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xiaomiwd

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[½»Á÷] È«¹ÌÌ¬ï®µç³ØÖе缫/µç½âÖʽçÃæ´¦µÄ¿Õ¼äµçºÉ²ã

È«¹ÌÌ¬ï®µç³ØÖÐÓùý¶É½ðÊôÑõ»¯Îï×öÕý¼«£¬Áò»¯Îï×öΪµç½âÖÊʱ£¬ÓÉÓÚLi+ÔÚÁ½ÖÖ²ÄÁÏÖÐµÄµç»¯Ñ§ÊÆ²»Í¬£¬»á³öÏÖÀàËÆÓÚµç×Óµ¼ÌåÖеÄpn½á£¬¼´Li+ÔÚµç½âÖÊ/µç¼«½çÃæ·Ö²¼Ëæ¿Õ¼ä·¢Éú±ä»¯£¬ÐγɿռäµçºÉ²ã£¬¿Õ¼äµçºÉ²ãµ¼Ö¸߽çÃæµç×裿ÕâÊÇÎÄÏ×ÖÐ˵µÄÔ­Òò£¬ÓÐûÓиßÊÖ˵һ˵ÕâÊÇʲôÒâ˼£¿Interfacial phenomena at the hetero-junction of ionic conductors are now categorized into ¡°nanoionics¡± [10],in which space-charge layer models for the hetero-junction between
ionic conductors are analogous to those at a semiconductor interface. The space-charge layers at the LiCoO2/electrolyte
interface will be largely developed as in the Schottky junction because of the electronic conduction in LiCoO2[11], which will
greatly suppress the ionic conduction at the interface. Therefore,we interposed thin buffer layers of oxides with ionic conduction
and electronic insulation, i.e. oxide solid electrolytes, between the LiCoO2 and the solid electrolyte. The interposition forms two interfaces: one between the
LiCoO2and the oxide solid electrolyte, and the other between the oxide and the sulfide electrolyte. The space-charge layers
will not be largely developed at both interfaces, because the former interface is between two oxides, between which the
electrochemical potential of lithium ions will not be largely different. The latter consists of electronic insulators, where the
space-charge layer will be less developed as atp¨Cnjunctions between semiconductors[11]. Therefore, we used Li4Ti5O12as the buffer layer material in our first study [5]
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  • 2013-11-12 13:58:31, 230.81 K

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xiaomiwd

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²¹ÉÏÈ«ÎÄ¡°Enhancement of the High-Rate Capability of Solid-State Lithium Batteries by Nanoscale Interfacial Modification¡±
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bbque2004

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xiaomiwd

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