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16Â¥2012-12-04 16:53:22
dfjk-123
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2Â¥2012-11-24 19:13:05
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3Â¥2012-11-25 10:04:22
dfjk-123
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ÎÒÊÇÈ¡µÄenergy without entropyºóÃæµÄÄÜÁ¿¡£ÎÒÓÖ²âÊÔÁËÏ£¬½«Á½¸ö²âÊÔµÄNBANDSÊýÉèÖÃΪһÑù£¬¼ÆËã³öµÄ½á¹û»ù±¾Éϲ¶àÁË¡£ÎÒÈÏΪ»¹ÊÇNBANDSµÄÔÒò¡£µ«ÊÇ£¬INCARÎļþûÓÐÉèÖÃNBANDSÊýʱ£¬Í¬ÑùµÄVASP°æ±¾£¬ÔÚ²»Í¬»úÆ÷ÉÏÈ´¸øµÄ²»Ò»Ñù£¬ÕâÊÇΪʲô£¿ ÁíÍ⣬×ÊÔ´ÓÐÏÞ£¬ÎÒµÄ×÷ÒµÐèҪʹÓÃÁ½¸ö»úÆ÷×ö¼ÆË㣬Èç¹ûµÃ³öµÄÄÜÁ¿²î±ðÈç´Ë´ó£¬ÄÇËã³öÀ´µÄÏà¶ÔÄÜÁ¿»¹ÄÜ׼ȷÂð£¿Ó¦¸ÃÏàÐÅÄÄÒ»¸ö£¿ |
4Â¥2012-11-25 12:08:56
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5Â¥2012-11-25 20:37:33
dfjk-123
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ºÃµÄ£¬Ð»Ð»¡£»¹ÓиöÎÊÌâÏëÇë½ÌÏ£¬ÎÒÔÚOUTCARÖз¢ÏÖÁËÏÂÃæµÄ¾¯¸æ£º | | | W W AA RRRRR N N II N N GGGG !!! | | W W A A R R NN N II NN N G G !!! | | W W A A R R N N N II N N N G !!! | | W WW W AAAAAA RRRRR N N N II N N N G GGG ! | | WW WW A A R R N NN II N NN G G | | W W A A R R N N II N N GGGG !!! | | | | Your highest band is occupied at some k-points! Unless you are | | performing a calculation for an insulator or semiconductor, without | | unoccupied bands, you have included TOO FEW BANDS!! Please increase | | the parameter NBANDS in file 'INCAR' to ensure that the highest band | | is unoccupied at all k-points. It is always recommended to | | include a few unoccupied bands to accelerate the convergence of | | molecular dynamics runs (even for insulators or semiconductors). | | Because the presence of unoccupied bands improves wavefunction | | prediction, and helps to suppress 'band-crossings.' | | Following all k-points will be listed (with the Fermi weights of | | the highest band given in paranthesis) ... : | | | | 1 ( 0.12000) | | 2 ( 0.05967) | | 4 ( 1.07820) | | 5 ( 0.22570) | | 8 ( 0.19163) | | 9 ( 1.07400) | | 10 ( 1.19262) | | 11 ( 0.11518) | | 12 ( 0.13723) | | 13 ( 0.37150) | | | | The total occupancy of band no. 448 is 0.72092 electrons ... | | | Õâ¸öÐèÒªÔö´óNBANDSµ½¶àÉÙ°¡£¿°´ÕÕVASPµÄ˵Ã÷ÊֲᣬNBANDS = NELECT/2 + NIONS/2 (non-spinpolarized) Õâ¸öÖµÊÇ×ã¹»µÄ°¡£¬ÎªÊ²Ã´»áÓÐÕâÑùµÄ¾¯¸æ£¿ |
6Â¥2012-11-27 15:45:53
dfjk-123
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7Â¥2012-11-27 15:58:54
dfjk-123
гæ (СÓÐÃûÆø)
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- É¢½ð: 757
- Ìû×Ó: 119
- ÔÚÏß: 24.5Сʱ
- ³æºÅ: 665485
- ×¢²á: 2008-12-01
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10Â¥2012-11-28 08:39:37













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