6ef4\u5916\u5ef6\u4ecb\u7ecd\u4e86\u6210\u6838\u70ed\u529b\u5b66\u548cQRs\u7684\u751f\u957f\u52a8\u529b\u5b66\uff0c\u5e76\u63d0\u51fa\u4e86\u4e00\u79cd\u57fa\u4e8e\u52a8\u529b\u5b66\u6a21\u578b\u5e94\u7528QRs\u5f62\u72b6\u6f14\u5316\u7684\u6a21\u62df\u65b9\u6cd5\u3002\u63a5\u7740\uff0c\u5f15\u5165\u4e86\u51e0\u79cd\u7406\u8bba\u5de5\u5177\u6765\u89e3\u51b3VLS\u8fc7\u7a0b\u4e2dNW\u7684\u6210\u6838\u548c\u751f\u957f\u3002\u6700\u540e\uff0c\u4ecb\u7ecd\u4e86\u70ed\u529b\u5b66\u5904\u7406\uff0c\u5305\u62ec\u5728\u7eb3\u7c73\u7ed3\u6784\u7684\u6e29\u5ea6\u4f9d\u8d56\u6027\u751f\u957f\u7684\u7edf\u8ba1\u673a\u68b0\u548c\u91cf\u5b50\u529b\u5b66\u6a21\u578b\u80cc\u666f\u4e0b\u7684\u70ed\u6ce2\u52a8\u7b49\u3002<\/p>\n<p>\u56fe8 \uff08a\uff09Ga\u548cAs\u539f\u5b50\u7684\u52a8\u529b\u5b66\u6269\u6563\uff0c\uff08b\uff09\u5177\u6709As\u73af\u5883\u7684Ga\u6db2\u6ef4\u7684\u7ed3\u6676\u8fc7\u7a0b<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-158713 size-full aligncenter\" src=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72479-3.png\" alt=\"\" width=\"571\" height=\"835\" srcset=\"\/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72479-3.png 571w, \/\/m.iemloyee.com\/wp-content\/uploads\/2018\/11\/\u56fe\u72479-3-205x300.png 205w\" sizes=\"(max-width: 571px) 100vw, 571px\" \/>Moriarty P\uff0cNanostructured materials. Rep Prog Phys 2001\uff0c64:297\u2013381<\/p>\n<p>\u6587\u732e\u94fe\u63a5\uff1a<a href=\"http:\/\/iopscience.iop.org\/0034-4885\/64\/3\/201\"><u>http:\/\/iopscience.iop.org\/0034-4885\/64\/3\/201<\/u><\/a><\/p>\n<p>L. Li, C.X. Wang, G.W. Yang\uff0cThermodynamic theory of growthof nanostructures\uff0cProgress in Materials Science 64 (2014) 121\u2013199<\/p>\n<p>\u6587\u732e\u94fe\u63a5\uff1a<a href=\"http:\/\/dx.doi.org\/10.1016\/j.pmatsci.2014.03.002\"><u>http:\/\/dx.doi.org\/10.1016\/j.pmatsci.2014.03.002<\/u><\/a><\/p>\n<p>\u672c\u6587\u7531\u6750\u6599\u4eba\u79d1\u6280\u987e\u95ee\u5f20\u535a\u58eb\u4f9b\u7a3f\uff0c\u6750\u6599\u4eba\u7f16\u8f91\u90e8\u7f16\u8f91\u3002<\/p>\n<p>\u6295\u7a3f\u4ee5\u53ca\u5185\u5bb9\u5408\u4f5c\u53ef\u52a0\u7f16\u8f91\u5fae\u4fe1\uff1acailiaorenvip\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","protected":false},"excerpt":{"rendered":"<p>\u5728\u5f53\u4eca\u6750\u6599\u79d1\u5b66\u7684\u7814\u7a76\u548c\u53d1\u5c55\u4e2d\uff0c\u57fa\u4e8e\u70ed\u529b\u5b66\u7684\u63a2\u7d22\u5df2\u7ecf\u975e\u5e38\u5e7f\u6cdb\uff0c\u5176\u4e2d\uff0c\u6709\u4e9b\u662f\u4ece\u8ba1\u7b97\u6a21\u62df\u7684\u89d2\u5ea6\u5f00\u53d1\u548c\u6539\u5584\u6750\u6599\uff0c\u6709\u4e9b\u662f\u5bf9\u4ee5\u524d\u7684\u7406\u8bba\u6216\u8ba1\u7b97\u6a21\u578b\u7684\u4fee\u6b63\uff0c\u6709\u4e9b\u5219\u662f\u5bf9\u7406\u8bba\u672c\u8eab\u7684&#8230;<\/p>\n","protected":false},"author":10213,"featured_media":0,"comment_status":"open","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[2810,2],"tags":[],"class_list":["post-158689","post","type-post","status-publish","format-standard","hentry","category-huizong","category-keji"],"_links":{"self":[{"href":"\/\/m.iemloyee.com\/index.php?rest_route=\/wp\/v2\/posts\/158689"}],"collection":[{"href":"\/\/m.iemloyee.com\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"\/\/m.iemloyee.com\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"\/\/m.iemloyee.com\/index.php?rest_route=\/wp\/v2\/users\/10213"}],"replies":[{"embeddable":true,"href":"\/\/m.iemloyee.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=158689"}],"version-history":[{"count":5,"href":"\/\/m.iemloyee.com\/index.php?rest_route=\/wp\/v2\/posts\/158689\/revisions"}],"predecessor-version":[{"id":158822,"href":"\/\/m.iemloyee.com\/index.php?rest_route=\/wp\/v2\/posts\/158689\/revisions\/158822"}],"wp:attachment":[{"href":"\/\/m.iemloyee.com\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=158689"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"\/\/m.iemloyee.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=158689"},{"taxonomy":"post_tag","embeddable":true,"href":"\/\/m.iemloyee.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=158689"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}