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scpchaos
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·Ç³£¸Ðл»Ø¸´~~ ²»ÖªµÀÊÇ·ñ¿ÉÒÔÕâôÈÏΪ£º¿ÉÒÔͨ¹ýcharged slab À´ÒýÈëhole£¬µ«ÊÇÕâÑù¼ÆËã³öÀ´µÄÄÜÁ¿ÊDz»¶ÔµÄ£¬ÐèÒªcorrection£¿ Èç¹ûÊÇÕâÑùµÄ»°£¬ÄÇ֮ǰÌáµ½µÄÄÇÆªËãco2- ÔÚtio2ÉÏ£¬²¢Ã»ÓÐcorrection£¬ÊDz»ÊÇÈÏΪÕâÑù¼ÆËãµÃµ½µÄ½á¹û²»×¼È·ÄØ£¿ J. Phys. Chem. C 2010, 114, 21474¨C21481 ÔÚVASP µÄFAQÀïÓÐÕâÑùÒ»¶Î: Q:I adsorb, an ionic species e.g. O$ ^-$ on an insulating surface. To select a specific charge state, I have increased the number of electrons by one compared to the neutral system. Now, I have no clue how to evalute the total energy properly (i.e. are there convergence corrections). A:Actually, you MUST NOT set the number of electrons manually for a slab calculation. I.e., when you calculate the slab-O$ ^-$ system you are not allowed to select a specific charge state for the oxygen ion, by increasing the number of electrons manually. Specific charge state calculations make sense only in 3D systems and for cluster calculations. If you conduct the calculations properly, i.e. if your slab is large enough and the lateral dimension (x,y) of your surface is large enough the energy should converge to the proper value, i.e. the O should acquire the correct charge state automatically. Reason: If you set the number of electrons in the INCAR file for a slab calculation you end up with a charged slab. The electrostatic energy of such a slab is however only conditionally convergent and worse, in practice, even infinite (BASIC, BASIC ELECTROSTATICS). Therefore, no method whatsoever exists to correct the error in the electrostatic energy. E.g. the energy converges towards infinity, when the vacuum width is increased. You can try to validate this, by simply increasing the vacuum width in VASP for a charged slab. You will find that the energy increases or decreases linearly with the vacuum width. Well, there is maybe one method that can surmount the aforementioned problem. You can charge the slab and increase systematically the distance between the O- species (by increasing the lateral dimensions of your supercell) at a fixed vacuum width, and finally extrapolate the energies towards infinite lateral distances. The energy should converge towards the correct value as 1/$ d$, where $ d$ is the distance between the adsorbed species. This might yield a converged value. The point is that, as I mentioned above, the electrostatic energy is only conditionally convergent for the case of a charged slab/system, and results depend on how you evaluate the limit towards infinity. However, to the best of my knowledge, this has not been done or attempted hereto (and therefore we can not assist you on that issue). ÕâÑùµÄ»°£¬Èç¹ûÎÒÖ»ÊÇÒª¼ÆËãAu/TiO2 ÖеÄcharge transferÓ¦¸Ã¿ÉÒÔ£¬µ«ÊÇÈç¹ûÔÚ¹â´ß»¯Ï£¬»¹ÓÐʲô·½·¨¿ÉÒÔ¼ÓÈëelectron ºÍhole ÄØ£¿ лл£¡ |
3Â¥2014-01-17 04:05:35
gump_813
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scpchaos: ½ð±Ò+10, ¡ï¡ï¡ïºÜÓаïÖú 2014-01-17 04:06:11
sunyang1988: ½ð±Ò+2, лл½»Á÷ 2014-01-17 13:54:41
scpchaos: ½ð±Ò+20, ¡ï¡ï¡ï¡ï¡ï×î¼Ñ´ð°¸ 2014-01-18 07:50:03
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scpchaos: ½ð±Ò+10, ¡ï¡ï¡ïºÜÓаïÖú 2014-01-17 04:06:11
sunyang1988: ½ð±Ò+2, лл½»Á÷ 2014-01-17 13:54:41
scpchaos: ½ð±Ò+20, ¡ï¡ï¡ï¡ï¡ï×î¼Ñ´ð°¸ 2014-01-18 07:50:03
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Ö»ÊÇ˵vaspÀïÃæÃ»Óз½·¨ÐÞÕýÄÜÁ¿charged slabµÃÄÜÁ¿ ÓÐЩÆäËû·½·¨¿ÉÒ﵀ µ«ÊǶ¼±È½ÏÄÑŪ ÐèÒª±È½ÏºÃµÄÀíÂۺͱà³Ì»ù´¡ Â¥Ö÷¿ÉÒÔ¿´¿´ÕâÁ½Æ¬ÎÄÕ£º PRL 102 016402 PRL 110 095505 ÓÈÆäµÚ¶þƪ½²Á˱íÃæµÄµçºÉÐÞÕý »¹ÓÐÒ»ÖÖ·½·¨¾ÍÊÇÓÃcluster model ûÓÐÖÜÆÚÐԱ߽çÌõ¼þµÄ ËùÒÔ¿ÉÒÔËæ±ã¼Ócharge µ«ÊÇvasp×ö²»ÁË ÏñFHI-aims bigdftÖ®ÀàµÄ¿ÉÒÔ ÓÃcluster modelµÄÎÊÌâ¾ÍÊDZ߽çÉϵÄÔ×ÓµÄÐÔÖʺͱíÃæÉϵÄÊDz»Ò»ÑùµÄ Ò²»áÔì³ÉºÜ¶àÎÊÌâ |
2Â¥2014-01-17 00:54:42
gump_813
½ð³æ (СÓÐÃûÆø)
- Ó¦Öú: 36 (СѧÉú)
- ½ð±Ò: 944.6
- ºì»¨: 4
- Ìû×Ó: 112
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¡ï ¡ï
sunyang1988: ½ð±Ò+2, лл½»Á÷ 2014-01-17 13:54:53
sunyang1988: ½ð±Ò+2, лл½»Á÷ 2014-01-17 13:54:53
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4Â¥2014-01-17 05:54:58
gump_813
½ð³æ (СÓÐÃûÆø)
- Ó¦Öú: 36 (СѧÉú)
- ½ð±Ò: 944.6
- ºì»¨: 4
- Ìû×Ó: 112
- ÔÚÏß: 60.3Сʱ
- ³æºÅ: 472700
- ×¢²á: 2007-12-04
- רҵ: ½ðÊô²ÄÁϵĺϽðÏà¡¢Ïà±ä¼°
5Â¥2014-01-17 05:58:16













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