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ÔÚJPCC 2007£¬111£¬18288£18293 ÕâÆªÎÄÕµĵÚËÄҳ̸µ½¹ØÓÚ¼Û´øVBºÍµ¼´øCBµÄ¼ÆËãʹÓÃÒ»¸ö¹«Ê½£º Evb£½X£E(e)+0.5Eg X is the electronegativity of the semiconductor, which is the geometric mean of the electronegativity of the constituent atoms. ¿´Á˰ëÌì²»ÖªµÀÕâ¸öXµ½µ×ÊÇʲôÒâ˼?ʲô½Ð°ëµ¼ÌåµÄµç¸ºÐÔ... »òÕß´óϺÓÐÆäËû·½·¨¼ÆËãµ¼ÌåµÄ¼Û´ø µ¼´ø(Âé·³¸øÒ»ÏÂÎÄÏ×),ллÁË [ Last edited by liuliu4411 on 2008-3-27 at 11:47 ] |
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lxtxgn
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3Â¥2008-03-27 08:56:04
lxtxgn
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X ×é³É°ëµ¼ÌåÔ×ӵļ¸ºÎƽ¾ùÊý ÁíÍ⣬ϣÍûÂ¥Ö÷¸øÖ¸Ê¾ һϠE£¨e£© ÊÇʲô¶«Î÷£¬ Ïë°ÑÕâ¸ö¹«Ê½¿´ÍêÕû |
2Â¥2008-03-27 08:51:32
liuliu4411
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where Evb the VB edge potential, X is the electronegativity of the semiconductor, which is the geometric mean of the electronegativity of the constituent atoms, E(e) is the energy of free electrons on the hydrogen scale (~4.5ev).Eg is the band gap energy of the semiconductor, and Ecb can be determined by ECB =EVB - Eg. The X values for BaTiO3 and Bi2O3 are ca. 5.242 and 5.986 eV, respectively. The calculated CB and VB edge potentials of BaTiO3 and Bi2O3 are shown in Figure 7. The CB edge potential of BaTiO3 (-0.83 eV) is more active than that of Bi2O3 (0.11 eV); hence, photoinduced electrons on the BaTiO3 particle surface transfer easily to Bi2O3 via interfaces; similarly, photoinduced holes on the Bi2O3 surface migrate to BaTiO3 owing to the different VB edge potentials. Bi µç¸ºÐÔÊÇ2.02ev OµÄµç¸ºÐÔÊÇ3.44ev ÔõôËã³öBi2O3µÄXÊÇ5.986evµÄ.... ¶øÇÒÆªÎÄÕ¼ÆËã³öÀ´µÄCB VB½á¹û¸úAmerican Mineralogist ,Volume 85,Pages 543-556,2000 ÉϼÆËã³öÀ´µÄCB VBÍêÈ«²»Ò»Ñù¡£¡£¡£¡£ [ Last edited by liuliu4411 on 2008-3-27 at 11:46 ] |

4Â¥2008-03-27 11:42:35
liuliu4411
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5Â¥2008-03-27 11:44:17













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